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| author | Roger Frank <rfrank@pglaf.org> | 2025-10-15 05:28:33 -0700 |
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| committer | Roger Frank <rfrank@pglaf.org> | 2025-10-15 05:28:33 -0700 |
| commit | 3a6de40b7e0ea6335d60c985c2d54d7b9f5afced (patch) | |
| tree | 0a0025aee62abb53d46650621e6877a8c5a0031d /6935-h | |
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diff --git a/6935-h/6935-h.htm b/6935-h/6935-h.htm new file mode 100644 index 0000000..8de6cb0 --- /dev/null +++ b/6935-h/6935-h.htm @@ -0,0 +1,10610 @@ +<?xml version="1.0" encoding="iso-8859-1"?> + +<!DOCTYPE html + PUBLIC "-//W3C//DTD XHTML 1.0 Strict//EN" + "http://www.w3.org/TR/xhtml1/DTD/xhtml1-strict.dtd" > + +<html xmlns="http://www.w3.org/1999/xhtml"> + <head> + <title> + The Project Gutenberg eBook of The Radio Amateur's Hand Book, by A. + Frederick Collins + </title> + </head> + <body> + <h1> + The Project Gutenberg eBook of The Radio Amateur's Hand Book, by A. + Frederick Collins + </h1> +<pre xml:space="preserve"> +Copyright laws are changing all over the world. Be sure to check the +copyright laws for your country before downloading or redistributing +this or any other Project Gutenberg eBook. + +This header should be the first thing seen when viewing this Project +Gutenberg file. Please do not remove it. Do not change or edit the +header without written permission. + +Please read the "legal small print," and other information about the +eBook and Project Gutenberg at the bottom of this file. Included is +important information about your specific rights and restrictions in +how the file may be used. You can also find out about how to make a +donation to Project Gutenberg, and how to get involved. + + +**Welcome To The World of Free Plain Vanilla Electronic Texts** + +**eBooks Readable By Both Humans and By Computers, Since 1971** + +*****These eBooks Were Prepared By Thousands of Volunteers!***** + + +Title: The Radio Amateur's Hand Book + +Author: A. Frederick Collins + +Release Date: November, 2004 [EBook #6935] +[This file was first posted on February 13, 2003] + +Edition: 10a + +Language: English + +Character set encoding: iso-8859-1 + +*** START OF THE PROJECT GUTENBERG EBOOK, THE RADIO AMATEUR'S HAND BOOK *** + + + + +Produced by Alan Millar and the Online Distributed Proofreading Team. + + + +</pre> + <p> + <b>THE RADIO AMATEUR'S HAND BOOK</b> + </p> + <table cellspacing="20" summary="Illustration"> + <tr> + <td align="center"> + <i>Photograph unavailable</i> + </td> + </tr> + <tr> + <td align="center"> + A. Frederick Collins, Inventor of the Wireless Telephone, 1899. + Awarded Gold Medal for same, Alaska Yukon Pacific Exposition, 1909. + </td> + </tr> + </table> + <hr /> + <h1> + THE RADIO AMATEUR'S HAND BOOK + </h1> + <p> + <i>A Complete, Authentic and Informative Work on Wireless Telegraphy and + Telephony</i> + </p> + <p> + BY<br /> FREDERICK COLLINS + </p> + <p> + Inventor of the Wireless Telephone 1899; Historian of Wireless 1901-1910; + Author of "Wireless Telegraphy" 1905 + </p> + <p> + 1922 + </p> + <hr /> + <p> + TO<br /> WILLIAM MARCONI<br /> INVENTOR OF THE WIRELESS TELEGRAPH + </p> + <hr /> + <h2> + <a name="intro" id="intro">INTRODUCTION</a> + </h2> + <p> + Before delving into the mysteries of receiving and sending messages + without wires, a word as to the history of the art and its present day + applications may be of service. While popular interest in the subject has + gone forward by leaps and bounds within the last two or three years, it + has been a matter of scientific experiment for more than a quarter of a + century. + </p> + <p> + The wireless telegraph was invented by William Marconi, at Bologna, Italy, + in 1896, and in his first experiments he sent dot and dash signals to a + distance of 200 or 300 feet. The wireless telephone was invented by the + author of this book at Narberth, Penn., in 1899, and in his first + experiments the human voice was transmitted to a distance of three blocks. + </p> + <p> + The first vital experiments that led up to the invention of the wireless + telegraph were made by Heinrich Hertz, of Germany, in 1888 when he showed + that the spark of an induction coil set up electric oscillations in an + open circuit, and that the energy of these waves was, in turn, sent out in + the form of electric waves. He also showed how they could be received at a + distance by means of a ring detector, which he called a <i>resonator</i>. + </p> + <p> + In 1890, Edward Branly, of France, showed that metal filings in a tube + cohered when electric waves acted on them, and this device he termed a <i>radio + conductor</i>; this was improved upon by Sir Oliver Lodge, who called it a + coherer. In 1895, Alexander Popoff, of Russia, constructed a receiving set + for the study of atmospheric electricity, and this arrangement was the + earliest on record of the use of a detector connected with an aerial and + the earth. + </p> + <p> + Marconi was the first to connect an aerial to one side of a spark gap and + a ground to the other side of it. He used an induction coil to energize + the spark gap, and a telegraph key in the primary circuit to break up the + current into signals. Adding a Morse register, which printed the dot and + dash messages on a tape, to the Popoff receptor he produced the first + system for sending and receiving wireless telegraph messages. + </p> + <table cellspacing="20" summary="Illustration"> + <tr> + <td align="center"> + <i>Photograph unavailable</i> + </td> + </tr> + <tr> + <td align="center"> + Collins' Wireless Telephone Exhibited at the Madison Square Garden, + October 1908. + </td> + </tr> + </table> + <p> + After Marconi had shown the world how to telegraph without connecting + wires it would seem, on first thought, to be an easy matter to telephone + without wires, but not so, for the electric spark sets up damped and + periodic oscillations and these cannot be used for transmitting speech. + Instead, the oscillations must be of constant amplitude and continuous. + That a direct current arc light transforms a part of its energy into + electric oscillations was shown by Firth and Rogers, of England, in 1893. + </p> + <p> + The author was the first to connect an arc lamp with an aerial and a + ground, and to use a microphone transmitter to modulate the sustained + oscillations so set up. The receiving apparatus consisted of a variable + contact, known as a <i>pill-box</i> detector, which Sir Oliver Lodge had + devised, and to this was connected an Ericsson telephone receiver, then + the most sensitive made. A later improvement for setting up sustained + oscillations was the author's <i>rotating oscillation arc.</i> + </p> + <p> + Since those memorable days of more than two decades ago, wonderful + advances have been made in both of these methods of transmitting + intelligence, and the end is as yet nowhere in sight. Twelve or fifteen + years ago the boys began to get fun out of listening-in to what the ship + and shore stations were sending and, further, they began to do a little + sending on their own account. These youngsters, who caused the + professional operators many a pang, were the first wireless amateurs, and + among them experts were developed who are foremost in the practice of the + art today. + </p> + <p> + Away back there, the spark coil and the arc lamp were the only known means + for setting up oscillations at the sending end, while the electrolytic and + crystal detectors were the only available means for the amateur to receive + them. As it was next to impossible for a boy to get a current having a + high enough voltage for operating an oscillation arc lamp, wireless + telephony was out of the question for him, so he had to stick to the spark + coil transmitter which needed only a battery current to energize it, and + this, of course, limited him to sending Morse signals. As the electrolytic + detector was cumbersome and required a liquid, the crystal detector which + came into being shortly after was just as sensitive and soon displaced the + former, even as this had displaced the coherer. + </p> + <p> + A few years ahead of these amateurs, that is to say in 1905, J. A. + Fleming, of England, invented the vacuum tube detector, but ten more years + elapsed before it was perfected to a point where it could compete with the + crystal detector. Then its use became general and workers everywhere + sought to, and did improve it. Further, they found that the vacuum tube + would not only act as a detector, but that if energized by a direct + current of high voltage it would set up sustained oscillations like the + arc lamp, and the value of sustained oscillations for wireless telegraphy + as well as wireless telephony had already been discovered. + </p> + <p> + The fact that the vacuum tube oscillator requires no adjustment of its + elements, that its initial cost is much less than the oscillation arc, + besides other considerations, is the reason that it popularized wireless + telephony; and because continuous waves have many advantages over periodic + oscillations is the reason the vacuum tube oscillator is replacing the + spark coil as a wireless telegraph transmitter. Moreover, by using a + number of large tubes in parallel, powerful oscillations can be set up + and, hence, the waves sent out are radiated to enormous distances. + </p> + <p> + While oscillator tubes were being experimented with in the research + laboratories of the General Electric, the Westinghouse, the Radio + Corporation of America, and other big companies, all the youthful amateurs + in the country had learned that by using a vacuum tube as a detector they + could easily get messages 500 miles away. The use of these tubes as + amplifiers also made it possible to employ a loud speaker, so that a room, + a hall, or an out-of-door audience could hear clearly and distinctly + everything that was being sent out. + </p> + <p> + The boy amateur had only to let father or mother listen-in, and they were + duly impressed when he told them they were getting it from KDKA (the + Pittsburgh station of the Westinghouse Co.), for was not Pittsburgh 500 + miles away! And so they, too, became enthusiastic wireless amateurs. This + new interest of the grown-ups was at once met not only by the + manufacturers of apparatus with complete receiving and sending sets, but + also by the big companies which began broadcasting regular programs + consisting of music and talks on all sorts of interesting subjects. + </p> + <p> + This is the wireless, or radio, as the average amateur knows it today. But + it is by no means the limit of its possibilities. On the contrary, we are + just beginning to realize what it may mean to the human race. The + Government is now utilizing it to send out weather, crop and market + reports. Foreign trade conditions are being reported. The Naval + Observatory at Arlington is wirelessing time signals. + </p> + <p> + Department stores are beginning to issue programs and advertise by radio! + Cities are also taking up such programs, and they will doubtless be + included soon among the regular privileges of the tax-payers. Politicians + address their constituents. Preachers reach the stay-at-homes. Great + singers thrill thousands instead of hundreds. Soon it will be possible to + hear the finest musical programs, entertainers, and orators, without + budging from one's easy chair. + </p> + <p> + In the World War wireless proved of inestimable value. Airplanes, instead + of flying aimlessly, kept in constant touch with headquarters. Bodies of + troops moved alertly and intelligently. Ships at sea talked freely, over + hundreds of miles. Scouts reported. Everywhere its invisible aid was + invoked. + </p> + <p> + In time of peace, however, it has proved and will prove the greatest + servant of mankind. Wireless messages now go daily from continent to + continent, and soon will go around the world with the same facility. Ships + in distress at sea can summon aid. Vessels everywhere get the day's news, + even to baseball scores. Daily new tasks are being assigned this tireless, + wireless messenger. + </p> + <p> + Messages have been sent and received by moving trains, the Lackawanna and + the Rock Island railroads being pioneers in this field. Messages have also + been received by automobiles, and one inventor has successfully + demonstrated a motor car controlled entirely by wireless. This method of + communication is being employed more and more by newspapers. It is also of + great service in reporting forest fires. + </p> + <p> + Colleges are beginning to take up the subject, some of the first being + Tufts College, Hunter College, Princeton, Yale, Harvard, and Columbia, + which have regularly organized departments for students in wireless. + </p> + <p> + Instead of the unwieldy and formidable looking apparatus of a short time + ago, experimenters are now vying with each other in making small or novel + equipment. Portable sets of all sorts are being fashioned, from one which + will go into an ordinary suitcase, to one so small it will easily slip + into a Brownie camera. One receiver depicted in a newspaper was one inch + square! Another was a ring for the finger, with a setting one inch by + five-eighths of an inch, and an umbrella as a "ground." Walking sets with + receivers fastened to one's belt are also common. Daily new novelties and + marvels are announced. + </p> + <p> + Meanwhile, the radio amateur to whom this book is addressed may have his + share in the joys of wireless. To get all of these good things out of the + ether one does not need a rod or a gun--only a copper wire made fast at + either end and a receiving set of some kind. If you are a sheer beginner, + then you must be very careful in buying your apparatus, for since the + great wave of popularity has washed wireless into the hearts of the + people, numerous companies have sprung up and some of these are selling + the veriest kinds of junk. + </p> + <p> + And how, you may ask, are you going to be able to know the good from the + indifferent and bad sets? By buying a make of a firm with an established + reputation. I have given a few offhand at the end of this book. Obviously + there are many others of merit--so many, indeed, that it would be quite + impossible to get them all in such a list, but these will serve as a guide + until you can choose intelligently for yourself. + </p> + <p> + F. C. + </p> + <hr /> + <h2> + <a name="contents" id="contents">CONTENTS</a> + </h2> + <p> + <b>CHAPTER</b> + </p> + <h3> + <a href="#chap01">I. HOW TO BEGIN WIRELESS</a> + </h3> + <p> + Kinds of Wireless Systems--Parts of a Wireless System--The Easiest Way to + Start--About Aerial Wire Systems--About the Receiving Apparatus--About + Transmitting Stations--Kinds of Transmitters--The Spark Gap Wireless + Telegraph Transmitter--The Vacuum Table Telegraph Transmitter--The + Wireless Telephone Transmitter. + </p> + <h3> + <a href="#chap02">II. PUTTING UP YOUR AERIAL</a> + </h3> + <p> + Kinds of Aerial Wire Systems--How to Put Up a Cheap Receiving Aerial--A + Two-wire Aerial--Connecting in the Ground--How to Put up a Good Aerial--An + Inexpensive Good Aerial--The Best Aerial That Can be Made--Assembling the + Aerial--Making a Good Ground. + </p> + <h3> + <a href="#chap03">III. SIMPLE TELEGRAPH AND TELEPHONE RECEIVING SETS</a> + </h3> + <p> + Assembled Wireless Receiving Sets--Assembling Your Own Receiving Set--The + Crystal Detector--The Tuning Coil--The Loose Coupled Tuning Coil--Fixed + and Variable Condensers--About Telephone Receivers-- Connecting Up the + Parts--Receiving Set No. 2--Adjusting the No. 1 Set--The Tuning + Coil--Adjusting the No. 2 Set. + </p> + <h3> + <a href="#chap04">IV. SIMPLE TELEGRAPH SENDING SETS</a> + </h3> + <p> + A Cheap Transmitting Set (No. 1)--The Spark Coil--The Battery--The + Telegraph Key--The Spark Gap--The Tuning Coil--The High-tension + Condenser--A Better Transmitting Set (No. 2)--The Alternating Current + Transformer--The Wireless Key--The Spark Gap--The High-tension + Condenser--The Oscillation Transformer--Connecting Up the Apparatus--For + Direct Current--How to Adjust Your Transmitter. Turning With a Hot Wire + Ammeter--To Send Out a 200-meter Wave Length--The Use of the Aerial + Switch--Aerial Switch for a Complete Sending and Receiving Set--Connecting + in the Lightning Switch. + </p> + <h3> + <a href="#chap05">V. ELECTRICITY SIMPLY EXPLAINED</a> + </h3> + <p> + Electricity at Rest and in Motion--The Electric Current and its + Circuit--Current and the Ampere--Resistance and the Ohm--What Ohm's Law + Is--What the Watt and Kilowatt Are--Electromagnetic Induction--Mutual + Induction--High-frequency Currents--Constants of an Oscillation + Circuit--What Capacitance Is--What Inductance Is--What Resistance Is--The + Effect of Capacitance. + </p> + <h3> + <a href="#chap06">VI. HOW THE TRANSMITTING AND RECEIVING SETS WORK</a> + </h3> + <p> + How Transmitting Set No. 1 Works--The Battery and Spark Coil + Circuit--Changing the Primary Spark Coil Current Into Secondary + Currents--What Ratio of Transformation Means--The Secondary Spark Coil + Circuit--The Closed Oscillation Circuit--How Transmitting Set No. 2 + Works-With Alternating Current--With Direct Current--The Rotary Spark + Gap--The Quenched Spark Gap--The Oscillation Transformer--How Receiving + Set No. 1 Works--How Receiving Set No. 2 Works. + </p> + <h3> + <a href="#chap07">VII. MECHANICAL AND ELECTRICAL TUNING</a> + </h3> + <p> + Damped and Sustained Mechanical Vibrations--Damped and Sustained + Oscillations--About Mechanical Tuning--About Electric Tuning. + </p> + <h3> + <a href="#chap08">VIII. A SIMPLE VACUUM TUBE DETECTOR RECEIVING SET</a> + </h3> + <p> + Assembled Vacuum Tube Receiving Set--A Simple Vacuum Tube Receiving + Set--The Vacuum Tube Detector--Three Electrode Vacuum Tube Detector--The + Dry Cell and Storage Batteries--The Filament Rheostat--Assembling the + Parts--Connecting Up the Parts--Adjusting the Vacuum Tube Detector + Receiving Set. + </p> + <h3> + <a href="#chap09">IX. VACUUM TUBE AMPLIFIER RECEIVING SETS</a> + </h3> + <p> + A Grid Leak Amplifier Receiving Set. With Crystal Detector--The Fixed + Resistance Unit, or Grid Leak--Assembling the Parts for a Crystal Detector + Set--Connecting up the Parts for a Crystal Detector--A Grid Leak + Amplifying Receiving Set With Vacuum Tube Detector--A Radio Frequency + Transformer Amplifying Receiving Set--An Audio Frequency Transformer + Amplifying Receiving Set--A Six Step Amplifier Receiving Set with a Loop + Aerial--How to Prevent Howling. + </p> + <h3> + <a href="#chap10">X. REGENERATIVE AMPLIFICATION RECEIVING SETS</a> + </h3> + <p> + The Simplest Type of Regenerative Receiving Set--With Loose Coupled Tuning + Coil--Connecting Up the Parts--An Efficient Regenerative Receiving Set. + With Three Coil Loose Coupler--The A Battery Potentiometer--The Parts and + How to Connect Them Up--A Regenerative Audio Frequency Amplifier--The + Parts and How to Connect Them Up. + </p> + <h3> + <a href="#chap11">XI. SHORT WAVE REGENERATIVE RECEIVING SETS</a> + </h3> + <p> + A Short Wave Regenerative Receiver, with One Variometer and Three Variable + Condensers--The Variocoupler--The Variometer--Connecting Up the + Parts--Short Wave Regenerative Receiver with Two Variometers and Two + Variable Condensers--The Parts and How to Connect Them Up. + </p> + <h3> + <a href="#chap12">XII. INTERMEDIATE AND LONG WAVE REGENERATIVE RECEIVING + SETS</a> + </h3> + <p> + Intermediate Wave Receiving Sets--Intermediate Wave Set With Loading + Coils--The Parts and How to Connect Them Up--An Intermediate Wave Set with + Variocoupler Inductance Coils--The Parts and How to Connect Them Up--A + Long Wave Receiving Set--The Parts and How to Connect Them Up. + </p> + <h3> + <a href="#chap13">XIII. HETERODYNE OR BEAT LONG WAVE TELEGRAPH RECEIVING + SET</a> + </h3> + <p> + What the Heterodyne or Beat Method Is--The Autodyne or Self-heterodyne + Long Wave Receiving Set--The Parts and Connections of an Autodyne or + Self-heterodyne, Receiving Set--The Separate Heterodyne Long Wave + Receiving Set--The Parts and Connections of a Separate Heterodyne Long + Wave Receiving Set. + </p> + <h3> + <a href="#chap14">XIV. HEADPHONES AND LOUD SPEAKERS</a> + </h3> + <p> + Wireless Headphones--How a Bell Telephone Receiver is Made--How a Wireless + Headphone is Made--About Resistance, Turns of Wire and Sensitivity of + Headphones--The Impedance of Headphones--How the Headphones Work--About + Loud Speakers--The Simplest Type of Loud Speaker--Another Simple Kind of + Loud Speaker--A Third Kind of Simple Loud Speaker--A Super Loud Speaker. + </p> + <h3> + <a href="#chap15">XV. OPERATION OF VACUUM TUBE RECEPTORS</a> + </h3> + <p> + What is Meant by Ionization--How Electrons are Separated from + Atoms--Action of the Two Electrode Vacuum Tube--How the Two Electrode Tube + Acts as a Detector--How the Three Electrode Tube Acts as a Detector--How + the Vacuum Tube Acts as an Amplifier--The Operation of a Simple Vacuum + Tube Receiving Set--Operation of a Regenerative Vacuum Tube Receiving + Set--Operation of Autodyne and Heterodyne Receiving Sets--The Autodyne, or + Self-Heterodyne Receiving Set--The Separate Heterodyne Receiving Set. + </p> + <h3> + <a href="#chap16">XVI. CONTINUOUS WAVE TELEGRAPH TRANSMITTING SETS WITH + DIRECT CURRENT</a> + </h3> + <p> + Sources of Current for Telegraph Transmitting Sets--An Experimental + Continuous Wave Telegraph Transmitter--The Apparatus You Need--The Tuning + Coil--The Condensers--The Aerial Ammeter--The Buzzer and Dry Cell--The + Telegraph Key--The Vacuum Tube Oscillator--The Storage Battery--The + Battery Rheostat--The Oscillation Choke Coil--Transmitter Connectors--The + Panel Cutout--Connecting Up the Transmitting Apparatus--A 100-mile C. W. + Telegraph Transmitter--The Apparatus You Need--The Tuning Coil--The Aerial + Condenser--The Aerial Ammeter--The Grid and Blocking Condensers--The Key + Circuit Apparatus--The 5 Watt Oscillator Vacuum Tube--The Storage Battery + and Rheostat--The Filament Voltmeter--The Oscillation Choke Coil--The + Motor-generator Set--The Panel Cut-out--The Protective + Condenser--Connecting Up the Transmitting Apparatus--A 200-mile C. W. + Telegraph Transmitter--A 500-mile C. W. Telegraph Transmitter--The + Apparatus and Connections-- The 50-watt Vacuum Tube Oscillator--The Aerial + Ammeter--The Grid Leak Resistance--The Oscillation Choke Coil--The + Filament Rheostat--The Filament Storage Battery--The Protective + Condenser--The Motor-generator--A 1000-mile C. W. Telegraph Transmitter. + </p> + <h3> + <a href="#chap17">XVII. CONTINUOUS WAVE TELEGRAPH TRANSMITTING SETS WITH + ALTERNATING CURRENT</a> + </h3> + <p> + A 100-mile C. W. Telegraph Transmitting Set--The Apparatus Required--The + Choke Coils--The Milli-ammeter--The A. C. Power Transformer--Connecting Up + the Apparatus--A 200- to 500-mile C. W. Telegraph Transmitting Set-A 500- + to 1000-mile C. W. Telegraph Transmitting Set--The Apparatus Required--The + Alternating Current Power Transformer-Connecting Up the Apparatus. + </p> + <h3> + <a href="#chap18">XVIII. WIRELESS TELEPHONE TRANSMITTING SETS WITH DIRECT + AND ALTERNATING CURRENTS</a> + </h3> + <p> + A Short Distance Wireless Telephone Transmitting Set--With 110-volt Direct + Lighting Current--The Apparatus You Need--The Microphone + Transmitter--Connecting Up the Apparatus--A 25- to 50-mile Wireless + Telephone Transmitter--With Direct Current Motor Generator--The Apparatus + You Need--The Telephone Induction Coil--The Microphone Transformer--The + Magnetic Modulator--How the Apparatus is Connected Up--A 50- to 100-mile + Wireless Telephone Transmitter--With Direct Current Motor Generator--The + Oscillation Choke Coil--The Plate and Grid Circuit Reactance + Coils--Connecting up the Apparatus--A 100- to 200-mile Wireless Telephone + Transmitter--With Direct Current Motor Generator--A 50- to 100-mile + Wireless Telephone Transmitting Set--With 100-volt Alternating + Current--The Apparatus You Need--The Vacuum Tube Rectifier--The Filter + Condensers--The Filter Reactance Coil-- Connecting Up the Apparatus--A + 100- to 200-mile Wireless Telephone Transmitting Set--With 110-volt + Alternating Current--Apparatus Required. + </p> + <h3> + <a href="#chap19">XIX. THE OPERATION OF VACUUM TUBE TRANSMITTERS</a> + </h3> + <p> + The Operation of the Vacuum Tube Oscillator--The Operation of C. W. + Telegraph Transmitters with Direct Current--Short Distance C. W. + Transmitter--The Operation of the Key Circuit--The Operation of C. W. + Telegraph Transmitting with Direct Current--The Operation of C. W. + Telegraph Transmitters with Alternating Current--With a Single Oscillator + Tube--Heating the Filament with Alternating Current--The Operation of C. + W. Telegraph Transmitters with Alternating Current-- With Two Oscillator + Tubes--The Operation of Wireless Telephone Transmitters with Direct + Current--Short Distance Transmitter--The Microphone Transmitter--The + Operation of Wireless Telephone Transmitters with Direct Current--Long + Distance Transmitters--The Operation of Microphone Modulators--The + Induction Coil--The Microphone Transformer--The Magnetic + Modulator--Operation of the Vacuum Tube as a Modulator--The Operation of + Wireless Telephone Transmitters with Alternating Current--The Operation of + Rectifier Vacuum Tubes--The Operation of Reactors and Condensers. + </p> + <h3> + <a href="#chap20">XX. HOW TO MAKE A RECEIVING SET FOR $5.00 OR LESS.</a> + </h3> + <p> + The Crystal Detector--The Tuning Coil--The Headphone--How to Mount the + Parts--The Condenser--How to Connect Up the Receptor. + </p> + <h3> + <a href="#appendix">APPENDIX</a> + </h3> + <p> + Useful Information--<a href="#glossary">Glossary</a>--<a href="#donts">Wireless + Don'ts</a>. + </p> + <h2> + LIST OF FIGURES + </h2> + <ul> + <li> + <a href="#fig001">Fig. 1.</a>--Simple Receiving Set + </li> + <li> + <a href="#fig001">Fig. 2.</a>--Simple Transmitting Set + </li> + <li> + <a href="#fig003">(A) Fig. 3.</a>--Flat Top, or Horizontal Aerial + </li> + <li> + <a href="#fig003">(B) Fig. 3.</a>--Inclined Aerial + </li> + <li> + <a href="#fig004">(A) Fig. 4.</a>--Inverted L Aerial + </li> + <li> + <a href="#fig004">(B) Fig. 4.</a>--T Aerial + </li> + <li> + <a href="#fig005">Fig. 5.</a>--Material for a Simple Aerial Wire System + </li> + <li> + <a href="#fig006a">(A) Fig. 6.</a>--Single Wire Aerial for Receiving + </li> + <li> + <a href="#fig006b">(B) Fig. 6.</a>--Receiving Aerial with Spark Gap + Lightning Arrester + </li> + <li> + <a href="#fig006c">(C) Fig. 6.</a>--Aerial with Lightning Switch + </li> + <li> + <a href="#fig007">Fig. 7.</a>--Two-wire Aerial + </li> + <li> + <a href="#fig008a">(A) Fig. 8.</a>--Part of a Good Aerial + </li> + <li> + <a href="#fig008b">(B) Fig. 8.</a>--The Spreaders + </li> + <li> + <a href="#fig009ab">(A) Fig. 9.</a>--The Middle Spreader + </li> + <li> + <a href="#fig009ab">(B) Fig. 9.</a>--One End of Aerial Complete + </li> + <li> + <a href="#fig009c">(C) Fig. 9.</a>--The Leading in Spreader + </li> + <li> + <a href="#fig010ab">(A) Fig. 10.</a>--Cross Section of Crystal Detector + </li> + <li> + <a href="#fig010ab">(B) Fig. 10.</a>--The Crystal Detector Complete + </li> + <li> + <a href="#fig011ab">(A) Fig. 11.</a>--Schematic Diagram of a Double + Slide Tuning Coil + </li> + <li> + <a href="#fig011ab">(B) Fig. 11.</a>--Double Slide Tuning Coil Complete + </li> + <li> + <a href="#fig012ab">(A) Fig. 12.</a>--Schematic Diagram of a Loose + Coupler + </li> + <li> + <a href="#fig012ab">(B) Fig. 12.</a>--Loose Coupler Complete + </li> + <li> + <a href="#fig013ab">(A) Fig. 13.</a>--How a Fixed Receiving Condenser is + Built up + </li> + <li> + <a href="#fig013ab">(B) Fig. 13.</a>--The Fixed Condenser Complete + </li> + <li> + <a href="#fig013cd">(C) and (D) Fig. 13.</a>--Variable Rotary Condenser + </li> + <li> + <a href="#fig014">Fig. 14.</a>--Pair of Wireless Headphones + </li> + <li> + <a href="#fig015a">(A) Fig. 15.</a>--Top View of Apparatus Layout for + Receiving Set No. 1 + </li> + <li> + <a href="#fig015b">(B) Fig. 15.</a>--Wiring Diagram for Receiving Set + No. 1 + </li> + <li> + <a href="#fig016a">(A) Fig. 16.</a>--Top View of Apparatus Layout for + Receiving Set No. 2 + </li> + <li> + <a href="#fig016b">(B) Fig. 16.</a>--Wiring Diagram for Receiving Set + No. 2 + </li> + <li> + <a href="#fig017">Fig. 17.</a>--Adjusting the Receiving Set + </li> + <li> + <a href="#fig018ab">(A) and (B) Fig. 18.</a>--Types of Spark Coils for + Set No. 1 + </li> + <li> + <a href="#fig018c">(C) Fig. 18.</a>--Wiring Diagram of Spark Coil + </li> + <li> + <a href="#fig019">Fig. 19.</a>--Other Parts for Transmitting Set No. 1 + </li> + <li> + <a href="#fig020a">(A) Fig. 20.</a>--Top View of Apparatus Layout for + Sending Set No. 1 + </li> + <li> + <a href="#fig020b">(B) Fig. 20.</a>--Wiring of Diagram for Sending Set + No. 1 + </li> + <li> + <a href="#fig021">Fig. 21.</a>--Parts for Transmitting Set No. 2 + </li> + <li> + <a href="#fig022a">(A) Fig. 22.</a>--Top View of Apparatus Layout for + Sending Set No. 2 + </li> + <li> + <a href="#fig022b">(B) Fig. 22.</a>--Wiring Diagram for Sending Set No. + 2 + </li> + <li> + <a href="#fig023">Fig. 23.</a>--Using a 110-volt Direct Current with an + Alternating current Transformer + </li> + <li> + <a href="#fig024">Fig. 24.</a>--Principle of the Hot Wire Ammeter + </li> + <li> + <a href="#fig025">Fig. 25.</a>--Kinds of Aerial Switches + </li> + <li> + <a href="#fig026">Fig. 26.</a>--Wiring Diagram for a Complete Sending + and Receiving Set No. 1 + </li> + <li> + <a href="#fig027">Fig. 27.</a>--Wiring Diagram for Complete Sending and + Receiving Set No. 2 + </li> + <li> + <a href="#fig028">Fig. 28.</a>--Water Analogue for Electric Pressure + </li> + <li> + <a href="#fig029">Fig. 29.</a>--Water Analogues for Direct and + Alternating Currents + </li> + <li> + <a href="#fig030">Fig. 30.</a>--How the Ammeter and Voltmeter are Used + </li> + <li> + <a href="#fig031">Fig. 31.</a>--Water Valve Analogue of Electric + Resistance + </li> + <li> + <a href="#fig032ab">(A) and (B) Fig. 32.</a>--How an Electric Current is + Changed into Magnetic Lines of Force and These into an Electric Current + </li> + <li> + <a href="#fig032cd">(C) and (D) Fig. 32.</a>--How an Electric Current + Sets up a Magnetic Field + </li> + <li> + <a href="#fig033">Fig. 33.</a>--The Effect of Resistance on the + Discharge of an Electric Current + </li> + <li> + <a href="#fig034">Fig. 34.</a>--Damped and Sustained Mechanical + Vibrations + </li> + <li> + <a href="#fig035">Fig. 35.</a>--Damped and Sustained Electric + Oscillations + </li> + <li> + <a href="#fig036">Fig. 36.</a>--Sound Wave and Electric Wave Tuned + Senders and Receptors + </li> + <li> + <a href="#fig037">Fig. 37.</a>--Two Electrode Vacuum Tube Detectors + </li> + <li> + <a href="#fig038">Fig. 38.</a>--Three Electrode Vacuum Tube Detector and + Battery Connections + </li> + <li> + <a href="#fig039">Fig. 39.</a>--A and B Batteries for Vacuum Tube + Detectors + </li> + <li> + <a href="#fig040">Fig. 40.</a>--Rheostat for the A or Storage-battery + Current + </li> + <li> + <a href="#fig041a">(A) Fig. 41.</a>--Top View of Apparatus Layout for + Vacuum Tube Detector Receiving Set + </li> + <li> + <a href="#fig041b">(B) Fig. 41.</a>--Wiring Diagram of a Simple Vacuum + Tube Receiving Set + </li> + <li> + <a href="#fig042">Fig. 42.</a>--Grid Leaks and How to Connect them Up + </li> + <li> + <a href="#fig043">Fig. 43.</a>--Crystal Detector Receiving Set with + Vacuum Tube Amplifier (Resistance Coupled) + </li> + <li> + <a href="#fig044a">(A) Fig. 44.</a>--Vacuum Tube Detector Receiving Set + with One Step Amplifier (Resistance Coupled) + </li> + <li> + <a href="#fig044b">(B) Fig. 44.</a>--Wiring Diagram for Using One A or + Storage Battery with an Amplifier and a Detector Tube + </li> + <li> + <a href="#fig045a">(A) Fig. 45.</a>--Wiring Diagram for Radio Frequency + Transformer Amplifying Receiving Set + </li> + <li> + <a href="#fig045b">(B) Fig. 45.</a>--Radio Frequency Transformer + </li> + <li> + <a href="#fig046a">(A) Fig. 46.</a>--Audio Frequency Transformer + </li> + <li> + <a href="#fig046b">(B) Fig. 46.</a>--Wiring Diagram for Audio Frequency + Transformer Amplifying Receiving Set. (With Vacuum Tube Detector and Two + Step Amplifier Tubes) + </li> + <li> + <a href="#fig047a">(A) Fig. 47.</a>--Six Step Amplifier with Loop Aerial + </li> + <li> + <a href="#fig047b">(B) Fig. 47.</a>--Efficient Regenerative Receiving + Set (With Three Coil Loose Coupler Tuner) + </li> + <li> + <a href="#fig048">Fig. 48.</a>--Simple Regenerative Receiving Set (With + Loose Coupler Tuner) + </li> + <li> + <a href="#fig049a">(A) Fig. 49.</a>--Diagram of Three Coil Loose Coupler + </li> + <li> + <a href="#fig049b">(B) Fig. 49.</a>--Three Coil Loose Coupler Tuner + </li> + <li> + <a href="#fig050">Fig. 50.</a>--Honeycomb Inductance Coil + </li> + <li> + <a href="#fig051a">Fig. 51.</a>--The Use of the Potentiometer + </li> + <li> + <a href="#fig052">Fig. 52.</a>--Regenerative Audio Frequency Amplifier + Receiving Set + </li> + <li> + <a href="#fig053">Fig. 53.</a>--How the Vario Coupler is Made and Works + </li> + <li> + <a href="#fig054">Fig. 54.</a>--How the Variometer is Made and Works + </li> + <li> + <a href="#fig055">Fig. 55.</a>--Short Wave Regenerative Receiving Set + (One Variometer and Three Variable Condensers) + </li> + <li> + <a href="#fig056">Fig. 56.</a>--Short Wave Regenerative Receiving Set + (Two Variometer and Two Variable Condensers) + </li> + <li> + <a href="#fig057">Fig. 57.</a>--Wiring Diagram Showing Fixed Loading + Coils for Intermediate Wave Set + </li> + <li> + <a href="#fig058">Fig. 58.</a>--Wiring Digram of Intermediate Wave + Receptor with One Vario Coupler and 12 Section Bank-wound Inductance + Coil + </li> + <li> + <a href="#fig059">Fig. 59.</a>--Wiring Diagram Showing Long Wave + Receptor with Vario Couplers and 8 Bank-wound Inductance Coils + </li> + <li> + <a href="#fig060">Fig. 60.</a>--Wiring Diagram of Long Wave Autodyne, or + Self-heterodyne Receptor (Compare with Fig. 77) + </li> + <li> + <a href="#fig061">Fig. 61.</a>--Wiring Diagram of Long Wave Separate + Heterodyne Receiving Set + </li> + <li> + <a href="#fig062">Fig. 62.</a>--Cross Section of Bell Telephone Receiver + </li> + <li> + <a href="#fig063">Fig. 63.</a>--Cross Section of Wireless Headphone + </li> + <li> + <a href="#fig064">Fig. 64.</a>--The Wireless Headphone + </li> + <li> + <a href="#fig065">Fig. 65.</a>--Arkay Loud Speaker + </li> + <li> + <a href="#fig066">Fig. 66.</a>--Amplitone Loud Speaker + </li> + <li> + <a href="#fig067">Fig. 67.</a>--Amplitron Loud Speaker + </li> + <li> + <a href="#fig068">Fig. 68.</a>--Magnavox Loud Speaker + </li> + <li> + <a href="#fig069">Fig. 69.</a>--Schematic Diagram of an Atom + </li> + <li> + <a href="#fig070">Fig. 70.</a>--Action of Two-electrode Vacuum Tube + </li> + <li> + <a href="#fig071ab">(A) and (B) Fig. 71.</a>--How a Two-electrode Tube + Acts as Relay or a Detector + </li> + <li> + <a href="#fig071c">(C) Fig. 71.</a>--Only the Positive Part of + Oscillations Goes through the Tube + </li> + <li> + <a href="#fig072ab">(A) and (B) Fig. 72.</a>--How the Positive and + Negative Voltages of the Oscillations Act on the Electrons + </li> + <li> + <a href="#fig072c">(C) Fig. 72.</a>--How the Three-electrode Tube Acts + as Detector and Amplifier + </li> + <li> + <a href="#fig072d">(D) Fig. 72.</a>--How the Oscillations Control the + Flow of the Battery Current through the Tube + </li> + <li> + <a href="#fig073">Fig. 73.</a>--How the Heterodyne Receptor Works + </li> + <li> + <a href="#fig074">Fig. 74.</a>--Separate Heterodyne Oscillator + </li> + <li> + <a href="#fig075a">(A) Fig. 75.</a>--Apparatus for Experimental C. W. + Telegraph Transmitter. + </li> + <li> + <a href="#fig075b">(B) Fig. 75.</a>--Apparatus for Experimental C. W. + Telegraph Transmitter. + </li> + <li> + <a href="#fig076">Fig. 76.</a>--Experimental C. W. Telegraph Transmitter + </li> + <li> + <a href="#fig077">Fig. 77.</a>--Apparatus of 100-mile C. W. Telegraph + Transmitter + </li> + <li> + <a href="#fig078">Fig. 78.</a>--5- to 50-watt C. W. Telegraph + Transmitter (with a Single Oscillation Tube) + </li> + <li> + <a href="#fig079">Fig. 79.</a>--200-mile C. W. Telegraph Transmitter + (with Two Tubes in Parallel) + </li> + <li> + <a href="#fig080">Fig. 80.</a>--50-watt Oscillator Vacuum Tube + </li> + <li> + <a href="#fig081">Fig. 81.</a>--Alternating Current Power Transformer + (for C. W. Telegraphy and Wireless Telephony) + </li> + <li> + <a href="#fig082">Fig. 82.</a>--Wiring Diagram for 200- to 500-mile C. + W. Telegraph Transmitting Set. (With Alternating Current.) + </li> + <li> + <a href="#fig083">Fig. 83.</a>--Wiring Diagram for 500- to 1000-mile C. + W. Telegraph Transmitter + </li> + <li> + <a href="#fig084">Fig. 84.</a>--Standard Microphone Transmitter + </li> + <li> + <a href="#fig085">Fig. 85.</a>--Wiring Diagram of Short Distance + Wireless Telephone Set. (Microphone in Aerial Wire.) + </li> + <li> + <a href="#fig086">Fig. 86.</a>--Telephone Induction Coil (used with + Microphone Transmitter). + </li> + <li> + <a href="#fig087">Fig. 87.</a>--Microphone Transformer Used with + Microphone Transmitter + </li> + <li> + <a href="#fig088">Fig. 88.</a>--Magnetic Modulator Used with Microphone + Transmitter + </li> + <li> + <a href="#fig089a">(A) Fig. 89.</a>--Wiring Diagram of 25--to 50-mile + Wireless Telephone. (Microphone Modulator Shunted Around Grid-leak + Condenser) + </li> + <li> + <a href="#fig089b">(B) Fig. 89.</a>--Microphone Modulator Connected in + Aerial Wire + </li> + <li> + <a href="#fig090">Fig. 90.</a>--Wiring Diagram of 50- to 100-mile + Wireless Telephone Transmitting Set + </li> + <li> + <a href="#fig091">Fig. 91.</a>--Plate and Grid Circuit Reactor + </li> + <li> + <a href="#fig092">Fig. 92.</a>--Filter Reactor for Smoothing Out + Rectified Currents + </li> + <li> + <a href="#fig093">Fig. 93.</a>--100- to 200-mile Wireless Telephone + Transmitter + </li> + <li> + <a href="#fig094ab">(A) and (B) Fig. 94.</a>--Operation of Vacuum Tube + Oscillators + </li> + <li> + <a href="#fig094c">(C) Fig. 94.</a>--How a Direct Current Sets up + Oscillations + </li> + <li> + <a href="#fig095">Fig. 95.</a>--Positive Voltage Only Sets up + Oscillations + </li> + <li> + <a href="#fig096">Fig. 96.</a>--Rasco Baby Crystal Detector + </li> + <li> + <a href="#fig097">Fig. 97.</a>--How the Tuning Coil is Made + </li> + <li> + <a href="#fig098">Fig. 98.</a>--Mesco loop-ohm Head Set + </li> + <li> + <a href="#fig099">Fig. 99.</a>--Schematic Layout of the $5.00 Receiving + Set + </li> + <li> + <a href="#fig100">Fig. 100.</a>--Wiring Diagram for the $5.00 Receiving + Set + </li> + </ul> + <h2> + LIST OF ILLUSTRATIONS + </h2> + <ul> + <li> + Frederick Collins, Inventor of the Wireless Telephone, 1899. Awarded + Gold Medal for same, Alaska Yukon Pacific Exposition, 1909 + </li> + <li> + Collins' Wireless Telephone Exhibited at the Madison Square Garden, + October, 1908 + </li> + <li> + General Pershing "Listening-in" + </li> + <li> + The World's Largest Radio Receiving Station. Owned by the Radio + Corporation of America at Rocky Point near Port Jefferson, L. I. + </li> + <li> + First Wireless College in the World, at Tufts College, Mass + </li> + <li> + Alexander Graham Bell, Inventor of the Telephone, now an ardent Radio + Enthusiast + </li> + <li> + World's Largest Loud Speaker ever made. Installed in Lytle Park, + Cincinnati, Ohio, to permit President Harding's Address at Point + Pleasant, Ohio, during the Grant Centenary Celebration to be heard + within a radius of one square + </li> + <li> + United States Naval High Power Station, Arlington, Va. General view of + Power Room. At the left can be seen the Control Switchboards, and + overhead, the great 30 K.W. Arc Transmitter with Accessories + </li> + <li> + The Transformer and Tuner of the World's Largest Radio Station. Owned by + the Radio Corporation of America at Rocky Point near Port Jefferson, L. + I. + </li> + <li> + Broadcasting Government Reports by Wireless from Washington. This shows + Mr. Gale at work with his set in the Post Office Department + </li> + <li> + Wireless Receptor, the size of a Safety Match Box. A Youthful Genius in + the person of Kenneth R. Hinman, who is only twelve years old, has made + a Wireless Receiving Set that fits neatly into a Safety Match Box. With + this Instrument and a Pair of Ordinary Receivers, he is able to catch + not only Code Messages but the regular Broadcasting Programs from + Stations Twenty and Thirty Miles Distant + </li> + <li> + Wireless Set made into a Ring, designed by Alfred G. Rinehart, of + Elizabeth, New Jersey. This little Receptor is a Practical Set; it will + receive Messages, Concerts, etc., measures 1" by 5/8" by 7/8". An + ordinary Umbrella is used as an Aerial + </li> + </ul> + <h2> + <a name="chap01" id="chap01">CHAPTER I</a> + </h2> + <h3> + HOW TO BEGIN WIRELESS + </h3> + <p> + In writing this book it is taken for granted that you are: <i>first</i>, + one of the several hundred thousand persons in the United States who are + interested in wireless telegraphy and telephony; <i>second</i>, that you + would like to install an apparatus in your home, and <i>third</i>, that it + is all new to you. + </p> + <p> + Now if you live in a city or town large enough to support an electrical + supply store, there you will find the necessary apparatus on sale, and + someone who can tell you what you want to know about it and how it works. + If you live away from the marts and hives of industry you can send to + various makers of wireless apparatus [Footnote: A list of makers of + wireless apparatus will be found in the <a href="#appendix">Appendix</a>.] + for their catalogues and price-lists and these will give you much useful + information. But in either case it is the better plan for you to know + before you start in to buy an outfit exactly what apparatus you need to + produce the result you have in mind, and this you can gain in easy steps + by reading this book. + </p> + <p> + <i>Kinds of Wireless Systems</i>.--There are two distinct kinds of + wireless systems and these are: the <i>wireless telegraph</i> system, and + the <i>wireless telephone</i> system. The difference between the wireless + telegraph and the wireless telephone is that the former transmits messages + by means of a <i>telegraph key</i>, and the latter transmits conversation + and music by means of a <i>microphone transmitter</i>. In other words, the + same difference exists between them in this respect as between the Morse + telegraph and the Bell telephone. + </p> + <p> + <i>Parts of a Wireless System</i>.--Every complete wireless station, + whether telegraph or telephone, consists of three chief separate and + distinct parts and these are: (<i>a</i>) the <i>aerial wire system</i>, or + <i>antenna</i> as it is often called, (<i>b</i>) the <i>transmitter</i>, + or <i>sender</i>, and (<i>c</i>) the <i>receiver</i>, or, more properly, + the <i>receptor</i>. The aerial wire is precisely the same for either + wireless telegraphy or wireless telephony. The transmitter of a wireless + telegraph set generally uses a <i>spark gap</i> for setting up the + electric oscillations, while usually for wireless telephony a <i>vacuum + tube</i> is employed for this purpose. The receptor for wireless + telegraphy and telephony is the same and may include either a <i>crystal + detector</i> or a <i>vacuum tube detector</i>, as will be explained + presently. + </p> + <p> + <i>The Easiest Way to Start.</i>--First of all you must obtain a + government license to operate a sending set, but you do not need a license + to put up and use a receiving set, though you are required by law to keep + secret any messages which you may overhear. Since no license is needed for + a receiving set the easiest way to break into the wireless game is to put + up an aerial and hook up a receiving set to it; you can then listen-in and + hear what is going on in the all-pervading ether around you, and you will + soon find enough to make things highly entertaining. + </p> + <p> + Nearly all the big wireless companies have great stations fitted with + powerful telephone transmitters and at given hours of the day and night + they send out songs by popular singers, dance music by jazz orchestras, + fashion talks by and for the ladies, agricultural reports, government + weather forecasts and other interesting features. Then by simply shifting + the slide on your tuning coil you can often tune-in someone who is sending + <i>Morse</i>, that is, messages in the dot and dash code, or, perhaps a + friend who has a wireless telephone transmitter and is talking. Of course, + if you want to <i>talk back</i> you must have a wireless transmitter, + either telegraphic or telephonic, and this is a much more expensive part + of the apparatus than the receptor, both in its initial cost and in its + operation. A wireless telegraph transmitter is less costly than a wireless + telephone transmitter and it is a very good scheme for you to learn to + send and receive telegraphic messages. + </p> + <p> + At the present time, however, there are fifteen amateur receiving stations + in the United States to every sending station, so you can see that the + majority of wireless folks care more for listening in to the broadcasting + of news and music than to sending out messages on their own account. The + easiest way to begin wireless, then, is to put up an aerial and hook up a + receiving set to it. + </p> + <p> + <i>About Aerial Wire Systems.</i>--To the beginner who wants to install a + wireless station the aerial wire system usually looms up as the biggest + obstacle of all, and especially is this true if his house is without a + flag pole, or other elevation from which the aerial wire can be + conveniently suspended. + </p> + <p> + If you live in the congested part of a big city where there are no yards + and, particularly, if you live in a flat building or an apartment house, + you will have to string your aerial wire on the roof, and to do this you + should get the owner's, or agent's, permission. This is usually an easy + thing to do where you only intend to receive messages, for one or two thin + wires supported at either end of the building are all that are needed. If + for any reason you cannot put your aerial on the roof then run a wire + along the building outside of your apartment, and, finally, if this is not + feasible, connect your receiver to a wire strung up in your room, or even + to an iron or a brass bed, and you can still get the near-by stations. + </p> + <p> + An important part of the aerial wire system is the <i>ground</i>, that is, + your receiving set must not only be connected with the aerial wire, but + with a wire that leads to and makes good contact with the moist earth of + the ground. Where a house or a building is piped for gas, water or steam, + it is easy to make a ground connection, for all you have to do is to + fasten the wire to one of the pipes with a clamp. [Footnote: Pipes are + often insulated from the ground, which makes them useless for this + purpose.] Where the house is isolated then a lot of wires or a sheet of + copper or of zinc must be buried in the ground at a sufficient depth to + insure their being kept moist. + </p> + <p> + <i>About the Receiving Apparatus</i>.--You can either buy the parts of the + receiving apparatus separate and hook them up yourself, or you can buy the + apparatus already assembled in a set which is, in the beginning, perhaps, + the better way. + </p> + <p> + The simplest receiving set consists of (1) a <i>detector</i>, (2) a <i>tuning + coil</i>, and (3) a <i>telephone receiver</i> and these three pieces of + apparatus are, of course, connected together and are also connected to the + aerial and ground as the diagram in <i>Fig. 1</i> clearly shows. There are + two chief kinds of detectors used at the present time and these are: (<i>a</i>) + the <i>crystal detector</i>, and (<i>b</i>) the <i>vacuum tube detector</i>. + The crystal detector is the cheapest and simplest, but it is not as + sensitive as the vacuum tube detector and it requires frequent adjustment. + A crystal detector can be used with or without a battery while the vacuum + tube detector requires two small batteries. + </p> + <p> + <a name="fig001" id="fig001"><img width="600" height="337" + src="images/fig001-002.jpg" + alt="Fig. 1.--Simple Receiving Set. Fig. 2.--Simple Transmitting Set." /></a> + </p> + <p> + A tuning coil of the simplest kind consists of a single layer of copper + wire wound on a cylinder with an adjustable, or sliding, contact, but for + sharp tuning you need a <i>loose coupled tuning coil</i>. Where a single + coil tuner is used a <i>fixed</i> condenser should be connected around the + telephone receivers. Where a loose coupled tuner is employed you should + have a variable condenser connected across the <i>closed oscillation + circuit</i> and a <i>fixed condenser</i> across the telephone receivers. + </p> + <p> + When listening-in to distant stations the energy of the received wireless + waves is often so very feeble that in order to hear distinctly an <i>amplifier</i> + must be used. To amplify the incoming sounds a vacuum tube made like a + detector is used and sometimes as many as half-a-dozen of these tubes are + connected in the receiving circuit, or in <i>cascade</i>, as it is called, + when the sounds are <i>amplified</i>, that is magnified, many hundreds of + times. + </p> + <p> + The telephone receiver of a receiving set is equally as important as the + detector. A single receiver can be used but a pair of receivers connected + with a head-band gives far better results. Then again the higher the + resistance of the receivers the more sensitive they often are and those + wound to as high a resistance as 3,200 ohms are made for use with the best + sets. To make the incoming signals, conversation or music, audible to a + room full of people instead of to just yourself you must use what is + called a <i>loud speaker</i>. In its simplest form this consists of a + metal cone like a megaphone to which is fitted a telephone receiver. + </p> + <p> + <i>About Transmitting Stations--Getting Your License.</i>--If you are + going to install a wireless sending apparatus, either telegraphic or + telephonic, you will have to secure a government license for which no fee + or charge of any kind is made. There are three classes of licenses issued + to amateurs who want to operate transmitting stations and these are: (1) + the <i>restricted amateur license</i>, (2) the <i>general amateur license</i>, + and (3) the <i>special amateur license</i>. + </p> + <p> + If you are going to set up a transmitter within five nautical miles of any + naval wireless station then you will have to get a <i>restricted amateur + license</i> which limits the current you use to half a <i>kilowatt</i> + [Footnote: A <i>Kilowatt</i> is 1,000 <i>watts</i>. There are 746 watts in + a horsepower.] and the wave length you send out to 200 <i>meters</i>. + Should you live outside of the five-mile range of a navy station then you + can get a general amateur license and this permits you to use a current of + 1 kilowatt, but you are likewise limited to a wave length of 200 meters. + But if you can show that you are doing some special kind of wireless work + and not using your sending station for the mere pleasure you are getting + out of it you may be able to get a <i>special amateur license</i> which + gives you the right to send out wave lengths up to 375 meters. + </p> + <p> + When you are ready to apply for your license write to the <i>Radio + Inspector</i> of whichever one of the following districts you live in: + </p> +<pre xml:space="preserve"> + First District..............Boston, Mass. + Second " ..............New York City + Third " ..............Baltimore, Md. + Fourth " ..............Norfolk, Va. + Fifth " ..............New Orleans, La. + Sixth " ............. San Francisco, Cal. + Seventh " ............. Seattle, Wash. + Eighth " ............. Detroit, Mich. + Ninth " ..............Chicago, Ill. +</pre> + <p> + <i>Kinds of Transmitters</i>.--There are two general types of transmitters + used for sending out wireless messages and these are: (1) <i>wireless + telegraph</i> transmitters, and (2) <i>wireless telephone</i> + transmitters. Telegraph transmitters may use either: (<i>a</i>) a <i>jump-spark</i>, + (<i>b</i>) an <i>electric arc</i>, or (<i>c</i>) a <i>vacuum tube</i> + apparatus for sending out dot and dash messages, while telephone + transmitters may use either, (<i>a</i>) an <i>electric arc</i>, or (<i>b</i>) + a <i>vacuum tube</i> for sending out vocal and musical sounds. Amateurs + generally use a <i>jump-spark</i> for sending wireless telegraph messages + and the <i>vacuum tube</i> for sending wireless telephone messages. + </p> + <p> + <i>The Spark Gap Wireless Telegraph Transmitter</i>.--The simplest kind of + a wireless telegraph transmitter consists of: (1) a <i>source of direct or + alternating current</i>, (2) a <i>telegraph key</i>, (3) a <i>spark-coil</i> + or a <i>transformer</i>, (4) a <i>spark gap</i>, (5) an <i>adjustable + condenser</i> and (6) an <i>oscillation transformer</i>. Where <i>dry + cells</i> or a <i>storage battery</i> must be used to supply the current + for energizing the transmitter a spark-coil can be employed and these may + be had in various sizes from a little fellow which gives 1/4-inch spark up + to a larger one which gives a 6-inch spark. Where more energy is needed it + is better practice to use a transformer and this can be worked on an + alternating current of 110 volts, or if only a 110 volt direct current is + available then an <i>electrolytic interrupter</i> must be used to make and + break the current. A simple transmitting set with an induction coil is + shown in <i>Fig. 2</i>. + </p> + <p> + A wireless key is made like an ordinary telegraph key except that where + large currents are to be used it is somewhat heavier and is provided with + large silver contact points. Spark gaps for amateur work are usually of: + (1) the <i>plain</i> or <i>stationary type</i>, (2) the <i>rotating type</i>, + and (3) the <i>quenched gap</i> type. The plain spark-gap is more suitable + for small spark-coil sets, and it is not so apt to break down the + transformer and condenser of the larger sets as the rotary gap. The rotary + gap on the other hand tends to prevent <i>arcing</i> and so the break is + quicker and there is less dragging of the spark. The quenched gap is more + efficient than either the plain or rotary gap and moreover it is + noiseless. + </p> + <p> + Condensers for spark telegraph transmitters can be ordinary Leyden jars or + glass plates coated with tin or copper foil and set into a frame, or they + can be built up of mica and sheet metal embedded in an insulating + composition. The glass plate condensers are the cheapest and will serve + your purpose well, especially if they are immersed in oil. Tuning coils, + sometimes called <i>transmitting inductances</i> and <i>oscillation + transformers</i>, are of various types. The simplest kind is a + transmitting inductance which consists of 25 or 30 turns of copper wire + wound on an insulating tube or frame. An oscillation transformer is a + loose coupled tuning coil and it consists of a primary coil formed of a + number of turns of copper wire wound on a fixed insulating support, and a + secondary coil of about twice the number of turns of copper wire which is + likewise fixed in an insulating support, but the coils are relatively + movable. An <i>oscillation transformer</i> (instead of a <i>tuning coil</i>), + is required by government regulations unless <i>inductively coupled</i>. + </p> + <p> + The <i>Vacuum Tube Telegraph Transmitter</i>.--This consists of: (1) a <i>source + of direct or alternating current</i>, (2) a <i>telegraph key</i>, (3) a <i>vacuum + tube oscillator</i>, (4) a <i>tuning coil</i>, and (5) a <i>condenser</i>. + This kind of a transmitter sets up <i>sustained</i> oscillations instead + of <i>periodic</i> oscillations which are produced by a spark gap set. The + advantages of this kind of a system will be found explained in <a + href="#chap16">Chapter XVI</a>. + </p> + <p> + <i>The Wireless Telephone Transmitter</i>.--Because a jump-spark sets up + <i>periodic oscillations</i>, that is, the oscillations are discontinuous, + it cannot be used for wireless telephony. An electric arc or a vacuum tube + sets up <i>sustained</i> oscillations, that is, oscillations which are + continuous. As it is far easier to keep the oscillations going with a + vacuum tube than it is with an arc the former means has all but supplanted + the latter for wireless telephone transmitters. The apparatus required and + the connections used for wireless telephone sets will be described in + later chapters. + </p> + <p> + <i>Useful Information</i>.--It would be wise for the reader to turn to the + <a href="#appendix">Appendix</a>, beginning with page 301 of this book, + and familiarize himself with the information there set down in tabular and + graphic form. For example, the first table gives abbreviations of + electrical terms which are in general use in all works dealing with the + subject. You will also find there brief definitions of electric and + magnetic units, which it would be well to commit to memory; or, at least, + to make so thoroughly your own that when any of these terms is mentioned, + you will know instantly what is being talked about. + </p> + <h2> + <a name="chap02" id="chap02">CHAPTER II</a> + </h2> + <h3> + PUTTING UP YOUR AERIAL + </h3> + <p> + As inferred in the first chapter, an aerial for receiving does not have to + be nearly as well made or put up as one for sending. But this does not + mean that you can slipshod the construction and installation of it, for + however simple it is, the job must be done right and in this case it is as + easy to do it right as wrong. + </p> + <p> + To send wireless telegraph and telephone messages to the greatest + distances and to receive them as distinctly as possible from the greatest + distances you must use for your aerial (1) copper or aluminum wire, (2) + two or more wires, (3) have them the proper length, (4) have them as high + in the air as you can, (5) have them well apart from each other, and (6) + have them well insulated from their supports. If you live in a flat + building or an apartment house you can string your aerial wires from one + edge of the roof to the other and support them by wooden stays as high + above it as may be convenient. + </p> + <p> + Should you live in a detached house in the city you can usually get your + next-door neighbor to let you fasten one end of the aerial to his house + and this will give you a good stretch and a fairly high aerial. In the + country you can stretch your wires between the house and barn or the + windmill. From this you will see that no matter where you live you can + nearly always find ways and means of putting up an aerial that will serve + your needs without going to the expense of erecting a mast. + </p> + <p> + <i>Kinds of Aerial Wire Systems</i>.--An amateur wireless aerial can be + anywhere from 25 feet to 100 feet long and if you can get a stretch of the + latter length and a height of from 30 to 75 feet you will have one with + which you can receive a thousand miles or more and send out as much energy + as the government will allow you to send. + </p> + <p> + The kind of an aerial that gives the best results is one whose wire, or + wires, are <i>horizontal</i>, that is, parallel with the earth under it as + shown at <i>A</i> in <i>Fig. 3.</i> If only one end can be fixed to some + elevated support then you can secure the other end to a post in the + ground, but the slope of the aerial should not be more than 30 or 35 + degrees from the horizontal at most as shown at <i>B</i>. + </p> + <p> + <a name="fig003" id="fig003"><img width="600" height="262" + src="images/fig003.jpg" + alt="(A) Fig. 3.--Flat top, or Horizontal Aerial. (B) Fig. 3.--Inclined Aerial." /> + </a> + </p> + <p> + The <i>leading-in wire</i>, that is, the wire that leads from and joins + the aerial wire with your sending and receiving set, can be connected to + the aerial anywhere it is most convenient to do so, but the best results + are had when it is connected to one end as shown at <i>A</i> in <i>Fig. 4</i>, + in which case it is called an <i>inverted L aerial</i>, or when it is + connected to it at the middle as shown at <i>B</i>, when it is called a <i>T + aerial</i>. The leading-in wire must be carefully insulated from the + outside of the building and also where it passes through it to the inside. + This is done by means of an insulating tube known as a <i>leading-in + insulator,</i> or <i>bulkhead insulator</i> as it is sometimes called. + </p> + <p> + <a name="fig004" id="fig004"><img width="532" height="160" + src="images/fig004.jpg" + alt="(A) Fig. 4.--Inverted L Aerial. (B) Fig. 4.--T Aerial." /></a> + </p> + <p> + As a protection against lightning burning out your instruments you can use + either: (1) an <i>air-gap lightning arrester,</i> (2) a <i>vacuum tube + protector,</i> or (3) a <i>lightning switch,</i> which is better. + Whichever of these devices is used it is connected in between the aerial + and an outside ground wire so that a direct circuit to the earth will be + provided at all times except when you are sending or receiving. So your + aerial instead of being a menace really acts during an electrical storm + like a lightning rod and it is therefore a real protection. The air-gap + and vacuum tube lightning arresters are little devices that can be used + only where you are going to receive, while the lightning switch must be + used where you are going to send; indeed, in some localities the <i>Fire + Underwriters</i> require a large lightning switch to be used for receiving + sets as well as sending sets. + </p> + <p> + <i>How to Put Up a Cheap Receiving Aerial.</i>--The kind of an aerial wire + system you put up will depend, chiefly, on two things, and these are: (1) + your pocketbook, and (2) the place where you live. + </p> + <p> + <i>A Single Wire Aerial.</i>--This is the simplest and cheapest kind of a + receiving aerial that can be put up. The first thing to do is to find out + the length of wire you need by measuring the span between the two points + of support; then add a sufficient length for the leading-in wire and + enough more to connect your receiving set with the radiator or water pipe. + </p> + <p> + You can use any size of copper or aluminum wire that is not smaller than + <i>No. 16 Brown and Sharpe gauge.</i> When you buy the wire get also the + following material: (1) two <i>porcelain insulators</i> as shown at <i>A</i> + in <i>Fig. 5</i>; (2) three or four <i>porcelain knob insulators</i>, see + <i>B</i>; (3) either (<i>a</i>) an <i>air gap lightning arrester,</i> see + <i>C</i>, or (<i>b</i>) a <i>lightning switch</i> see <i>D</i>; (4) a <i>leading-in + porcelain tube insulator,</i> see <i>E</i>, and (5) a <i>ground clamp</i>, + see <i>F</i>. + </p> + <p> + <a name="fig005" id="fig005"><img width="600" height="251" + src="images/fig005.jpg" + alt="Fig. 5.--Material for a Simple Aerial Wire System." /></a> + </p> + <p> + To make the aerial slip each end of the wire through a hole in each + insulator and twist it fast; next cut off and slip two more pieces of wire + through the other holes in the insulators and twist them fast and then + secure these to the supports at the ends of the building. Take the piece + you are going to use for the leading-in wire, twist it around the aerial + wire and solder it there when it will look like <i>A</i> in <i>Fig. 6</i>. + Now if you intend to use the <i>air gap lightning arrester</i> fasten it + to the wall of the building outside of your window, and bring the + leading-in wire from the aerial to the top binding post of your arrester + and keep it clear of everything as shown at <i>B</i>. If your aerial is on + the roof and you have to bring the leading-in wire over the cornice or + around a corner fix a porcelain knob insulator to the one or the other and + fasten the wire to it. + </p> + <p> + <a name="fig006a" id="fig006a"><img width="600" height="233" + src="images/fig006a.jpg" + alt="(A) Fig. 6.--Single Wire Aerial for Receiving." /></a> <a + name="fig006b" id="fig006b"><img width="600" height="711" + src="images/fig006b.jpg" + alt="(B) Fig. 6.--Receiving Aerial with Air Gap Lightning Arrester." /></a> + <a name="fig006c" id="fig006c"><img width="600" height="323" + src="images/fig006c.jpg" alt="(C) Fig. 6.--Aerial with Lightning Switch." /></a> + </p> + <p> + Next bore a hole through the frame of the window at a point nearest your + receiving set and push a porcelain tube 5/8 inch in diameter and 5 or 6 + inches long, through it. Connect a length of wire to the top post of the + arrester or just above it to the wire, run this through the leading-in + insulator and connect it to the slider of your tuning coil. Screw the end + of a piece of heavy copper wire to the lower post of the arrester and run + it to the ground, on porcelain knobs if necessary, and solder it to an + iron rod or pipe which you have driven into the earth. Finally connect the + fixed terminal of your tuning coil with the water pipe or radiator inside + of the house by means of the ground clamp as shown in the diagrammatic + sketch at <i>B</i> in <i>Fig. 6</i> and you are ready to tune in. + </p> + <p> + If you want to use a lightning switch instead of the air-gap arrester then + fasten it to the outside wall instead of the latter and screw the free end + of the leading-in wire from the aerial to the middle post of it as shown + at <i>C</i> in <i>Fig. 6</i>. Run a wire from the top post through the + leading-in insulator and connect it with the slider of your tuning coil. + Next screw one end of a length of heavy copper wire to the lower post of + the aerial switch and run it to an iron pipe in the ground as described + above in connection with the spark-gap lightning arrester; then connect + the fixed terminal of your tuning coil with the radiator or water pipe and + your aerial wire system will be complete as shown at <i>C</i> in <i>Fig. 6</i>. + </p> + <p> + <i>A Two-wire Aerial.</i>--An aerial with two wires will give better + results than a single wire and three wires are better than two, but you + must keep them well apart. To put up a two-wire aerial get (1) enough <i>No. + 16</i>, or preferably <i>No. 14</i>, solid or stranded copper or aluminum + wire, (2) four porcelain insulators, see <i>B</i> in <i>Fig. 5</i>, and + (3) two sticks about 1 inch thick, 3 inches wide and 3 or 4 feet long, for + the <i>spreaders</i>, and bore 1/8-inch hole through each end of each one. + Now twist the ends of the wires to the insulators and then cut off four + pieces of wire about 6 feet long and run them through the holes in the + wood spreaders. Finally twist the ends of each pair of short wires to the + free ends of the insulators and then twist the free ends of the wires + together. + </p> + <p> + For the leading-in wire that goes to the lightning switch take two lengths + of wire and twist one end of each one around the aerial wires and solder + them there. Twist the short wire around the long wire and solder this + joint also when the aerial will look like <i>Fig. 7</i>. Bring the free + end of the leading-in wire down to the middle post of the lightning switch + and fasten it there and connect up the receiver to it and the ground as + described under the caption of <i>A Single Wire Aerial</i>. + </p> + <p> + <a name="fig007" id="fig007"><img width="600" height="277" + src="images/fig007.jpg" alt="Fig. 7.--Two Wire Aerial." /></a> + </p> + <p> + <i>Connecting in the Ground.</i>--If there is a gas or water system or a + steam-heating plant in your house you can make your ground connection by + clamping a ground clamp to the nearest pipe as has been previously + described. Connect a length of bare or insulated copper wire with it and + bring this up to the table on which you have your receiving set. If there + are no grounded pipes available then you will have to make a good ground + which we shall describe presently and lead the ground wire from your + receiving set out of the window and down to it. + </p> + <p> + <i>How to Put Up a Good Aerial.</i>--While you can use the cheap aerial + already described for a small spark-coil sending set you should have a + better insulated one for a 1/2 or a 1 <i>kilowatt</i> transformer set. The + cost for the materials for a good aerial is small and when properly made + and well insulated it will give results that are all out of proportion to + the cost of it. + </p> + <p> + <i>An Inexpensive Good Aerial</i>.--A far better aerial, because it is + more highly insulated, can be made by using <i>midget insulators</i> + instead of the porcelain insulators described under the caption of <i>A + Single Wire Aerial</i> and using a small <i>electrose leading-in insulator</i> + instead of the porcelain bushing. This makes a good sending aerial for + small sets as well as a good receiving aerial. + </p> + <p> + <i>The Best Aerial that Can Be Made.</i>--To make this aerial get the + following material together: (1) enough <i>stranded or braided wire</i> + for three or four lengths of parallel wires, according to the number you + want to use (2) six or eight <i>electrose ball insulators</i>, see <i>B</i>, + <i>Fig. 8</i>; (3) two 5-inch or 10-inch <i>electrose strain insulators</i>, + see <i>C</i>; (4) six or eight <i>S-hooks</i>, <i>see D</i>; one large <i>withe</i> + with one eye for middle of end spreader, see <i>E</i>; (6) two smaller <i>withes</i> + with one eye each for end spreader, see <i>E</i>; (7) two still smaller <i>withes</i>, + with two eyes each for the ends of the end spreaders, see <i>E</i> (8) two + <i>thimbles</i>, see <i>F</i>, for 1/4-inch wire cable; (9) six or eight + <i>hard rubber tubes</i> or <i>bushings</i> as shown at <i>G</i>; and (10) + two <i>end spreaders</i>, see <i>H</i>; one <i>middle spreader, see I</i>; + and one <i>leading-in spreader</i>, see <i>J</i>. + </p> + <p> + <a name="fig008a" id="fig008a"><img width="595" height="480" + src="images/fig008a.jpg" alt="(A) Fig. 8--Part of a Good Aerial." /></a> <a + name="fig008b" id="fig008b"><img width="578" height="240" + src="images/fig008b.jpg" alt="(B) Fig. 8.--The Spreaders." /></a> + </p> + <p> + For this aerial any one of a number of kinds of wire can be used and among + these are (<i>a</i>) <i>stranded copper wire;</i> (<i>b</i>) <i>braided + copper wire;</i> (<i>c</i>) <i>stranded silicon bronze wire,</i> and (<i>d</i>) + <i>stranded phosphor bronze wire</i>. Stranded and braided copper wire is + very flexible as it is formed of seven strands of fine wire twisted or + braided together and it is very good for short and light aerials. Silicon + bronze wire is stronger than copper wire and should be used where aerials + are more than 100 feet long, while phosphor bronze wire is the strongest + aerial wire made and is used for high grade aerials by the commercial + companies and the Government for their high-power stations. + </p> + <p> + The spreaders should be made of spruce, and should be 4 feet 10 inches + long for a three-wire aerial and 7 feet 1 inch long for a four-wire aerial + as the distance between the wires should be about 27 inches. The end + spreaders can be turned cylindrically but it makes a better looking job if + they taper from the middle to the ends. They should be 2-1/4 inches in + diameter at the middle and 1-3/4 inches at the ends. The middle spreader + can be cylindrical and 2 inches in diameter. It must have holes bored + through it at equidistant points for the hard rubber tubes; each of these + should be 5/8 inch in diameter and have a hole 5/32 inch in diameter + through it for the aerial wire. The leading-in spreader is also made of + spruce and is 1-1/2 inches square and 26 inches long. Bore three or four + 5/8-inch holes at equidistant points through this spreader and insert hard + rubber tubes in them as with the middle spreader. + </p> + <p> + <i>Assembling the Aerial.</i>--Begin by measuring off the length of each + wire to be used and see to it that all of them are of exactly the same + length. Now push the hard rubber insulators through the holes in the + middle spreader and thread the wires through the holes in the insulators + as shown at <i>A</i> in <i>Fig 9</i>. + </p> + <p> + Next twist the ends of each wire to the rings of the ball insulators and + then put the large withes on the middle of each of the end spreaders; fix + the other withes on the spreaders so that they will be 27 inches apart and + fasten the ball insulators to the eyes in the withes with the S-hooks. Now + slip a thimble through the eye of one of the long strain insulators, + thread a length of stranded steel wire 1/4 inch in diameter through it and + fasten the ends of it to the eyes in the withes on the ends of the + spreaders. + </p> + <p> + <a name="fig009ab" id="fig009ab"><img width="600" height="441" + src="images/fig009ab.jpg" + alt="(A) Fig. 9.--Middle Spreader. (B) Fig. 9.--One End of Aerial Complete." /> + </a> <a name="fig009c" id="fig009c"><img width="600" height="422" + src="images/fig009c.jpg" alt="(C) Fig. 9.--Leading in Spreader." /></a> + </p> + <p> + Finally fasten a 40-inch length of steel stranded wire to each of the eyes + of the withes on the middle of each of the spreaders, loop the other end + over the thimble and then wrap the end around the wires that are fixed to + the ends of the spreaders. One end of the aerial is shown complete at <i>B</i> + in <i>Fig. 9</i>, and from this you can see exactly how it is assembled. + Now cut off three or four pieces of wire 15 or 20 feet long and twist and + solder each one to one of the aerial wires; then slip them through the + hard rubber tubes in the leading-in spreader, bring their free ends + together as at <i>C</i> and twist and solder them to a length of wire long + enough to reach to your lightning switch or instruments. + </p> + <p> + <i>Making a Good Ground</i>.--Where you have to make a <i>ground</i> you + can do so either by (1) burying sheets of zinc or copper in the moist + earth; (2) burying a number of wires in the moist earth, or (3) using a <i>counterpoise</i>. + To make a ground of the first kind take half a dozen large sheets of + copper or zinc, cut them into strips a foot wide, solder them all together + with other strips and bury them deeply in the ground. + </p> + <p> + It is easier to make a wire ground, say of as many or more wires as you + have in your aerial and connect them together with cross wires. To put + such a ground in the earth you will have to use a plow to make the furrows + deep enough to insure them always being moist. In the counterpoise ground + you make up a system of wires exactly like your aerial, that is, you + insulate them just as carefully; then you support them so that they will + be as close to the ground as possible and yet not touch it or anything + else. This and the other two grounds just described should be placed + directly under the aerial wire if the best results are to be had. In using + a counterpoise you must bring the wire from it up to and through another + leading-in insulator to your instruments. + </p> + <h2> + <a name="chap03" id="chap03">CHAPTER III</a> + </h2> + <h3> + SIMPLE TELEGRAPH AND TELEPHONE RECEIVING SETS + </h3> + <p> + With a crystal detector receiving set you can receive either telegraphic + dots and dashes or telephonic speech and music. You can buy a receiving + set already assembled or you can buy the different parts and assemble them + yourself. An assembled set is less bother in the beginning but if you like + to experiment you can <i>hook up</i>, that is, connect the separate parts + together yourself and it is perhaps a little cheaper to do it this way. + Then again, by so doing you get a lot of valuable experience in wireless + work and an understanding of the workings of wireless that you cannot get + in any other way. + </p> + <p> + <i>Assembled Wireless Receiving Sets</i>.--The cheapest assembled + receiving set [Footnote: The Marvel, made by the Radio Mfg. Co., New York + City.] advertised is one in which the detector and tuning coil is mounted + in a box. It costs $15.00, and can be bought of dealers in electric + supplies generally. + </p> + <p> + This price also includes a crystal detector, an adjustable tuning coil, a + single telephone receiver with head-band and the wire, porcelain + insulators, lightning switch and ground clamp for the aerial wire system. + It will receive wireless telegraph and telephone messages over a range of + from 10 to 25 miles. + </p> + <p> + Another cheap unit receptor, that is, a complete wireless receiving set + already mounted which can be used with a single aerial is sold for $25.00. + [Footnote: The Aeriola Jr., made by the Westinghouse Company, Pittsburgh, + Pa.] This set includes a crystal detector, a variable tuning coil, a fixed + condenser and a pair of head telephone receivers. It can also be used to + receive either telegraph or telephone messages from distances up to 25 + miles. The aerial equipment is not included in this price, but it can be + bought for about $2.50 extra. + </p> + <p> + <i>Assembling Your Own Receiving Set</i>.--In this chapter we shall go + only into the apparatus used for two simple receiving sets, both of which + have a <i>crystal detector</i>. The first set includes a <i>double-slide + tuning coil</i> and the second set employs a <i>loose-coupled tuning coil</i>, + or <i>loose coupler</i>, as it is called for short. For either set you can + use a pair of 2,000- or 3,000-ohm head phones. + </p> + <table cellspacing="20" summary="Illustration"> + <tr> + <td align="center"> + <i>Photograph unavailable</i> + </td> + </tr> + <tr> + <td align="center"> + original © Underwood and Underwood.<br /> General Pershing + Listening In. + </td> + </tr> + </table> + <p> + <i>The Crystal Detector</i>.--A crystal detector consists of: (1) <i>the + frame</i>, (2) <i>the crystal</i>, and (3) <i>the wire point</i>. There + are any number of different designs for frames, the idea being to provide + a device that will (<i>a</i>) hold the sensitive crystal firmly in place, + and yet permit of its removal, (<i>b</i>) to permit the <i>wire point</i>, + or <i>electrode</i>, to be moved in any direction so that the free point + of it can make contact with the most sensitive spot on the crystal and (<i>c</i>) + to vary the pressure of the wire on the crystal. + </p> + <p> + A simple detector frame is shown in the cross-section at <i>A</i> in <i>Fig. + 10</i>; the crystal, which may be <i>galena</i>, <i>silicon</i> or <i>iron + pyrites</i>, is held securely in a holder while the <i>phosphor-bronze + wire point</i> which makes contact with it, is fixed to one end of a + threaded rod on the other end of which is a knob. This rod screws into and + through a sleeve fixed to a ball that sets between two brass standards and + this permits an up and down or a side to side adjustment of the metal + point while the pressure of it on the crystal is regulated by the screw. + </p> + <p> + <a name="fig010ab" id="fig010ab"><img width="600" height="316" + src="images/fig010ab.jpg" + alt="(A) Fig. 10.--Cross Section of Crystal Detector. (B) Fig. 10.--The Crystal Detector Complete." /> + </a> + </p> + <p> + A crystal of this kind is often enclosed in a glass cylinder and this + makes it retain its sensitiveness for a much longer time than if it were + exposed to dust and moisture. An upright type of this detector can be + bought for $2.25, while a horizontal type, as shown at <i>B</i>, can be + bought for $2.75. Galena is the crystal that is generally used, for, while + it is not quite as sensitive as silicon and iron pyrites, it is easier to + obtain a sensitive piece. + </p> + <p> + <i>The Tuning Coil</i>.--It is with the tuning coil that you <i>tune in</i> + and <i>tune out</i> different stations and this you do by sliding the + contacts to and fro over the turns of wire; in this way you vary the <i>inductance</i> + and <i>capacitance</i>, that is, the <i>constants</i> of the receiving + circuits and so make them receive <i>electric waves</i>, that is, wireless + waves, of different lengths. + </p> + <p> + <i>The Double Slide Tuning Coil</i>.--With this tuning coil you can + receive waves from any station up to 1,000 meters in length. One of the + ends of the coil of wire connects with the binding post marked <i>a</i> in + <i>Fig. 11</i>, and the other end connects with the other binding post + marked <i>b</i>, while one of the sliding contacts is connected to the + binding post <i>c</i>, and the <i>other sliding contact</i> is connected + with the binding post <i>d</i>. + </p> + <p> + <a name="fig011ab" id="fig011ab"><img width="600" height="234" + src="images/fig011ab.jpg" + alt="(A) Fig. 11.--Schematic Diagram of Double Slide Tuning Coil. (B) Fig. 11.--Double Slide Tuning Coil Complete." /> + </a> + </p> + <p> + When connecting in the tuning coil, only the post <i>a</i> or the post <i>b</i> + is used as may be most convenient, but the other end of the wire which is + connected to a post is left free; just bear this point in mind when you + come to connect the tuning coil up with the other parts of your receiving + set. The tuning coil is shown complete at <i>B</i> and it costs $3.00 or + $4.00. A <i>triple slide</i> tuning coil constructed like the double slide + tuner just described, only with more turns of wire on it, makes it + possible to receive wave lengths up to 1,500 meters. It costs about $6.00. + </p> + <p> + <i>The Loose Coupled Tuning Coil</i>.--With a <i>loose coupler</i>, as + this kind of a tuning coil is called for short, very <i>selective tuning</i> + is possible, which means that you can tune in a station very sharply, and + it will receive any wave lengths according to size of coils. The primary + coil is wound on a fixed cylinder and its inductance is varied by means of + a sliding contact like the double slide tuning coil described above. The + secondary coil is wound on a cylinder that slides in and out of the + primary coil. The inductance of this coil is varied by means of a switch + that makes contact with the fixed points, each of which is connected with + every twentieth turn of wire as shown in the diagram <i>A</i> in <i>Fig. + 12</i>. The loose coupler, which is shown complete at <i>B</i>, costs in + the neighborhood of $8.00 or $10.00. + </p> + <p> + <a name="fig012ab" id="fig012ab"><img width="600" height="326" + src="images/fig012ab.jpg" + alt="(A) Fig. 12.--Schematic Diagram of Loose Coupler. (B) Fig. 12.--Loose Coupler Complete." /> + </a> + </p> + <p> + <i>Fixed and Variable Condensers</i>.--You do not require a condenser for + a simple receiving set, but if you will connect a <i>fixed condenser</i> + across your headphones you will get better results, while a <i>variable + condenser</i> connected in the <i>closed circuit of a direct coupled + receiving set</i>, that is, one where a double slide tuning coil is used, + makes it easy to tune very much more sharply; a variable condenser is + absolutely necessary where the circuits are <i>inductively coupled</i>, + that is, where a loose coupled tuner is used. + </p> + <p> + A fixed condenser consists of a number of sheets of paper with leaves of + tin-foil in between them and so built up that one end of every other leaf + of tin-foil projects from the opposite end of the paper as shown at <i>A</i> + in <i>Fig. 13</i>. The paper and tin-foil are then pressed together and + impregnated with an insulating compound. A fixed condenser of the exact + capacitance required for connecting across the head phones is mounted in a + base fitted with binding posts, as shown at <i>B</i>, and costs 75 cents. + (Paper ones 25 cents.) + </p> + <p> + <a name="fig013ab" id="fig013ab"><img width="593" height="240" + src="images/fig013ab.jpg" + alt="(A) Fig. 13.--How a Fixed Receiving Condenser is Built up. (B) Fig. 13.--The Fixed Condenser Complete." /> + </a> <a name="fig013cd" id="fig013cd"><img width="584" height="280" + src="images/fig013cd.jpg" + alt="(C) and (D) Fig. 13.--The Variable Rotary Condenser." /></a> + </p> + <p> + A variable condenser, see <i>C</i>, of the rotating type is formed of a + set of fixed semi-circular metal plates which are slightly separated from + each other and between these a similar set of movable semi-circular metal + plates is made to interleave; the latter are secured to a shaft on the top + end of which is a knob and by turning it the capacitance of the condenser, + and, hence, of the circuit in which it is connected, is varied. This + condenser, which is shown at <i>D</i>, is made in two sizes, the smaller + one being large enough for all ordinary wave lengths while the larger one + is for proportionately longer wave lengths. These condensers cost $4.00 + and $5.00 respectively. + </p> + <p> + <i>About Telephone Receivers.</i>--There are a number of makes of head + telephone receivers on the market that are designed especially for + wireless work. These phones are wound to <i>resistances</i> of from 75 <i>ohms</i> + to 8,000 <i>ohms</i>, and cost from $1.25 for a receiver without a cord or + headband to $15.00 for a pair of phones with a cord and head band. You can + get a receiver wound to any resistance in between the above values but for + either of the simple receiving sets such as described in this chapter you + ought to have a pair wound to at least 2,000 ohms and these will cost you + about $5.00. A pair of head phones of this type is shown in <i>Fig. 14.</i> + </p> + <p> + <a name="fig014" id="fig014"><img width="389" height="400" + src="images/fig014.jpg" alt="Fig. 14.--Pair of Wireless Head Phones." /></a> + </p> + <p> + <i>Connecting Up the Parts</i>--<i>Receiving Set No. 1.</i>--For this set + get (1) a <i>crystal detector</i>, (2) a <i>two-slide tuning coil</i>, (3) + a <i>fixed condenser</i>, and (4) a pair of 2,000 ohm head phones. Mount + the detector on the right-hand side of a board and the tuning coil on the + left-hand side. Screw in two binding posts for the cord ends of the + telephone receivers at <i>a</i> and <i>b</i> as shown at <i>A</i> in <i>Fig. + 15</i>. This done connect one of the end binding posts of the tuning coil + with the ground wire and a post of one of the contact slides with the + lightning arrester or switch which leads to the aerial wire. + </p> + <p> + <a name="fig015a" id="fig015a"><img width="600" height="526" + src="images/fig015a.jpg" + alt="Fig. 15.--Top View of Apparatus Layout for Receiving Set No. 1." /></a> + <a name="fig015b" id="fig015b"><img width="516" height="520" + src="images/fig015b.jpg" + alt="(B) Fig. 15.--Wiring Diagram for Receiving Set No. 1." /></a> + </p> + <p> + Now connect the post of the other contact slide to one of the posts of the + detector and the other post of the latter with the binding post <i>a</i>, + then connect the binding post <i>b</i> to the ground wire and solder the + joint. Next connect the ends of the telephone receiver cord to the posts + <i>a</i> and <i>b</i> and connect a fixed condenser also with these posts, + all of which are shown in the wiring diagram at <i>B</i>, and you are + ready to adjust the set for receiving. + </p> + <p> + <i>Receiving Set No. 2.</i>--Use the same kind of a detector and pair of + head phones as for <i>Set No. 1</i>, but get (1) a <i>loose coupled tuning + coil</i>, and (2) a <i>variable condenser</i>. Mount the loose coupler at + the back of a board on the left-hand side and the variable condenser on + the right-hand side. Then mount the detector in front of the variable + condenser and screw two binding posts, <i>a</i> and <i>b</i>, in front of + the tuning coil as shown at <i>A</i> in <i>Fig. 16</i>. + </p> + <p> + <a name="fig016a" id="fig016a"><img width="600" height="598" + src="images/fig016a.jpg" + alt="Fig. 16.--Top view of Apparatus Layout for Receiving Set No. 2." /></a> + <a name="fig016b" id="fig016b"><img width="600" height="485" + src="images/fig016b.jpg" + alt="(B) Fig. 16.--Wiring Diagram for Receiving Set No. 2." /></a> + </p> + <p> + Now connect the post of the sliding contact of the loose coupler with the + wire that runs to the lightning switch and thence to the aerial; connect + the post of the primary coil, which is the outside coil, with the ground + wire; then connect the binding post leading to the switch of the secondary + coil, which is the inside coil, with one of the posts of the variable + condenser, and finally, connect the post that is joined to one end of the + secondary coil with the other post of the variable condenser. + </p> + <p> + This done, connect one of the posts of the condenser with one of the posts + of the detector, the other post of the detector with the binding post <i>a</i>, + and the post <i>b</i> to the other post of the variable condenser. Next + connect a fixed condenser to the binding posts <i>a</i> and <i>b</i> and + then connect the telephone receivers to these same posts, all of which is + shown in the wiring diagram at <i>B</i>. You are now ready to adjust the + instruments. In making the connections use No. 16 or 18 insulated copper + wire and scrape the ends clean where they go into the binding posts. See, + also, that all of the connections are tight and where you have to cross + the wires keep them apart by an inch or so and always cross them at right + angles. + </p> + <p> + <i>Adjusting the No. 1 Set</i>--<i>The Detector.</i>--The first thing to + do is to test the detector in order to find out if the point of the + contact wire is on a sensitive spot of the crystal. To do this you need a + <i>buzzer</i>, a <i>switch</i> and a <i>dry cell</i>. An electric bell + from which the gong has been removed will do for the buzzer, but you can + get one that is made specially for the purpose, for 75 cents, which gives + out a clear, high-pitched note that sounds like a high-power station. + </p> + <p> + Connect one of the binding posts of the buzzer with one post of the + switch, the other post of the latter with the zinc post of the dry cell + and the carbon post of this to the other post of the buzzer. Then connect + the post of the buzzer that is joined to the vibrator, to the ground wire + as shown in the wiring diagram, <i>Fig. 17.</i> Now close the switch of + the buzzer circuit, put on your head phones, and move the wire point of + the detector to various spots on the crystal until you hear the sparks + made by the buzzer in your phones. + </p> + <p> + <a name="fig017" id="fig017"><img width="434" height="640" + src="images/fig017.jpg" alt="Fig. 17.--Adjusting the Receiving Set." /></a> + </p> + <p> + Then vary the pressure of the point on the crystal until you hear the + sparks as loud as possible. After you have made the adjustment open the + switch and disconnect the buzzer wire from the ground wire of your set. + This done, be very careful not to jar the detector or you will throw it + out of adjustment and then you will have to do it all over again. You are + now ready to tune the set with the tuning coil and listen in. + </p> + <p> + <i>The Tuning Coil.</i>--To tune this set move the slide <i>A</i> of the + double-slide tuner, see <i>B</i> in <i>Fig. 15</i>, over to the end of the + coil that is connected with the ground wire and the slide <i>B</i> near + the opposite end of the coil, that is, the one that has the free end. Now + move the slide <i>A</i> toward the <i>B</i> slide and when you hear the + dots and dashes, or speech or music, that is coming in as loud as you can + move the <i>B</i> slide toward the <i>A</i> slide until you hear still + more loudly. A very few trials on your part and you will be able to tune + in or tune out any station you can hear, if not too close or powerful. + </p> + <table cellspacing="20" summary="Illustration"> + <tr> + <td align="center"> + <i>Photograph unavailable</i> + </td> + </tr> + <tr> + <td align="center"> + original © Underwood and Underwood.<br /> The World's Largest + Radio Receiving Station. Owned by the Radio Corporation of America at + Rocky Point near Point Jefferson, L.I. + </td> + </tr> + </table> + <p> + <i>Adjusting the No. 2 Set.</i>--First adjust the crystal detector with + the buzzer set as described above with <i>Set No. 1,</i> then turn the + knob of your variable condenser so that the movable plates are just + half-way in, pull the secondary coil of your loose-coupled tuner half way + out; turn the switch lever on it until it makes a contact with the middle + contact point and set the slider of the primary coil half way between the + ends. + </p> + <p> + Now listen in for telegraphic signals or telephonic speech or music; when + you hear one or the other slide the secondary coil in and out of the + primary coil until the sounds are loudest; now move the contact switch + over the points forth and back until the sounds are still louder, then + move the slider to and fro until the sounds are yet louder and, finally, + turn the knob of the condenser until the sounds are clear and crisp. When + you have done all of these things you have, in the parlance of the + wireless operator, <i>tuned in</i> and you are ready to receive whatever + is being sent. + </p> + <h2> + <a name="chap04" id="chap04">CHAPTER IV</a> + </h2> + <h3> + SIMPLE TELEGRAPH SENDING SETS + </h3> + <p> + A wireless telegraph transmitting set can be installed for a very small + amount of money provided you are content with one that has a limited + range. Larger and better instruments can, of course, be had for more + money, but however much you are willing to spend still you are limited in + your sending radius by the Government's rules and regulations. The best + way, and the cheapest in the end, to install a telegraph set is to buy the + separate parts and hook them up yourself. + </p> + <p> + The usual type of wireless telegraph transmitter employs a <i>disruptive + discharge,</i> or <i>spark,</i> as it is called, for setting up the + oscillating currents in the aerial wire system and this is the type of + apparatus described in this chapter. There are two ways to set up the + sparks and these are: (1) with an <i>induction coil,</i> or <i>spark-coil,</i> + as it is commonly called, and (2) with an <i>alternating current + transformer</i>, or <i>power transformer</i>, as it is sometimes called. + Where you have to generate the current with a battery you must use a spark + coil, but if you have a 110-volt direct or alternating lighting current in + your home you can use a transformer which will give you more power. + </p> + <p> + <i>A Cheap Transmitting Set (No. 1)</i>.--For this set you will need: (1) + a <i>spark-coil</i>, (2) a <i>battery</i> of dry cells, (3) a <i>telegraph + key</i>, (4) a <i>spark gap</i>, (5) a <i>high-tension condenser</i>, and + (6) an <i>oscillation transformer</i>. There are many different makes and + styles of these parts but in the last analysis all of them are built on + the same underlying bases and work on the same fundamental principles. + </p> + <p> + <i>The Spark-Coil</i>.--Spark coils for wireless work are made to give + sparks from 1/4 inch in length up to 6 inches in length, but as a spark + coil that gives less than a 1-inch spark has a very limited output it is + best to get a coil that gives at least a 1-inch spark, as this only costs + about $8.00, and if you can get a 2- or a 4-inch spark coil so much the + better. There are two general styles of spark coils used for wireless and + these are shown at <i>A</i> and <i>B</i> in <i>Fig. 18</i>. + </p> + <p> + <a name="fig018ab" id="fig018ab"><img width="600" height="276" + src="images/fig018ab.jpg" + alt="(A) and (B) Fig. 18.--Types of Spark Coils for Set. No. 1." /></a> <a + name="fig018c" id="fig018c"><img width="600" height="435" + src="images/fig018c.jpg" alt="(C) Fig. 18.--Wiring Diagram of Spark Coil" /></a> + </p> + <p> + A spark coil of either style consists of (<i>a</i>) a soft <i>iron core</i> + on which is wound (<i>b</i>) a couple of layers of heavy insulated wire + and this is called the <i>primary coil</i>, (<i>c</i>) while over this, + but insulated from it, is wound a large number of turns of very fine + insulated copper wire called the <i>secondary coil</i>; (<i>d</i>) an <i>interrupter</i>, + or <i>vibrator</i>, as it is commonly called, and, finally, (<i>e</i>) a + <i>condenser</i>. The core, primary and secondary coils form a unit and + these are set in a box or mounted on top of a hollow wooden base. The + condenser is placed in the bottom of the box, or on the base, while the + vibrator is mounted on one end of the box or on top of the base, and it is + the only part of the coil that needs adjusting. + </p> + <p> + The vibrator consists of a stiff, flat spring fixed at one end to the box + or base while it carries a piece of soft iron called an <i>armature</i> on + its free end and this sets close to one end of the soft iron core. + Insulated from this spring is a standard that carries an adjusting screw + on the small end of which is a platinum point and this makes contact with + a small platinum disk fixed to the spring. The condenser is formed of + alternate sheets of paper and tinfoil built up in the same fashion as the + receiving condenser described under the caption of <i>Fixed and Variable + Condensers</i>, in <a href="#chap03">Chapter III</a>. + </p> + <p> + The wiring diagram <i>C</i> shows how the spark coil is wired up. One of + the battery binding posts is connected with one end of the primary coil + while the other end of the latter which is wound on the soft iron core + connects with the spring of the vibrator. The other battery binding post + connects with the standard that supports the adjusting screw. The + condenser is shunted across the vibrator, that is, one end of the + condenser is connected with the spring and the other end of the condenser + is connected with the adjusting screw standard. The ends of the secondary + coil lead to two binding posts, which are usually placed on top of the + spark coil and it is to these that the spark gap is connected. + </p> + <p> + <i>The Battery.</i>--This can be formed of dry cells or you can use a + storage battery to energize your coil. For all coils that give less than a + 1-inch spark you should use 5 dry cells; for 1-and 2-inch spark coils use + 6 or 8 dry cells, and for 3 to 4-inch spark coils use 8 to 10 dry cells. + The way the dry cells are connected together to form a battery will be + shown presently. A dry cell is shown at <i>A</i> in <i>Fig, 19</i>. + </p> + <p> + <a name="fig019" id="fig019"><img width="600" height="389" + src="images/fig019.jpg" + alt="Fig. 19.--Other parts for Transmitting Set No. 1" /></a> + </p> + <p> + <i>The Telegraph Key.</i>--You can use an ordinary Morse telegraph key for + the sending set and you can get one with a japanned iron base for $1.50 + (or better, one made of brass and which has 1/8-inch silver contact points + for $3.00. A key of the latter kind is shown at <i>B</i>). + </p> + <p> + <i>The Spark gap.</i>--It is in the <i>spark gap</i> that the high tension + spark takes place. The apparatus in which the spark takes place is also + called the <i>spark gap</i>. It consists of a pair of zinc plugs, called + <i>electrodes</i>, fixed to the ends of a pair of threaded rods, with + knobs on the other ends, and these screw into and through a pair of + standards as shown at <i>c</i>. This is called a <i>fixed</i>, or <i>stationary + spark gap</i> and costs about $1.00. + </p> + <p> + <i>The Tuning Coil.</i>--The <i>transmitting inductance</i>, or <i>sending + tuning coil</i>, consists of 20 to 30 turns of <i>No. 8 or 9</i> hard + drawn copper wire wound on a slotted insulated form and mounted on a + wooden base. It is provided with <i>clips</i> so that you can cut in and + cut out as many turns of wire as you wish and so tune the sending circuits + to send out whatever wave length you desire. It is shown at <i>d</i>, and + costs about $5.00. See also <i>Oscillation Transformer</i>, page 63 + [Chapter IV]. + </p> + <p> + <i>The High Tension Condenser.</i>--High tension condensers, that is, + condensers which will stand up under <i>high potentials</i>, or electric + pressures, can be bought in units or sections. These condensers are made + up of thin brass plates insulated with a special compound and pressed into + a compact form. The <i>capacitance</i> [Footnote: This is the capacity of + the condenser.] of one section is enough for a transmitting set using a + spark coil that gives a 2 inch spark or less and two sections connected + together should be used for coils giving from 2 to 4 inch sparks. It is + shown at <i>e</i>. + </p> + <p> + <i>Connecting Up the Apparatus</i>.--Your sending set should be mounted on + a table, or a bench, where it need not be moved. Place the key in about + the middle of the table and down in front, and the spark coil to the left + and well to the back but so that the vibrator end will be to the right, as + this will enable you to adjust it easily. Place the battery back of the + spark coil and the tuning coil (oscillation transformer) to the right of + the spark coil and back of the key, all of which is shown in the layout at + <i>A</i> in <i>Fig. 20</i>. + </p> + <p> + <a name="fig020a" id="fig020a"><img width="600" height="549" + src="images/fig020a.jpg" + alt="(A) Fig. 20.--Top View of Apparatus Layout for Sending Set No. 1." /></a> + <a name="fig020b" id="fig020b"><img width="600" height="437" + src="images/fig020b.jpg" + alt="(B) Fig. 20.--Wiring of Diagram for Sending Set No. 1." /></a> + </p> + <p> + For the <i>low voltage circuit</i>, that is the battery circuit, use <i>No. + 12</i> or <i>14</i> insulated copper wire. Connect all of the dry cells + together in <i>series</i>, that is, connect the zinc of one cell with the + carbon of the next and so on until all of them are connected up. Then + connect the carbon of the end cell with one of the posts of the key, the + zinc of the other end cell with one of the primary posts of the spark coil + and the other primary post of the spark coil with the other post of the + key, when the primary circuit will be complete. + </p> + <p> + For the <i>high tension circuits</i>, that is, the <i>oscillation circuits</i>, + you may use either bare or insulated copper wire but you must be careful + that they do not touch the table, each other, or any part of the + apparatus, except, of course, the posts they are connected with. Connect + one of the posts of the secondary coil of the spark coil with one of the + posts of the spark gap, and the other post with one of the posts of the + condenser; then connect the other post of the condenser with the lower + spring clip of the tuning coil and also connect this clip with the ground. + This done, connect the middle spring clip with one of the posts of the + spark gap, and, finally, connect the top clip with the aerial wire and + your transmitting set is ready to be tuned. A wiring diagram of the + connections is shown at <i>B</i>. As this set is tuned in the same way as + <i>Set No. 2</i> which follows, you are referred to the end of this + chapter. + </p> + <p> + <i>A Better Transmitting Set (No. 2).</i>--The apparatus for this set + includes: (1) an <i>alternating current transformer</i>, (2) a <i>wireless + telegraph key</i>, (3) a <i>fixed</i>, a <i>rotary</i>, or a <i>quenched + spark gap</i>, (4) a <i>condenser</i>, and (5) an <i>oscillation + transformer</i>. If you have a 110 volt direct lighting current in your + home instead of 110 volt alternating current, then you will also need (6) + an <i>electrolytic interrupter</i>, for in this case the primary circuit + of the transformer must be made and broken rapidly in order to set up + alternating currents in the secondary coil. + </p> + <p> + <i>The Alternating Current Transformer.</i>--An alternating current, or + power, transformer is made on the same principle as a spark coil, that is, + it has a soft iron core, a primary coil formed of a couple of layers of + heavy wire, and a secondary coil wound up of a large number of turns of + very fine wire. Unlike the spark coil, however, which has an <i>open + magnetic core</i> and whose secondary coil is wound on the primary coil, + the transformer has a <i>closed magnetic core</i>, with the primary coil + wound on one of the legs of the core and the secondary wound on the other + leg. It has neither a vibrator nor a condenser. A plain transformer is + shown at <i>A</i> in <i>Fig. 21</i>. + </p> + <p> + <a name="fig021" id="fig021"><img width="600" height="584" + src="images/fig021.jpg" alt="Fig. 21.--Parts for Transmitting Set No. 2." /></a> + </p> + <p> + A transformer of this kind can be bought either (a) <i>unmounted</i>, that + is, just the bare transformer, or (b) <i>fully mounted</i>, that is, + fitted with an iron stand, mounted on an insulating base on which are a + pair of primary binding posts, while the secondary is provided with a <i>safety + spark gap</i>. There are three sizes of transformers of this kind made and + they are rated at 1/4, 1/2 and 1 kilowatt, respectively, they deliver a + secondary current of 9,000, 11,000 and 25,000 volts, according to size, + and cost $16.00, $22.00 and $33.00 when fully mounted; a reduction of + $3.00, $4.00 and $5.00 is made when they are unmounted. All of these + transformers operate on 110 volt, 60 cycle current and can be connected + directly to the source of alternating current. + </p> + <p> + <i>The Wireless Key</i>.--For this transmitting set a standard wireless + key should be used as shown at <i>B</i>. It is made about the same as a + regular telegraph key but it is much heavier, the contact points are + larger and instead of the current being led through the bearings as in an + ordinary key, it is carried by heavy conductors directly to the contact + points. This key is made in three sizes and the first will carry a current + of 5 <i>amperes</i> [Footnote: See <a href="#appendix">Appendix</a> for + definition.] and costs $4.00, the second will carry a current of 10 + amperes and costs $6.50, while the third will carry a current of 20 + amperes and costs $7.50. + </p> + <p> + <i>The Spark Gap.</i>--Either a fixed, a rotary, or a quenched spark gap + can be used with this set, but the former is seldom used except with + spark-coil sets, as it is very hard to keep the sparks from arcing when + large currents are used. A rotary spark gap comprises a wheel, driven by a + small electric motor, with projecting plugs, or electrodes, on it and a + pair of stationary plugs on each side of the wheel as shown at <i>C</i>. + The number of sparks per second can be varied by changing the speed of the + wheel and when it is rotated rapidly it sends out signals of a high pitch + which are easy to read at the receiving end. A rotary gap with a 110-volt + motor costs about $25.00. + </p> + <p> + A quenched spark gap not only eliminates the noise of the ordinary gap + but, when properly designed, it increases the range of an induction coil + set some 200 per cent. A 1/4 kilowatt quenched gap costs $10.00. + [Footnote: See <a href="#appendix">Appendix</a> for definition.] + </p> + <p> + <i>The High Tension Condenser</i>.--Since, if you are an amateur, you can + only send out waves that are 200 meters in length, you can only use a + condenser that has a capacitance of .007 <i>microfarad</i>. [Footnote: See + <a href="#appendix">Appendix</a> for definition.] A sectional high tension + condenser like the one described in connection with <i>Set No. 1</i> can + be used with this set but it must have a capacitance of not more than .007 + microfarad. A condenser of this value for a 1/4-kilowatt transformer costs + $7.00; for a 1/2-kilowatt transformer $14.00, and for a 1-kilowatt + transformer $21.00. See <i>E, Fig. 19</i>. + </p> + <p> + <i>The Oscillation Transformer</i>.--With an oscillation transformer you + can tune much more sharply than with a single inductance coil tuner. The + primary coil is formed of 6 turns of copper strip, or No. 9 copper wire, + and the secondary is formed of 9 turns of strip, or wire. The primary + coil, which is the outside coil, is hinged to the base and can be raised + or lowered like the lid of a box. When it is lowered the primary and + secondary coils are in the same plane and when it is raised the coils set + at an angle to each other. It is shown at <i>D</i> and costs $5.00. + </p> + <p> + <i>Connecting Up the Apparatus. For Alternating Current.</i>--Screw the + key to the table about the middle of it and near the front edge; place the + high tension condenser back of it and the oscillation transformer back of + the latter; set the alternating current transformer to the left of the + oscillation transformer and place the rotary or quenched spark gap in + front of it. + </p> + <p> + Now bring a pair of <i>No. 12</i> or <i>14</i> insulated wires from the + 110 volt lighting leads and connect them with a single-throw, double-pole + switch; connect one pole of the switch with one of the posts of the + primary coil of the alternating power transformer and connect the other + post of the latter with one of the posts of your key, and the other post + of this with the other pole of the switch. Now connect the motor of the + rotary spark gap to the power circuit and put a single-pole, single-throw + switch in the motor circuit, all of which is shown at <i>A</i> in <i>Fig. + 22</i>. + </p> + <p> + <a name="fig022a" id="fig022a"><img width="600" height="614" + src="images/fig022a.jpg" + alt="(A) Fig. 22.--Top View of Apparatus Layout for Sending Set No. 2." /></a> + <a name="fig022b" id="fig022b"><img width="600" height="453" + src="images/fig022b.jpg" + alt="(B) Fig. 22.--Wiring Diagram for Sending Set No. 2." /></a> + </p> + <p> + Next connect the posts of the secondary coil to the posts of the rotary or + quenched spark gap and connect one post of the latter to one post of the + condenser, the other post of this to the post of the primary coil of the + oscillation transformer, which is the inside coil, and the clip of the + primary coil to the other spark gap post. This completes the closed + oscillation circuit. Finally connect the post of the secondary coil of the + oscillation transformer to the ground and the clip of it to the wire + leading to the aerial when you are ready to tune the set. A wiring diagram + of the connections is shown at <i>B</i>. + </p> + <p> + <i>For Direct Current.</i>--Where you have 110 volt direct current you + must connect in an electrolytic interrupter. This interrupter, which is + shown at <i>A</i> and <i>B</i> in <i>Fig. 23</i>, consists of (1) a jar + filled with a solution of 1 part of sulphuric acid and 9 parts of water, + (2) a lead electrode having a large surface fastened to the cover of + surface that sets in a porcelain sleeve and whose end rests on the bottom + of the jar. + </p> + <p> + <a name="fig023" id="fig023"><img width="600" height="412" + src="images/fig023.jpg" + alt="Fig. 23.--Using 110 Volt Direct Current with an Alternating Current Transformer." /> + </a> + </p> + <p> + When these electrodes are connected in series with the primary of a large + spark coil or an alternating current transformer, see <i>C</i>, and a + direct current of from 40 to 110 volts is made to pass through it, the + current is made and broken from 1,000 to 10,000 times a minute. By raising + or lowering the sleeve, thus exposing more or less of the platinum, or + alloy point, the number of interruptions per minute can be varied at will. + As the electrolytic interrupter will only operate in one direction, you + must connect it with its platinum, or alloy anode, to the + or <i>positive</i> + power lead and the lead cathode to the - or <i>negative</i> power lead. + You can find out which is which by connecting in the interrupter and + trying it, or you can use a polarity indicator. An electrolytic + interrupter can be bought for as little as $3.00. + </p> + <p> + <i>How to Adjust Your Transmitter. Tuning With a Hot Wire Ammeter</i>.--A + transmitter can be tuned in two different ways and these are: (1) by + adjusting the length of the spark gap and the tuning coil so that the + greatest amount of energy is set up in the oscillating circuits, and (2) + by adjusting the apparatus so that it will send out waves of a given + length. + </p> + <p> + To adjust the transmitter so that the circuits will be in tune you should + have a <i>hot wire ammeter</i>, or radiation ammeter, as it is called, + which is shown in <i>Fig. 24</i>. It consists of a thin platinum wire + through which the high-frequency currents surge and these heat it; the + expansion and contraction of the wire moves a needle over a scale marked + off into fractions of an ampere. When the spark gap and tuning coil of + your set are properly adjusted, the needle will swing farthest to the + right over the scale and you will then know that the aerial wire system, + or open oscillation circuit, and the closed oscillation circuit are in + tune and radiating the greatest amount of energy. + </p> + <p> + <a name="fig024" id="fig024"><img width="400" height="427" + src="images/fig024.jpg" alt="Fig. 24.--Principle of the Hot Wire Ammeter." /></a> + </p> + <p> + <i>To Send Out a 200 Meter Wave Length.</i>--If you are using a condenser + having a capacitance of .007 microfarad, which is the largest capacity + value that the Government will allow an amateur to use, then if you have a + hot wire ammeter in your aerial and tune the inductance coil or coils + until the ammeter shows the largest amount of energy flowing through it + you will know that your transmitter is tuned and that the aerial is + sending out waves whose length is 200 meters. To tune to different wave + lengths you must have a <i>wave-meter</i>. + </p> + <p> + <i>The Use of the Aerial Switch.</i>--Where you intend to install both a + transmitter and a receptor you will need a throwover switch, or <i>aerial + switch</i>, as it is called. An ordinary double-pole, double-throw switch, + as shown at <i>A</i> in <i>Fig. 25</i>, can be used, or a switch made + especially for the purpose as at <i>B</i> is handier because the arc of + the throw is much less. + </p> + <p> + <a name="fig025" id="fig025"><img width="600" height="279" + src="images/fig025.jpg" alt="Fig. 25.--Kinds of Aerial Switches." /></a> + </p> + <p> + <i>Aerial Switch for a Complete Sending and Receiving Set</i>.--You can + buy a double-pole, double-throw switch mounted on a porcelain base for + about 75 cents and this will serve for <i>Set No. 1</i>. Screw this switch + on your table between the sending and receiving sets and then connect one + of the middle posts of it with the ground wire and the other middle post + with the lightning switch which connects with the aerial. Connect the post + of the tuning coil with one of the end posts of the switch and the clip of + the tuning coil with the other and complementary post of the switch. This + done, connect one of the opposite end posts of the switch to the post of + the receiving tuning coil and connect the sliding contact of the latter + with the other and complementary post of the switch as shown in <i>Fig. 26</i>. + </p> + <p> + <a name="fig026" id="fig026"><img width="600" height="451" + src="images/fig026.jpg" + alt="Fig. 26.--Wiring Diagram for Complete Sending and Receiving Set No. 1." /> + </a> + </p> + <p> + <i>Connecting in the Lightning Switch.</i>--The aerial wire connects with + the middle post of the lightning switch, while one of the end posts lead + to one of the middle posts of the aerial switch. The other end post of the + lightning switch leads to a separate ground outside the building, as the + wiring diagrams <i>Figs. 26</i> and <i>27</i> show. + </p> + <p> + <a name="fig027" id="fig027"><img width="600" height="386" + src="images/fig027.jpg" + alt="Fig. 27.--Wiring Diagram for Complete Sending and Receiving Set No. 2." /> + </a> + </p> + <h2> + <a name="chap05" id="chap05">CHAPTER V</a> + </h2> + <h3> + ELECTRICITY SIMPLY EXPLAINED + </h3> + <p> + It is easy to understand how electricity behaves and what it does if you + get the right idea of it at the start. In the first place, if you will + think of electricity as being a fluid like water its fundamental actions + will be greatly simplified. Both water and electricity may be at rest or + in motion. When at rest, under certain conditions, either one will develop + pressure, and this pressure when released will cause them to flow through + their respective conductors and thus produce a current. + </p> + <p> + <i>Electricity at Rest and in Motion</i>.--Any wire or a conductor of any + kind can be charged with electricity, but a Leyden jar, or other + condenser, is generally used to hold an electric charge because it has a + much larger <i>capacitance</i>, as its capacity is called, than a wire. As + a simple analogue of a condenser, suppose you have a tank of water raised + above a second tank and that these are connected together by means of a + pipe with a valve in it, as shown at <i>A</i> in <i>Fig. 28</i>. + </p> + <p> + <a name="fig028" id="fig028"><img width="594" height="320" + src="images/fig028.jpg" + alt="Fig. 28.--Water Analogue for Electric Pressure." /></a> + </p> + <table cellspacing="20" summary="Illustration"> + <tr> + <td align="center"> + <i>Photograph unavailable</i> + </td> + </tr> + <tr> + <td align="center"> + original © Underwood and Underwood.<br /> First Wireless College + in the World, at Tufts College, Mass. + </td> + </tr> + </table> + <p> + Now if you fill the upper tank with water and the valve is turned off, no + water can flow into the lower tank but there is a difference of pressure + between them, and the moment you turn the valve on a current of water will + flow through the pipe. In very much the same way when you have a condenser + charged with electricity the latter will be under <i>pressure,</i> that + is, a <i>difference of potential</i> will be set up, for one of the sheets + of metal will be charged positively and the other one, which is insulated + from it, will be charged negatively, as shown at <i>B</i>. On closing the + switch the opposite charges rush together and form a current which flows + to and fro between the metal plates. [Footnote: Strictly speaking it is + the difference of potential that sets up the electromotive force.] + </p> + <p> + <i>The Electric Current and Its Circuit</i>.--Just as water flowing + through a pipe has <i>quantity</i> and <i>pressure</i> back of it and the + pipe offers friction to it which tends to hold back the water, so, + likewise, does electricity flowing in a circuit have: (1) <i>quantity</i>, + or <i>current strength</i>, or just <i>current</i>, as it is called for + short, or <i>amperage</i>, and (2) <i>pressure</i>, or <i>potential + difference</i>, or <i>electromotive force</i>, or <i>voltage</i>, as it is + variously called, and the wire, or circuit, in which the current is + flowing has (3) <i>resistance</i> which tends to hold back the current. + </p> + <p> + A definite relation exists between the current and its electromotive force + and also between the current, electromotive force and the resistance of + the circuit; and if you will get this relationship clearly in your mind + you will have a very good insight into how direct and alternating currents + act. To keep a quantity of water flowing in a loop of pipe, which we will + call the circuit, pressure must be applied to it and this may be done by a + rotary pump as shown at <i>A in Fig. 29;</i> in the same way, to keep a + quantity of electricity flowing in a loop of wire, or circuit, a battery, + or other means for generating electric pressure must be used, as shown at + <i>B</i>. + </p> + <p> + <a name="fig029" id="fig029"><img width="600" height="291" + src="images/fig029.jpg" + alt="Fig. 29.--Water Analogues for Direct and Alternating Currents." /></a> + </p> + <p> + If you have a closed pipe connected with a piston pump, as at <i>C</i>, as + the piston moves to and fro the water in the pipe will move first one way + and then the other. So also when an alternating current generator is + connected to a wire circuit, as at <i>D</i>, the current will flow first + in one direction and then in the other, and this is what is called an <i>alternating + current</i>. + </p> + <p> + <i>Current and the Ampere</i>.--The amount of water flowing in a closed + pipe is the same at all parts of it and this is also true of an electric + current, in that there is exactly the same quantity of electricity at one + point of the circuit as there is at any other. + </p> + <p> + The amount of electricity, or current, flowing in a circuit in a second is + measured by a unit called the <i>ampere</i>, [Footnote: For definition of + <i>ampere</i> see <a href="#appendix">Appendix.</a>] and it is expressed + by the symbol I. [Footnote: This is because the letter <i>C</i> is used + for the symbol of <i>capacitance</i>] Just to give you an idea of the + quantity of current an <i>ampere</i> is we will say that a dry cell when + fresh gives a current of about 20 amperes. To measure the current in + amperes an instrument called an <i>ammeter</i> is used, as shown at <i>A</i> + in <i>Fig. 30</i>, and this is always connected in <i>series</i> with the + line, as shown at <i>B</i>. + </p> + <p> + <a name="fig030" id="fig030"><img width="600" height="547" + src="images/fig030.jpg" + alt="Fig. 30.--How the Ammeter and Voltmeter are Used." /></a> + </p> + <p> + <i>Electromotive Force and the Volt</i>.--When you have a pipe filled with + water or a circuit charged with electricity and you want to make them flow + you must use a pump in the first case and a battery or a dynamo in the + second case. It is the battery or dynamo that sets up the electric + pressure as the circuit itself is always charged with electricity. + </p> + <p> + The more cells you connect together in <i>series</i> the greater will be + the electric pressure developed and the more current it will move along + just as the amount of water flowing in a pipe can be increased by + increasing the pressure of the pump. The unit of electromotive force is + the <i>volt</i>, and this is the electric pressure which will force a + current of <i>1 ampere</i> through a resistance of <i>1 ohm</i>; it is + expressed by the symbol <i>E</i>. A fresh dry cell will deliver a current + of about 1.5 volts. To measure the pressure of a current in volts an + instrument called a <i>voltmeter</i> is used, as shown at <i>C</i> in <i>Fig. + 30</i>, and this is always connected across the circuit, as shown at <i>D</i>. + </p> + <p> + <i>Resistance and the Ohm.</i>--Just as a water pipe offers a certain + amount of resistance to the flow of water through it, so a circuit opposes + the flow of electricity in it and this is called <i>resistance</i>. + Further, in the same way that a small pipe will not allow a large amount + of water to flow through it, so, too, a thin wire limits the flow of the + current in it. + </p> + <p> + If you connect a <i>resistance coil</i> in a circuit it acts in the same + way as partly closing the valve in a pipe, as shown at <i>A</i> and <i>B</i> + in <i>Fig. 31</i>. The resistance of a circuit is measured by a unit + called the <i>ohm</i>, and it is expressed by the symbol <i>R</i>. A No. + 10, Brown and Sharpe gauge soft copper wire, 1,000 feet long, has a + resistance of about 1 ohm. To measure the resistance of a circuit an + apparatus called a <i>resistance bridge is used</i>. The resistance of a + circuit can, however, be easily calculated, as the following shows. + </p> + <p> + <a name="fig031" id="fig031"><img width="600" height="370" + src="images/fig031.jpg" + alt="Fig. 31.--Water Valve Analogue of Electric Resistance. A- a valve limits the flow of water. B- a resistance limits the flow of current." /> + </a> + </p> + <p> + <i>What Ohm's Law Is</i>.--If, now, (1) you know what the current flowing + in a circuit is in <i>amperes</i>, and the electromotive force, or + pressure, is in <i>volts</i>, you can then easily find what the resistance + is in <i>ohms</i> of the circuit in which the current is flowing by this + formula: + </p> +<pre xml:space="preserve"> + Volts E + --------- = Ohms, or --- = R + Amperes I +</pre> + <p> + That is, if you divide the current in amperes by the electromotive force + in volts the quotient will give you the resistance in ohms. + </p> + <p> + Or (2) if you know what the electromotive force of the current is in <i>volts</i> + and the resistance of the circuit is in <i>ohms</i> then you can find what + the current flowing in the circuit is in <i>amperes</i>, thus: + </p> +<pre xml:space="preserve"> + Volts E + ----- = Amperes, or --- = I + Ohms R +</pre> + <p> + That is, by dividing the resistance of the circuit in ohms, by the + electromotive force of the current you will get the amperes flowing in the + circuit. + </p> + <p> + Finally (3) if you know what the resistance of the circuit is in <i>ohms</i> + and the current is in <i>amperes</i> then you can find what the + electromotive force is in <i>volts</i> since: + </p> +<pre xml:space="preserve"> + Ohms x Amperes = Volts, or R x I = E +</pre> + <p> + That is, if you multiply the resistance of the circuit in ohms by the + current in amperes the result will give you the electromotive force in + volts. + </p> + <p> + From this you will see that if you know the value of any two of the + constants you can find the value of the unknown constant by a simple + arithmetical process. This relation between these three constants is known + as <i>Ohm's Law</i> and as they are very important you should memorize + them. + </p> + <p> + <i>What the Watt and Kilowatt Are.</i>--Just as <i>horsepower</i> or <i>H.P.</i>, + is the unit of work that steam has done or can do, so the <i>watt</i> is + the unit of work that an electric current has done or can do. To find the + <i>watts</i> a current develops you need only to multiply the <i>amperes</i> + by the <i>volts</i>. There are <i>746 watts</i> to <i>1 horsepower, and + 1,000 watts are equal to 1 kilowatt</i>. + </p> + <p> + <i>Electromagnetic Induction.</i>--To show that a current of electricity + sets up a magnetic field around it you have only to hold a compass over a + wire whose ends are connected with a battery when the needle will swing at + right angles to the length of the wire. By winding an insulated wire into + a coil and connecting the ends of the latter with a battery you will find, + if you test it with a compass, that the coil is magnetic. + </p> + <p> + This is due to the fact that the energy of an electric current flowing in + the wire is partly changed into magnetic lines of force which rotate at + right angles about it as shown at <i>A</i> in <i>Fig. 32</i>. The magnetic + field produced by the current flowing in the coil is precisely the same as + that set up by a permanent steel magnet. Conversely, when a magnetic line + of force is set up a part of its energy goes to make up electric currents + which whirl about in a like manner, as shown at <i>B</i>. + </p> + <p> + <a name="fig032ab" id="fig032ab"><img width="600" height="429" + src="images/fig032ab.jpg" + alt="(A) and (B) Fig. 32.--How an Electric Current is Changed into Magnetic Lines of Force and These into an Electric Current." /> + </a> <a name="fig032cd" id="fig032cd"><img width="600" height="504" + src="images/fig032cd.jpg" + alt="(C) and (D) Fig. 32.--How an Electric Current Sets up a Magnetic Field." /> + </a> + </p> + <p> + <i>Self-induction or Inductance</i>.--When a current is made to flow in a + coil of wire the magnetic lines of force produced are concentrated, as at + C, just as a lens concentrates rays of light, and this forms an intense <i>magnetic + field</i>, as it is called. Now if a bar of soft iron is brought close to + one end of the coil of wire, or, better still, if it is pushed into the + coil, it will be magnetized by <i>electromagnetic induction,</i> see <i>D,</i> + and it will remain a magnet until the current is cut off. + </p> + <p> + <i>Mutual Induction</i>.--When two loops of wire, or better, two coils of + wire, are placed close together the electromagnetic induction between them + is reactive, that is, when a current is made to flow through one of the + coils closed magnetic lines of force are set up and when these cut the + other loop or turns of wire of the other coil, they in turn produce + electric currents in it. + </p> + <p> + It is the mutual induction that takes place between two coils of wire + which makes it possible to transform <i>low voltage currents</i> from a + battery or a 110 volt source of current into high pressure currents, or <i>high + potential currents</i>, as they are called, by means of a spark coil or a + transformer, as well as to <i>step up</i> and <i>step down</i> the + potential of the high frequency currents that are set up in sending and + receiving oscillation transformers. Soft iron cores are not used in + oscillation inductance coils and oscillation transformers for the reason + that the frequency of the current is so high the iron would not have time + to magnetize and demagnetize and so would not help along the mutual + induction to any appreciable extent. + </p> + <p> + <i>High-Frequency Currents</i>.--High frequency currents, or electric + oscillations as they are called, are currents of electricity that surge to + and fro in a circuit a million times, more or less, per second. Currents + of such high frequencies will <i>oscillate</i>, that is, surge to and fro, + in an <i>open circuit</i>, such as an aerial wire system, as well as in a + <i>closed circuit</i>. + </p> + <p> + Now there is only one method by which currents of high frequency, or <i>radio-frequency</i>, + as they are termed, can be set up by spark transmitters, and this is by + discharging a charged condenser through a circuit having a small + resistance. To charge a condenser a spark coil or a transformer is used + and the ends of the secondary coil, which delivers the high potential + alternating current, are connected with the condenser. To discharge the + condenser automatically a <i>spark,</i> or an <i>arc,</i> or the <i>flow + of electrons</i> in a vacuum tube, is employed. + </p> + <p> + <i>Constants of an Oscillation Circuit.</i>--An oscillation circuit, as + pointed out before, is one in which high frequency currents surge or + oscillate. Now the number of times a high frequency current will surge + forth and back in a circuit depends upon three factors of the latter and + these are called the constants of the circuit, namely: (1) its <i>capacitance,</i> + (2) its <i>inductance</i> and (3) its <i>resistance.</i> + </p> + <p> + <i>What Capacitance Is</i>.--The word <i>capacitance</i> means the <i>electrostatic + capacity</i> of a condenser or a circuit. The capacitance of a condenser + or a circuit is the quantity of electricity which will raise its pressure, + or potential, to a given amount. The capacitance of a condenser or a + circuit depends on its size and form and the voltage of the current that + is charging it. + </p> + <p> + The capacitance of a condenser or a circuit is directly proportional to + the quantity of electricity that will keep the charge at a given + potential. The <i>farad,</i> whose symbol is<i>M,</i> is the unit of + capacitance and a condenser or a circuit to have a capacitance of one + farad must be of such size that one <i>coulomb,</i> which is the unit of + electrical quantity, will raise its charge to a potential of one volt. + Since the farad is far too large for practical purposes a millionth of a + farad, or <i>microfarad</i>, whose symbol is <i>mfd.</i>, is used. + </p> + <p> + <i>What Inductance Is.</i>--Under the sub-caption of <i>Self-induction</i> + and <i>Inductance</i> in the beginning of this chapter it was shown that + it was the inductance of a coil that makes a current flowing through it + produce a strong magnetic field, and here, as one of the constants of an + oscillation circuit, it makes a high-frequency current act as though it + possessed <i>inertia</i>. + </p> + <p> + Inertia is that property of a material body that requires time and energy + to set in motion, or stop. Inductance is that property of an oscillation + circuit that makes an electric current take time to start and time to + stop. Because of the inductance, when a current flows through a circuit it + causes the electric energy to be absorbed and changes a large part of it + into magnetic lines of force. Where high frequency currents surge in a + circuit the inductance of it becomes a powerful factor. The practical unit + of inductance is the <i>henry</i> and it is represented by the symbol <i>L</i>. + </p> + <p> + <i>What Resistance Is.</i>--The resistance of a circuit to high-frequency + currents is different from that for low voltage direct or alternating + currents, as the former do not sink into the conductor to nearly so great + an extent; in fact, they stick practically to the surface of it, and hence + their flow is opposed to a very much greater extent. The resistance of a + circuit to high frequency currents is generally found in the spark gap, + arc gap, or the space between the electrodes of a vacuum tube. The unit of + resistance is, as stated, the <i>ohm</i>, and its symbol is <i>R</i>. + </p> + <p> + <i>The Effect of Capacitance, Inductance and Resistance on Electric + Oscillations</i>.--If an oscillation circuit in which high frequency + currents surge has a large resistance, it will so oppose the flow of the + currents that they will be damped out and reach zero gradually, as shown + at <i>A</i> in <i>Fig. 33</i>. But if the resistance of the circuit is + small, and in wireless circuits it is usually so small as to be + negligible, the currents will oscillate, until their energy is damped out + by radiation and other losses, as shown at <i>B</i>. + </p> + <p> + <a name="fig033" id="fig033"><img width="600" height="370" + src="images/fig033.jpg" + alt="Fig. 33.--The Effect of Resistance on the Discharge of an Electric Current." /> + </a> + </p> + <p> + As the capacitance and the inductance of the circuit, which may be made of + any value, that is amount, you wish, determines the <i>time period</i>, + that is, the length of time for a current to make one complete + oscillation, it must be clear that by varying the values of the condenser + and the inductance coil you can make the high frequency current oscillate + as fast or as slow as you wish within certain limits. Where the electric + oscillations that are set up are very fast, the waves sent out by the + aerial will be short, and, conversely, where the oscillations are slow the + waves emitted will be long. + </p> + <h2> + <a name="chap06" id="chap06">CHAPTER VI</a> + </h2> + <h3> + HOW THE TRANSMITTING AND RECEIVING SETS WORK + </h3> + <p> + The easiest way to get a clear conception of how a wireless transmitter + sends out electric waves and how a wireless receptor receives them is to + take each one separately and follow: (1) in the case of the transmitter, + the transformation of the low voltage direct, or alternating current into + high potential alternating currents; then find out how these charge the + condenser, how this is discharged by the spark gap and sets up + high-frequency currents in the oscillation circuits; then (2) in the case + of the receptor, to follow the high frequency currents that are set up in + the aerial wire and learn how they are transformed into oscillations of + lower potential when they have a larger current strength, how these are + converted into intermittent direct currents by the detector and which then + flow into and operate the telephone receiver. + </p> + <p> + <i>How Transmitting Set No. 1 Works. The Battery and Spark Coil Circuit</i>.--When + you press down on the knob of the key the silver points of it make contact + and this closes the circuit; the low voltage direct current from the + battery now flows through the primary coil of the spark coil and this + magnetizes the soft iron core. The instant it becomes magnetic it pulls + the spring of the vibrator over to it and this breaks the circuit; when + this takes place the current stops flowing through the primary coil; this + causes the core to lose its magnetism when the vibrator spring flies back + and again makes contact with the adjusting screw; then the cycle of + operations is repeated. + </p> + <p> + A condenser is connected across the contact points of the vibrator since + this gives a much higher voltage at the ends of the secondary coil than + where the coil is used without it; this is because: (1) the self-induction + of the primary coil makes the pressure of the current rise and when the + contact points close the circuit again it discharges through the primary + coil, and (2) when the break takes place the current flows into the + condenser instead of arcing across the contact points. + </p> + <p> + <i>Changing the Primary Spark Coil Current Into Secondary Currents</i>.--Now + every time the vibrator contact points close the primary circuit the + electric current in the primary coil is changed into closed magnetic lines + of force and as these cut through the secondary coil they set up in it a + <i>momentary current</i> in one direction. Then the instant the vibrator + points break apart the primary circuit is opened and the closed magnetic + lines of force contract and as they do so they cut the turns of wire in + the secondary coil in the opposite direction and this sets up another + momentary current in the secondary coil in the other direction. The result + is that the low voltage direct current of the battery is changed into + alternating currents whose frequency is precisely that of the spring + vibrator, but while the frequency of the currents is low their potential, + or voltage, is enormously increased. + </p> + <p> + <i>What Ratio of Transformation Means.</i>--To make a spark coil step up + the low voltage direct current into high potential alternating current the + primary coil is wound with a couple of layers of thick insulated copper + wire and the secondary is wound with a thousand, more or less, number of + turns with very fine insulated copper wire. If the primary and secondary + coils were wound with the same number of turns of wire then the pressure, + or voltage, of the secondary coil at its terminals would be the same as + that of the current which flowed through the primary coil. Under these + conditions the <i>ratio of transformation</i>, as it is called, would be + unity. + </p> + <p> + The ratio of transformation is directly proportional to the number of + turns of wire on the primary and secondary coils and, since this is the + case, if you wind 10 turns of wire on the primary coil and 1,000 turns of + wire on the secondary coil then you will get 100 times as high a pressure, + or voltage, at the terminals of the secondary as that which you caused to + flow through the primary coil, but, naturally, the current strength, or + amperage, will be proportionately decreased. + </p> + <p> + <i>The Secondary Spark Coil Circuit.</i>--This includes the secondary coil + and the spark gap which are connected together. When the alternating, but + high potential, currents which are developed by the secondary coil, reach + the balls, or <i>electrodes</i>, of the spark gap the latter are + alternately charged positively and negatively. + </p> + <p> + Now take a given instant when one electrode is charged positively and the + other one is charged negatively, then when they are charged to a high + enough potential the electric strain breaks down the air gap between them + and the two charges rush together as described in the chapter before this + one in connection with the discharge of a condenser. When the charges rush + together they form a current which burns out the air in the gap and this + gives rise to the spark, and as the heated gap between the two electrodes + is a very good conductor the electric current surges forth and back with + high frequency, perhaps a dozen times, before the air replaces that which + has burned out. It is the inrushing air to fill the vacuum of the gap that + makes the crackling noise which accompanies the discharge of the electric + spark. + </p> + <p> + In this way then electric oscillations of the order of a million, more or + less, are produced and if an aerial and a ground wire are connected to the + spark balls, or electrodes, the oscillations will surge up and down it and + the energy of these in turn, are changed into electric waves which travel + out into space. An open circuit transmitter of this kind will send out + waves that are four times as long as the aerial itself, but as the waves + it sends out are strongly damped the Government will not permit it to be + used. + </p> + <p> + <i>The Closed Oscillation Circuit.</i>--By using a closed oscillation + circuit the transmitter can be tuned to send out waves of a given length + and while the waves are not so strongly damped more current can be sent + into the aerial wire system. The closed oscillation circuit consists of: + (1) a <i>spark gap</i>, (2) a <i>condenser</i> and (3) an <i>oscillation + transformer</i>. The high potential alternating current delivered by the + secondary coil not only charges the spark gap electrodes which necessarily + have a very small capacitance, but it charges the condenser which has a + large capacitance and the value of which can be changed at will. + </p> + <p> + Now when the condenser is fully charged it discharges through the spark + gap and then the electric oscillations set up surge to and fro through the + closed circuit. As a closed circuit is a very poor radiator of energy, + that is, the electric oscillations are not freely converted into electric + waves by it, they surge up to, and through the aerial wire; now as the + aerial wire is a good radiator nearly all of the energy of the electric + oscillations which surge through it are converted into electric waves. + </p> + <p> + <i>How Transmitting Set No. 2 Works. With Alternating Current.</i> The + operation of a transmitting set that uses an alternating current + transformer, or <i>power transformer,</i> as it is sometimes called, is + even more simple than one using a spark coil. The transformer needs no + vibrator when used with alternating current. The current from a generator + flows through the primary coil of the transformer and the alternations of + the usual lighting current is 60 cycles per second. This current sets up + an alternating magnetic field in the core of the transformer and as these + magnetic lines of force expand and contract they set up alternating + currents of the same frequency but of much higher voltage at the terminals + of the secondary coil according to the ratio of the primary and secondary + turns of wire as explained under the sub-caption of <i>Ratio of + Transformation</i>. + </p> + <p> + <i>With Direct Current</i>.--When a 110 volt direct current is used to + energize the power transformer an <i>electrolytic</i> interruptor is + needed to make and break the primary circuit, just as a vibrator is needed + for the same purpose with a spark coil. When the electrodes are connected + in series with the primary coil of a transformer and a source of direct + current having a potential of 40 to 110 volts, bubbles of gas are formed + on the end of the platinum, or alloy anode, which prevent the current from + flowing until the bubbles break and then the current flows again, in this + way the current is rapidly made and broken and the break is very sharp. + </p> + <p> + Where this type of interrupter is employed the condenser that is usually + shunted around the break is not necessary as the interrupter itself has a + certain inherent capacitance, due to electrolytic action, and which is + called its <i>electrolytic capacitance</i>, and this is large enough to + balance the self-induction of the circuit since the greater the number of + breaks per minute the smaller the capacitance required. + </p> + <p> + <i>The Rotary Spark Gap</i>.--In this type of spark gap the two fixed + electrodes are connected with the terminals of the secondary coil of the + power transformer and also with the condenser and primary of the + oscillation transformer. Now whenever any pair of electrodes on the + rotating disk are in a line with the pair of fixed electrodes a spark will + take place, hence the pitch of the note depends on the speed of the motor + driving the disk. This kind of a rotary spark-gap is called <i>non-synchronous</i> + and it is generally used where a 60 cycle alternating current is available + but it will work with other higher frequencies. + </p> + <p> + <i>The Quenched Spark Gap</i>.--If you strike a piano string a single + quick blow it will continue to vibrate according to its natural period. + This is very much the way in which a quenched spark gap sets up + oscillations in a coupled closed and open circuit. The oscillations set up + in the primary circuit by a quenched spark make only three or four sharp + swings and in so doing transfer all of their energy over to the secondary + circuit, where it will oscillate some fifty times or more before it is + damped out, because the high frequency currents are not forced, but simply + oscillate to the natural frequency of the circuit. For this reason the + radiated waves approach somewhat the condition of continuous waves, and so + sharper tuning is possible. + </p> + <p> + <i>The Oscillation Transformer.</i>--In this set the condenser in the + closed circuit is charged and discharged and sets up oscillations that + surge through the closed circuit as in <i>Set No. 1</i>. In this set, + however, an oscillation transformer is used and as the primary coil of it + is included in the closed circuit the oscillations set up in it produce + strong oscillating magnetic lines of force. The magnetic field thus + produced sets up in turn electric oscillations in the secondary coil of + the oscillation transformer and these surge through the aerial wire system + where their energy is radiated in the form of electric waves. + </p> + <p> + The great advantage of using an oscillation transformer instead of a + simple inductance coil is that the capacitance of the closed circuit can + be very much larger than that of the aerial wire system. This permits more + energy to be stored up by the condenser and this is impressed on the + aerial when it is radiated as electric waves. + </p> + <p> + <i>How Receiving Set No. I Works.</i>--When the electric waves from a + distant sending station impinge on the wire of a receiving aerial their + energy is changed into electric oscillations that are of exactly the same + frequency (assuming the receptor is tuned to the transmitter) but whose + current strength (amperage) and potential (voltage) are very small. These + electric waves surge through the closed circuit but when they reach the + crystal detector the contact of the metal point on the crystal permits + more current to flow through it in one direction than it will allow to + pass in the other direction. For this reason a crystal detector is + sometimes called a <i>rectifier</i>, which it really is. + </p> + <p> + Thus the high frequency currents which the steel magnet cores of the + telephone receiver would choke off are changed by the detector into + intermittent direct currents which can flow through the magnet coils of + the telephone receiver. Since the telephone receiver chokes off the + oscillations, a small condenser can be shunted around it so that a + complete closed oscillation circuit is formed and this gives better + results. + </p> + <p> + When the intermittent rectified current flows through the coils of the + telephone receiver it energizes the magnet as long as it lasts, when it is + de-energized; this causes the soft iron disk, or <i>diaphragm</i> as it is + called, which sets close to the ends of the poles of the magnet, to + vibrate; and this in turn gives forth sounds such as dots and dashes, + speech or music, according to the nature of the electric waves that sent + them out at the distant station. + </p> + <p> + <i>How Receiving Set No. 2 Works.</i>--When the electric oscillations that + are set up by the incoming electric waves on the aerial wire surge through + the primary coil of the oscillation transformer they produce a magnetic + field and as the lines of force of the latter cut the secondary coil, + oscillations of the same frequency are set up in it. The potential + (voltage) of these oscillations are, however, <i>stepped down</i> in the + secondary coil and, hence, their current strength (amperes) is increased. + </p> + <p> + The oscillations then flow through the closed circuit where they are + rectified by the crystal detector and transformed into sound waves by the + telephone receiver as described in connection with <i>Set No. 1</i>. The + variable condenser shunted across the closed circuit permits finer + secondary tuning to be done than is possible without it. Where you are + receiving continuous waves from a wireless telephone transmitter (speech + or music) you have to tune sharper than is possible with the tuning coil + alone and to do this a variable condenser connected in parallel with the + secondary coil is necessary. + </p> + <h2> + <a name="chap07" id="chap07">CHAPTER VII</a> + </h2> + <h3> + MECHANICAL AND ELECTRICAL TUNING + </h3> + <p> + There is a strikingly close resemblance between <i>sound waves</i> and the + way they are set up in <i>the air</i> by a mechanically vibrating body, + such as a steel spring or a tuning fork, and <i>electric waves</i> and the + way they are set up in <i>the ether</i> by a current oscillating in a + circuit. As it is easy to grasp the way that sound waves are produced and + behave something will be told about them in this chapter and also an + explanation of how electric waves are produced and behave and thus you + will be able to get a clear understanding of them and of tuning in + general. + </p> + <p> + <i>Damped and Sustained Mechanical Vibrations</i>.--If you will place one + end of a flat steel spring in a vice and screw it up tight as shown at <i>A</i> + in <i>Fig. 34</i>, and then pull the free end over and let it go it will + vibrate to and fro with decreasing amplitude until it comes to rest as + shown at <i>B</i>. When you pull the spring over you store up energy in it + and when you let it go the stored up energy is changed into energy of + motion and the spring moves forth and back, or <i>vibrates</i> as we call + it, until all of its stored up energy is spent. + </p> + <p> + <a name="fig034" id="fig034"><img width="600" height="474" + src="images/fig034.jpg" + alt="Fig. 34.--Damped and Sustained Mechanical Vibrations." /></a> + </p> + <p> + If it were not for the air surrounding it and other frictional losses, the + spring would vibrate for a very long time as the stored up energy and the + energy of motion would practically offset each other and so the energy + would not be used up. But as the spring beats the air the latter is sent + out in impulses and the conversion of the vibrations of the spring into + waves in the air soon uses up the energy you have imparted to it and it + comes to rest. + </p> + <p> + In order to send out <i>continuous waves</i> in the air instead of <i>damped + waves</i> as with a flat steel spring you can use an <i>electric driven + tuning fork</i>, see <i>C</i>, in which an electromagnet is fixed on the + inside of the prongs and when this is energized by a battery current the + vibrations of the prongs of the fork are kept going, or are <i>sustained</i>, + as shown in the diagram at <i>D</i>. + </p> + <p> + <i>Damped and Sustained Electric Oscillations</i>.--The vibrating steel + spring described above is a very good analogue of the way that damped + electric oscillations which surge in a circuit set up and send out + periodic electric waves in the ether while the electric driven tuning fork + just described is likewise a good analogue of how sustained oscillations + surge in a circuit and set up and send out continuous electric waves in + the ether as the following shows. + </p> + <p> + Now the inductance and resistance of a circuit such as is shown at <i>A</i> + in <i>Fig. 35</i>, slows down, and finally damps out entirely, the + electric oscillations of the high frequency currents, see <i>B</i>, where + these are set up by the periodic discharge of a condenser, precisely as + the vibrations of the spring are damped out by the friction of the air and + other resistances that act upon it. As the electric oscillations surge to + and fro in the circuit it is opposed by the action of the ether which + surrounds it and electric waves are set up in and sent out through it and + this transformation soon uses up the energy of the current that flows in + the circuit. + </p> + <p> + <a name="fig035" id="fig035"><img width="600" height="435" + src="images/fig035.jpg" + alt="Fig. 35.--Damped and Sustained Electric Oscillations." /></a> + </p> + <p> + To send out <i>continuous waves</i> in the ether such as are needed for + wireless telephony instead of <i>damped waves</i> which are, at the + present writing, generally used for wireless telegraphy, an <i>electric + oscillation arc</i> or a <i>vacuum tube oscillator</i> must be used, see + <i>C</i>, instead of a spark gap. Where a spark gap is used the condenser + in the circuit is charged periodically and with considerable lapses of + time between each of the charging processes, when, of course, the + condenser discharges periodically and with the same time element between + them. Where an oscillation arc or a vacuum tube is used the condenser is + charged as rapidly as it is discharged and the result is the oscillations + are sustained as shown at <i>D</i>. + </p> + <p> + <i>About Mechanical Tuning</i>.--A tuning fork is better than a spring or + a straight steel bar for setting up mechanical vibrations. As a matter of + fact a tuning fork is simply a steel bar bent in the middle so that the + two ends are parallel. A handle is attached to middle point of the fork so + that it can be held easily and which also allows it to vibrate freely, + when the ends of the prongs alternately approach and recede from one + another. When the prongs vibrate the handle vibrates up and down in unison + with it, and imparts its motion to the <i>sounding box</i>, or <i>resonance + case</i> as it is sometimes called, where one is used. + </p> + <p> + If, now, you will mount the fork on a sounding box which is tuned so that + it will be in resonance with the vibrations of the fork there will be a + direct reinforcement of the vibrations when the note emitted by it will be + augmented in strength and quality. This is called <i>simple resonance</i>. + Further, if you mount a pair of forks, each on a separate sounding box, + and have the forks of the same size, tone and pitch, and the boxes + synchronized, that is, tuned to the same frequency of vibration, then set + the two boxes a foot or so apart, as shown at A in <i>Fig. 36</i>, when + you strike one of the forks with a rubber hammer it will vibrate with a + definite frequency and, hence, send out sound waves of a given length. + When the latter strike the second fork the impact of the molecules of air + of which the sound waves are formed will set its prongs to vibrating and + it will, in turn, emit sound waves of the same length and this is called + <i>sympathetic resonance</i>, or as we would say in wireless the forks are + <i>in tune</i>. + </p> + <p> + <a name="fig036" id="fig036"><img width="600" height="351" + src="images/fig036.jpg" + alt="Fig. 36.--Sound Wave and Electric Wave Tuned Senders and Receptors. A - variable tuning forks for showing sound wave tuning. B - variable oscillation circuits for showing electric wave tuning." /> + </a> + </p> + <p> + Tuning forks are made with adjustable weights on their prongs and by + fixing these to different parts of them the frequency with which the forks + vibrate can be changed since the frequency varies inversely with the + square of the length and directly with the thickness [Footnote: This law + is for forks having a rectangular cross-section. Those having a round + cross-section vary as the radius.] of the prongs. Now by adjusting one of + the forks so that it vibrates at a frequency of, say, 16 per second and + adjusting the other fork so that it vibrates at a frequency of, say, 18 or + 20 per second, then the forks will not be in tune with each other and, + hence, if you strike one of them the other will not respond. But if you + make the forks vibrate at the same frequency, say 16, 20 or 24 per second, + when you strike one of them the other will vibrate in unison with it. + </p> + <p> + <i>About Electric Tuning</i>.--Electric resonance and electric tuning are + very like those of acoustic resonance and acoustic tuning which I have + just described. Just as acoustic resonance may be simple or sympathetic so + electric resonance may be simple or sympathetic. Simple acoustic resonance + is the direct reinforcement of a simple vibration and this condition is + had when a tuning fork is mounted on a sounding box. In simple electric + resonance an oscillating current of a given frequency flowing in a circuit + having the proper inductance and capacitance may increase the voltage + until it is several times greater than its normal value. Tuning the + receptor circuits to the transmitter circuits are examples of sympathetic + electric resonance. As a demonstration if you have two Leyden jars + (capacitance) connected in circuit with two loops of wire (inductance) + whose inductance can be varied as shown at <i>B</i> in <i>Fig. 36,</i> + when you make a spark pass between the knobs of one of them by means of a + spark coil then a spark will pass in the gap of the other one provided the + inductance of the two loops of wire is the same. But if you vary the + inductance of the one loop so that it is larger or smaller than that of + the other loop no spark will take place in the second circuit. + </p> + <p> + When a tuning fork is made to vibrate it sends out waves in the air, or + sound waves, in all directions and just so when high frequency currents + surge in an oscillation circuit they send out waves in the ether, or + electric waves, that travel in all directions. For this reason electric + waves from a transmitting station cannot be sent to one particular + station, though they do go further in one direction than in another, + according to the way your aerial wire points. + </p> + <p> + Since the electric waves travel out in all directions any receiving set + properly tuned to the wave length of the sending station will receive the + waves and the only limit on your ability to receive from high-power + stations throughout the world depends entirely on the wave length and + sensitivity of your receiving set. As for tuning, just as changing the + length and the thickness of the prongs of a tuning fork varies the + frequency with which it vibrates and, hence, the length of the waves it + sends out, so, too, by varying the capacitance of the condenser and the + inductance of the tuning coil of the transmitter the frequency of the + electric oscillations set up in the circuit may be changed and, + consequently, the length of the electric waves they send out. Likewise, by + varying the capacitance and the inductance of the receptor the circuits + can be tuned to receive incoming electric waves of whatever length within + the limitation of the apparatus. + </p> + <h2> + <a name="chap08" id="chap08">CHAPTER VIII</a> + </h2> + <h3> + A SIMPLE VACUUM TUBE DETECTOR RECEIVING SET + </h3> + <p> + While you can receive dots and dashes from spark wireless telegraph + stations and hear spoken words and music from wireless telephone stations + with a crystal detector receiving set such as described in <a + href="#chap03">Chapter III</a>, you can get stations that are much farther + away and hear them better with a <i>vacuum tube detector</i> receiving + set. + </p> + <p> + Though the vacuum tube detector requires two batteries to operate it and + the receiving circuits are somewhat more complicated than where a crystal + detector is used still the former does not have to be constantly adjusted + as does the latter and this is another very great advantage. Taken all in + all the vacuum tube detector is the most sensitive and the most + satisfactory of the detectors that are in use at the present time. + </p> + <p> + Not only is the vacuum tube a detector of electric wave signals and speech + and music but it can also be used to <i>amplify</i> them, that is, to make + them stronger and, hence, louder in the telephone receiver and further its + powers of amplification are so great that it will reproduce them by means + of a <i>loud speaker</i>, just as a horn amplifies the sounds of a + phonograph reproducer, until they can be heard by a room or an auditorium + full of people. There are two general types of loud speakers, though both + use the principle of the telephone receiver. The construction of these + loud speakers will be fully described in a later chapter. + </p> + <p> + <i>Assembled Vacuum Tube Receiving Sets</i>.--You can buy a receiving set + with a vacuum tube detector from the very simplest type, which is + described in this chapter, to those that are provided with <i>regenerative + circuits</i> and <i>amplifying</i> tubes or both, which we shall describe + in later chapters, from dealers in electrical apparatus generally. While + one of these sets costs more than you can assemble a set for yourself, + still, especially in the beginning, it is a good plan to buy an assembled + one for it is fitted with a <i>panel</i> on which the adjusting knobs of + the rheostat, tuning coil and condenser are mounted and this makes it + possible to operate it as soon as you get it home and without the + slightest trouble on your part. + </p> + <p> + You can, however, buy all the various parts separately and mount them + yourself. If you want the receptor simply for receiving then it is a good + scheme to have all of the parts mounted in a box or enclosed case, but if + you want it for experimental purposes then the parts should be mounted on + a base or a panel so that all of the connections are in sight and + accessible. + </p> + <p> + <i>A Simple Vacuum Tube Receiving Set.</i>--For this set you should use: + (1) a <i>loose coupled tuning coil,</i> (2) a <i>variable condenser,</i> + (3) a <i>vacuum tube detector,</i> (4) an <i>A</i> or <i>storage battery</i> + giving 6 volts, (5) a <i>B</i> or <i>dry cell battery</i> giving 22-1/2 + volts, (6) a <i>rheostat</i> for varying the storage battery current, and + (7) a pair of 2,000-ohm <i>head telephone receivers</i>. The loose coupled + tuning coil, the variable condenser and the telephone receivers are the + same as those described in <a href="#chap03">Chapter III</a>. + </p> + <p> + <i>The Vacuum Tube Detector. With Two Electrodes.</i>--A vacuum tube in + its simplest form consists of a glass bulb like an incandescent lamp in + which a <i>wire filament</i> and a <i>metal plate</i> are sealed as shown + in <i>Fig. 37</i>, The air is then pumped out of the tube and a vacuum + left or after it is exhausted it is filled with nitrogen, which cannot + burn. + </p> + <p> + <a name="fig037" id="fig037"><img width="493" height="480" + src="images/fig037.jpg" + alt="Fig. 37.--Two Electrode Vacuum Tube Detectors." /></a> + </p> + <p> + When the vacuum tube is used as a detector, the wire filament is heated + red-hot and the metal plate is charged with positive electricity though it + remains cold. The wire filament is formed into a loop like that of an + incandescent lamp and its outside ends are connected with a 6-volt storage + battery, which is called the <i>A</i> battery; then the + or <i>positive</i> + terminal of a 22-1/2 volt dry cell battery, called the <i>B</i> battery, + is connected to the metal plate while the - or <i>negative</i> terminal of + the battery is connected to one of the terminals of the wire filament. The + diagram, <i>Fig. 37</i>, simply shows how the two electrode vacuum tube, + the <i>A</i> or dry battery, and the <i>B</i> or storage battery are + connected up. + </p> + <p> + <i>Three Electrode Vacuum Tube Detector.</i>--The three electrode vacuum + tube detector shown at <i>A</i> in <i>Fig. 38</i>, is much more sensitive + than the two electrode tube and has, in consequence, all but supplanted + it. In this more recent type of vacuum tube the third electrode, or <i>grid</i>, + as it is called, is placed between the wire filament and the metal plate + and this allows the current to be increased or decreased at will to a very + considerable extent. + </p> + <p> + <a name="fig038" id="fig038"><img width="600" height="531" + src="images/fig038.jpg" + alt="Fig. 38.--Three Electrode Vacuum Tube Detector and Battery Connections." /> + </a> + </p> + <p> + The way the three electrode vacuum tube detector is connected with the + batteries is shown at <i>B</i>. The plate, the <i>A</i> or dry cell + battery and one terminal of the filament are connected in <i>series</i>--that + is, one after the other, and the ends of the filament are connected to the + <i>B</i> or storage battery. In assembling a receiving set you must, of + course, have a socket for the vacuum tube. A vacuum tube detector costs + from $5.00 to $6.00. + </p> + <p> + <i>The Dry Cell and Storage Batteries</i>.--The reason that a storage + battery is used for heating the filament of the vacuum tube detector is + because the current delivered is constant, whereas when a dry cell battery + is used the current soon falls off and, hence, the heat of the filament + gradually grows less. The smallest <i>A</i> or 6 volt storage battery on + the market has a capacity of 20 to 40 ampere hours, weighs 13 pounds and + costs about $10.00. It is shown at <i>A</i> in <i>Fig. 39</i>. The <i>B</i> + or dry cell battery for the vacuum tube plate circuit that gives 22-1/2 + volts can be bought already assembled in sealed boxes. The small size is + fitted with a pair of terminals while the larger size is provided with <i>taps</i> + so that the voltage required by the plate can be adjusted as the proper + operation of the tube requires careful regulation of the plate voltage. A + dry cell battery for a plate circuit is shown at <i>B</i>. + </p> + <p> + <a name="fig039" id="fig039"><img width="600" height="336" + src="images/fig039.jpg" + alt="Fig. 39.--<i>A</i> and <i>B</i> Batteries for Vacuum Tube Detectors." /> + </a> + </p> + <p> + <i>The Filament Rheostat</i>.--An adjustable resistance, called a <i>rheostat</i>, + must be used in the filament and storage battery circuit so that the + current flowing through the filament can be controlled to a nicety. The + rheostat consists of an insulating and a heat resisting form on which is + wound a number of turns of resistance wire. A movable contact arm that + slides over and presses on the turns of wire is fixed to the knob on top + of the rheostat. A rheostat that has a resistance of 6 ohms and a current + carrying capacity of 1.5 amperes which can be mounted on a panel board is + the right kind to use. It is shown at <i>A</i> and <i>B</i> in <i>Fig. 40</i> + and costs $1.25. + </p> + <p> + <a name="fig040" id="fig040"><img width="600" height="411" + src="images/fig040.jpg" + alt="Fig. 40.--Rheostat for the <i>A</i> or Storage Battery Current." /> + </a> + </p> + <p> + <i>Assembling the Parts</i>.--Begin by placing all of the separate parts + of the receiving set on a board or a base of other material and set the + tuning coil on the left hand side with the adjustable switch end toward + the right hand side so that you can reach it easily. Then set the variable + condenser in front of it, set the vacuum tube detector at the right hand + end of the tuning coil and the rheostat in front of the detector. Place + the two sets of batteries back of the instruments and screw a couple of + binding posts <i>a</i> and <i>b</i> to the right hand lower edge of the + base for connecting in the head phones all of which is shown at <i>A</i> + in <i>Fig. 41</i>. + </p> + <p> + <a name="fig041a" id="fig041a"><img width="600" height="473" + src="images/fig041a.jpg" + alt="(A) Fig. 41.--Top View of Apparatus Layout for a Vacuum Tube Detector Receiving Set." /> + </a> <a name="fig041b" id="fig041b"><img width="600" height="482" + src="images/fig041b.jpg" + alt="(B) Fig. 41.--Wiring Diagram of a Simple Vacuum Tube Receiving Set." /> + </a> + </p> + <p> + <i>Connecting Up the Parts.</i>--To wire up the different parts begin by + connecting the sliding contact of the primary coil of the loose coupled + tuning coil (this you will remember is the outside one that is wound with + fine wire) to the upper post of the lightning switch and connect one + terminal of this coil with the water pipe. Now connect the free end of the + secondary coil of the tuning coil (this is the inside coil that is wound + with heavy wire) to one of the binding posts of the variable condenser and + connect the movable contact arm of the adjustable switch of the primary of + the tuning coil with the other post of the variable condenser. + </p> + <p> + Next connect the grid of the vacuum tube to one of the posts of the + condenser and then connect the plate of the tube to the <i>carbon terminal</i> + of the <i>B</i> or dry cell battery which is the + or <i>positive pole</i> + and connect the <i>zinc terminal</i> of the - or <i>negative</i> pole to + the binding post <i>a</i>, connect the post <i>b</i> to the other side of + the variable condenser and then connect the terminals of the head phones + to the binding posts <i>a</i> and <i>b</i>. Whatever you do be careful not + to get the plate connections of the battery reversed. + </p> + <p> + Now connect one of the posts of the rheostat to one terminal of the + filament and the other terminal of the filament to the - or <i>negative</i> + terminal of the <i>A</i> or storage battery and the + or <i>positive</i> + terminal of the <i>A</i> or storage battery to the other post of the + rheostat. Finally connect the + or positive terminal of the <i>A</i> or + storage battery with the wire that runs from the head phones to the + variable condenser, all of which is shown in the wiring diagram at <i>B</i> + in <i>Fig. 41</i>. + </p> + <p> + <i>Adjusting the Vacuum Tube Detector Receiving Set</i>.--A vacuum tube + detector is tuned exactly in the same way as the <i>Crystal Detector Set + No. 2</i> described in <a href="#chap03">Chapter III</a>, in-so-far as the + tuning coil and variable condenser are concerned. The sensitivity of the + vacuum tube detector receiving set and, hence, the distance over which + signals and other sounds can be heard depends very largely on the + sensitivity of the vacuum tube itself and this in turn depends on: (1) the + right amount of heat developed by the filament, or <i>filament brilliancy</i> + as it is called, (2) the right amount of voltage applied to the plate, and + (3) the extent to which the tube is exhausted where this kind of a tube is + used. + </p> + <p> + To vary the current flowing from the <i>A</i> or storage battery through + the filament so that it will be heated to the right degree you adjust the + rheostat while you are listening in to the signals or other sounds. By + carefully adjusting the rheostat you can easily find the point at which it + makes the tube the most sensitive. A rheostat is also useful in that it + keeps the filament from burning out when the current from the battery + first flows through it. You can very often increase the sensitiveness of a + vacuum tube after you have used it for a while by recharging the <i>A</i> + or storage battery. + </p> + <p> + The degree to which a vacuum tube has been exhausted has a very pronounced + effect on its sensitivity. The longer the tube is used the lower its + vacuum gets and generally the less sensitive it becomes. When this takes + place (and you can only guess at it) you can very often make it more + sensitive by warming it over the flame of a candle. Vacuum tubes having a + gas content (in which case they are, of course, no longer vacuum tubes in + the strict sense) make better detectors than tubes from which the air has + been exhausted and which are sealed off in this evacuated condition + because their sensitiveness is not dependent on the degree of vacuum as in + the latter tubes. Moreover, a tube that is completely exhausted costs more + than one that is filled with gas. + </p> + <h2> + <a name="chap09" id="chap09">CHAPTER IX</a> + </h2> + <h3> + VACUUM TUBE AMPLIFIER RECEIVING SETS + </h3> + <p> + The reason a vacuum tube detector is more sensitive than a crystal + detector is because while the latter merely <i>rectifies</i> the + oscillating current that surges in the receiving circuits, the former acts + as an <i>amplifier</i> at the same time. The vacuum tube can be used as a + separate amplifier in connection with either: (1) a <i>crystal detector</i> + or (2) a <i>vacuum tube detector</i>, and (<i>a</i>) it will amplify + either the <i>radio frequency currents</i>, that is the high frequency + oscillating currents which are set up in the oscillation circuits or (<i>b</i>) + it will amplify the <i>audio frequency currents</i>, that is, the <i>low + frequency alternating</i> currents that flow through the head phone + circuit. + </p> + <p> + To use the amplified radio frequency oscillating currents or amplified + audio frequency alternating currents that are set up by an amplifier tube + either a high resistance, called a <i>grid leak</i>, or an <i>amplifying + transformer</i>, with or without an iron core, must be connected with the + plate circuit of the first amplifier tube and the grid circuit of the next + amplifier tube or detector tube, or with the wire point of a crystal + detector. Where two or more amplifier tubes are coupled together in this + way the scheme is known as <i>cascade amplification.</i> + </p> + <p> + Where either a <i>radio frequency transformer</i>, that is one without the + iron core, or an <i>audio frequency transformer</i>, that is one with the + iron core, is used to couple the amplifier tube circuits together better + results are obtained than where a high resistance grid leak is used, but + the amplifying tubes have to be more carefully shielded from each other or + they will react and set up a <i>howling</i> noise in the head phones. On + the other hand grid leaks cost less but they are more troublesome to use + as you have to find out for yourself the exact resistance value they must + have and this you can do only by testing them out. + </p> + <p> + <i>A Grid Leak Amplifier Receiving Set. With Crystal Detector.</i>--The + apparatus you need for this set includes: (1) a <i>loose coupled tuning + coil</i>, (2) a <i>variable condenser</i>, (3) <i>two fixed condensers</i>, + (4) a <i>crystal detector</i>, or better a <i>vacuum tube detector</i>, + (5) an <i>A</i> or <i>6 volt storage battery</i>, (6) a <i>rheostat</i>, + (7) a <i>B</i> or 22-1/2 <i>volt dry cell battery</i>, (8) a fixed + resistance unit, or <i>leak grid</i> as it is called, and (9) a pair of <i>head-phones</i>. + The tuning coil, variable condenser, fixed condensers, crystal detectors + and head-phones are exactly the same as those described in <i>Set No. 2</i> + in <a href="#chap03">Chapter III</a>. The <i>A</i> and <i>B batteries</i> + are exactly the same as those described in <a href="#chap08">Chapter VIII</a>. + The <i>vacuum tube amplifier</i> and the <i>grid leak</i> are the only new + pieces of apparatus you need and not described before. + </p> + <p> + <i>The Vacuum Tube Amplifier</i>.--This consists of a three electrode + vacuum tube exactly like the vacuum tube detector described in <a + href="#chap08">Chapter VIII</a> and pictured in <i>Fig. 38</i>, except + that instead of being filled with a non-combustible gas it is evacuated, + that is, the air has been completely pumped out of it. The gas filled + tube, however, can be used as an amplifier and either kind of tube can be + used for either radio frequency or audio frequency amplification, though + with the exhausted tube it is easier to obtain the right plate and + filament voltages for good working. + </p> + <p> + <i>The Fixed Resistance Unit, or Grid Leak</i>.--Grid leaks are made in + different ways but all of them have an enormously high resistance. One way + of making them consists of depositing a thin film of gold on a sheet of + mica and placing another sheet of mica on top to protect it the whole + being enclosed in a glass tube as shown at <i>A</i> in <i>Fig. 42</i>. + These grid leaks are made in units of from 50,000 ohms (.05 megohm) to + 5,000,000 ohms (5 megohms) and cost from $1 to $2. + </p> + <p> + <a name="fig042" id="fig042"><img width="600" height="531" + src="images/fig042.jpg" + alt="Fig. 42.--Grid Leaks and How to Connect Them up." /></a> + </p> + <p> + As the <i>value</i> of the grid leak you will need depends very largely + upon the construction of the different parts of your receiving set and on + the kind of aerial wire system you use with it you will have to try out + various resistances until you hit the right one. The resistance that will + give the best results, however, lies somewhere between 500,000 ohms (1/2 a + megohm) and 3,000,000 ohms (3 megohms) and the only way for you to find + this out is to buy 1/2, 1 and 2 megohm grid leak resistances and connect + them up in different ways, as shown at <i>B</i>, until you find the right + value. + </p> + <p> + <i>Assembling the Parts for a Crystal Detector Set</i>.--Begin by laying + the various parts out on a base or a panel with the loose coupled tuning + coil on the left hand side, but with the adjustable switch of the + secondary coil on the right hand end or in front according to the way it + is made. Then place the variable condenser, the rheostat, the crystal + detector and the binding posts for the head phones in front of and in a + line with each other. Set the vacuum tube amplifier back of the rheostat + and the <i>A</i> and <i>B</i> batteries back of the parts or in any other + place that may be convenient. The fixed condensers and the grid leak can + be placed anywhere so that it will be easy to connect them in and you are + ready to wire up the set. + </p> + <p> + <i>Connecting Up the Parts for a Crystal Detector</i>.--First connect the + sliding contact of the primary of the tuning coil to the leading-in wire + and one of the end wires of the primary to the water pipe, as shown in <i>Fig. + 43</i>. Now connect the adjustable arm that makes contact with one end of + the secondary of the tuning coil to one of the posts of the variable + condenser; then connect the other post of the latter with a post of the + fixed condenser and the other post of this with the grid of the amplifying + tube. + </p> + <p> + <a name="fig043" id="fig043"><img width="600" height="404" + src="images/fig043.jpg" + alt="Fig. 43.--Crystal Detector Receiving Set with Vacuum Tube Amplifier (Resistance Coupled)." /> + </a> + </p> + <p> + Connect the first post of the variable condenser to the + or <i>positive + electrode</i> of the <i>A</i> battery and its - or <i>negative electrode</i> + with the rotating contact arm of the rheostat. Next connect one end of the + resistance coil of the rheostat to one of the posts of the amplifier tube + that leads to the filament and the other filament post to the + or <i>positive + electrode</i> of the <i>A</i> battery. This done connect the <i>negative</i>, + that is, the <i>zinc pole</i> of the <i>B</i> battery to the positive + electrode of the <i>A</i> battery and connect the <i>positive</i>, or <i>carbon + pole</i> of the former with one end of the grid leak and connect the other + end of this to the plate of the amplifier tube. + </p> + <p> + To the end of the grid leak connected with the plate of the amplifier tube + connect the metal point of your crystal detector, the crystal of the + latter with one post of the head phones and the other post of them with + the other end of the grid leak and, finally, connect a fixed condenser in + <i>parallel</i> with--that is across the ends of the grid leak, all of + which is shown in the wiring diagram in <i>Fig. 43</i>. + </p> + <p> + <i>A Grid Leak Amplifying Receiving Set With Vacuum Tube Detector</i>.--A + better amplifying receiving set can be made than the one just described by + using a vacuum tube detector instead of the crystal detector. This set is + built up exactly like the crystal detector described above and shown in <i>Fig. + 43</i> up to and including the grid leak resistance, but shunted across + the latter is a vacuum tube detector, which is made and wired up precisely + like the one shown at <i>A</i> in <i>Fig. 41</i> in the chapter ahead of + this one. The way a grid leak and vacuum tube detector with a one-step + amplifier are connected up is shown at <i>A</i> in <i>Fig. 44</i>. Where + you have a vacuum tube detector and one or more amplifying tubes connected + up, or in <i>cascade</i> as it is called, you can use an <i>A</i>, or + storage battery of 6 volts for all of them as shown at <i>B</i> in <i>Fig. + 44</i>, but for every vacuum tube you use you must have a <i>B</i> or + 22-1/2 volt dry battery to charge the plate with. + </p> + <p> + <a name="fig044a" id="fig044a"><img width="600" height="375" + src="images/fig044a.jpg" + alt="(A) Fig. 44--Vacuum Tube Detector Set with One Step Amplifier (Resistance Coupled)." /> + </a> <a name="fig044b" id="fig044b"><img width="582" height="320" + src="images/fig044b.jpg" + alt="(B) Fig. 44.--Wiring Diagram for Using One A or Storage Battery with an Amplifier and a Detector Tube." /> + </a> + </p> + <p> + <i>A Radio Frequency Transformer Amplifying Receiving Set</i>.--Instead of + using a grid leak resistance to couple up the amplifier and detector tube + circuits you can use a <i>radio frequency transformer</i>, that is, a + transformer made like a loose coupled tuning coil, and without an iron + core, as shown in the wiring diagram at <i>A</i> in <i>Fig. 45</i>. In + this set, which gives better results than where a grid leak is used, the + amplifier tube is placed in the first oscillation circuit and the detector + tube in the second circuit. + </p> + <p> + <a name="fig045a" id="fig045a"><img width="600" height="394" + src="images/fig045a.jpg" + alt="(A) Fig. 45.--Wiring Diagram for a Radio Frequency Transformer Amplifying Receiving Set." /> + </a> <a name="fig045b" id="fig045b"><img width="412" height="320" + src="images/fig045b.jpg" alt="(B) Fig. 45.--Radio Frequency Transformer." /></a> + </p> + <p> + Since the radio frequency transformer has no iron core the high frequency, + or <i>radio frequency</i> oscillating currents, as they are called, surge + through it and are not changed into low frequency, or <i>audio frequency</i> + pulsating currents, until they flow through the detector. Since the + diagram shows only one amplifier and one radio frequency transformer, it + is consequently a <i>one step amplifier</i>; however, two, three or more, + amplifying tubes can be connected up by means of an equal number of radio + frequency transformers when you will get wonderful results. Where a six + step amplifier, that is, where six amplifying tubes are connected + together, or in <i>cascade</i>, the first three are usually coupled up + with radio frequency transformers and the last three with audio frequency + transformers. A radio frequency transformer is shown at <i>B</i> and costs + $6 to $7. + </p> + <p> + <i>An Audio Frequency Transformer Amplifying Receiving Set</i>.--Where + audio frequency transformers are used for stepping up the voltage of the + current of the detector and amplifier tubes, the radio frequency current + does not get into the plate circuit of the detector at all for the reason + that the iron core of the transformer chokes them off, hence, the + succeeding amplifiers operate at audio frequencies. An audio frequency + transformer is shown at <i>A</i> in <i>Fig. 46</i> and a wiring diagram + showing how the tubes are connected in <i>cascade</i> with the + transformers is shown at <i>B</i>; it is therefore a two-step audio + frequency receiving set. + </p> + <p> + <a name="fig046a" id="fig046a"><img width="400" height="304" + src="images/fig046a.jpg" alt="(A) Fig. 46.--Audio Frequency Transformer." /></a> + <a name="fig046b" id="fig046b"><img width="600" height="331" + src="images/fig046b.jpg" + alt="(B) Fig. 46--Wiring Diagram for an Audio Frequency Transformer Amplifying Receiving Set. (With Vacuum Tube Detector and Two Step Amplifier Tubes.)" /> + </a> + </p> + <p> + <i>A Six Step Amplifier Receiving Set With a Loop Aerial.</i>--By using a + receiving set having a three step radio frequency and a three step audio + frequency, that is, a set in which there are coupled three amplifying + tubes with radio frequency transformers and three amplifying tubes with + audio frequency transformers as described under the caption <i>A Radio + Frequency Transformer Receiving Set</i>, you can use a <i>loop aerial</i> + in your room thus getting around the difficulties--if such there be--in + erecting an out-door aerial. You can easily make a loop aerial by winding + 10 turns of <i>No. 14</i> or <i>16</i> copper wire about 1/16 inch apart + on a wooden frame two feet on the side as shown in <i>Fig. 47</i>. With + this six step amplifier set and loop aerial you can receive wave lengths + of 150 to 600 meters from various high power stations which are at + considerable distances away. + </p> + <p> + <a name="fig047a" id="fig047a"><img width="600" height="346" + src="images/fig047a.jpg" + alt="(A) Fig. 47.--Six Step Amplifier with Loop Aerial." /></a> <a + name="fig047b" id="fig047b"><img width="600" height="453" + src="images/fig047b.jpg" + alt="(B) Fig. 47.--Efficient Regenerative Receiving Set. (With Three Coil Loose Coupler Tuner.)" /> + </a> + </p> + <p> + <i>How to Prevent Howling</i>.--Where radio frequency or audio frequency + amplifiers are used to couple your amplifier tubes in cascade you must + take particular pains to shield them from one another in order to prevent + the <i>feed back</i> of the currents through them, which makes the head + phones or loud speaker <i>howl</i>. To shield them from each other the + tubes should be enclosed in metal boxes and placed at least 6 inches apart + while the transformers should be set so that their cores are at right + angles to each other and these also should be not less than six inches + apart. + </p> + <h2> + <a name="chap10" id="chap10">CHAPTER X</a> + </h2> + <h3> + REGENERATIVE AMPLIFICATION RECEIVING SETS + </h3> + <p> + While a vacuum tube detector has an amplifying action of its own, and this + accounts for its great sensitiveness, its amplifying action can be further + increased to an enormous extent by making the radio frequency currents + that are set up in the oscillation circuits react on the detector. + </p> + <p> + Such currents are called <i>feed-back</i> or <i>regenerative</i> currents + and when circuits are so arranged as to cause the currents to flow back + through the detector tube the amplification keeps on increasing until the + capacity of the tube itself is reached. It is like using steam over and + over again in a steam turbine until there is no more energy left in it. A + system of circuits which will cause this regenerative action to take place + is known as the <i>Armstrong circuits</i> and is so called after the young + man who discovered it. + </p> + <p> + Since the regenerative action of the radio frequency currents is produced + by the detector tube itself and which sets up an amplifying effect without + the addition of an amplifying tube, this type of receiving set has found + great favor with amateurs, while in combination with amplifying tubes it + multiplies their power proportionately and it is in consequence used in + one form or another in all the better sets. + </p> + <p> + There are many different kinds of circuits which can be used to produce + the regenerative amplification effect while the various kinds of tuning + coils will serve for coupling them; for instance a two or three slide + single tuning coil will answer the purpose but as it does not give good + results it is not advisable to spend either time or money on it. A better + scheme is to use a loose coupler formed of two or three honeycomb or other + compact coils, while a <i>variocoupler</i> or a <i>variometer</i> or two + will produce the maximum regenerative action. + </p> + <p> + <i>The Simplest Type of Regenerative Receiving Set. With Loose Coupled + Tuning Coil</i>.--While this regenerative set is the simplest that will + give anything like fair results it is here described not on account of its + desirability, but because it will serve to give you the fundamental idea + of how the <i>feed-back</i> circuit is formed. + </p> + <p> + For this set you need: (1) a <i>loose-coupled tuning coil</i> such as + described in <a href="#chap03">Chapter III</a>, (2) a <i>variable + condenser</i> of <i>.001 mfd.</i> (microfarad) capacitance; (3) one <i>fixed + condenser</i> of <i>.001 mfd.</i>; (4) one <i>fixed condenser</i> for the + grid leak circuit of <i>.00025 mfd.</i>; (5) a <i>grid leak</i> of 1/2 to + 2 megohms resistance; (6) a <i>vacuum tube detector</i>; (7) an <i>A 6 + volt battery</i>; (8) a <i>rheostat</i>; (9) a <i>B 22 1/2 volt battery</i>; + and (10) a pair of <i>2000 ohm head phones</i>. + </p> + <p> + <i>Connecting Up the Parts.</i>--Begin by connecting the leading-in wire + of the aerial with the binding post end of the primary coil of the loose + coupler as shown in the wiring diagram <i>Fig. 48</i> and then connect the + sliding contact with the water pipe or other ground. Connect the binding + post end of the primary coil with one post of the variable condenser, + connect the other post of this with one of the posts of the <i>.00025 mfd.</i> + condenser and the other end of this with the grid of the detector tube; + then around this condenser shunt the grid leak resistance. + </p> + <p> + <a name="fig048" id="fig048"><img width="600" height="510" + src="images/fig048.jpg" + alt="Fig. 48.--Simple Regenerative Receiving Set. (With Loose Coupler Tuner.)" /> + </a> + </p> + <p> + Next connect the sliding contact of the primary coil with the other post + of the variable condenser and from this lead a wire on over to one of the + terminals of the filament of the vacuum tube; to the other terminal of the + filament connect one of the posts of the rheostat and connect the other + post to the - or negative electrode of the <i>A</i> battery and then + connect the + or positive electrode of it to the other terminal of the + filament. + </p> + <p> + Connect the + or positive electrode of the <i>A</i> battery with one post + of the .001 mfd. fixed condenser and connect the other post of this to one + of the ends of the secondary coil of the tuning coil and which is now + known as the <i>tickler coil</i>; then connect the other end of the + secondary, or tickler coil to the plate of the vacuum tube. In the wiring + diagram the secondary, or tickler coil is shown above and in a line with + the primary coil but this is only for the sake of making the connections + clear; in reality the secondary, or tickler coil slides to and fro in the + primary coil as shown and described in <a href="#chap03">Chapter III</a>. + Finally connect the <i>negative</i>, or zinc pole of the <i>B battery</i> + to one side of the fixed condenser, the <i>positive</i>, or carbon, pole + to one of the terminals of the head phones and the other terminal of this + to the other post of the fixed condenser when your regenerative set is + complete. + </p> + <p> + <i>An Efficient Regenerative Receiving Set. With Three Coil Loose Coupler.</i>--To + construct a really good regenerative set you must use a loose coupled + tuner that has three coils, namely a <i>primary</i>, a <i>secondary</i> + and a <i>tickler coil</i>. A tuner of this kind is made like an ordinary + loose coupled tuning coil but it has a <i>third</i> coil as shown at <i>A</i> + and <i>B</i> in <i>Fig. 49</i>. The middle coil, which is the <i>secondary</i>, + is fixed to the base, and the large outside coil, which is the <i>primary</i>, + is movable, that is it slides to and fro over the middle coil, while the + small inside coil, which is the <i>tickler</i>, is also movable and can + slide in or out of the middle <i>coil</i>. None of these coils is + variable; all are wound to receive waves up to 360 meters in length when + used with a variable condenser of <i>.001 mfd</i>. capacitance. In other + words you slide the coils in and out to get the right amount of coupling + and you tune by adjusting the variable condenser to get the exact wave + length you want. + </p> + <p> + <a name="fig049a" id="fig049a"><img width="600" height="355" + src="images/fig049a.jpg" + alt="(A) Fig. 49.--Diagram of a Three Coil Coupler." /></a> <a + name="fig049b" id="fig049b"><img width="553" height="240" + src="images/fig049b.jpg" + alt="(B) Fig. 49.--Three Coil Loose Coupler Tuner." /></a> + </p> + <p> + <i>With Compact Coils</i>.--Compact coil tuners are formed of three fixed + inductances wound in flat coils, and these are pivoted in a mounting so + that the distance between them and, therefore, the coupling, can be + varied, as shown at <i>A</i> in <i>Fig. 50</i>. These coils are wound up + by the makers for various wave lengths ranging from a small one that will + receive waves of any length up to 360 meters to a large one that has a + maximum of 24,000 meters. For an amateur set get three of the smallest + coils when you can not only hear amateur stations that send on a 200 meter + wave but broadcasting stations that send on a 360 meter wave. + </p> + <p> + <a name="fig050" id="fig050"><img width="599" height="320" + src="images/fig050.jpg" alt="Fig. 50.--Honeycomb Inductance Coil." /></a> + </p> + <p> + These three coils are mounted with panel plugs which latter fit into a + stand, or mounting, so that the middle coil is fixed, that is, stationary, + while the two outside coils can be swung to and fro like a door; this + scheme permits small variations of coupling to be had between the coils + and this can be done either by handles or by means of knobs on a panel + board. While I have suggested the use of the smallest size coils, you can + get and use those wound for any wave length you want to receive and when + those are connected with variometers and variable condensers, and with a + proper aerial, you will have a highly efficient receptor that will work + over all ranges of wave lengths. The smallest size coils cost about $1.50 + apiece and the mounting costs about $6 or $7 each. + </p> + <p> + <i>The A Battery Potentiometer</i>.--This device is simply a resistance + like the rheostat described in connection with the preceding vacuum tube + receiving sets but it is wound to 200 or 300 ohms resistance as against + 1-1/2 to 6 ohms of the rheostat. It is, however, used as well as the + rheostat. With a vacuum tube detector, and especially with one having a + gas-content, a potentiometer is very necessary as it is only by means of + it that the potential of the plate of the detector can be accurately + regulated. The result of proper regulation is that when the critical + potential value is reached there is a marked increase in the loudness of + the sounds that are emitted by the head phones. + </p> + <p> + As you will see from <i>A</i> in <i>Fig. 51</i> it has three taps. The two + taps which are connected with the ends of the resistance coil are shunted + around the <i>A</i> battery and the third tap, which is attached to the + movable contact arm, is connected with the <i>B</i> battery tap, see <i>B</i>, + at which this battery gives 18 volts. Since the <i>A</i> battery gives 6 + volts you can vary the potential of the plate from 18 to 24 volts. The + potentiometer must never be shunted around the <i>B</i> battery or the + latter will soon run down. A potentiometer costs a couple of dollars. + </p> + <p> + <a name="fig051a" id="fig051a"><img width="600" height="392" + src="images/fig051a.jpg" alt="(A) Fig. 51.--The Use of the Potentiometer." /></a> + </p> + <p> + <i>The Parts and How to Connect Them Up.</i>--For this regenerative set + you will need: (1) a <i>honeycomb</i> or other compact <i>three-coil tuner</i>, + (2) two <i>variable</i> (<i>.001</i> and <i>.0005 mfd</i>.) <i>condensers</i>; + (3) a <i>.00025 mfd. fixed condenser</i>; (4) a <i>1/2 to 2 megohm grid + leak</i>; (5) a <i>tube detector</i>; (6) a <i>6 volt A battery</i>; (7) + <i>a rheostat</i>; (8) a <i>potentiometer</i>; (9) an <i>18</i> or <i>20 + volt B battery</i>; (10) a <i>fixed condenser</i> of <i>.001 mfd. fixed + condenser</i>; and (11) a <i>pair of 2000 ohm head phones</i>. + </p> + <p> + To wire up the parts connect the leading-in wire of the aerial with the + primary coil, which is the middle one of the tuner, and connect the other + terminal with the ground. Connect the ends of the secondary coil, which is + the middle one, with the posts of the variable condenser and connect one + of the posts of the latter with one post of the fixed .00025 mfd. + condenser and the other post of this with the grid; then shunt the grid + leak around it. Next connect the other post of the variable condenser to + the - or <i>negative</i> electrode of the <i>A battery</i>; the + or <i>positive</i> + electrode of this to one terminal of the detector filament and the other + end of the latter to the electrode of the <i>A</i> battery. + </p> + <p> + Now connect one end of the tickler coil with the detector plate and the + other post to the fixed .001 mfd. condenser, then the other end of this to + the positive or carbon pole of the <i>B</i> battery. + </p> + <p> + This done shunt the potentiometer around the <i>A</i> battery and run a + wire from the movable contact of it (the potentiometer) over to the 18 + volt tap, (see <i>B</i>, <i>Fig. 51</i>), of the <i>B</i> battery. + Finally, shunt the head phones and the .001 mfd. fixed condenser and you + are ready to try out conclusions. + </p> + <p> + <i>A Regenerative Audio Frequency Amplifier Receiving Set.</i>--The use of + amateur regenerative cascade audio frequency receiving sets is getting to + be quite common. To get the greatest amplification possible with + amplifying tubes you have to keep a negative potential on the grids. You + can, however, get very good results without any special charging + arrangement by simply connecting one post of the rheostat with the + negative terminal of the filament and connecting the <i>low potential</i> + end of the secondary of the tuning coil with the - or negative electrode + of the <i>A</i> battery. This scheme will give the grids a negative bias + of about 1 volt. You do not need to bother about these added factors that + make for high efficiency until after you have got your receiving set in + working order and understand all about it. + </p> + <p> + <i>The Parts and How to Connect Them Up.</i>--Exactly the same parts are + needed for this set as the one described above, but in addition you will + want: (1) two more <i>rheostats</i>; (2) <i>two</i> more sets of <i>B</i> + 22-1/2 <i>volt batteries</i>; (3) <i>two amplifier tubes</i>, and (4) <i>two + audio frequency transformers</i> as described in <a href="#chap09">Chapter + IX</a> and pictured at <i>A</i> in <i>Fig. 46</i>. + </p> + <p> + To wire up the parts begin by connecting the leading-in wire to one end of + the primary of the tuning coil and then connect the other end of the coil + with the ground. A variable condenser of .001 mfd. capacitance can be + connected in the ground wire, as shown in <i>Fig. 52</i>, to good + advantage although it is not absolutely needed. Now connect one end of the + secondary coil to one post of a <i>.001 mfd.</i> variable condenser and + the other end of the secondary to the other post of the condenser. + </p> + <p> + <a name="fig052" id="fig052"><img width="600" height="348" + src="images/fig052.jpg" + alt="Fig. 52.--Regenerative Audio Frequency Amplifier Receiving Set." /></a> + </p> + <p> + Next bring a lead (wire) from the first post of the variable condenser + over to the post of the first fixed condenser and connect the other post + of the latter with the grid of the detector tube. Shunt 1/2 to 2 megohm + grid leak resistance around the fixed condenser and then connect the + second post of the variable condenser to one terminal of the detector tube + filament. Run this wire on over and connect it with the first post of the + second rheostat, the second post of which is connected with one terminal + of the filament of the first amplifying tube; then connect the first post + of the rheostat with one end of the secondary coil of the first audio + frequency transformer, and the other end of this coil with the grid of the + first amplifier tube. + </p> + <p> + Connect the lead that runs from the second post of variable condenser to + the first post of the third rheostat, the second post of which is + connected with one terminal of the second amplifying tube; then connect + the first post of the rheostat with one end of the secondary coil of the + second audio frequency transformer and the other end of this coil with the + grid of the second amplifier tube. + </p> + <p> + This done connect the - or negative electrode of the <i>A</i> battery with + the second post of the variable condenser and connect the + or positive + electrode with the free post of the first rheostat, the other post of + which connects with the free terminal of the filament of the detector. + From this lead tap off a wire and connect it to the free terminal of the + filament of the first amplifier tube, and finally connect the end of the + lead with the free terminal of the filament of the second amplifier tube. + </p> + <p> + Next shunt a potentiometer around the <i>A</i> battery and connect the + third post, which connects with the sliding contact, to the negative or + zinc pole of a <i>B</i> battery, then connect the positive or carbon pole + of it to the negative or zinc pole of a second <i>B</i> battery and the + positive or carbon pole of the latter with one end of the primary coil of + the second audio frequency transformer and the other end of it to the + plate of the first amplifying tube. Run the lead on over and connect it to + one of the terminals of the second fixed condenser and the other terminal + of this with the plate of the second amplifying tube. Then shunt the + headphones around the condenser. + </p> + <p> + Finally connect one end of the tickler coil of the tuner with the plate of + the detector tube and connect the other end of the tickler to one end of + the primary coil of the first audio frequency transformer and the other + end of it to the wire that connects the two <i>B</i> batteries together. + </p> + <h2> + <a name="chap11" id="chap11">CHAPTER XI</a> + </h2> + <h3> + SHORT WAVE REGENERATIVE RECEIVING SETS + </h3> + <p> + A <i>short wave receiving set</i> is one that will receive a range of wave + lengths of from 150 to 600 meters while the distance over which the waves + can be received as well as the intensity of the sounds reproduced by the + headphones depends on: (1) whether it is a regenerative set and (2) + whether it is provided with amplifying tubes. + </p> + <p> + High-grade regenerative sets designed especially for receiving amateur + sending stations that must use a short wave length are built on the + regenerative principle just like those described in the last chapter and + further amplification can be had by the use of amplifier tubes as + explained in <a href="#chap09">Chapter IX</a>, but the new feature of + these sets is the use of the <i>variocoupler</i> and one or more <i>variometers</i>. + These tuning devices can be connected up in different ways and are very + popular with amateurs at the present time. + </p> + <p> + Differing from the ordinary loose coupler the variometer has no movable + contacts while the variometer is provided with taps so that you can + connect it up for the wave length you want to receive. All you have to do + is to tune the oscillation circuits to each other is to turn the <i>rotor</i>, + which is the secondary coil, around in the <i>stator</i>, as the primary + coil is called in order to get a very fine variation of the wave length. + It is this construction that makes <i>sharp tuning</i> with these sets + possible, by which is meant that all wave lengths are tuned out except the + one which the receiving set is tuned for. + </p> + <p> + <i>A Short Wave Regenerative Receiver--With One Variometer and Three + Variable Condensers.</i>--This set also includes a variocoupler and a <i>grid + coil</i>. The way that the parts are connected together makes it a simple + and at the same time a very efficient regenerative receiver for short + waves. While this set can be used without shielding the parts from each + other the best results are had when shields are used. + </p> + <p> + The parts you need for this set include: (1) one <i>variocoupler</i>; (2) + one <i>.001 microfarad variable condenser</i>; (3) one <i>.0005 microfarad + variable condenser</i>; (4) one <i>.0007 microfarad variable condenser</i>; + (5) <i>one 2 megohm grid leak</i>; (6) one <i>vacuum tube detector</i>; + (7) one <i>6 volt A battery</i>; (8) one <i>6 ohm</i>, 1-1/2 <i>ampere + rheostat</i>; (9) one <i>200 ohm potentiometer</i>; (10) one 22-1/2 <i>volt + B battery</i>; (11) one <i>.001 microfarad fixed condenser</i>, (12) one + pair of <i>2,000 ohm headphones</i>, and (13) a <i>variometer</i>. + </p> + <p> + <i>The Variocoupler</i>.--A variocoupler consists of a primary coil wound + on the outside of a tube of insulating material and to certain turns of + this taps are connected so that you can fix the wave length which your + aerial system is to receive from the shortest wave; <i>i.e.</i>, 150 + meters on up by steps to the longest wave, <i>i.e.</i>, 600 meters, which + is the range of most amateur variocouplers that are sold in the open + market. This is the part of the variocoupler that is called the <i>stator</i>. + </p> + <p> + The secondary coil is wound on the section of a ball mounted on a shaft + and this is swung in bearings on the stator so that it can turn in it. + This part of the variocoupler is called the <i>rotor</i> and is arranged + so that it can be mounted on a panel and adjusted by means of a knob or a + dial. A diagram of a variocoupler is shown at <i>A</i> in <i>Fig. 53</i>, + and the coupler itself at <i>B</i>. There are various makes and + modifications of variocouplers on the market but all of them are about the + same price which is $6.00 or $8.00. + </p> + <p> + <a name="fig053" id="fig053"><img width="600" height="461" + src="images/fig053.jpg" + alt="Fig. 53.--How the Variocoupler is Made and Works." /></a> + </p> + <p> + <i>The Variometer.</i>--This device is quite like the variocoupler, but + with these differences: (1) the rotor turns in the stator, which is also + the section of a ball, and (2) one end of the primary is connected with + one end of the secondary coil. To be really efficient a variometer must + have a small resistance and a large inductance as well as a small + dielectric loss. To secure the first two of these factors the wire should + be formed of a number of fine, pure copper wires each of which is + insulated and the whole strand then covered with silk. This kind of wire + is the best that has yet been devised for the purpose and is sold under + the trade name of <i>litzendraht</i>. + </p> + <p> + A new type of variometer has what is known as a <i>basket weave</i>, or <i>wavy + wound</i> stator and rotor. There is no wood, insulating compound or other + dielectric materials in large enough quantities to absorb the weak + currents that flow between them, hence weaker sounds can be heard when + this kind of a variometer is used. With it you can tune sharply to waves + under 200 meters in length and up to and including wave lengths of 360 + meters. When amateur stations of small power are sending on these short + waves this style of variometer keeps the electric oscillations at their + greatest strength and, hence, the reproduced sounds will be of maximum + intensity. A wiring diagram of a variometer is shown at <i>A</i> in <i>Fig. + 54</i> and a <i>basketball</i> variometer is shown complete at <i>B</i>. + </p> + <p> + <a name="fig054" id="fig054"><img width="600" height="329" + src="images/fig054.jpg" + alt="Fig. 54.--How the Variometer is Made and Works." /></a> + </p> + <p> + <i>Connecting Up the Parts</i>.--To hook-up the set connect the leading-in + wire to one end of the primary coil, or stator, of the variocoupler and + solder a wire to one of the taps that gives the longest wave length you + want to receive. Connect the other end of this wire with one post of a + .001 microfarad variable condenser and connect the other post with the + ground as shown in <i>Fig. 55</i>. Now connect one end of the secondary + coil, or rotor, to one post of a .0007 mfd. variable condenser, the other + post of this to one end of the grid coil and the other end of this with + the remaining end of the rotor of the variocoupler. + </p> + <p> + <a name="fig055" id="fig055"><img width="600" height="386" + src="images/fig055.jpg" + alt="Fig. 55.--Short Wave Regenerative Receiving Set (one Variometer and three Variable Condensers.)" /> + </a> + </p> + <p> + Next connect one post of the .0007 mfd. condenser with one of the + terminals of the detector filament; then connect the other post of this + condenser with one post of the .0005 mfd. variable condenser and the other + post of this with the grid of the detector, then shunt the megohm grid + leak around the latter condenser. This done connect the other terminal of + the filament to one post of the rheostat, the other post of this to the - + or negative electrode of the 6 volt <i>A</i> battery and the + or positive + electrode of the latter to the other terminal of the filament. + </p> + <p> + Shunt the potentiometer around the <i>A</i> battery and connect the + sliding contact with the - or zinc pole of the <i>B</i> battery and the + + or carbon pole with one terminal of the headphone; connect the other + terminal to one of the posts of the variometer and the other post of the + variometer to the plate of the detector. Finally shunt a .001 mfd. fixed + condenser around the headphones. If you want to amplify the current with a + vacuum tube amplifier connect in the terminals of the amplifier circuit + shown at <i>A</i> in <i>Figs. 44</i> or <i>45</i> at the point where they + are connected with the secondary coil of the loose coupled tuning coil, in + those diagrams with the binding posts of <i>Fig. 55</i> where the phones + are usually connected in. + </p> + <p> + <i>Short Wave Regenerative Receiver. With Two Variometers and Two Variable + Condensers.</i>--This type of regenerative receptor is very popular with + amateurs who are using high-grade short-wave sets. When you connect up + this receptor you must keep the various parts well separated. Screw the + variocoupler to the middle of the base board or panel, and secure the + variometers on either side of it so that the distance between them will be + 9 or 10 inches. By so placing them the coupling will be the same on both + sides and besides you can shield them from each other easier. + </p> + <p> + For the shield use a sheet of copper on the back of the panel and place a + sheet of copper between the parts, or better, enclose the variometers and + detector and amplifying tubes if you use the latter in sheet copper boxes. + When you set up the variometers place them so that their stators are at + right angles to each other for otherwise the magnetic lines of force set + up by the coils of each one will be mutually inductive and this will make + the headphones or loud speaker <i>howl</i>. Whatever tendency the receptor + has to howl with this arrangement can be overcome by putting in a grid + leak of the right resistance and adjusting the condenser. + </p> + <p> + <i>The Parts and How to Connect Them Up.</i>--For this set you require: + (1) one <i>variocoupler</i>; (2) two <i>variometers</i>; (3) one <i>.001 + microfarad variable condenser</i>; (4) one <i>.0005 microfarad variable + condenser</i>; (5) one <i>2 megohm grid leak resistance</i>; (6) one <i>vacuum + tube detector</i>; (7) one <i>6 volt A battery</i>; (8) one <i>200 ohm + potentiometer</i>; (9) one <i>22-1/2 volt B battery</i>; (10) one <i>.001 + microfarad fixed condenser</i>, and (11) one pair of <i>2,000 ohm + headphones</i>. + </p> + <p> + To wire up the set begin by connecting the leading-in wire to the fixed + end of the primary coil, or <i>stator</i>, of the variocoupler, as shown + in <i>Fig. 56</i>, and connect one post of the .001 mfd. variable + condenser to the stator by soldering a short length of wire to the tap of + the latter that gives the longest wave you want to receive. Now connect + one end of the secondary coil, or <i>rotor</i>, of the variocoupler with + one post of the .0005 mfd. variable condenser and the other part to the + grid of the detector tube. Connect the other end of the rotor of the + variocoupler to one of the posts of the first variometer and the other + post of this to one of the terminals of the detector filament. + </p> + <p> + <a name="fig056" id="fig056"><img width="600" height="349" + src="images/fig056.jpg" + alt="Fig. 56.--Short Wave Regenerative Receiving Set (two Variometers and two Variable Condensers.)" /> + </a> + </p> + <p> + Connect this filament terminal with the - or negative electrode of the <i>A</i> + battery and the + or positive electrode of this with one post of the + rheostat and lead a wire from the other post to the free terminal of the + filament. This done shunt the potential around the <i>A</i> battery and + connect the sliding contact to the - or zinc pole of the <i>B</i> battery + and the + or carbon pole of this to one terminal of the headphones, while + the other terminal of this leads to one of the posts of the second + variometer, the other post of which is connected to the plate of the + detector tube. If you want to add an amplifier tube then connect it to the + posts instead of the headphones as described in the foregoing set. + </p> + <h2> + <a name="chap12" id="chap12">CHAPTER XII</a> + </h2> + <h3> + INTERMEDIATE AND LONG WAVE REGENERATIVE RECEIVING SETS + </h3> + <p> + All receiving sets that receive over a range of wave lengths of from 150 + meters to 3,000 meters are called <i>intermediate wave sets</i> and all + sets that receive wave lengths over a range of anything more than 3,000 + meters are called <i>long wave sets</i>. The range of intermediate wave + receptors is such that they will receive amateur, broadcasting, ship and + shore Navy, commercial, Arlington's time and all other stations using <i>spark + telegraph damped waves</i> or <i>arc</i> or <i>vacuum tube telephone + continuous waves</i> but not <i>continuous wave telegraph signals</i>, + unless these have been broken up into groups at the transmitting station. + To receive continuous wave telegraph signals requires receiving sets of + special kind and these will be described in the next chapter. + </p> + <p> + <i>Intermediate Wave Receiving Sets</i>.--There are two chief schemes + employed to increase the range of wave lengths that a set can receive and + these are by using: (1) <i>loading coils</i> and <i>shunt condensers</i>, + and (2) <i>bank-wound coils</i> and <i>variable condensers</i>. If you + have a short-wave set and plan to receive intermediate waves with it then + loading coils and fixed condensers shunted around them affords you the way + to do it, but if you prefer to buy a new receptor then the better way is + to get one with bank-wound coils and variable condensers; this latter way + preserves the electrical balance of the oscillation circuits better, the + electrical losses are less and the tuning easier and sharper. + </p> + <p> + <i>Intermediate Wave Set With Loading Coils.</i>--For this intermediate + wave set you can use either of the short-wave sets described in the + foregoing chapter. For the loading coils use <i>honeycomb coils</i>, or + other good compact inductance coils, as shown in <a href="#chap10">Chapter + X</a> and having a range of whatever wave length you wish to receive. The + following table shows the range of wave length of the various sized coils + when used with a variable condenser having a .001 microfarad <i>capacitance</i>, + the approximate <i>inductance</i> of each coil in <i>millihenries</i> and + prices at the present writing: + </p> + <h3> + TABLE OF CHARACTERISTICS OF HONEYCOMB COILS + </h3> +<pre xml:space="preserve"> + Approximate Wave + Length in Meters in + + Millihenries + Inductance .001 mfd. Variable Mounted + Appx. Air Condenser. on Plug + + .040 130-- 375 $1.40 + .075 180-- 515 1.40 + .15 240-- 730 1.50 + .3 330-- 1030 1.50 + .6 450-- 1460 1.55 + 1.3 660-- 2200 1.60 + 2.3 930-- 2850 1.65 + 4.5 1300-- 4000 1.70 + 6.5 1550-- 4800 1.75 + 11. 2050-- 6300 1.80 + 20. 3000-- 8500 2.00 + 40. 4000--12000 2.15 + 65. 5000--15000 2.35 + 100. 6200--19000 2.60 + 125. 7000--21000 3.00 + 175. 8200--24000 3.50 +</pre> + <p> + These and other kinds of compact coils can be bought at electrical supply + houses that sell wireless goods. If your aerial is not very high or long + you can use loading coils, but to get anything like efficient results with + them you must have an aerial of large capacitance and the only way to get + this is to put up a high and long one with two or more parallel wires + spaced a goodly distance apart. + </p> + <p> + <i>The Parts and How to Connect Them Up</i>.--Get (1) <i>two honeycomb or + other coils</i> of the greatest wave length you want to receive, for in + order to properly balance the aerial, or primary oscillation circuit, and + the closed, or secondary oscillation circuit, you have to tune them to the + same wave length; (2) two <i>.001 mfd. variable condensers</i>, though + fixed condensers will do, and (3) two small <i>single-throw double-pole + knife switches</i> mounted on porcelain bases. + </p> + <p> + To use the loading coils all you have to do is to connect one of them in + the aerial above the primary coil of the loose coupler, or variocoupler as + shown in the wiring diagram in <i>Fig. 57</i>, then shunt one of the + condensers around it and connect one of the switches around this; this + switch enables you to cut in or out the loading coil at will. Likewise + connect the other loading coil in one side of the closed, or secondary + circuit between the variable .0007 mfd. condenser and the secondary coil + of the loose coupler or variocoupler as shown in <i>Fig. 53</i>. The other + connections are exactly the same as shown in <i>Figs. 44 and 45</i>. + </p> + <p> + <a name="fig057" id="fig057"><img width="600" height="638" + src="images/fig057.jpg" + alt="Fig. 57.--Wiring Diagram Showing Fixed Loading Coils for Intermediate Wave Set." /> + </a> + </p> + <p> + <i>An Intermediate Wave Set With Variocoupler Inductance Coils</i>.--By + using the coil wound on the rotor of the variocoupler as the tickler the + coupling between the detector tube circuits and the aerial wire system + increases as the set is tuned for greater wave lengths. This scheme makes + the control of the regenerative circuit far more stable than it is where + an ordinary loose coupled tuning coil is used. + </p> + <p> + When the variocoupler is adjusted for receiving very long waves the rotor + sets at right angles to the stator and, since when it is in this position + there is no mutual induction between them, the tickler coil serves as a + loading coil for the detector plate oscillation circuit. Inductance coils + for short wave lengths are usually wound in single layers but <i>bank-wound + coils</i>, as they are called are necessary to get compactness where long + wave lengths are to be received. By winding inductance coils with two or + more layers the highest inductance values can be obtained with the least + resistance. A wiring diagram of a multipoint inductance coil is shown in + <i>Fig. 58</i>. You can buy this intermediate wave set assembled and ready + to use or get the parts and connect them up yourself. + </p> + <p> + <a name="fig058" id="fig058"><img width="600" height="469" + src="images/fig058.jpg" + alt="Fig. 58.--Wiring Diagram for Intermediate Wave Receptor with one Variocoupler and 12 section Bank-wound Inductance Coil." /> + </a> + </p> + <p> + <i>The Parts and How to Connect Them Up.</i>--For this regenerative + intermediate wave set get: (1) one <i>12 section triple bank-wound + inductance coil</i>, (2) one <i>variometer</i>, and (3) all the other + parts shown in the diagram <i>Fig. 58</i> except the variocoupler. First + connect the free end of the condenser in the aerial to one of the + terminals of the stator of the variocoupler; then connect the other + terminal of the stator with one of the ends of the bank-wound inductance + coil and connect the movable contact of this with the ground. + </p> + <p> + Next connect a wire to the aerial between the variable condenser and the + stator and connect this to one post of a .0005 microfarad fixed condenser, + then connect the other post of this with the grid of the detector and + shunt a 2 megohm grid leak around it. Connect a wire to the ground wire + between the bank-wound inductance coil and the ground proper, <i>i.e.</i>, + the radiator or water pipe, connect the other end of this to the + + electrode of the <i>A</i> battery and connect this end also to one of the + terminals of the filament. This done connect the other terminal of the + filament to one post of the rheostat and the other post of this to the - + or negative side of the <i>A</i> battery. + </p> + <p> + To the + electrode of the <i>A</i> battery connect the - or zinc pole of + the <i>B</i> battery and connect the + or carbon pole of the latter with + one post of the fixed .001 microfarad condenser. This done connect one + terminal of the tickler coil which is on the rotor of the variometer to + the plate of the detector and the other terminal of the tickler to the + other post of the .001 condenser and around this shunt your headphones. Or + if you want to use one or more amplifying tubes connect the circuit of the + first one, see <i>Fig. 45</i>, to the posts on either side of the fixed + condenser instead of the headphones. + </p> + <p> + <i>A Long Wave Receiving Set.</i>--The vivid imagination of Jules Verne + never conceived anything so fascinating as the reception of messages + without wires sent out by stations half way round the world; and in these + days of high power cableless stations on the five continents you can + listen-in to the messages and hear what is being sent out by the Lyons, + Paris and other French stations, by Great Britain, Italy, Germany and even + far off Russia and Japan. + </p> + <p> + A long wave set for receiving these stations must be able to tune to wave + lengths up to 20,000 meters. Differing from the way in which the + regenerative action of the short wave sets described in the preceding + chapter is secured and which depends on a tickler coil and the coupling + action of the detector in this long wave set, [Footnote: All of the short + wave and intermediate wave receivers described, are connected up according + to the wiring diagram used by the A. H. Grebe Company, Richmond Hill, Long + Island, N. Y.] this action is obtained by the use of a tickler coil in the + plate circuit which is inductively coupled to the grid circuit and this + feeds back the necessary amount of current. This is a very good way to + connect up the circuits for the reason that: (1) the wiring is simplified, + and (2) it gives a single variable adjustment for the entire range of wave + lengths the receptor is intended to cover. + </p> + <p> + <i>The Parts and How to Connect Them Up.</i>--The two chief features as + far as the parts are concerned of this long wave length receiving set are + (1) the <i>variable condensers</i>, and (2) the <i>tuning inductance coils</i>. + The variable condenser used in series with the aerial wire system has 26 + plates and is equal to a capacitance of <i>.0008 mfd.</i> which is the + normal aerial capacitance. The condenser used in the secondary coil + circuit has 14 plates and this is equal to a capacitance of <i>.0004 mfd</i>. + </p> + <p> + There are a number of inductance coils and these are arranged so that they + can be connected in or cut out and combinations are thus formed which give + a high efficiency and yet allow them to be compactly mounted. The + inductance coils of the aerial wire system and those of the secondary coil + circuit are practically alike. For wave lengths up to 2,200 meters <i>bank + litz-wound coils</i> are used and these are wound up in 2, 4 and 6 banks + in order to give the proper degree of coupling and inductance values. + </p> + <p> + Where wave lengths of more than 2,200 meters are to be received <i>coto-coils</i> + are used as these are the "last word" in inductance coil design, and are + especially adapted for medium as well as long wave lengths. [Footnote: Can + be had of the Coto Coil Co., Providence, R. I.] These various coils are + cut in and out by means of two five-point switches which are provided with + auxiliary levers and contactors for <i>dead-ending</i> the right amount of + the coils. In cutting in coils for increased wave lengths, that is from + 10,000 to 20,000 meters, all of the coils of the aerial are connected in + series as well as all of the coils of the secondary circuit. The + connections for a long wave receptor are shown in the wiring diagram in <i>Fig. + 59</i>. + </p> + <p> + <a name="fig059" id="fig059"><img width="600" height="427" + src="images/fig059.jpg" + alt="Fig. 59.--Wiring Diagram Showing Long Wave Receptor with Variocouplers and Bank-wound Inductance Coils" /> + </a> + </p> + <h2> + <a name="chap13" id="chap13">CHAPTER XIII</a> + </h2> + <h3> + HETERODYNE OR BEAT LONG WAVE TELEGRAPH RECEIVING SET + </h3> + <p> + Any of the receiving sets described in the foregoing chapters will respond + to either: (1) a wireless telegraph transmitter that uses a spark gap and + which sends out periodic electric waves, or to (2) a wireless telephone + transmitter that uses an arc or a vacuum tube oscillator and which sends + out continuous electric waves. To receive wireless <i>telegraph</i> + signals, however, from a transmitter that uses an arc or a vacuum tube + oscillator and which sends out continuous waves, either the transmitter or + the receptor must be so constructed that the continuous waves will be + broken up into groups of audio frequency and this is done in several + different ways. + </p> + <p> + There are four different ways employed at the present time to break up the + continuous waves of a wireless telegraph transmitter into groups and these + are: (<i>a</i>) the <i>heterodyne</i>, or <i>beat</i>, method, in which + waves of different lengths are impressed on the received waves and so + produces beats; (<i>b</i>) the <i>tikker</i>, or <i>chopper</i> method, in + which the high frequency currents are rapidly broken up; (<i>c</i>) the + variable condenser method, in which the movable plates are made to rapidly + rotate; (<i>d</i>) the <i>tone wheel</i>, or <i>frequency transformer</i>, + as it is often called, and which is really a modified form of and an + improvement on the tikker. The heterodyne method will be described in this + chapter. + </p> + <p> + <i>What the Heterodyne or Beat Method Is.</i>--The word <i>heterodyne</i> + was coined from the Greek words <i>heteros</i> which means <i>other</i>, + or <i>different</i>, and <i>dyne</i> which means <i>power</i>; in other + words it means when used in connection with a wireless receptor that + another and different high frequency current is used besides the one that + is received from the sending station. In music a <i>beat</i> means a + regularly recurrent swelling caused by the reinforcement of a sound and + this is set up by the interference of sound waves which have slightly + different periods of vibration as, for instance, when two tones take place + that are not quite in tune with each other. This, then, is the principle + of the heterodyne, or beat, receptor. + </p> + <p> + In the heterodyne, or beat method, separate sustained oscillations, that + are just about as strong as those of the incoming waves, are set up in the + receiving circuits and their frequency is just a little higher or a little + lower than those that are set up by the waves received from the distant + transmitter. The result is that these oscillations of different + frequencies interfere and reinforce each other when <i>beats</i> are + produced, the period of which is slow enough to be heard in the + headphones, hence the incoming signals can be heard only when waves from + the sending station are being received. A fuller explanation of how this + is done will be found in <a href="#chap15">Chapter XV</a>. + </p> + <p> + <i>The Autodyne or Self-Heterodyne Long-Wave Receiving Set.</i>--This is + the simplest type of heterodyne receptor and it will receive periodic + waves from spark telegraph transmitters or continuous waves from an arc or + vacuum tube telegraph transmitter. In this type of receptor the detector + tube itself is made to set up the <i>heterodyne oscillations</i> which + interfere with those that are produced by the incoming waves that are a + little out of tune with it. + </p> + <p> + With a long wave <i>autodyne</i>, or <i>self-heterodyne</i> receptor, as + this type is called, and a two-step audio-frequency amplifier you can + clearly hear many of the cableless stations of Europe and others that send + out long waves. For receiving long wave stations, however, you must have a + long aerial--a single wire 200 or more feet in length will do--and the + higher it is the louder will be the signals. Where it is not possible to + put the aerial up a hundred feet or more above the ground, you can use a + lower one and still get messages in <i>International Morse</i> fairly + strong. + </p> + <p> + <i>The Parts and Connections of an Autodyne, or Self-Heterodyne, Receiving + Set.</i>--For this long wave receiving set you will need: (1) one <i>variocoupler</i> + with the primary coil wound on the stator and the secondary coil and + tickler coil wound on the rotor, or you can use three honeycomb or other + good compact coils of the longest wave you want to receive, a table of + which is given in <a href="#chap07">Chapter XII</a>; (2) two <i>.001 mfd. + variable condensers</i>; (3) one <i>.0005 mfd. variable condenser</i>; (4) + one <i>.5 to 2 megohm grid leak resistance</i>; (5) one <i>vacuum tube + detector</i>; (6) one <i>A battery</i>; (7) one <i>rheostat</i>; (8) one + <i>B battery</i>; (9) one <i>potentiometer</i>; (10) one <i>.001 mfd. + fixed condenser</i> and (11) one pair of <i>headphones</i>. For the + two-step amplifier you must, of course, have besides the above parts the + amplifier tubes, variable condensers, batteries rheostats, potentiometers + and fixed condensers as explained in <a href="#chap09">Chapter IX</a>. The + connections for the autodyne, or self-heterodyne, receiving set are shown + in <i>Fig. 60</i>. + </p> + <p> + <a name="fig060" id="fig060"><img width="600" height="446" + src="images/fig060.jpg" + alt="Fig. 60.--Wiring Diagram of Long Wave Antodyne, or Self-Heterodyne Receptor." /> + </a> + </p> + <p> + <i>The Separate Heterodyne Long Wave Receiving Set.</i>--This is a better + long wave receptor than the self heterodyne set described above for + receiving wireless telegraph signals sent out by a continuous long wave + transmitter. The great advantage of using a separate vacuum tube to + generate the heterodyne oscillations is that you can make the frequency of + the oscillations just what you want it to be and hence you can make it a + little higher or a little lower than the oscillations set up by the + received waves. + </p> + <p> + <i>The Parts and Connections of a Separate Heterodyne Long Wave Receiving + Set.</i>--The parts required for this long wave receiving set are: (1) + four honeycomb or other good <i>compact inductance</i> coils of the + longest wave length that you want to receive; (2) three <i>.001 mfd. + variable condensers</i>; (3) one <i>.0005 mfd. variable condenser</i>; (4) + one <i>1 megohm grid leak resistance</i>; (5) one <i>vacuum tube detector</i>; + (6) one <i>A battery</i>; (7) two rheostats; (8) two <i>B batteries</i>, + one of which is supplied with taps; (9) one <i>potentiometer</i>; (10) one + <i>vacuum tube amplifier</i>, for setting up the heterodyne oscillations; + (11) a pair of <i>headphones</i> and (12) all of the parts for a <i>two-step + amplifier</i> as detailed in <a href="#chap09">Chapter IX</a>, that is if + you are going to use amplifiers. The connections are shown in <i>Fig. 61</i>. + </p> + <p> + <a name="fig061" id="fig061"><img width="600" height="571" + src="images/fig061.jpg" + alt="Fig. 61.--Wiring Diagram of Long Wave Separate Heterodyne Receiving Set." /> + </a> + </p> + <p> + In using either of these heterodyne receivers be sure to carefully adjust + the <i>B</i> battery by means of the potentiometer. + </p> + <p> + [Footnote: The amplifier tube in this case is used as a generator of + oscillations.] + </p> + <h2> + <a name="chap14" id="chap14">CHAPTER XIV</a> + </h2> + <h3> + HEADPHONES AND LOUD SPEAKERS + </h3> + <p> + <i>Wireless Headphones.</i>--A telephone receiver for a wireless receiving + set is made exactly on the same principle as an ordinary Bell telephone + receiver. The only difference between them is that the former is made flat + and compact so that a pair of them can be fastened together with a band + and worn on the head (when it is called a <i>headset</i>), while the + latter is long and cylindrical so that it can be held to the ear. A + further difference between them is that the wireless headphone is made as + sensitive as possible so that it will respond to very feeble currents, + while the ordinary telephone receiver is far from being sensitive and will + respond only to comparatively large currents. + </p> + <p> + <i>How a Bell Telephone Receiver Is Made.</i>--An ordinary telephone + receiver consists of three chief parts and these are: (1) a hard-rubber, + or composition, shell and cap, (2) a permanent steel bar magnet on one end + of which is wound a coil of fine insulated copper wire, and (3) a soft + iron disk, or <i>diaphragm</i>, all of which are shown in the + cross-section in <i>Fig. 62</i>. The bar magnet is securely fixed inside + of the handle so that the outside end comes to within about 1/32 of an + inch of the diaphragm when this is laid on top of the shell and the cap is + screwed on. + </p> + <p> + <a name="fig062" id="fig062"><img width="586" height="400" + src="images/fig062.jpg" + alt="Fig. 62.--Cross-section of Bell telephone Receiver." /></a> + </p> + <table cellspacing="20" summary="Illustration"> + <tr> + <td align="center"> + <i>Photograph unavailable</i> + </td> + </tr> + <tr> + <td align="center"> + original © Underwood and Underwood.<br /> Alexander Graham Bell, + Inventor of the Telephone, now an ardent Radio Enthusiast. + </td> + </tr> + </table> + <p> + The ends of the coil of wire are connected with two binding posts which + are in the end of the shell, but are shown in the picture at the sides for + the sake of clearness. This coil usually has a resistance of about 75 ohms + and the meaning of the <i>ohmic resistance</i> of a receiver and its + bearing on the sensitiveness of it will be explained a little farther + along. After the disk, or diaphragm, which is generally made of thin, soft + sheet iron that has been tinned or japanned, [Footnote: A disk of + photographic tin-type plate is generally used.] is placed over the end of + the magnet, the cap, which has a small opening in it, is screwed on and + the receiver is ready to use. + </p> + <p> + <i>How a Wireless Headphone Is Made.</i>--For wireless work a receiver of + the watch-case type is used and nearly always two such receivers are + connected with a headband. It consists of a permanent bar magnet bent so + that it will fit into the shell of the receiver as shown at <i>A</i> in <i>Fig. + 63</i>. + </p> + <p> + <a name="fig063" id="fig063"><img width="320" height="397" + src="images/fig063.jpg" alt="Fig. 63.--Wireless Headphone." /></a> + </p> + <p> + The ends of this magnet, which are called <i>poles</i>, are bent up, and + hence this type is called a <i>bipolar</i> receiver. The magnets are wound + with fine insulated wire as before and the diaphragm is held securely in + place over them by screwing on the cap. + </p> + <p> + <i>About Resistance, Turns of Wire and Sensitivity of Headphones.</i>--If + you are a beginner in wireless you will hear those who are experienced + speak of a telephone receiver as having a resistance of 75 ohms, 1,000 + ohms, 2,000 or 3,000 ohms, as the case may be; from this you will gather + that the higher the resistance of the wire on the magnets the more + sensitive the receiver is. In a sense this is true, but it is not the + resistance of the magnet coils that makes it sensitive, in fact, it cuts + down the current, but it is the <i>number of turns</i> of wire on them + that determines its sensitiveness; it is easy to see that this is so, for + the larger the number of turns the more often will the same current flow + round the cores of the magnet and so magnetize them to a greater extent. + </p> + <p> + But to wind a large number of turns of wire close enough to the cores to + be effective the wire must be very small and so, of course, the higher the + resistance will be. Now the wire used for winding good receivers is + usually No. 40, and this has a diameter of .0031 inch; consequently, when + you know the ohmic resistance you get an idea of the number of turns of + wire and from this you gather in a general way what the sensitivity of the + receiver is. + </p> + <p> + A receiver that is sensitive enough for wireless work should be wound to + not less than 1,000 ohms (this means each ear phone), while those of a + better grade are wound to as high as 3,000 ohms for each one. A high-grade + headset is shown in <i>Fig. 64</i>. Each phone of a headset should be + wound to the same resistance, and these are connected in series as shown. + Where two or more headsets are used with one wireless receiving set they + must all be of the same resistance and connected in series, that is, the + coils of one head set are connected with the coils of the next head set + and so on to form a continuous circuit. + </p> + <p> + <a name="fig064" id="fig064"><img width="549" height="360" + src="images/fig064.jpg" alt="Fig. 64.--Wireless Headphone." /></a> + </p> + <p> + <i>The Impedance of Headphones.</i>--When a current is flowing through a + circuit the material of which the wire is made not only opposes its + passage--this is called its <i>ohmic resistance</i>--but a <i>counter-electromotive + force</i> to the current is set up due to the inductive effects of the + current on itself and this is called <i>impedance</i>. Where a wire is + wound in a coil the impedance of the circuit is increased and where an + alternating current is used the impedance grows greater as the frequency + gets higher. The impedance of the magnet coils of a receiver is so great + for high frequency oscillations that the latter cannot pass through them; + in other words, they are choked off. + </p> + <p> + <i>How the Headphones Work.</i>--As you will see from the cross-sections + in <i>Figs. 62</i> and <i>63</i> there is no connection, electrical or + mechanical, between the diaphragm and the other parts of the receiver. Now + when either feeble oscillations, which have been rectified by a detector, + or small currents from a <i>B</i> battery, flow through the magnet coils + the permanent steel magnet is energized to a greater extent than when no + current is flowing through it. This added magnetic energy makes the magnet + attract the diaphragm more than it would do by its own force. If, on the + other hand, the current is cut off the pull of the magnet is lessened and + as its attraction for the diaphragm is decreased the latter springs back + to its original position. When varying currents flow through the coils the + diaphragm vibrates accordingly and sends out sound waves. + </p> + <p> + <i>About Loud Speakers.</i>--The simplest acoustic instrument ever + invented is the <i>megaphone</i>, which latter is a Greek word meaning <i>great + sound</i>. It is a very primitive device and our Indians made it out of + birch-bark before Columbus discovered America. In its simplest form it + consists of a cone-shaped horn and as the speaker talks into the small end + the concentrated sound waves pass out of the large end in whatever + direction it is held. + </p> + <p> + Now a loud speaker of whatever kind consists of two chief parts and these + are: (1) a <i>telephone receiver</i>, and (2) a <i>megaphone</i>, or <i>horn</i> + as it is called. A loud speaker when connected with a wireless receiving + set makes it possible for a room, or an auditorium, full of people, or an + outdoor crowd, to hear what is being sent out by a distant station instead + of being limited to a few persons listening-in with headphones. To use a + loud speaker you should have a vacuum tube detector receiving set and this + must be provided with a one-step amplifier at least. + </p> + <p> + To get really good results you need a two-step amplifier and then energize + the plate of the second vacuum tube amplifier with a 100 volt <i>B</i> + battery; or if you have a three-step amplifier then use the high voltage + on the plate of the third amplifier tube. Amplifying tubes are made to + stand a plate potential of 100 volts and this is the kind you must use. + Now it may seem curious, but when the current flows through the coils of + the telephone receiver in one direction it gives better results than when + it flows through in the other direction; to find out the way the current + gives the best results try it out both ways and this you can do by simply + reversing the connections. + </p> + <p> + <i>The Simplest Type of Loud Speaker.</i>--This loud speaker, which is + called, the Arkay, [Footnote: Made by the Riley-Klotz Mfg. Co., Newark, N. + J.] will work on a one- or two-step amplifier. It consists of a brass horn + with a curve in it and in the bottom there is an adapter, or frame, with a + set screw in it so that you can fit in one of your headphones and this is + all there is to it. The construction is rigid enough to prevent overtones, + or distortion of speech or music. It is shown in <i>Fig. 65</i>. + </p> + <p> + <a name="fig065" id="fig065"><img width="280" height="325" + src="images/fig065.jpg" alt="Fig. 65.--Arkay Loud Speaker." /></a> + </p> + <p> + <i>Another Simple Kind of Loud Speaker.</i>--Another loud speaker, see <i>Fig. + 66</i>, is known as the <i>Amplitone</i> [Footnote: Made by the American + Pattern, Foundry and Machine Co., 82 Church Street, N. Y. C.] and it + likewise makes use of the headphones as the sound producer. This device + has a cast metal horn which improves the quality of the sound, and all you + have to do is to slip the headphones on the inlet tubes of the horn and it + is ready for use. The two headphones not only give a longer volume of + sound than where a single one is used but there is a certain blended + quality which results from one phone smoothing out the imperfections of + the other. + </p> + <p> + <a name="fig066" id="fig066"><img width="280" height="312" + src="images/fig066.jpg" alt="Fig. 66.--Amplitone Loud Speaker." /></a> + </p> + <p> + <i>A Third Kind of Simple Loud Speaker.</i>--The operation of the <i>Amplitron</i>, + [Footnote: Made by the Radio Service Co., 110 W. 40th Street, N. Y.] as + this loud speaker is called, is slightly different from others used for + the same purpose. The sounds set up by the headphone are conveyed to the + apex of an inverted copper cone which is 7 inches long and 10 inches in + diameter. Here it is reflected by a parabolic mirror which greatly + amplifies the sounds. The amplification takes place without distortion, + the sounds remaining as clear and crisp as when projected by the + transmitting station. By removing the cap from the receiver the shell is + screwed into a receptacle on the end of the loud speaker and the + instrument is ready for use. It is pictured in <i>Fig. 67</i>. + </p> + <p> + <a name="fig067" id="fig067"><img width="400" height="390" + src="images/fig067.jpg" alt="Fig. 67.--Amplitron Loud Speaker." /></a> + </p> + <p> + <i>A Super Loud Speaker.</i>--This loud speaker, which is known as the <i>Magnavox + Telemegafone</i>, was the instrument used by Lt. Herbert E. Metcalf, 3,000 + feet in the air, and which startled the City of Washington on April 2, + 1919, by repeating President Wilson's <i>Victory Loan Message</i> from an + airplane in flight so that it was distinctly heard by 20,000 people below. + </p> + <p> + This wonderful achievement was accomplished through the installation of + the <i>Magnavox</i> and amplifiers in front of the Treasury Building. + Every word Lt. Metcalf spoke into his wireless telephone transmitter was + caught and swelled in volume by the <i>Telemegafones</i> below and persons + blocks away could hear the message plainly. Two kinds of these loud + speakers are made and these are: (1) a small loud speaker for the use of + operators so that headphones need not be worn, and (2) a large loud + speaker for auditorium and out-door audiences. + </p> + <table cellspacing="20" summary="Illustration"> + <tr> + <td align="center"> + <i>Photograph unavailable</i> + </td> + </tr> + <tr> + <td align="center"> + original © Underwood and Underwood.<br /> World's Largest Loud + Speaker ever made. Installed in Lytle Park, Cincinnati, Ohio, to + permit President Harding's Address at Point Pleasant, Ohio, during the + Grant Centenary Celebration to be heard within a radius of one square. + </td> + </tr> + </table> + <p> + Either kind may be used with a one- or two-step amplifier or with a + cascade of half a dozen amplifiers, according to the degree of loudness + desired. The <i>Telemegafone</i> itself is not an amplifier in the true + sense inasmuch as it contains no elements which will locally increase the + incoming current. It does, however, transform the variable electric + currents of the wireless receiving set into sound vibrations in a most + wonderful manner. + </p> + <p> + A <i>telemegafone</i> of either kind is formed of: (1) a telephone + receiver of large proportions, (2) a step-down induction coil, and (3) a 6 + volt storage battery that energizes a powerful electromagnet which works + the diaphragm. An electromagnet is used instead of a permanent magnet and + this is energized by a 6-volt storage battery as shown in the wiring + diagram at <i>A</i> in <i>Fig. 68</i>. One end of the core of this magnet + is fixed to the iron case of the speaker and together these form the + equivalent of a horseshoe magnet. A movable coil of wire is supported from + the center of the diaphragm the edge of which is rigidly held between the + case and the small end of the horn. This coil is placed over the upper end + of the magnet and its terminals are connected to the secondary of the + induction coil. Now when the coil is energized by the current from the + amplifiers it and the core act like a solenoid in that the coil tends to + suck the core into it; but since the core is fixed and the coil is movable + the core draws the coil down instead. The result is that with every + variation of the current that flows through the coil it moves up and down + and pulls and pushes the diaphragm down and up with it. The large + amplitude of the vibrations of the latter set up powerful sound waves + which can be heard several blocks away from the horn. In this way then are + the faint incoming signals, speech and music which are received by the + amplifying receiving set reproduced and magnified enormously. The <i>Telemegafone</i> + is shown complete at <i>B</i>. + </p> + <p> + <a name="fig068" id="fig068"><img width="600" height="517" + src="images/fig068.jpg" alt="Fig. 68.--Magnavox Loud Speaker." /></a> + </p> + <h2> + <a name="chap15" id="chap15">CHAPTER XV</a> + </h2> + <h3> + OPERATION OF VACUUM TUBE RECEPTORS + </h3> + <p> + From the foregoing chapters you have seen that the vacuum tube can be used + either as a <i>detector</i> or an <i>amplifier</i> or as a <i>generator</i> + of electric oscillations, as in the case of the heterodyne receiving set. + To understand how a vacuum tube acts as a detector and as an amplifier you + must first know what <i>electrons</i> are. The way in which the vacuum + tube sets up sustained oscillations will be explained in <a href="#chap18">Chapter + XVIII</a> in connection with the <i>Operation of Vacuum Tube Transmitters</i>. + </p> + <p> + <i>What Electrons Are.</i>--Science teaches us that masses of matter are + made up of <i>molecules</i>, that each of these is made up of <i>atoms</i>, + and each of these, in turn, is made up of a central core of positive + particles of electricity surrounded by negative particles of electricity + as shown in the schematic diagram, <i>Fig. 69</i>. The little black + circles inside the large circle represent <i>positive particles of + electricity</i> and the little white circles outside of the large circle + represent <i>negative particles of electricity</i>, or <i>electrons</i> as + they are called. + </p> + <p> + <a name="fig069" id="fig069"><img width="600" height="410" + src="images/fig069.jpg" alt="Fig. 69.--Schematic Diagram of an Atom." /></a> + </p> + <p> + It is the number of positive particles of electricity an atom has that + determines the kind of an element that is formed when enough atoms of the + same kind are joined together to build it up. Thus hydrogen, which is the + lightest known element, has one positive particle for its nucleus, while + uranium, the heaviest element now known, has 92 positive particles. Now + before leaving the atom please note that it is as much smaller than the + diagram as the latter is smaller than our solar system. + </p> + <p> + <i>What Is Meant by Ionization.</i>--A hydrogen atom is not only lighter + but it is smaller than the atom of any other element while an electron is + more than a thousand times smaller than the atom of which it is a part. + Now as long as all of the electrons remain attached to the surface of an + atom its positive and negative charges are equalized and it will, + therefore, be neither positive nor negative, that is, it will be perfectly + neutral. When, however, one or more of its electrons are separated from + it, and there are several ways by which this can be done, the atom will + show a positive charge and it is then called a <i>positive ion</i>. + </p> + <p> + In other words a <i>positive ion</i> is an atom that has lost some of its + negative electrons while a <i>negative ion</i> is one that has acquired + some additional negative <i>electrons</i>. When a number of electrons are + being constantly given by the atoms of an element, which let us suppose is + a metal, and are being attracted to atoms of another element, which we + will say is also a metal, a flow of electrons takes place between the two + oppositely charged elements and form a current of negative electricity as + represented by the arrows at <i>A</i> in <i>Fig. 70</i>. + </p> + <p> + <a name="fig070" id="fig070"><img width="600" height="277" + src="images/fig070.jpg" + alt="Fig. 70.--Action of Two-electrode Vacuum Tube." /></a> + </p> + <p> + When a stream of electrons is flowing between two metal elements, as a + filament and a plate in a vacuum tube detector, or an amplifier, they act + as <i>carriers</i> for more negative electrons and these are supplied by a + battery as we shall presently explain. It has always been customary for us + to think of a current of electricity as flowing from the positive pole of + a battery to the negative pole of it and hence we have called this the <i>direction + of the current</i>. Since the electronic theory has been evolved it has been + shown that the electrons, or negative charges of electricity, flow from + the negative to the positive pole and that the ionized atoms, which are + more positive than negative, flow in the opposite direction as shown at <i>B</i>. + </p> + <p> + <i>How Electrons are Separated from Atoms</i>.--The next question that + arises is how to make a metal throw off some of the electrons of the atoms + of which it is formed. There are several ways that this can be done but in + any event each atom must be given a good, hard blow. A simple way to do + this is to heat a metal to incandescence when the atoms will bombard each + other with terrific force and many of the electrons will be knocked off + and thrown out into the surrounding space. + </p> + <p> + But all, or nearly all, of them will return to the atoms from whence they + came unless a means of some kind is employed to attract them to the atoms + of some other element. This can be done by giving the latter piece of + metal a positive charge. If now these two pieces of metal are placed in a + bulb from which the air has been exhausted and the first piece of metal is + heated to brilliancy while the second piece of metal is kept positively + electrified then a stream of electrons will flow between them. + </p> + <p> + <i>Action of the Two Electrode Vacuum Tube.</i>--Now in a vacuum tube + detector a wire filament, like that of an incandescent lamp, is connected + with a battery and this forms the hot element from which the electrons are + thrown off, and a metal plate with a terminal wire secured to it is + connected to the positive or carbon tap of a dry battery; now connect the + negative or zinc tap of this with one end of a telephone receiver and the + other end of this with the terminals of the filament as shown at <i>A</i> + in <i>Fig. 71</i>. If now you heat the filament and hold the phone to your + ear you can hear the current from the <i>B</i> battery flowing through the + circuit. + </p> + <p> + <a name="fig071ab" id="fig071ab"><img width="600" height="321" + src="images/fig071ab.jpg" + alt="(A) and (B) Fig. 71.--How a Two Electrode Tube Acts as a Relay or a Detector." /> + </a> <a name="fig071c" id="fig071c"><img width="600" height="396" + src="images/fig071c.jpg" + alt="(C) Fig. 71.--Only the Positive Part of Oscillations Goes through the Tube." /> + </a> + </p> + <p> + Since the electrons are negative charges of electricity they are not only + thrown off by the hot wire but they are attracted by the positive charged + metal plate and when enough electrons pass, or flow, from the hot wire to + the plate they form a conducting path and so complete the circuit which + includes the filament, the plate and the <i>B</i> or plate battery, when + the current can then flow through it. As the number of electrons that are + thrown off by the filament is not great and the voltage of the plate is + not high the current that flows between the filament and the plate is + always quite small. + </p> + <p> + <i>How the Two Electrode Tube Acts as a Detector.</i>--As the action of a + two electrode tube as a detector [Footnote: The three electrode vacuum + tube has entirely taken the place of the two electrode type.] is simpler + than that of the three electrode vacuum tube we shall describe it first. + The two electrode vacuum tube was first made by Mr. Edison when he was + working on the incandescent lamp but that it would serve as a detector of + electric waves was discovered by Prof. Fleming, of Oxford University, + London. As a matter of fact, it is not really a detector of electric + waves, but it acts as: (1) a <i>rectifier</i> of the oscillations that are + set up in the receiving circuits, that is, it changes them into pulsating + direct currents so that they will flow through and affect a telephone + receiver, and (2) it acts as a <i>relay</i> and the feeble received + oscillating current controls the larger direct current from the <i>B</i> + battery in very much the same way that a telegraph relay does. This latter + relay action will be explained when we come to its operation as an + amplifier. + </p> + <p> + We have just learned that when the stream of electrons flow from the hot + wire to the cold positive plate in the tube they form a conducting path + through which the battery current can flow. Now when the electric + oscillations surge through the closed oscillation circuit, which includes + the secondary of the tuning coil, the variable condenser, the filament and + the plate as shown at <i>B</i> in <i>Fig. 71</i> the positive part of them + passes through the tube easily while the negative part cannot get through, + that is, the top, or positive, part of the wave-form remains intact while + the lower, or negative, part is cut off as shown in the diagram at <i>C</i>. + As the received oscillations are either broken up into wave trains of + audio frequency by the telegraph transmitter or are modulated by a + telephone transmitter they carry the larger impulses of the direct current + from the <i>B</i> battery along with them and these flow through the + headphones. This is the reason the vacuum tube amplifies as well as + detects. + </p> + <p> + <i>How the Three Electrode Tube Acts as a Detector.</i>--The vacuum tube + as a detector has been made very much more sensitive by the use of a third + electrode shown in <i>Fig. 72</i>. In this type of vacuum tube the third + electrode, or <i>grid</i>, is placed between the filament and the plate + and this controls the number of electrons flowing from the filament to the + plate; in passing between these two electrodes they have to go through the + holes formed by the grid wires. + </p> + <p> + <a name="fig072ab" id="fig072ab"><img width="600" height="359" + src="images/fig072ab.jpg" + alt="(A) and (B) Fig. 72.--How the Positive and Negative Voltages of Oscillations Act on the Electrons." /> + </a> <a name="fig072c" id="fig072c"><img width="600" height="342" + src="images/fig072c.jpg" + alt="(C) Fig. 72.--How the Three Electrode Tube Acts as a Detector and Amplifier." /> + </a> <a name="fig072d" id="fig072d"><img width="600" height="448" + src="images/fig072d.jpg" + alt="(D) Fig. 72.--How the Oscillations Control the Flow of the Battery Current through the Tube." /> + </a> + </p> + <p> + If now the grid is charged to a higher <i>negative</i> voltage than the + filament the electrons will be stopped by the latter, see <i>A</i>, though + some of them will go through to the plate because they travel at a high + rate of speed. The higher the negative charge on the grid the smaller will + be the number of electrons that will reach the plate and, of course, the + smaller will be the amount of current that will flow through the tube and + the headphones from the <i>B</i> battery. + </p> + <p> + On the other hand if the grid is charged <i>positively</i>, see <i>B</i>, + then more electrons will strike the plate than when the grid is not used + or when it is negatively charged. But when the three electrode tube is + used as a detector the oscillations set up in the circuits change the grid + alternately from negative to positive as shown at <i>C</i> and hence the + voltage of the <i>B</i> battery current that is allowed to flow through + the detector from the plate to the filament rises and falls in unison with + the voltage of the oscillating currents. The way the positive and negative + voltages of the oscillations which are set up by the incoming waves, + energize the grid; how the oscillator tube clips off the negative parts of + them, and, finally, how these carry the battery current through the tube + are shown graphically by the curves at <i>D</i>. + </p> + <p> + <i>How the Vacuum Tube Acts as an Amplifier</i>.--If you connect up the + filament and the plate of a three electrode tube with the batteries and do + not connect in the grid, you will find that the electrons which are thrown + off by the filament will not get farther than the grid regardless of how + high the voltage is that you apply to the plate. This is due to the fact + that a large number of electrons which are thrown off by the filament + strike the grid and give it a negative charge, and consequently, they + cannot get any farther. Since the electrons do not reach the plate the + current from the <i>B</i> battery cannot flow between it and the filament. + </p> + <p> + Now with a properly designed amplifier tube a very small negative voltage + on the grid will keep a very large positive voltage on the plate from + sending a current through the tube, and oppositely, a very small positive + voltage on the grid will let a very large plate current flow through the + tube; this being true it follows that any small variation of the voltage + from positive to negative on the grid and the other way about will vary a + large current flowing from the plate to the filament. + </p> + <p> + In the Morse telegraph the relay permits the small current that is + received from the distant sending station to energize a pair of magnets, + and these draw an armature toward them and close a second circuit when a + large current from a local battery is available for working the sounder. + The amplifier tube is a variable relay in that the feeble currents set up + by the incoming waves constantly and proportionately vary a large current + that flows through the headphones. This then is the principle on which the + amplifying tube works. + </p> + <p> + <i>The Operation of a Simple Vacuum Tube Receiving Set</i>.--The way a + simple vacuum tube detector receiving set works is like this: when the + filament is heated to brilliancy it gives off electrons as previously + described. Now when the electric waves impinge on the aerial wire they set + up oscillations in it and these surge through the primary coil of the + loose coupled tuning coil, a diagram of which is shown at <i>B</i> in <i>Fig. + 41</i>. + </p> + <p> + The energy of these oscillations sets up oscillations of the same + frequency in the secondary coil and these high frequency currents whose + voltage is first positive and then negative, surge in the closed circuit + which includes the secondary coil and the variable condenser. At the same + time the alternating positive and negative voltage of the oscillating + currents is impressed on the grid; at each change from + to - and back + again it allows the electrons to strike the plate and then shuts them off; + as the electrons form the conducting path between the filament and the + plate the larger direct current from the <i>B</i> battery is permitted to + flow through the detector tube and the headphones. + </p> + <p> + <i>Operation of a Regenerative Vacuum Tube Receiving Set</i>.--By feeding + back the pulsating direct current from the <i>B</i> battery through the + tickler coil it sets up other and stronger oscillations in the secondary + of the tuning coil when these act on the detector tube and increase its + sensitiveness to a remarkable extent. The regenerative, or <i>feed back</i>, + action of the receiving circuits used will be easily understood by + referring back to <i>B</i> in <i>Fig. 47</i>. + </p> + <p> + When the waves set up oscillations in the primary of the tuning coil the + energy of them produces like oscillations in the closed circuit which + includes the secondary coil and the condenser; the alternating positive + and negative voltages of these are impressed on the grid and these, as we + have seen before, cause similar variations of the direct current from the + <i>B</i> battery which acts on the plate and which flows between the + latter and the filament. + </p> + <p> + This varying direct current, however, is made to flow back through the + third, or tickler coil of the tuning coil and sets up in the secondary + coil and circuits other and larger oscillating currents and these augment + the action of the oscillations produced by the incoming waves. These extra + and larger currents which are the result of the feedback then act on the + grid and cause still larger variations of the current in the plate voltage + and hence of the current of the <i>B</i> battery that flows through the + detector and the headphones. At the same time the tube keeps on responding + to the feeble electric oscillations set up in the circuits by the incoming + waves. This regenerative action of the battery current augments the + original oscillations many times and hence produce sounds in the + headphones that are many times greater than where the vacuum tube detector + alone is used. + </p> + <p> + <i>Operation of Autodyne and Heterodyne Receiving Sets</i>.--On page <i>109</i> + [Chapter VII] we discussed and at <i>A</i> in <i>Fig. 36</i> is shown a + picture of two tuning forks mounted on sounding boxes to illustrate the + principle of electrical tuning. When a pair of these forks are made to + vibrate exactly the same number of times per second there will be a + condensation of the air between them and the sound waves that are sent out + will be augmented. But if you adjust one of the forks so that it will + vibrate 256 times a second and the other fork so that it will vibrate 260 + times a second then there will be a phase difference between the two sets + of waves and the latter will augment each other 4 times every second and + you will hear these rising and falling sounds as <i>beats</i>. + </p> + <p> + Now electric oscillations set up in two circuits that are coupled together + act in exactly the same way as sound waves produced by two tuning forks + that are close to each other. Since this is true if you tune one of the + closed circuits so that the oscillations in it will have a frequency of a + 1,000,000 and tune the other circuit so that the oscillations in it have a + frequency of 1,001,000 a second then the oscillations will augment each + other 1,000 times every second. + </p> + <p> + As these rising and falling currents act on the pulsating currents from + the B battery which flow through the detector tube and the headphones you + will hear them as beats. A graphic representation of the oscillating + currents set up by the incoming waves, those produced by the heterodyne + oscillator and the beats they form is shown in <i>Fig. 73</i>. To produce + these beats a receptor can use: (1) a single vacuum tube for setting up + oscillations of both frequencies when it is called an <i>autodyne</i>, or + <i>self-heterodyne</i> receptor, or (2) a separate vacuum tube for setting + up the oscillations for the second circuit when it is called a <i>heterodyne</i> + receptor. + </p> + <p> + <a name="fig073" id="fig073"><img width="600" height="680" + src="images/fig073.jpg" alt="Fig. 73.--How the Heterodyne Receptor Works." /></a> + </p> + <p> + <i>The Autodyne, or Self-Heterodyne Receiving Set</i>.--Where only one + vacuum tube is used for producing both frequencies you need only a + regenerative, or feed-back receptor; then you can tune the aerial wire + system to the incoming waves and tune the closed circuit of the secondary + coil so that it will be out of step with the former by 1,000 oscillations + per second, more or less, the exact number does not matter in the least. + From this you will see that any regenerative set can be used for autodyne, + or self-heterodyne, reception. + </p> + <p> + <i>The Separate Heterodyne Receiving Set.</i>--The better way, however, is + to use a separate vacuum tube for setting up the heterodyne oscillations. + The latter then act on the oscillations that are produced by the incoming + waves and which energize the grid of the detector tube. Note that the + vacuum tube used for producing the heterodyne oscillations is a <i>generator</i> + of electric oscillations; the latter are impressed on the detector + circuits through the variable coupling, the secondary of which is in + series with the aerial wire as shown in <i>Fig. 74</i>. The way in which + the tube acts as a generator of oscillations will be told in <a + href="#chap18">Chapter XVIII</a>. + </p> + <p> + <a name="fig074" id="fig074"><img width="461" height="400" + src="images/fig074.jpg" alt="Fig. 74.--Separate Heterodyne Oscillator." /></a> + </p> + <h2> + <a name="chap16" id="chap16">CHAPTER XVI</a> + </h2> + <h3> + CONTINUOUS WAVE TELEGRAPH TRANSMITTING SETS WITH DIRECT CURRENT + </h3> + <p> + In the first part of this book we learned about spark-gap telegraph sets + and how the oscillations they set up are <i>damped</i> and the waves they + send out are <i>periodic</i>. In this and the next chapter we shall find + out how vacuum tube telegraph transmitters are made and how they set up + oscillations that are <i>sustained</i> and radiate waves that are <i>continuous</i>. + </p> + <p> + Sending wireless telegraph messages by continuous waves has many features + to recommend it as against sending them by periodic waves and among the + most important of these are that the transmitter can be: (1) more sharply + tuned, (2) it will send signals farther with the same amount of power, and + (3) it is noiseless in operation. The disadvantageous features are that: + (1) a battery current is not satisfactory, (2) its circuits are somewhat + more complicated, and (3) the oscillator tubes burn out occasionally. + There is, however, a growing tendency among amateurs to use continuous + wave transmitters and they are certainly more up-to-date and interesting + than spark gap sets. + </p> + <p> + Now there are two practical ways by which continuous waves can be set up + for sending either telegraphic signals or telephonic speech and music and + these are with: (a) an <i>oscillation arc lamp</i>, and (b) a <i>vacuum + tube oscillator</i>. The oscillation arc was the earliest known way of + setting up sustained oscillations, and it is now largely used for + commercial high power, long distance work. But since the vacuum tube has + been developed to a high degree of efficiency and is the scheme that is + now in vogue for amateur stations we shall confine our efforts here to + explaining the apparatus necessary and how to wire the various parts + together to produce several sizes of vacuum tube telegraph transmitters. + </p> + <p> + <i>Sources of Current for Telegraph Transmitting Sets</i>.--Differing from + a spark-gap transmitter you cannot get any appreciable results with a low + voltage battery current to start with. For a purely experimental vacuum + tube telegraph transmitter you can use enough <i>B</i> batteries to + operate it but the current strength of these drops so fact when they are + in use, that they are not at all satisfactory for the work. + </p> + <p> + You can, however, use 110 volt direct current from a lighting circuit as + your initial source of power to energize the plate of the vacuum tube + oscillator of your experimental transmitter. Where you have a 110 volt <i>direct + current</i> lighting service in your home and you want a higher voltage + for your plate, you will then have to use a motor-generator set and this + costs money. If you have 110 volt <i>alternating current</i> lighting + service at hand your troubles are over so far as cost is concerned for you + can step it up to any voltage you want with a power transformer. In this + chapter will be shown how to use a direct current for your source of + initial power and in the next chapter how to use an alternating current + for the initial power. + </p> + <p> + <i>An Experimental Continuous Wave Telegraph Transmitter.</i>--You will + remember that in <a href="#chap15">Chapter XV</a> we learned how the + heterodyne receiver works and that in the separate heterodyne receiving + set the second vacuum tube is used solely to set up oscillations. Now + while this extra tube is used as a generator of oscillations these are, of + course, very weak and hence a detector tube cannot be used to generate + oscillations that are useful for other purposes than heterodyne receptors + and measurements. + </p> + <p> + There is a vacuum tube amplifier [Footnote: This is the <i>radiation</i> + UV-<i>201</i>, made by the Radio Corporation of America, Woolworth Bldg., + New York City.] made that will stand a plate potential of 100 volts, and + this can be used as a generator of oscillations by energizing it with a + 110 volt direct current from your lighting service. Or in a pinch you can + use five standard <i>B</i> batteries to develop the plate voltage, but + these will soon run down. But whatever you do, never use a current from a + lighting circuit on a tube of any kind that has a rated plate potential of + less than 100 volts. + </p> + <p> + <i>The Apparatus You Need</i>.--For this experimental continuous wave + telegraph transmitter get the following pieces of apparatus: (1) one <i>single + coil tuner with three clips</i>; (2) one <i>.002 mfd. fixed condenser</i>; + (3) three <i>.001 mfd. condensers</i>; (4) one <i>adjustable grid leak</i>; + (5) one <i>hot-wire ammeter</i>; (6) one <i>buzzer</i>; (7) one <i>dry + cell</i>; (8) one <i>telegraph key</i>; (9) one <i>100 volt plate vacuum + tube amplifier</i>; (10) one <i>6 volt storage battery</i>; (11) one <i>rheostat</i>; + (12) one <i>oscillation choke coil</i>; (13) one <i>panel cut-out</i> with + a <i>single-throw, double-pole switch</i>, and a pair of <i>fuse sockets</i> + on it. + </p> + <p> + <i>The Tuning Coil</i>.--You can either make this tuning coil or buy one. + To make it get two disks of wood 3/4-inch thick and 5 inches in diameter + and four strips of hard wood, or better, hard rubber or composition + strips, such as <i>bakelite</i>, 1/2-inch thick, 1 inch wide and 5-3/4 + inches long, and screw them to the disks as shown at <i>A</i> in <i>Fig. + 75</i>. Now wrap on this form about 25 turns of No. 8 or 10, Brown and + Sharpe gauge, bare copper wire with a space of 1/8-inch between each turn. + Get three of the smallest size terminal clips, see <i>B</i>, and clip them + on to the different turns, when your tuning coil is ready for use. You can + buy a coil of this kind for $4.00 or $5.00. + </p> + <p> + <i>The Condensers</i>.--For the aerial series condenser get one that has a + capacitance of .002 mfd. and that will stand a potential of 3,000 volts. + [Footnote: The U C-1014 <i>Faradon</i> condenser made by the Radio + Corporation of America will serve the purpose.] It is shown at <i>C</i>. + The other three condensers, see <i>D</i>, are also of the fixed type and + may have a capacitance of .001 mfd.; [Footnote: List No. 266; fixed + receiving condenser, sold by the Manhattan Electrical Supply Co.] the + blocking condenser should preferably have a capacitance of 1/2 a mfd. In + these condensers the leaves of the sheet metal are embedded in + composition. The aerial condenser will cost you $2.00 and the others 75 + cents each. + </p> + <p> + <a name="fig075a" id="fig075a"><img width="587" height="800" + src="images/fig075a.jpg" + alt="(A) Fig. 75.--Apparatus for Experimental C. W. Telegraph Transmitter." /> + </a> <a name="fig075b" id="fig075b"><img width="600" height="526" + src="images/fig075b.jpg" + alt="Fig. 75.--Apparatus for Experimental C. W. Telegraph Transmitter." /> + </a> + </p> + <p> + <i>The Aerial Ammeter.</i>--This instrument is also called a <i>hot-wire</i> + ammeter because the oscillating currents flowing through a piece of wire + heat it according to their current strength and as the wire contracts and + expands it moves a needle over a scale. The ammeter is connected in the + aerial wire system, either in the aerial side or the ground side--the + latter place is usually the most convenient. When you tune the transmitter + so that the ammeter shows the largest amount of current surging in the + aerial wire system you can consider that the oscillation circuits are in + tune. A hot-wire ammeter reading to 2.5 amperes will serve your needs, it + costs $6.00 and is shown at <i>E</i> in <i>Fig. 75</i>. + </p> + <table cellspacing="20" summary="Illustration"> + <tr> + <td align="center"> + <i>Photograph unavailable</i> + </td> + </tr> + <tr> + <td align="center"> + United States Naval High Power Station, Arlington Va. General view of + Power Room. At the left can be seen the Control Switchboards, and + overhead, the great 30 K.W. Arc Transmitter with Accessories. + </td> + </tr> + </table> + <p> + <i>The Buzzer and Dry Cell</i>.--While a heterodyne, or beat, receptor can + receive continuous wave telegraph signals an ordinary crystal or vacuum + tube detector receiving set cannot receive them unless they are broken up + into trains either at the sending station or at the receiving station, and + it is considered the better practice to do this at the former rather than + at the latter station. For this small transmitter you can use an ordinary + buzzer as shown at <i>F</i>. A dry cell or two must be used to energize + the buzzer. You can get one for about 75 cents. + </p> + <p> + <i>The Telegraph Key</i>.--Any kind of a telegraph key will serve to break + up the trains of sustained oscillations into dots and dashes. The key + shown at <i>G</i> is mounted on a composition base and is the cheapest key + made, costing $1.50. + </p> + <p> + <i>The Vacuum Tube Oscillator</i>.--As explained before you can use any + amplifying tube that is made for a plate potential of 100 volts. The + current required for heating the filament is about 1 ampere at 6 volts. A + porcelain socket should be used for this tube as it is the best insulating + material for the purpose. An amplifier tube of this type is shown at <i>H</i> + and costs $6.50. + </p> + <p> + <i>The Storage Battery</i>.--A storage battery is used to heat the + filament of the tube, just as it is with a detector tube, and it can be of + any make or capacity as long as it will develop 6 volts. The cheapest 6 + volt storage battery on the market has a 20 to 40 ampere-hour capacity and + sells for $13.00. + </p> + <p> + <i>The Battery Rheostat</i>.--As with the receptors a rheostat is needed + to regulate the current that heats the filament. A rheostat of this kind + is shown at <i>I</i> and is listed at $1.25. + </p> + <p> + <i>The Oscillation Choke Coil</i>.--This coil is connected in between the + oscillation circuits and the source of current which feeds the oscillator + tube to keep the oscillations set up by the latter from surging back into + the service wires where they would break down the insulation. You can make + an oscillation choke coil by winding say 100 turns of No. 28 Brown and + Sharpe gauge double cotton covered magnet wire on a cardboard cylinder 2 + inches in diameter and 2-1/2 inches long. + </p> + <p> + <i>Transmitter Connectors</i>.--For connecting up the different pieces of + apparatus of the transmitter it is a good scheme to use <i>copper braid</i>; + this is made of braided copper wire in three sizes and sells for 7,15 and + 20 cents a foot respectively. A piece of it is pictured at <i>J</i>. + </p> + <p> + <i>The Panel Cut-Out</i>.--This is used to connect the cord of the + 110-volt lamp socket with the transmitter. It consists of a pair of <i>plug + cutouts and a single-throw, double-pole</i> switch mounted on a porcelain + base as shown at <i>K</i>. In some localities it is necessary to place + these in an iron box to conform to the requirements of the fire + underwriters. + </p> + <p> + <i>Connecting Up the Transmitting Apparatus</i>.--The way the various + pieces of apparatus are connected together is shown in the wiring diagram. + <i>Fig. 76</i>. Begin by connecting one post of the ammeter with the wire + that leads to the aerial and the other post of it to one end of the tuning + coil; connect clip <i>1</i> to one terminal of the .002 mfd. 3,000 volt + aerial condenser and the other post of this with the ground. + </p> + <p> + <a name="fig076" id="fig076"><img width="600" height="538" + src="images/fig076.jpg" + alt="Fig. 76--Experimental C.W. Telegraph Transmitter" /></a> + </p> + <p> + Now connect the end of the tuning coil that leads to the ammeter with one + end of the .001 mfd. grid condenser and the other end of this with the + grid of the vacuum tube. Connect the telegraph key, the buzzer and the dry + cell in series and then shunt them around the grid condenser. Next connect + the plate of the tube with one end of the .001 mfd. blocking condenser and + the other end of this with the clip <i>2</i> on the tuning coil. + </p> + <p> + Connect one end of the filament with the + or positive electrode of the + storage battery, the - or negative electrode of this with one post of the + rheostat and the other post of the latter with the other end of the + filament; then connect clip <i>3</i> with the + or positive side of the + storage battery. This done connect one end of the choke coil to the + conductor that leads to the plate and connect the other end of the choke + coil to one of the taps of the switch on the panel cut-out. Connect the + + or positive electrode of the storage battery to the other switch tap and + between the switch and the choke coil connect the protective condenser + across the 110 volt feed wires. Finally connect the lamp cord from the + socket to the plug fuse taps when your experimental continuous wave + telegraph transmitter is ready to use. + </p> + <p> + <i>A 100 Mile C. W. Telegraph Transmitter</i>.--Here is a continuous wave + telegraph transmitter that will cover distances up to 100 miles that you + can rely on. It is built on exactly the same lines as the experimental + transmitter just described, but instead of using a 100 volt plate + amplifier as a makeshift generator of oscillations it employs a vacuum + tube made especially for setting up oscillations and instead of having a + low plate voltage it is energized with 350 volts. + </p> + <p> + <i>The Apparatus You Need</i>.--For this transmitter you require: (1) one + <i>oscillation transformer</i>; (2) one <i>hot-wire ammeter</i>; (3) one + <i>aerial series condenser</i>; (4) one <i>grid leak resistance</i>; (5) + one <i>chopper</i>; (6) one <i>key circuit choke coil</i>; (7) one <i>5 + watt vacuum tube oscillator</i>; (8) one <i>6 volt storage battery</i>; + (9) one <i>battery rheostat</i>; (10) one <i>battery voltmeter</i>; (11) + one <i>blocking condenser</i>; (12) one <i>power circuit choke coil</i>, + and (13) one <i>motor-generator</i>. + </p> + <p> + <i>The Oscillation Transformer</i>.--The tuning coil, or <i>oscillation + transformer</i> as this one is called, is a conductively coupled + tuner--that is, the primary and secondary coils form one continuous coil + instead of two separate coils. This tuner is made up of 25 turns of thin + copper strip, 3/8 inch wide and with its edges rounded, and this is + secured to a wood base as shown at <i>A</i> in <i>Fig. 77</i>. It is + fitted with one fixed tap and three clips to each of which a length of + copper braid is attached. It has a diameter of 6-1/4 inches, a height of + 7-7/8 inches and a length of 9-3/8 inches, and it costs $11.00. + </p> + <p> + <a name="fig077" id="fig077"><img width="548" height="800" + src="images/fig077.jpg" + alt="Fig. 77.--Apparatus of 100 Mile C. W. Telegraph Transmitter." /></a> + </p> + <p> + <i>The Aerial Condenser</i>.--This condenser is made up of three fixed + condensers of different capacitances, namely .0003, .0004 and .0005 mfd., + and these are made to stand a potential of 7500 volts. The condenser is + therefore adjustable and, as you will see from the picture <i>B</i>, it + has one terminal wire at one end and three terminal wires at the other end + so that one, two or three condensers can be used in series with the + aerial. A condenser of this kind costs $5.40. + </p> + <p> + <i>The Aerial Ammeter</i>.--This is the same kind of a hot-wire ammeter + already described in connection with the experimental set, but it reads to + 5 amperes. + </p> + <p> + <i>The Grid and Blocking Condensers</i>.--Each of these is a fixed + condenser of .002 mfd. capacitance and is rated to stand 3,000 volts. It + is made like the aerial condenser but has only two terminals. It costs + $2.00. + </p> + <p> + <i>The Key Circuit Apparatus</i>.--This consists of: (1) the <i>grid leak</i>; + (2) the <i>chopper</i>; (3) the <i>choke coil</i>, and (4) the <i>key</i>. + The grid leak is connected in the lead from the grid to the aerial to keep + the voltage on the grid at the right potential. It has a resistance of + 5000 ohms with a mid-tap at 2500 ohms as shown at <i>C</i>. It costs + $2.00. + </p> + <p> + The chopper is simply a rotary interrupter driven by a small motor. It + comprises a wheel of insulating material in which 30 or more metal + segments are set in an insulating disk as shown at <i>D</i>. A metal + contact called a brush is fixed on either side of the wheel. It costs + about $7.00 and the motor to drive it is extra. The choke coil is wound up + of about 250 turns of No. 30 Brown and Sharpe gauge cotton covered magnet + wire on a spool which has a diameter of 2 inches and a length of 3-1/4 + inches. + </p> + <p> + <i>The 5 Watt Oscillator Vacuum Tube</i>.--This tube is made like the + amplifier tube described for use with the preceding experimental + transmitter, but it is larger, has a more perfect vacuum, and will stand a + plate potential of 350 volts while the plate current is .045 ampere. The + filament takes a current of a little more than 2 amperes at 7.5 volts. A + standard 4-tap base is used with it. The tube costs $8.00 and the + porcelain base is $1.00 extra. It is shown at <i>E</i>. + </p> + <p> + <i>The Storage Battery and Rheostat</i>.--This must be a 5-cell battery so + that it will develop 10 volts. A storage battery of any capacity can be + used but the lowest priced one costs about $22.00. The rheostat for + regulating the battery current is the same as that used in the preceding + experimental transmitter. + </p> + <p> + <i>The Filament Voltmeter</i>.--To get the best results it is necessary + that the voltage of the current which heats the filament be kept at the + same value all of the time. For this transmitter a direct current + voltmeter reading from 0 to 15 volts is used. It is shown at <i>F</i> and + costs $7.50. + </p> + <p> + <i>The Oscillation Choke Coil</i>.--This is made exactly like the one + described in connection with the experimental transmitter. + </p> + <p> + <i>The Motor-Generator Set</i>.--Where you have only a 110 or a 220 volt + direct current available as a source of power you need a <i>motor-generator</i> + to change it to 350 volts, and this is an expensive piece of apparatus. It + consists of a single armature core with a motor winding and a generator + winding on it and each of these has its own commutator. Where the low + voltage current flows into one of the windings it drives its as a motor + and this in turn generates the higher voltage current in the other + winding. Get a 100 watt 350 volt motor-generator; it is shown at <i>F</i> + and costs about $75.00. + </p> + <p> + <i>The Panel Cut-Out</i>.--This switch and fuse block is the same as that + used in the experimental set. + </p> + <p> + <i>The Protective Condenser</i>.--This is a fixed condenser having a + capacitance of 1 mfd. and will stand 750 volts. It costs $2.00. + </p> + <p> + <i>Connecting Up the Transmitting Apparatus</i>.--From all that has gone + before you have seen that each piece of apparatus is fitted with terminal, + wires, taps or binding posts. To connect up the parts of this transmitter + it is only necessary to make the connections as shown in the wiring + diagram <i>Fig. 78</i>. + </p> + <p> + <a name="fig078" id="fig078"><img width="600" height="458" + src="images/fig078.jpg" + alt="Fig. 78.--5 to 50 Watt C. W. Telegraph Transmitter. (With Single Oscillation Tube.)" /> + </a> + </p> + <p> + <i>A 200 Mile C. W. Telegraph Transmitter</i>.--To make a continuous wave + telegraph transmitter that will cover distances up to 200 miles all you + have to do is to use two 5 watt vacuum tubes in <i>parallel</i>, all of + the rest of the apparatus being exactly the same. Connecting the + oscillator tubes up in parallel means that the two filaments are connected + across the leads of the storage battery, the two grids on the same lead + that goes to the aerial and the two plates on the same lead that goes to + the positive pole of the generator. Where two or more oscillator tubes are + used only one storage battery is needed, but each filament must have its + own rheostat. The wiring diagram <i>Fig. 79</i> shows how the two tubes + are connected up in parallel. + </p> + <p> + <a name="fig079" id="fig079"><img width="600" height="367" + src="images/fig079.jpg" + alt="Fig. 79.--200 Mile C.W. Telegraph Transmitter (With Two Tubes in Parallel.)" /> + </a> + </p> + <p> + <i>A 500 Mile C. W. Telegraph Transmitter</i>.--For sending to distances + of over 200 miles and up to 500 miles you can use either: (1) three or + four 5 watt oscillator tubes in parallel as described above, or (2) one 50 + watt oscillator tube. Much of the apparatus for a 50 watt tube set is + exactly the same as that used for the 5 watt sets. Some of the parts, + however, must be proportionately larger though the design all the way + through remains the same. + </p> + <p> + <i>The Apparatus and Connections</i>.--The aerial series condenser, the + blocking condenser, the grid condenser, the telegraph key, the chopper, + the choke coil in the key circuit, the filament voltmeter and the + protective condenser in the power circuit are identical with those + described for the 5 watt transmitting set. + </p> + <p> + <i>The 50 Watt Vacuum Tube Oscillator</i>.--This is the size of tube + generally used by amateurs for long distance continuous wave telegraphy. A + single tube will develop 2 to 3 amperes in your aerial. The filament takes + a 10 volt current and a plate potential of 1,000 volts is needed. One of + these tubes is shown in <i>Fig. 80</i> and the cost is $30.00. A tube + socket to fit it costs $2.50 extra. + </p> + <p> + <a name="fig080" id="fig080"><img width="560" height="235" + src="images/fig080.jpg" alt="Fig. 80.--50 Watt Oscillator Vacuum Tube." /></a> + </p> + <p> + <i>The Aerial Ammeter</i>.--This should read to 5 amperes and the cost is + $6.25. + </p> + <p> + <i>The Grid Leak Resistance</i>.--It has the same resistance, namely 5,000 + ohms as the one used with the 5 watt tube transmitter, but it is a little + larger. It is listed at $1.65. + </p> + <p> + <i>The Oscillation Choke Coil</i>.--The choke coil in the power circuit is + made of about 260 turns of No. 30 B. & S. cotton covered magnet wire + wound on a spool 2-1/4 inches in diameter and 3-1/4 inches long. + </p> + <p> + <i>The Filament Rheostat</i>.--This is made to take care of a 10 volt + current and it costs $10.00. + </p> + <p> + <i>The Filament Storage Battery</i>.--This must develop 12 volts and one + having an output of 40 ampere-hours costs about $25.00. + </p> + <p> + <i>The Protective Condenser</i>.--This condenser has a capacitance of 1 + mfd. and costs $2.00. + </p> + <p> + <i>The Motor-Generator</i>.--Where you use one 50 watt oscillator tube you + will need a motor-generator that develops a plate potential of 1000 volts + and has an output of 200 watts. This machine will stand you about $100.00. + </p> + <p> + The different pieces of apparatus for this set are connected up exactly + the same as shown in the wiring diagram in <i>Fig. 78</i>. + </p> + <p> + <i>A 1000 Mile C. W. Telegraph Transmitter</i>.--All of the parts of this + transmitting set are the same as for the 500 mile transmitter just + described except the motor generator and while this develops the same + plate potential, <i>i.e.</i>, 1,000 volts, it must have an output of 500 + watts; it will cost you in the neighborhood of $175.00. For this long + distance transmitter you use two 50 watt oscillator tubes in parallel and + all of the parts are connected together exactly the same as for the 200 + mile transmitter shown in the wiring diagram in <i>Fig. 79</i>. + </p> + <h2> + <a name="chap17" id="chap17">CHAPTER XVII</a> + </h2> + <h3> + CONTINUOUS WAVE TELEGRAPH TRANSMITTING SETS WITH ALTERNATING CURRENT + </h3> + <p> + Within the last few years alternating current has largely taken the place + of direct current for light, heat and power purposes in and around towns + and cities and if you have alternating current service in your home you + can install a long distance continuous wave telegraph transmitter with + very little trouble and at a comparatively small expense. + </p> + <p> + <i>A 100 Mile C. W. Telegraph Transmitting Set</i>.--The principal pieces + of apparatus for this transmitter are the same as those used for the <i>100 + Mile Continuous Wave Telegraph Transmitting Set</i> described and pictured + in the preceding chapter which used direct current, except that an <i>alternating + current power transformer</i> is employed instead of the more costly <i>motor-generator</i>. + </p> + <p> + <i>The Apparatus Required</i>.--The various pieces of apparatus you will + need for this transmitting set are: (1) one <i>hot-wire ammeter</i> for + the aerial as shown at <i>E</i> in <i>Fig. 75</i>, but which reads to 5 + amperes instead of to 2.5 amperes; (2) one <i>tuning coil</i> as shown at + <i>A</i> in <i>Fig. 77</i>; (3) one aerial condenser as shown at <i>B</i> + in <i>Fig. 77</i>; (4) one <i>grid leak</i> as shown at <i>C</i> in <i>Fig. + 77</i>; (5) one <i>telegraph key</i> as shown at <i>G</i> in <i>Fig. 75</i>; + (6) one <i>grid condenser</i>, made like the aerial condenser but having + only two terminals; (7) one <i>5 watt oscillator tube</i> as shown at <i>E</i> + in <i>Fig. 77</i>; (8) one <i>.002 mfd. 3,000 volt by-pass condenser</i>, + made like the aerial and grid condensers; (9) one pair of <i>choke coils</i> + for the high voltage secondary circuit; (10) one <i>milli-ammeter</i>; + (11) one A. C. <i>power transformer</i>; (12) one <i>rheostat</i> as shown + at <i>I</i> in <i>Fig. 75</i>, and (13) one <i>panel cut-out</i> as shown + at <i>K</i> in <i>Fig. 75</i>. + </p> + <p> + <i>The Choke Coils</i>.--Each of these is made by winding about 100 turns + of No. 28, Brown and Sharpe gauge, cotton covered magnet wire on a spool 2 + inches in diameter and 2-1/2 inches long, when it will have an inductance + of about 0.5 <i>millihenry</i> [Footnote: A millihenry is 1/1000th part of + a henry.] at 1,000 cycles. + </p> + <p> + <i>The Milli-ammeter</i>.--This is an alternating current ammeter and + reads from 0 to 250 <i>milli</i>amperes; [Footnote: A <i>milliampere</i> + is the 1/1000th part of an ampere.] and is used for measuring the + secondary current that energizes the plate of the oscillator tube. It + looks like the aerial ammeter and costs about $7.50. + </p> + <p> + <i>The A. C. Power Transformer</i>.--Differing from the motor generator + set the power transformer has no moving parts. For this transmitting set + you need a transformer that has an input of 325 volts. It is made to work + on a 50 to 60 cycle current at 102.5 to 115 volts, which is the range of + voltage of the ordinary alternating lighting current. This adjustment for + voltage is made by means of taps brought out from the primary coil to a + rotary switch. + </p> + <p> + The high voltage secondary coil which energizes the plate has an output of + 175 watts and develops a potential of from 350 to 1,100 volts. The low + voltage secondary coil which heats the filament has an output of 175 watts + and develops 7.5 volts. This transformer, which is shown in <i>Fig. 81</i>, + is large enough to take care of from one to four 5 watt oscillator tubes. + It weighs about 15 pounds and sells for $25.00. + </p> + <p> + <a name="fig081" id="fig081"><img width="600" height="661" + src="images/fig081.jpg" + alt="Fig. 81.--Alternation Current Power Transformer. (For C. W. Telegraphy and Wireless Telephony.)" /> + </a> + </p> + <table cellspacing="20" summary="Illustration"> + <tr> + <td align="center"> + <i>Photograph unavailable</i> + </td> + </tr> + <tr> + <td align="center"> + The Transformer and Tuner of the World's Largest Radio Station. Owned + by the Radio Corporation of America at Rocky Point near Port Jefferson + L.I. + </td> + </tr> + </table> + <p> + <i>Connecting Up the Apparatus</i>.--The wiring diagram <i>Fig. 82</i> + shows clearly how all of the connections are made. It will be observed + that a storage battery is not needed as the secondary coil of the + transformer supplies the current to heat the filament of the oscillator. + The filament voltmeter is connected across the filament secondary coil + terminals, while the plate milli-ammeter is connected to the mid-taps of + the plate secondary coil and the filament secondary coil. + </p> + <p> + <a name="fig082" id="fig082"><img width="600" height="337" + src="images/fig082.jpg" + alt="Fig. 82. Wiring Diagram for 200 to 500 Mile C.W. Telegraph Transmitting Set. (With Alternating Current)" /> + </a> + </p> + <p> + <i>A 200 to 500 Mile C. W. Telegraph Transmitting Set</i>.--Distances of + from 200 to 500 miles can be successfully covered with a telegraph + transmitter using two, three or four 5 watt oscillator tubes in parallel. + The apparatus needed is identical with that used for the 100 mile + transmitter just described. The tubes are connected in parallel as shown + in the wiring diagram in <i>Fig. 83</i>. + </p> + <p> + <a name="fig083" id="fig083"><img width="600" height="306" + src="images/fig083.jpg" + alt="Fig. 83.--Wiring Diagram for 500 to 1000 Mile C. W. Telegraph Transmitter." /> + </a> + </p> + <p> + <i>A 500 to 1,000 Mile C. W. Telegraph Transmitting Set</i>.--With the + apparatus described for the above set and a single 50 watt oscillator tube + a distance of upwards of 500 miles can be covered, while with two 50 watt + oscillator tubes in parallel you can cover a distance of 1,000 miles + without difficulty, and nearly 2,000 miles have been covered with this + set. + </p> + <p> + <i>The Apparatus Required</i>.--All of the apparatus for this C. W. + telegraph transmitting set is the same as that described for the 100 and + 200 mile sets but you will need: (1) one or two <i>50 watt oscillator + tubes with sockets;</i> (2) one <i>key</i> <i>condenser</i> that has a + capacitance of 1 mfd., and a rated potential of 1,750 volts; (3) one <i>0 + to 500 milli-ammeter</i>; (4) one <i>aerial ammeter</i> reading to 5 + amperes, and (5) an <i>A. C. power transformer</i> for one or two 50 watt + tubes. + </p> + <table cellspacing="20" summary="Illustration"> + <tr> + <td align="center"> + <i>Photograph unavailable</i> + </td> + </tr> + <tr> + <td align="center"> + Broadcasting Government Reports by Wireless from Washington. This + shows Mr. Gale at work with his set in the Post Office Department. + </td> + </tr> + </table> + <p> + <i>The Alternating Current Power Transformer</i>.--This power transformer + is made exactly like the one described in connection with the preceding + 100 mile transmitter and pictured in <i>Fig. 81</i>, but it is + considerably larger. Like the smaller one, however, it is made to work + with a 50 to 60 cycle current at 102.5 to 115 volts and, hence, can be + used with any A. C. lighting current. + </p> + <p> + It has an input of 750 volts and the high voltage secondary coil which + energizes the plate has an output of 450 watts and develops 1,500 to 3,000 + volts. The low voltage secondary coil which heats the filament develops + 10.5 volts. This transformer will supply current for one or two 50-watt + oscillator tubes and it costs about $40.00. + </p> + <p> + <i>Connecting Up the Apparatus</i>.--Where a single oscillator tube is + used the parts are connected as shown in <i>Fig. 82</i>, and where two + tubes are connected in parallel the various pieces of apparatus are wired + together as shown in <i>Fig. 83</i>. The only difference between the 5 + watt tube transmitter and the 50 watt tube transmitter is in the size of + the apparatus with one exception; where one or two 50 watt tubes are used + a second condenser of large capacitance (1 mfd.) is placed in the grid + circuit and the telegraph key is shunted around it as shown in the diagram + <i>Fig. 83</i>. + </p> + <h2> + <a name="chap18" id="chap18">CHAPTER XVIII</a> + </h2> + <h3> + WIRELESS TELEPHONE TRANSMITTING SETS WITH DIRECT AND ALTERNATING CURRENTS + </h3> + <p> + In time past the most difficult of all electrical apparatus for the + amateur to make, install and work was the wireless telephone. This was + because it required a <i>direct current</i> of not less than 500 volts to + set up the sustained oscillations and all ordinary direct current for + lighting purposes is usually generated at a potential of 110 volts. + </p> + <p> + Now as you know it is easy to <i>step-up</i> a 110 volt alternating + current to any voltage you wish with a power transformer but until within + comparatively recent years an alternating current could not be used for + the production of sustained oscillations for the very good reason that the + state of the art had not advanced that far. In the new order of things + these difficulties have all but vanished and while a wireless telephone + transmitter still requires a high voltage direct current to operate it + this is easily obtained from 110 volt source of alternating current by + means of <i>vacuum tube rectifiers</i>. + </p> + <p> + The pulsating direct currents are then passed through a filtering + reactance coil, called a <i>reactor</i>, and one or more condensers, and + these smooth them out until they approximate a continuous direct current. + The latter is then made to flow through a vacuum tube oscillator when it + is converted into high frequency oscillations and these are <i>varied</i>, + or <i>modulated</i>, as it is called, by a <i>microphone transmitter</i> + such as is used for ordinary wire telephony. The energy of these sustained + modulated oscillations is then radiated into space from the aerial in the + form of electric waves. + </p> + <p> + The distance that can be covered with a wireless telephone transmitter is + about one-fourth as great as that of a wireless telegraph transmitter + having the same input of initial current, but it is long enough to satisfy + the most enthusiastic amateur. For instance with a wireless telephone + transmitter where an amplifier tube is used to set up the oscillations and + which is made for a plate potential of 100 volts, distances up to 10 or 15 + miles can be covered. + </p> + <p> + With a single 5 watt oscillator tube energized by a direct current of 350 + volts from either a motor-generator or from a power transformer (after it + has been rectified and smoothed out) speech and music can be transmitted + to upwards of 25 miles. Where two 5 watt tubes connected in parallel are + used wireless telephone messages can be transmitted to distances of 40 or + 50 miles. Further, a single 50 watt oscillator tube will send to distances + of 50 to 100 miles while two of these tubes in parallel will send from 100 + to 200 miles. Finally, where four or five oscillator tubes are connected + in parallel proportionately greater distances can be covered. + </p> + <p> + <i>A Short Distance Wireless Telephone Transmitting Set-With 110 Volt + Direct Lighting Current</i>.--For this very simple, short distance + wireless telephone transmitting set you need the same apparatus as that + described and pictured in the beginning of <a href="#chap16">Chapter XVI</a> + for a <i>Short Distance C. W. Telegraph Transmitter</i>, except that you + use a <i>microphone transmitter</i> instead of a <i>telegraph key</i>. If + you have a 110 volt direct lighting current in your home you can put up + this short distance set for very little money and it will be well worth + your while to do so. + </p> + <p> + <i>The Apparatus You Need</i>.--For this set you require: (1) one <i>tuning + coil</i> as shown at <i>A</i> and <i>B</i> in <i>Fig. 75</i>; (2) one <i>aerial + ammeter</i> as shown at <i>C</i> in <i>Fig. 75</i>; (3) one <i>aerial + condenser</i> as shown at <i>C</i> in <i>Fig. 75</i>; (4) one <i>grid, + blocking and protective condenser</i> as shown at <i>D</i> in <i>Fig. 75</i>; + (5) one <i>grid leak</i> as shown at <i>C</i> in <i>Fig. 77</i>; (6) one + <i>vacuum tube amplifier</i> which is used as an <i>oscillator</i>; (7) + one <i>6 volt storage battery</i>; (8) one <i>rheostat</i> as shown at <i>I</i> + in <i>Fig. 75</i>; (9) one <i>oscillation choke coil</i>; (10) one <i>panel + cut-out</i> as shown at <i>K</i> in <i>Fig. 75</i> and an ordinary <i>microphone + transmitter</i>. + </p> + <p> + The <i>Microphone Transmitter</i>.--The best kind of a microphone to use + with this and other telephone transmitting sets is a <i>Western Electric + No. 284-W</i>. [Footnote: Made by the Western Electric Company, Chicago, + Ill.] This is known as a solid back transmitter and is the standard + commercial type used on all long distance Bell telephone lines. It + articulates sharply and distinctly and there are no current variations to + distort the wave form of the voice and it will not buzz or sizzle. It is + shown in <i>Fig. 84</i> and costs $2.00. Any other good microphone + transmitter can be used if desired. + </p> + <p> + <a name="fig084" id="fig084"><img width="600" height="365" + src="images/fig084.jpg" alt="Fig. 84.--Standard Microphone Transmitter." /></a> + </p> + <p> + <i>Connecting Up the Apparatus</i>.--Begin by connecting the leading-in + wire with one of the terminals of the microphone transmitter, as shown in + the wiring diagram <i>Fig. 85</i>, and the other terminal of this to one + end of the tuning coil. Now connect <i>clip 1</i> of the tuning coil to + one of the posts of the hot-wire ammeter, the other post of this to one + end of aerial condenser and, finally, the other end of the latter with the + water pipe or other ground. The microphone can be connected in the ground + wire and the ammeter in the aerial wire and the results will be + practically the same. + </p> + <p> + <a name="fig085" id="fig085"><img width="600" height="526" + src="images/fig085.jpg" + alt="Fig. 85.--Wiring Diagram of Short Distance Wireless Telephone Set. (Microphone in Aerial Wire.)" /> + </a> + </p> + <p> + Next connect one end of the grid condenser to the post of the tuning coil + that makes connection with the microphone and the other end to the grid of + the tube, and then shunt the grid leak around the condenser. Connect the + + or <i>positive</i> electrode of the storage battery with one terminal of + the filament of the vacuum tube, the other terminal of the filament with + one post of the rheostat and the other post of this with the - or <i>negative</i> + electrode of the battery. This done, connect <i>clip 2</i> of the tuning + coil to the + or <i>positive</i> electrode of the battery and bring a lead + from it to one of the switch taps of the panel cut-out. + </p> + <p> + Now connect <i>clip 3</i> of the tuning coil with one end of the blocking + condenser, the other end of this with one terminal of the choke coil and + the other terminal of the latter with the other switch tap of the cut-out. + Connect the protective condenser across the direct current feed wires + between the panel cut-out and the choke coil. Finally connect the ends of + a lamp cord to the fuse socket taps of the cut-out, and connect the other + ends to a lamp plug and screw it into the lamp socket of the feed wires. + Screw in a pair of 5 ampere <i>fuse plugs</i>, close the switch and you + are ready to tune the transmitter and talk to your friends. + </p> + <p> + <i>A 25 to 50 Mile Wireless Telephone Transmitter--With Direct Current + Motor Generator</i>.--Where you have to start with 110 or 220 volt direct + current and you want to transmit to a distance of 25 miles or more you + will have to install a <i>motor-generator</i>. To make this transmitter + you will need exactly the same apparatus as that described and pictured + for the <i>100 Mile C. W. Telegraph Transmitting Set</i> in <a + href="#chap16">Chapter XVI</a>, except that you must substitute a <i>microphone + transmitter</i> and a <i>telephone induction coil</i>, or a <i>microphone + transformer</i>, or still better, a <i>magnetic modulator</i>, for the + telegraph key and chopper. + </p> + <p> + <i>The Apparatus You Need</i>.--To reiterate; the pieces of apparatus you + need are: (1) one <i>aerial ammeter</i> as shown at <i>E</i> in <i>Fig. 75</i>; + (2) one <i>tuning coil</i> as shown at <i>A</i> in <i>Fig. 77</i>; (3) one + <i>aerial condenser</i> as shown at <i>B</i> in <i>Fig. 77</i>; (4) one <i>grid + leak</i> as shown at <i>C</i> in <i>Fig. 77</i>; (5) one <i>grid, blocking</i> + and <i>protective condenser</i>; (6) one <i>5 watt oscillator tube</i> as + shown at <i>E</i> in <i>Fig. 77</i>; (7) one <i>rheostat</i> as shown at + <i>I</i> in <i>Fig. 75</i>; (8) one <i>10 volt (5 cell) storage battery</i>; + (9) one <i>choke coil</i>; (10) one <i>panel cut-out</i> as shown at <i>K</i> + in <i>Fig. 75</i>, and (11) a <i>motor-generator</i> having an input of + 110 or 220 volts and an output of 350 volts. + </p> + <p> + In addition to the above apparatus you will need: (12) a <i>microphone + transmitter</i> as shown in <i>Fig. 84</i>; (13) a battery of four dry + cells or a 6 volt storage battery, and either (14) a <i>telephone + induction coil</i> as shown in <i>Fig. 86</i>; (15) a <i>microphone + transformer</i> as shown in <i>Fig. 87</i>; or a <i>magnetic modulator</i> + as shown in <i>Fig. 88</i>. All of these parts have been described, as + said above, in <a href="#chap16">Chapter XVI</a>, except the microphone + modulators. + </p> + <p> + <a name="fig086" id="fig086"><img width="600" height="508" + src="images/fig086.jpg" + alt="Fig. 86.--Telephone Induction Coil. (Used with Microphone Transmitter.)" /> + </a> <a name="fig087" id="fig087"><img width="600" height="712" + src="images/fig087.jpg" + alt="Fig. 87.--Microphone Transformer. (Used with Microphone Transmitter.)" /> + </a> <a name="fig088" id="fig088"><img width="600" height="692" + src="images/fig088.jpg" + alt="Fig. 88.--Magnetic Modulator. (Used with Microphone Transmitter.)" /> + </a> + </p> + <p> + <i>The Telephone Induction Coil</i>.--This is a little induction coil that + transforms the 6-volt battery current after it has flowed through and been + modulated by the microphone transmitter into alternating currents that + have a potential of 1,000 volts of more. It consists of a primary coil of + <i>No. 20 B. and S.</i> gauge cotton covered magnet wire wound on a core + of soft iron wires while around the primary coil is wound a secondary coil + of <i>No. 30</i> magnet wire. Get a <i>standard telephone induction coil</i> + that has a resistance of 500 or 750 ohms and this will cost you a couple + of dollars. + </p> + <p> + <i>The Microphone Transformer</i>.--This device is built on exactly the + same principle as the telephone induction coil just described but it is + more effective because it is designed especially for modulating the + oscillations set up by vacuum tube transmitters. As with the telephone + induction coil, the microphone transmitter is connected in series with the + primary coil and a 6 volt dry or storage battery. + </p> + <p> + In the better makes of microphone transformer, there is a third winding, + called a <i>side tone</i> coil, to which a headphone can be connected so + that the operator who is speaking into the microphone can listen-in and so + learn if his transmitter is working up to standard. + </p> + <p> + <i>The Magnetic Modulator</i>.--This is a small closed iron core + transformer of peculiar design and having a primary and a secondary coil + wound on it. This device is used to control the variations of the + oscillating currents that are set up by the oscillator tube. It is made in + three sizes and for the transmitter here described you want the smallest + size, which has an output of 1/2 to 1-1/2 amperes. It costs about $10.00. + </p> + <p> + <i>How the Apparatus Is Connected Up</i>.--The different pieces of + apparatus are connected together in exactly the same way as the <i>100 + Mile C. W. Telegraph Set</i> in <a href="#chap16">Chapter XVI</a> except + that the microphone transmitter and microphone modulator (whichever kind + you use) is substituted for the telegraph key and chopper. + </p> + <p> + Now there are three different ways that the microphone and its modulator + can be connected in circuit. Two of the best ways are shown at <i>A</i> + and <i>B</i> in <i>Fig. 89</i>. In the first way the secondary terminals + of the modulator are shunted around the grid leak in the grid circuit as + at <i>A</i>, and in the second the secondary terminals are connected in + the aerial as at <i>B</i>. Where an induction coil or a microphone + transformer is used they are shunted around a condenser, but this is not + necessary with the magnetic modulator. Where a second tube is used as in + <i>Fig. 90</i> then the microphone and its modulator are connected with + the grid circuit and <i>clip 3</i> of the tuning coil. + </p> + <p> + <a name="fig089a" id="fig089a"><img width="600" height="432" + src="images/fig089a.jpg" + alt="Fig. 89.--Wiring Diagram of 25 to 50 Mile Wireless Telephone. (Microphone Modulator Shunted Around Grid-Leak Condenser.)" /> + </a> <a name="fig089b" id="fig089b"><img width="560" height="705" + src="images/fig089b.jpg" + alt="(B) Fig. 89.--Microphone Modulator Connected in Aerial Wire." /> </a> + <a name="fig090" id="fig090"><img width="600" height="379" + src="images/fig090.jpg" + alt="Fig. 90.--Wiring Diagram of 50 to 100 Mile Wireless Telephone Transmitting Set." /> + </a> + </p> + <p> + <i>A 50 to 100 Mile Wireless Telephone Transmitter--With Direct Current + Motor Generator</i>.--As the initial source of current available is taken + to be a 110 or 220 volt direct current a motor-generator having an output + of 350 volts must be used as before. The only difference between this + transmitter and the preceding one is that: (1) two 5 watt tubes are used, + the first serving as an <i>oscillator</i> and the second as a <i>modulator</i>; + (2) an <i>oscillation choke coil</i> is used in the plate circuit; (3) a + <i>reactance coil</i> or <i>reactor</i>, is used in the plate circuit; and + (4) a <i>reactor</i> is used in the grid circuit. + </p> + <p> + <i>The Oscillation Choke Coil</i>.--You can make this choke coil by + winding about 275 turns of <i>No. 28 B. and S. gauge</i> cotton covered + magnet wire on a spool 2 inches in diameter and 4 inches long. Give it a + good coat of shellac varnish and let it dry thoroughly. + </p> + <p> + <i>The Plate and Grid Circuit Reactance Coils</i>.--Where a single tube is + used as an oscillator and a second tube is employed as a modulator, a <i>reactor</i>, + which is a coil of wire wound on an iron core, is used in the plate + circuit to keep the high voltage direct current of the motor-generator the + same at all times. Likewise the grid circuit reactor is used to keep the + voltage of the grid at a constant value. These reactors are made alike and + a picture of one of them is shown in <i>Fig. 91</i> and each one will cost + you $5.75. + </p> + <p> + <a name="fig091" id="fig091"><img width="511" height="680" + src="images/fig091.jpg" alt="Fig. 91.--Plate and Grid Circuit Reactor." /></a> + </p> + <p> + <i>Connecting up the Apparatus</i>.--All of the different pieces of + apparatus are connected up as shown in <i>Fig. 89</i>. One of the ends of + the secondary of the induction coil, or the microphone transformer, or the + magnetic modulator is connected to the grid circuit and the other end to + <i>clip 3</i> of the tuning coil. + </p> + <p> + <i>A 100 to 200 Mile Wireless Telephone Transmitter--With Direct Current + Motor Generator</i>.--By using the same connections shown in the wiring + diagrams in <i>Fig. 89</i> and a single 50 watt oscillator tube your + transmitter will then have a range of 100 miles or so, while if you + connect up the apparatus as shown in <i>Fig. 90</i> and use two 50 watt + tubes you can work up to 200 miles. Much of the apparatus for a 50 watt + oscillator set where either one or two tubes are used is of the same size + and design as that just described for the 5 watt oscillator sets, but, as + in the C. W. telegraph sets, some of the parts must be proportionately + larger. The required parts are (1) the <i>50 watt tube</i>; (2) the <i>grid + leak resistance</i>; (3) the <i>filament rheostat</i>; (4) the <i>filament + storage battery</i>; and (5) the <i>magnetic modulator</i>. All of these + parts, except the latter, are described in detail under the heading of a + <i>500 Mile C. W. Telegraph Transmitting Set</i> in <a href="#chap16">Chapter + XVI</a>, and are also pictured in that chapter. + </p> + <p> + It is not advisable to use an induction coil for the modulator for this + set, but use, instead, either a telephone transformer, or better, a + magnetic modulator of the second size which has an output of from 1-1/2 to + 3-1/2 amperes. The magnetic modulator is described and pictured in this + chapter. + </p> + <p> + <i>A 50 to 100 Mile Wireless Telephone Transmitting Set--With 110 Volt + Alternating Current</i>.--If you have a 110 volt [Footnote: Alternating + current for lighting purposes ranges from 102.5 volts to 115 volts, so we + take the median and call it 110 volts.] alternating current available you + can use it for the initial source of energy for your wireless telephone + transmitter. The chief difference between a wireless telephone + transmitting set that uses an alternating current and one that uses a + direct current is that: (1) a <i>power transformer</i> is used for + stepping up the voltage instead of a motor-generator, and (2) a <i>vacuum + tube rectifier</i> must be used to convert the alternating current into + direct current. + </p> + <p> + <i>The Apparatus You Need</i>.--For this telephone transmitting set you + need: (1) one <i>aerial ammeter</i>; (2) one <i>tuning coil</i>; (3) one + <i>telephone modulator</i>; (4) one <i>aerial series condenser</i>; (5) + one <i>4 cell dry battery</i> or a 6 volt storage battery; (6) one <i>microphone + transmitter</i>; (7) one <i>battery switch</i>; (8) one <i>grid condenser</i>; + (9) one <i>grid leak</i>; (10) two <i>5 watt oscillator tubes with sockets</i>; + (11) one <i>blocking condenser</i>; (12) one <i>oscillation choke coil</i>; + (13) two <i>filter condensers</i>; (14) one <i>filter reactance coil</i>; + (15) an <i>alternating current power transformer</i>, and (16) two <i>20 + watt rectifier vacuum tubes</i>. + </p> + <p> + All of the above pieces of apparatus are the same as those described for + the <i>100 Mile C. W. Telegraph Transmitter in Chapter XVII</i>, except: + (a) the <i>microphone modulator</i>; (b) the <i>microphone transmitter</i> + and (c) the <i>dry</i> or <i>storage battery</i>, all of which are + described in this chapter; and the new parts which are: (d) the <i>rectifier + vacuum tubes</i>; (e) the <i>filter condensers</i>; and (f) the <i>filter + reactance coil</i>; further and finally, the power transformer has a <i>third</i> + secondary coil on it and it is this that feeds the alternating current to + the rectifier tubes, which in turn converts it into a pulsating direct + current. + </p> + <p> + <i>The Vacuum Tube Rectifier</i>.--This rectifier has two electrodes, that + is, it has a filament and a plate like the original vacuum tube detector, + The smallest size rectifier tube requires a plate potential of 550 volts + which is developed by one of the secondary coils of the power transformer. + The filament terminal takes a current of 7.5 volts and this is supplied by + another secondary coil of the transformer. This rectifier tube delivers a + direct current of 20 watts at 350 volts. It looks exactly like the 5 watt + oscillator tube which is pictured at <i>E</i> in <i>Fig. 77</i>. The price + is $7.50. + </p> + <p> + <i>The Filter Condensers</i>.--These condensers are used in connection + with the reactance coil to smooth out the pulsating direct current after + it has passed through the rectifier tube. They have a capacitance of 1 + mfd. and will stand 750 volts. These condensers cost about $2.00 each. + </p> + <p> + <i>The Filter Reactance Coil</i>.--This reactor which is shown in <i>Fig. + 92</i>, has about the same appearance as the power transformer but it is + somewhat smaller. It consists of a coil of wire wound on a soft iron core + and has a large inductance, hence the capacitance of the filter condensers + are proportionately smaller than where a small inductance is used which + has been the general practice. The size you require for this set has an + output of 160 milliamperes and it will supply current for one to four 5 + watt oscillator tubes. This size of reactor costs $11.50. + </p> + <p> + <a name="fig092" id="fig092"><img width="560" height="714" + src="images/fig092.jpg" + alt="Fig. 92.--Filter Reactor for Smoothing out Rectified Currents." /></a> + </p> + <p> + <i>Connecting Up the Apparatus</i>.--The wiring diagram in <i>Fig. 93</i> + shows how the various pieces of apparatus for this telephone transmitter + are connected up. You will observe: (1) that the terminals of the power + transformer secondary coil which develops 10 volts are connected to the + filaments of the oscillator tubes; (2) that the terminals of the other + secondary coil which develops 10 volts are connected with the filaments of + the rectifier tubes; (3) that the terminals of the third secondary coil + which develops 550 volts are connected with the plates of the rectifier + tubes; (4) that the pair of filter condensers are connected in parallel + and these are connected to the mid-taps of the two filament secondary + coils; (5) that the reactance coil and the third filter condenser are + connected together in series and these are shunted across the filter + condensers, which are in parallel; and, finally, (6) a lead connects the + mid-tap of the 550-volt secondary coil of the power transformer with the + connection between the reactor and the third filter condenser. + </p> + <p> + <a name="fig093" id="fig093"><img width="600" height="330" + src="images/fig093.jpg" + alt="Fig 93.--100 to 200 Mile Wireless Telephone Transmitter." /></a> + </p> + <p> + <i>A 100 to 200 Mile Wireless Telephone Transmitting Set--With 110 Volt + Alternating Current</i>.--This telephone transmitter is built up of + exactly the same pieces of apparatus and connected up in precisely the + same way as the one just described and shown in <i>Fig. 93</i>. + </p> + <p> + <i>Apparatus Required</i>.--The only differences between this and the + preceding transmitter are: (1) the <i>magnetic modulator</i>, if you use + one, should have an output of 3-1/2 to 5 amperes; (2) you will need two <i>50 + watt oscillator tubes with sockets</i>; (3) two <i>150 watt rectifier + tubes with sockets</i>; (4) an <i>aerial ammeter</i> that reads to <i>5 + amperes</i>; (5) three <i>1 mfd. filter condensers</i> in parallel; (6) <i>two + filter condensers of 1 mfd. capacitance</i> that will stand <i>1750 volts</i>; + and (6) a <i>300 milliampere filter reactor</i>. + </p> + <p> + The apparatus is wired up as shown in <i>Fig. 93</i>. + </p> + <h2> + <a name="chap19" id="chap19">CHAPTER XIX</a> + </h2> + <h3> + THE OPERATION OF VACUUM TUBE TRANSMITTERS + </h3> + <p> + The three foregoing chapters explained in detail the design and + construction of (1) two kinds of C. W. telegraph transmitters, and (2) two + kinds of wireless telephone transmitters, the difference between them + being whether they used (<i>A</i>) a direct current, or (<i>B</i>) an + alternating current as the initial source of energy. Of course there are + other differences between those of like types as, for instance, the + apparatus and connections used (<i>a</i>) in the key circuits, and (<i>b</i>) + in the microphone circuits. But in all of the transmitters described of + whatever type or kind the same fundamental device is used for setting up + sustained oscillations and this is the <i>vacuum tube</i>. + </p> + <p> + <i>The Operation of the Vacuum Tube Oscillator</i>.--The operation of the + vacuum tube in producing sustained oscillations depends on (1) the action + of the tube as a valve in setting up the oscillations in the first place + and (2) the action of the grid in amplifying the oscillations thus set up, + both of which we explained in <a href="#chap14">Chapter XIV</a>. In that + chapter it was also pointed out that a very small change in the grid + potential causes a corresponding and larger change in the amount of + current flowing from the plate to the filament; and that if a vacuum tube + is used for the production of oscillations the initial source of current + must have a high voltage, in fact the higher the plate voltage the more + powerful will be the oscillations. + </p> + <p> + To understand how oscillations are set up by a vacuum tube when a direct + current is applied to it, take a look at the simple circuits shown in <i>Fig. + 94</i>. Now when you close the switch the voltage from the battery charges + the condenser and keeps it charged until you open it again; the instant + you do this the condenser discharges through the circuit which includes it + and the inductance coil, and the discharge of a condenser is always + oscillatory. + </p> + <p> + <a name="fig094ab" id="fig094ab"><img width="600" height="392" + src="images/fig094ab.jpg" + alt="(A) and (B) Fig. 94. Operation of Vacuum Tube Oscillators." /></a> + </p> + <p> + Where an oscillator tube is included in the circuits as shown at <i>A</i> + and <i>B</i> in <i>Fig. 94</i>, the grid takes the place of the switch and + any slight change in the voltage of either the grid or the plate is + sufficient to start a train of oscillations going. As these oscillations + surge through the tube the positive parts of them flow from the plate to + the filament and these carry more of the direct current with them. + </p> + <p> + To make a tube set up powerful oscillations then, it is only necessary + that an oscillation circuit shall be provided which will feed part of the + oscillations set up by the tube back to the grid circuit and when this is + done the oscillations will keep on being amplified until the tube reaches + the limit of its output. + </p> + <p> + <a name="fig094c" id="fig094c"><img width="484" height="240" + src="images/fig094c.jpg" + alt="(C) Fig. 94.--How a Direct Current Sets up Oscillations." /></a> + </p> + <p> + <i>The Operation of C. W. Telegraph Transmitters With Direct + Current--Short Distance C. W. Transmitter</i>.--In the transmitter shown + in the wiring diagram in <i>Fig. 76</i> the positive part of the 110 volt + direct current is carried down from the lamp socket through one side of + the panel cut-out, thence through the choke coil and to the plate of the + oscillator tube, when the latter is charged to the positive sign. The + negative part of the 110 volt direct current then flows down the other + wire to the filament so that there is a difference of potential between + the plate and the filament of 110 volts. Now when the 6-volt battery + current is switched on the filament is heated to brilliancy, and the + electrons thrown off by it form a conducting path between it and the + plate; the 110 volt current then flows from the latter to the former. + </p> + <p> + Now follow the wiring from the plate over to the blocking condenser, + thence to <i>clip 3</i> of the tuning coil, through the turns of the + latter to <i>clip 2</i> and over to the filament and, when the latter is + heated, you have a <i>closed oscillation circuit</i>. The oscillations + surging in the latter set up other and like oscillations in the tuning + coil between the end of which is connected with the grid, the aerial and + the <i>clip 2</i>, and these surge through the circuit formed by this + portion of the coil, the grid condenser and the filament; this is the + amplifying circuit and it corresponds to the regenerative circuit of a + receiving set. + </p> + <p> + When oscillations are set up in it the grid is alternately charged to the + positive and negative signs. These reversals of voltage set up stronger + and ever stronger oscillations in the plate circuit as before explained. + Not only do the oscillations surge in the closed circuits but they run to + and fro on the aerial wire when their energy is radiated in the form of + electric waves. The oscillations are varied by means of the telegraph key + which is placed in the grid circuit as shown in <i>Fig. 76</i>. + </p> + <p> + <i>The Operation of the Key Circuit</i>.--The effect in a C. W. + transmitter when a telegraph key is connected in series with a buzzer and + a battery and these are shunted around the condenser in the grid circuit, + is to rapidly change the wave form of the sustained oscillations, and + hence, the length of the waves that are sent out. While no sound can be + heard in the headphones at the receiving station so long as the points of + the key are not in contact, when they are in contact the oscillations are + modulated and sounds are heard in the headphones that correspond to the + frequency of the buzzer in the key circuit. + </p> + <p> + <i>The Operation of C. W. Telegraph Transmitters with Direct Current</i>.--The + chief differences between the long distance sets which use a direct + current, i.e., those described in <a href="#chap16">Chapter XVI</a>, and + the short distance transmitting sets are that the former use: (1) a + motor-generator set for changing the low voltage direct current into high + voltage direct current, and (2) a chopper in the key circuit. The way the + motor-generator changes the low- into high-voltage current has been + explained in <a href="#chap16">Chapter XVI</a>. + </p> + <p> + The chopper interrupts the oscillations surging through the grid circuit + at a frequency that the ear can hear, that is to say, about 800 to 1,000 + times per second. When the key is open, of course, the sustained + oscillations set up in the circuits will send out continuous waves but + when the key is closed these oscillations are broken up and then they send + out discontinuous waves. If a heterodyne receiving set, see <a + href="#chap15">Chapter XV</a>, is being used at the other end you can + dispense with the chopper and the key circuit needed is very much + simplified. The operation of key circuits of the latter kind will be + described presently. + </p> + <p> + <i>The Operation of C. W. Telegraph Transmitters with Alternating + Current--With a Single Oscillator Tube</i>.--Where an oscillator tube + telegraph transmitter is operated by a 110 volt alternating current as the + initial source of energy, a buzzer, chopper or other interruptor is not + needed in the key circuit. This is because oscillations are set up only + when the plate is energized with the positive part of the alternating + current and this produces an intermittent musical tone in the headphones. + Hence this kind of a sending set is called a <i>tone transmitter</i>. + </p> + <p> + Since oscillations are set up only by the positive part or voltage of an + alternating current it is clear that, as a matter of fact, this kind of a + transmitter does not send out continuous waves and therefore it is not a + C. W. transmitter. This is graphically shown by the curve of the wave form + of the alternating current and the oscillations that are set up by the + positive part of it in <i>Fig. 95</i>. Whenever the positive half of the + alternating current energizes the plate then oscillations are set up by + the tube and, conversely, when the negative half of the current charges + the plate no oscillations are produced. + </p> + <p> + <a name="fig095" id="fig095"><img width="592" height="240" + src="images/fig095.jpg" + alt="Fig. 95.--Positive Voltage only sets up Oscillations." /></a> + </p> + <p> + You will also observe that the oscillations set up by the positive part of + the current are not of constant amplitude but start at zero the instant + the positive part begins to energize the plate and they keep on increasing + in amplitude as the current rises in voltage until the latter reaches its + maximum; then as it gradually drops again to zero the oscillations + decrease proportionately in amplitude with it. + </p> + <p> + <i>Heating the Filament with Alternating Current</i>.--Where an + alternating current power transformer is used to develop the necessary + plate voltage a second secondary coil is generally provided for heating + the filament of the oscillation tube. This is better than a direct current + for it adds to the life of the filament. When you use an alternating + current to heat the filament keep it at the same voltage rather than at + the same amperage (current strength). To do this you need only to use a + voltmeter across the filament terminals instead of an ammeter in series + with it; then regulate the voltage of the filament with a rheostat. + </p> + <p> + <i>The Operation of C. W. Telegraph Transmitters with Alternating + Current--With Two Oscillator Tubes</i>.--By using two oscillator tubes and + connecting them up with the power transformer and oscillating circuits as + shown in the wiring diagram in <i>Fig. 83</i> the plates are positively + energized alternately with every reversal of the current and, + consequently, there is no time period between the ending of the + oscillations set up by one tube and the beginning of the oscillations set + up by the other tube. In other words these oscillations are sustained but + as in the case of those of a single tube, their amplitude rises and falls. + This kind of a set is called a <i>full wave rectification transmitter</i>. + </p> + <p> + The waves radiated by this transmitter can be received by either a crystal + detector or a plain vacuum-tube detector but the heterodyne receptor will + give you better results than either of the foregoing types. + </p> + <p> + <i>The Operation of Wireless Telephone Transmitters with Direct + Current--Short Distance Transmitter</i>.--The operation of this short + distance wireless telephone transmitter, a wiring diagram of which is + shown in <i>Fig. 85</i> is exactly the same as that of the <i>Direct + Current Short Distance C. W. Telegraph Transmitter</i> already explained + in this chapter. The only difference in the operation of these sets is the + substitution of the <i>microphone transmitter</i> for the telegraph key. + </p> + <p> + <i>The Microphone Transmitter</i>.--The microphone transmitter that is + used to vary, or modulate, the sustained oscillations set up by the + oscillator tube and circuits is shown in <i>Fig. 84</i>. By referring to + the diagram at <i>A</i> in this figure you will readily understand how it + operates. When you speak into the mouthpiece the <i>sound waves</i>, which + are waves in the air, impinge upon the diaphragm and these set it into + vibration--that is, they make it move to and fro. + </p> + <p> + When the diaphragm moves toward the back of the transmitter it forces the + carbon granules that are in the cup closer together; this lowers their + resistance and allows more current from the battery to flow through them; + when the pressure of the air waves is removed from the diaphragm it + springs back toward the mouth-piece and the carbon granules loosen up when + the resistance offered by them is increased and less current can flow + through them. Where the oscillation current in the aerial wire is small + the transmitter can be connected directly in series with the latter when + the former will surge through it. As you speak into the microphone + transmitter its resistance is varied and the current strength of the + oscillations is varied accordingly. + </p> + <p> + <i>The Operation of Wireless Telephone Transmitters with Direct + Current--Long Distance Transmitters</i>.--In the wireless telephone + transmitters for long distance work which were shown and described in the + preceding chapter a battery is used to energize the microphone + transmitter, and these two elements are connected in series with a <i>microphone + modulator</i>. This latter device may be either (1) a <i>telephone + induction coil</i>, (2) a <i>microphone transformer</i>, or (3) a <i>magnetic + modulator</i>; the first two of these devices step-up the voltage of the + battery current and the amplified voltage thus developed is impressed on + the oscillations that surge through the closed oscillation circuit or the + aerial wire system according to the place where you connect it. The third + device works on a different principle and this will be described a little + farther along. + </p> + <p> + <i>The Operation of Microphone Modulators--The Induction Coil</i>.--This + device is really a miniature transformer, see <i>A</i> in <i>Fig. 86</i>, + and its purpose is to change the 6 volt direct current that flows through + the microphone into 100 volts alternating current; in turn, this is + impressed on the oscillations that are surging in either (1) the grid + circuit as shown at <i>A</i> in <i>Fig. 89</i>, and in <i>Fig. 90</i>, (2) + the aerial wire system, as shown at <i>B</i> in <i>Fig. 89</i> and <i>Fig. + 93</i>. When the current from the battery flows through the primary coil + it magnetizes the soft iron core and as the microphone varies the strength + of the current the high voltage alternating currents set up in the + secondary coil of the induction coil are likewise varied, when they are + impressed upon and modulate the oscillating currents. + </p> + <p> + <i>The Microphone Transformer</i>.--This is an induction coil that is + designed especially for wireless telephone modulation. The iron core of + this transformer is also of the open magnetic circuit type, see <i>A</i> + in <i>Fig. 87</i>, and the <i>ratio</i> of the turns [Footnote: See + Chapter VI] of the primary and the secondary coil is such that when the + secondary current is impressed upon either the grid circuit or the aerial + wire system it controls the oscillations flowing through it with the + greatest efficiency. + </p> + <p> + <i>The Magnetic Modulator</i>.--This piece of apparatus is also called a + <i>magnetic amplifier</i>. The iron core is formed of very thin plates, or + <i>laminations</i> as they are called, and this permits high-frequency + oscillations to surge in a coil wound on it. In this transformer, see <i>A</i> + in <i>Fig. 88</i>, the current flowing through the microphone varies the + magnetic permeability of the soft iron core by the magnetic saturation of + the latter. Since the microphone current is absolutely distinct from the + oscillating currents surging through the coil of the transformer a very + small direct current flowing through a coil on the latter will vary or + modulate very large oscillating currents surging through the former. It is + shown connected in the aerial wire system at <i>A</i> in <i>Fig. 88</i>, + and in <i>Fig. 93</i>. + </p> + <p> + <i>Operation of the Vacuum Tube as a Modulator</i>.--Where a microphone + modulator of the induction coil or microphone transformer type is + connected in the grid circuit or aerial wire system the modulation is not + very effective, but by using a second tube as a <i>modulator</i>, as shown + in <i>Fig. 90</i>, an efficient degree of modulation can be had. Now there + are two methods by which a vacuum tube can be used as a modulator and + these are: (1) by the <i>absorption</i> of the energy of the current set + up by the oscillator tube, and (2) by <i>varying</i> the direct current + that energizes the plate of the oscillator tube. + </p> + <p> + The first of these two methods is not used because it absorbs the energy + of the oscillating current produced by the tube and it is therefore + wasteful. The second method is an efficient one, as the direct current is + varied before it passes into the oscillator tube. This is sufficient + reason for describing only the second method. The voltage of the grid of + the modulator tube is varied by the secondary coil of the induction coil + or microphone transformer, above described. In this way the modulator tube + acts like a variable resistance but it amplifies the variations impressed + on the oscillations set up by the oscillator tube. As the magnetic + modulator does the same thing a vacuum tube used as a modulator is not + needed where the former is employed. For this reason a magnetic modulator + is the cheapest in the long run. + </p> + <p> + <i>The Operation of Wireless Telephone Transmitters with Alternating + Current</i>.--Where an initial alternating current is used for wireless + telephony, the current must be rectified first and then smoothed out + before passing into the oscillator tube to be converted into oscillations. + Further so that the oscillations will be sustained, two oscillator tubes + must be used, and, finally, in order that the oscillations may not vary in + amplitude the alternating current must be first changed into direct + current by a pair of rectifier vacuum tubes, as shown in <i>Fig. 93.</i> + When this is done the plates will be positively charged alternately with + every reversal of the current in which case there will be no break in the + continuity of the oscillations set up and therefore in the waves that are + sent out. + </p> + <p> + <i>The Operation of Rectifier Vacuum Tubes</i>.--The vacuum tube rectifier + is simply a two electrode vacuum tube. The way in which it changes a + commercial alternating current into pulsating direct current is the same + as that in which a two electrode vacuum tube detector changes an + oscillating current into pulsating direct currents and this has been + explained in detail under the heading of <i>The Operation of a Two + Electrode Vacuum Tube Detector</i> in <a href="#chap12">Chapter XII</a>. + In the <i>C. W. Telegraph Transmitting Sets</i> described in <a + href="#chap17">Chapter XVII</a>, the oscillator tubes act as rectifiers as + well as oscillators but for wireless telephony the alternating current + must be rectified first so that a continuous direct current will result. + </p> + <p> + <i>The Operation of Reactors and Condensers</i>.--A reactor is a single + coil of wire wound on an iron core, see <i>Fig. 90</i> and <i>A</i> in <i>Fig. + 91</i>, and it should preferably have a large inductance. The reactor for + the plate and grid circuit of a wireless telephone transmitter where one + or more tubes are used as modulators as shown in the wiring diagram in <i>Fig. + 90</i>, and the filter reactor shown in <i>Fig. 92</i>, operate in the + same way. + </p> + <p> + When an alternating current flows through a coil of wire the reversals of + the current set up a <i>counter electromotive force</i> in it which + opposes, that is <i>reacts</i>, on the current, and the <i>higher</i> the + frequency of the current the <i>greater</i> will be the <i>reactance</i>. + When the positive half of an alternating current is made to flow through a + large resistance the current is smoothed out but at the same time a large + amount of its energy is used up in producing heat. + </p> + <p> + But when the positive half of an alternating current is made to flow + through a large inductance it acts like a large resistance as before and + likewise smooths out the current, but none of its energy is wasted in heat + and so a coil having a large inductance, which is called an <i>inductive + reactance</i>, or just <i>reactor</i> for short, is used to smooth out, or + filter, the alternating current after it has been changed into a pulsating + direct current by the rectifier tubes. + </p> + <p> + A condenser also has a reactance effect on an alternating current but + different from an induction coil the <i>lower</i> the frequency the <i>greater</i> + will be the reactance. For this reason both a filter reactor and <i>filter + condensers</i> are used to smooth out the pulsating direct currents. + </p> + <h2> + <a name="chap20" id="chap20">CHAPTER XX</a> + </h2> + <h3> + HOW TO MAKE A RECEIVING SET FOR $5.00 OR LESS + </h3> + <p> + In the chapters on <i>Receptors</i> you have been told how to build up + high-grade sets. But there are thousands of boys, and, probably, not a few + men, who cannot afford to invest $25.00, more or less, in a receiving set + and would like to experiment in a small way. + </p> + <p> + The following set is inexpensive, and with this cheap, little portable + receptor you can get the Morse code from stations a hundred miles distant + and messages and music from broadcasting stations if you do not live too + far away from them. All you need for this set are: (1) a <i>crystal + detector</i>, (2) a <i>tuning coil</i> and (3) an <i>earphone</i>. You can + make a crystal detector out of a couple of binding posts, a bit of galena + and a piece of brass wire, or, better, you can buy one all ready to use + for 50 cents. + </p> + <table cellspacing="20" summary="Illustration"> + <tr> + <td align="center"> + <i>Photograph unavailable</i> + </td> + </tr> + <tr> + <td align="center"> + Wireless Receptor, the size of a Safety Match Box. A Youthful Genius + in the person of Kenneth R. Hinman, Who is only twelve years old, has + made a Wireless Receiving Set that fits neatly into a Safety Match + Box. With this Instrument and a Pair of Ordinary Receivers, He is able + to catch not only Code Messages but the regular Broadcasting Programs + from Stations Twenty and Thirty Miles Distant. + </td> + </tr> + </table> + <p> + <i>The Crystal Detector</i>.--This is known as the <i>Rasco baby</i> + detector and it is made and sold by the <i>Radio Specialty Company</i>, 96 + Park Place, New York City. It is shown in <i>Fig. 96</i>. The base is made + of black composition and on it is mounted a standard in which a rod slides + and on one end of this there is fixed a hard rubber adjusting knob while + the other end carries a thin piece of <i>phosphor-bronze wire</i>, called + a <i>cat-whisker</i> To secure the galena crystal in the cup you simply + unscrew the knurled cap, place it in the cavity of the post and screw the + cap back on again. The free end of the cat-whisker wire is then adjusted + so that it will rest lightly on the exposed part of the galena. + </p> + <p> + <a name="fig096" id="fig096"><img width="600" height="347" + src="images/fig096.jpg" alt="Fig. 96.--Rasco Baby Crystal Detector." /></a> + </p> + <p> + The <i>Tuning Coil</i>.--You will have to make this tuning coil, which you + can do at a cost of less than $1.00, as the cheapest tuning coil you can + buy costs at least $3.00, and we need the rest of our $5.00 to invest in + the earphone. Get a cardboard tube, such as is used for mailing purposes, + 2 inches in diameter and 3 inches long, see <i>A</i> in <i>Fig. 97</i>. + Now wind on 250 turns of <i>No. 40 Brown and Sharpe gauge plain enameled + magnet wire</i>. You can use <i>No. 40 double cotton covered magnet wire</i>, + in which case you will have to shellac the tube and the wire after you get + it on. + </p> + <p> + <a name="fig097" id="fig097"><img width="600" height="359" + src="images/fig097.jpg" alt="Fig. 97.--How the Tuning Coil is Made." /></a> + </p> + <p> + As you wind on the wire take off a tap at every 15th turn, that is, scrape + the wire and solder on a piece about 7 inches long, as shown in <i>Fig. 99</i>; + and do this until you have 6 taps taken off. Instead of leaving the wires + outside of the tube bring them to the inside of it and then out through + one of the open ends. Now buy a <i>round wood-base switch</i> with 7 + contact points on it as shown at <i>B</i> in <i>Fig. 97</i>. This will + cost you <i>25</i> or <i>50</i> cents. + </p> + <p> + <i>The Headphone</i>.--An ordinary Bell telephone receiver is of small use + for wireless work as it is wound to too low a resistance and the diaphragm + is much too thick. If you happen to have a Bell phone you can rewind it + with <i>No. 40</i> single covered silk magnet wire, or enameled wire of + the same size, when its sensitivity will be very greatly improved. Then + you must get a thin diaphragm and this should <i>not</i> be enameled, as + this tends to dampen the vibrations of it. You can get a diaphragm of the + right kind for 5 cents. + </p> + <p> + The better way, though, is to buy an earphone made especially for wireless + work. You can get one wound to 1000 ohms resistance for $1.75 and this + price includes a cord. [Footnote: This is Mesco, No. 470 wireless phone. + Sold by the Manhattan Electrical Supply Co., Park Place, N.Y.C.] For $1.00 + extra you can get a head-band for it, and then your phone will look like + the one pictured in <i>Fig. 98</i>. + </p> + <p> + <a name="fig098" id="fig098"><img width="345" height="360" + src="images/fig098.jpg" alt="Fig. 98.--Mesco 1000 Ohm Head Set." /></a> + </p> + <p> + <i>How to Mount the Parts</i>.--Now mount the coil on a wood base, 1/2 or + 1 inch thick, 3-1/2 inches wide and 5-1/2 inches long, and then connect + one end of the coil to one of the end points on the switch, and connect + each succeeding tap to one of the switch points, as shown schematically in + <i>Fig. 99</i> and diagrammatically in <i>Fig. 100</i>. This done, screw + the switch down to the base. Finally screw the detector to the base and + screw two binding posts in front of the coil. These are for the earphone. + </p> + <p> + <a name="fig099" id="fig099"><img width="600" height="554" + src="images/fig099.jpg" + alt="Fig. 99.--Schematic Layout of $5.00 Receiving Set." /></a> <a + name="fig100" id="fig100"><img width="480" height="585" + src="images/fig100.jpg" + alt="Fig. 100.--Wiring Diagram for $5.00 Receiving Set." /></a> + </p> + <p> + <i>The Condenser</i>.--You do not have to connect a condenser across the + earphone but if you do you will improve the receiving qualities of the + receptor. + </p> + <p> + <i>How to Connect Up the Receptor</i>.--Now connect up all the parts as + shown in <i>Figs. 99</i> and <i>100</i>, then connect the leading-in wire + of the aerial with the lever of the switch; and connect the free end of + the tuning coil with the <i>ground</i>. If you have no aerial wire try + hooking it up to a rain pipe that is <i>not grounded</i> or the steel + frame of an umbrella. For a <i>ground</i> you can use a water pipe, an + iron pipe driven into the ground, or a hydrant. Put on your headphone, + adjust the detector and move the lever over the switch contacts until it + is in adjustment and then, if all your connections are properly made, you + should be able to pick up messages. + </p> + <table cellspacing="20" summary="Illustration"> + <tr> + <td align="center"> + <i>Photograph unavailable</i> + </td> + </tr> + <tr> + <td align="center"> + Wireless Set made into a Ring, designed by Alfred G. Rinehart, of + Elizabeth, New Jersey. This little Receptor is a Practical Set; it + will receive Messages, Concerts, etc., Measures 1" by 5/8" by 7/8". An + ordinary Umbrella is used as an Aerial. + </td> + </tr> + </table> + <h2> + <a name="appendix" id="appendix">APPENDIX</a> + </h2> + <h3> + USEFUL INFORMATION + </h3> + <h3> + ABBREVIATIONS OF UNITS + </h3> +<pre xml:space="preserve"> + Unit Abbreviation + + ampere amp. + ampere-hours amp.-hr. + centimeter cm. + centimeter-gram-second c.g.s. + cubic centimeters cm.^3 + cubic inches cu. in. + cycles per second ~ + degrees Centigrade °C. + degrees Fahrenheit °F. + feet ft. + foot-pounds ft.-lb. + grams g. + henries h. + inches in. + kilograms kg. + kilometers km. + kilowatts kw. + kilowatt-hours kw.-hr. + kilovolt-amperes kv.-a. + meters m. + microfarads [Greek: mu]f. + micromicrofarads [Greek: mu mu]f. + millihenries mh. + millimeters mm. + pounds lb. + seconds sec. + square centimeters cm.^2 + square inches sq. in. + volts v. + watts w. +</pre> + <h3> + PREFIXES USED WITH METRIC SYSTEM UNITS + </h3> +<pre xml:space="preserve"> + Prefix Abbreviation Meaning + + micro [Greek: mu]. 1 millionth + milli m. 1 thousandth + centi c. 1 hundredth + deci d. 1 tenth + deka dk. 10 + hekto h. 1 hundred + kilo k. 1 thousand + mega m. 1 million +</pre> + <h3> + SYMBOLS USED FOR VARIOUS QUANTITIES + </h3> + <p> + <img width="600" height="530" src="images/symbols-quantities.jpg" + alt="Symbols for quantities" /> + </p> +<pre xml:space="preserve"> +Quantity Symbol + +capacitance <i>C</i> + +conductance <i>g</i> + +coupling co-efficient <i>k</i> + +current, instantaneous <i>i</i> + +current, effective value <i>I</i> + +decrement <i>[Greek: delta]</i> + +dielectric constant <i>[Greek: alpha]</i> + +electric field intensity <i>[Greek: epsilon]</i> + +electromotive force,<br /> +instantaneous value <i>E</i> + +electromotive force,<br /> +effective value <i>F</i> + +energy <i>W</i> + +force <i>F</i> + +frequency <i>f</i> + +frequency x 2[Greek: pi] <i>[Greek: omega]</i> + +impedance <i>Z</i> + +inductance, self <i>L</i> + +inductance, mutual <i>M</i> + +magnetic field intensity <i>A</i> + +magnetic flux <i>[Greek: Phi]</i> + +magnetic induction <i>B</i> + +period of a complete<br /> +oscillation <i>T</i> + +potential difference <i>V</i> + +quantity of electricity <i>Q</i> + +ratio of the<br /> +circumference of a<br /> +circle to its diameter<br /> +=3.1416 <i>[Greek: pi]</i> + +reactance <i>X</i> + +resistance <i>R</i> + +time <i>t</i> + +velocity <i>v</i> + +velocity of light <i>c</i> + +wave length <i>[Greek: lambda]</i> + +wave length in meters <i>[Greek: lambda]m</i> + +work <i>W</i> + +permeability <i>[Greek: mu]</i> + +Square root <i>[Math: square root]</i> +</pre> + <h3> + TABLE OF ENAMELED WIRE + </h3> +<pre xml:space="preserve"> + No. of Turns Turns Ohms per + Wire, per per Cubic Inch + B.& S. Linear Square of + Gauge Inch Inch Winding + + 20 30 885 .748 + 22 37 1400 1.88 + 24 46 2160 4.61 + 26 58 3460 11.80 + 28 73 5400 29.20 + 30 91 8260 70.90 + 32 116 21,000 7547.00 + 34 145 13,430 2968.00 + 36 178 31,820 1098.00 + 38 232 54,080 456.00 + 40 294 86,500 183.00 +</pre> + <h3> + TABLE OF FREQUENCY AND WAVE LENGTHS + </h3> +<pre xml:space="preserve"> + W. L.--Wave Lengths in Meters. + F.--Number of Oscillations per Second. + O. or square root L. C. is called Oscillation Constant. + C.--Capacity in Microfarads. + L.--Inductance in Centimeters. + 1000 Centimeters = 1 Microhenry. +</pre> +<pre xml:space="preserve"> + W.L. F O L.C. + 50 6,000,000 .839 .7039 + 100 3,000,000 1.68 2.82 + 150 2,000,000 2.52 6.35 + 200 1,500,000 3.36 11.29 + 250 1,200,000 4.19 17.55 + 300 1,000,000 5.05 25.30 + 350 857,100 5.87 34.46 + 400 750,000 6.71 45.03 + 450 666,700 7.55 57.00 + 500 600,000 8.39 70.39 + 550 545,400 9.23 85.19 + 600 500,000 10.07 101.41 + 700 428,600 11.74 137.83 + 800 375,000 13.42 180.10 + 900 333,300 15.10 228.01 + 1,000 300,000 16.78 281.57 + 1,100 272,730 18.45 340.40 + 1,200 250,000 20.13 405.20 + 1,300 230,760 21.81 475.70 + 1,400 214,380 23.49 551.80 + 1,500 200,000 25.17 633.50 + 1,600 187,500 26.84 720.40 + 1,700 176,460 28.52 813.40 + 1,800 166,670 30.20 912.00 + 1,900 157,800 31.88 1,016.40 + 2,000 150,000 33.55 1,125.60 + 2,100 142,850 35.23 1,241.20 + 2,200 136,360 36.91 1,362.40 + 2,300 130,430 38.59 1,489.30 + 2,400 125,000 40.27 1,621.80 + 2,500 120,000 41.95 1,759.70 + 2,600 115,380 43.62 1,902.60 + 2,700 111,110 45.30 2,052.00 + 2,800 107,140 46.89 2,207.00 + 2,900 103,450 48.66 2,366.30 + 3,000 100,000 50.33 2,533.20 + 4,000 75,000 67.11 4,504.00 + 5,000 60,000 83.89 7,038.00 + 6,000 50,000 100.7 10,130.00 + 7,000 41,800 117.3 13,630.00 + 8,000 37,500 134.1 18,000.00 + 9,000 33,300 151.0 22,820.00 + 10,000 30,000 167.9 28,150.00 + 11,000 27,300 184.8 34,150.00 + 12,000 25,000 201.5 40,600.00 + 13,000 23,100 218.3 47,600.00 + 14,000 21,400 235.0 55,200.00 + 15,000 20,000 252.0 63,500.00 + 16,000 18,750 269.0 72,300.00 +</pre> + <h3> + PRONUNCIATION OF GREEK LETTERS + </h3> + <p> + Many of the physical quantities use Greek letters for symbols. The + following is the Greek alphabet with the way the letters are pronounced:<br /> + <img width="600" height="230" src="images/symbols-greek-letters.jpg" + alt="Greek symbols" /> + </p> +<pre xml:space="preserve"> + a alpha + b beta + g gamma + d delta + e epsilon + z zeta + ae eta + th theta + i iota + k kappa + l lambda + m mu + n nu + x Xi(Zi) + o omicron + p pi + r rho + s sigma + t tau + u upsilon + ph phi + ch chi + ps psi + o omega +</pre> + <h3> + TABLE OF SPARKING DISTANCES + </h3> + <p> + In Air for Various Voltages between Needle Points + </p> +<pre xml:space="preserve"> + Volts Distance + Inches Centimeter + 5,000 .225 .57 + 10,000 .470 1.19 + 15,000 .725 1.84 + 20,000 1.000 2.54 + 25,000 1.300 3.30 + 30,000 1.625 4.10 + 35,000 2.000 5.10 + 40,000 2.450 6.20 + 45,000 2.95 7.50 + 50,000 3.55 9.90 + 60,000 4.65 11.8 + 70,000 5.85 14.9 + 80,000 7.10 18.0 + 90,000 8.35 21.2 + 100,000 9.60 24.4 + 110,000 10.75 27.3 + 120,000 11.85 30.1 + 130,000 12.95 32.9 + 140,000 13.95 35.4 + 150,000 15.00 38.1 +</pre> + <h3> + FEET PER POUND OF INSULATED MAGNET WIRE + </h3> +<pre xml:space="preserve"> + No. of Single Double Single Double + B.& S. Cotton, Cotton, Silk, Silk, Enamel + Gauge 4-Mils 8-Mils 1-3/4-Mils 4-Mils + + 20 311 298 319 312 320 + 21 389 370 408 389 404 + 22 488 461 503 498 509 + 23 612 584 636 631 642 + 24 762 745 800 779 810 + 25 957 903 1,005 966 1,019 + 26 1,192 1,118 1,265 1,202 1,286 + 27 1,488 1,422 1,590 1,543 1,620 + 28 1,852 1,759 1,972 1,917 2,042 + 29 2,375 2,207 2,570 2,435 2,570 + 30 2,860 2,534 3,145 2,900 3,240 + 31 3,800 2,768 3,943 3,683 4,082 + 32 4,375 3,737 4,950 4,654 5,132 + 33 5,590 4,697 6,180 5,689 6,445 + 34 6,500 6,168 7,740 7,111 8,093 + 35 8,050 6,737 9,600 8,584 10,197 + 36 9,820 7,877 12,000 10,039 12,813 + 37 11,860 9,309 15,000 10,666 16,110 + 38 14,300 10,636 18,660 14,222 20,274 + 39 17,130 11,907 23,150 16,516 25,519 + 40 21,590 14,222 28,700 21,333 32,107 +</pre> + <h3> + INTERNATIONAL MORSE CODE AND CONVENTIONAL SIGNALS + </h3> + <p> + <b>TO BE USED FOR ALL GENERAL PUBLIC SERVICE RADIO COMMUNICATION</b> + </p> + <ol> + <li> + A dash is equal to three dots. + </li> + <li> + The space between parts of the same letter is equal to one dot. + </li> + <li> + The space between two letters is equal to three dots. + </li> + <li> + The space between two words is equal to five dots. + </li> + </ol> + <p> + [Note: period denotes Morse dot, hyphen denotes Morse dash] + </p> +<pre xml:space="preserve"> +A .- + +B -... + +C -.-. + +D -.. + +E . + +F ..-. + +G --. + +H .... + +I .. + +J .--- + +K -.- + +L .-.. + +M -- + +N -. + +O --- + +P .--. + +Q --.- + +R .-. + +S ... + +T - + +U ..- + +V ...- + +W .-- + +X -..- + +Y -.-- + +Z --.. + +Ä (German) .-.- + +Á or Å (Spanish-Scandinavian) .--.- + +CH (German-Spanish) ---- + +É (French) ..-.. + +Ñ (Spanish) --.-- + +Ö (German) ---. + +Ü (German) ..-- + +1 .---- + +2 ..--- + +3 ...-- + +4 ....- + +5 ..... + +6 -.... + +7 --... + +8 ---.. + +9 ----. + +0 ----- + +Period .. .. .. + +Semicolon -.-.-. + +Comma -.-.-. + +Colon ---... + +Interrogation ..--.. + +Exclamation point --..-- + +Apostrophe .----. + +Hyphen -....- + +Bar indicating fraction -..-. + +Parenthesis -.--.- + +Inverted commas .-..-. + +Underline ..--.- + +Double dash -...- + +Distress Call ...---... + +Attention call to precede every transmission -.-.- + +General inquiry call -.-. --.- + +From (de) -.. . + +Invitation to transmit (go ahead) -.- + +Warning--high power --..-- + +Question (please repeat after ...)--interrupting long messages ..--.. + +Wait .-... + +Break (Bk.) (double dash) -...- + +Understand ...-. + +Error ........ + +Received (O.K.) .-. + +Position report (to precede all position messages) - .-. + +End of each message (cross) .-.-. + +Transmission finished (end of work) (conclusion of correspondence) ...-.- + +</pre> + <h3> + INTERNATIONAL RADIOTELEGRAPHIC CONVENTION + </h3> + <p> + <b>LIST OF ABBREVIATIONS TO BE USED IN RADIO COMMUNICATION</b> + </p> +<pre xml:space="preserve"> +ABBREVIATION QUESTION ANSWER OR REPLY + +PRB Do you wish to communicate I wish to communicate by means + by means of the International of the International Signal Code. + Signal Code? + +QRA What ship or coast station is This is.... + that? + +QRB What is your distance? My distance is.... + +QRC What is your true bearing? My true bearing is.... + +QRD Where are you bound for? I am bound for.... + +QRF Where are you bound from? I am bound from.... + +QRG What line do you belong to? I belong to the ... Line. + +QRH What is your wave length in My wave length is ... meters. + meters? + +QRJ How many words have you to send? I have ... words to send. + +QRK How do you receive me? I am receiving well. + +QRL Are you receiving badly? I am receiving badly. Please + Shall I send 20? send 20. + ...-. ...-. + for adjustment? for adjustment. + +QRM Are you being interfered with? I am being interfered with. + +QRN Are the atmospherics strong? Atmospherics are very strong. + +QRO Shall I increase power? Increase power. + +QRP Shall I decrease power? Decrease power. + +QRQ Shall I send faster? Send faster. + +QRS Shall I send slower? Send slower. + +QRT Shall I stop sending? Stop sending. + +QRU Have you anything for me? I have nothing for you. + +QRV Are you ready? I am ready. All right now. + +QRW Are you busy? I am busy (or: I am busy with...). + Please do not interfere. + +QRX Shall I stand by? Stand by. I will call you when + required. + +QRY When will be my turn? Your turn will be No.... + +QRZ Are my signals weak? You signals are weak. + +QSA Are my signals strong? You signals are strong. + +QSB Is my tone bad? The tone is bad. + Is my spark bad? The spark is bad. + +QSC Is my spacing bad? Your spacing is bad. + +QSD What is your time? My time is.... + +QSF Is transmission to be in Transmission will be in + alternate order or in series? alternate order. + +QSG Transmission will be in a + series of 5 messages. + +QSH Transmission will be in a + series of 10 messages. + +QSJ What rate shall I collect for...? Collect.... + +QSK Is the last radiogram canceled? The last radiogram is canceled. + +QSL Did you get my receipt? Please acknowledge. + +QSM What is your true course? My true course is...degrees. + +QSN Are you in communication with land? I am not in communication with land. + +QSO Are you in communication with I am in communication with... + any ship or station (through...). + (or: with...)? + +QSP Shall I inform...that you are Inform...that I am calling him. + calling him? + +QSQ Is...calling me? You are being called by.... + +QSR Will you forward the radiogram? I will forward the radiogram. + +QST Have you received the general General call to all stations. + call? + +QSU Please call me when you have Will call when I have finished. + finished (or: at...o'clock)? + +QSV Is public correspondence being Public correspondence is being + handled? handled. Please do not interfere. +</pre> + <p> + [Footnote: Public correspondence is any radio work, official or private, + handled on commercial wave lengths.] + </p> +<pre xml:space="preserve"> +QSW Shall I increase my spark Increase your spark frequency. + frequency? + +QSX Shall I decrease my spark Decrease your spark frequency. + frequency? + +QSY Shall I send on a wavelength Let us change to the wave length + of ... meters? of ... meters. + +QSZ Send each word twice. I have + difficulty in receiving you. + +QTA Repeat the last radiogram. +</pre> + <p> + When an abbreviation is followed by a mark of interrogation, it refers to + the question indicated for that abbreviation. + </p> + <p> + <b>Useful Information</b> + </p> + <h3> + Symbols Used For Apparatus + </h3> + <p> + <img width="509" height="800" src="images/symbols-apparatus.jpg" + alt="Symbols" /> + </p> + <p> + alternator<br /> ammeter<br /> aerial<br /> arc<br /> battery<br /> buzzer<br /> + condenser<br /> variable condenser<br /> connection of wires<br /> no + connection<br /> coupled coils<br /> variable coupling<br /> detector<br /> + gap, plain<br /> gap, quenched<br /> ground<br /> hot wire ammeter<br /> + inductor<br /> variable inductor<br /> key<br /> resistor<br /> variable + resistor<br /> switch s.p.s.t.<br /> " s.p.d.t.<br /> " d.p.s.t.<br /> " + d.p.d.t.<br /> " reversing<br /> phone receiver<br /> " transmitter<br /> + thermoelement<br /> transformer<br /> vacuum tube<br /> voltmeter<br /> choke + coil + </p> + <h3> + DEFINITIONS OF ELECTRIC AND MAGNETIC UNITS + </h3> + <p> + The <i>ohm</i> is the resistance of a thread of mercury at the temperature + of melting ice, 14.4521 grams in mass, of uniform cross-section and a + length of 106.300 centimeters. + </p> + <p> + The <i>ampere</i> is the current which when passed through a solution of + nitrate of silver in water according to certain specifications, deposits + silver at the rate of 0.00111800 of a gram per second. + </p> + <p> + The <i>volt</i> is the electromotive force which produces a current of 1 + ampere when steadily applied to a conductor the resistance of which is 1 + ohm. + </p> + <p> + The <i>coulomb</i> is the quantity of electricity transferred by a current + of 1 ampere in 1 second. + </p> + <p> + The <i>ampere-hour</i> is the quantity of electricity transferred by a + current of 1 ampere in 1 hour and is, therefore, equal to 3600 coulombs. + </p> + <p> + The <i>farad</i> is the capacitance of a condenser in which a potential + difference of 1 volt causes it to have a charge of 1 coulomb of + electricity. + </p> + <p> + The <i>henry</i> is the inductance in a circuit in which the electromotive + force induced is 1 volt when the inducing current varies at the rate of 1 + ampere per second. + </p> + <p> + The <i>watt</i> is the power spent by a current of 1 ampere in a + resistance of 1 ohm. + </p> + <p> + The <i>joule</i> is the energy spent in I second by a flow of 1 ampere in + 1 ohm. + </p> + <p> + The <i>horse-power</i> is used in rating steam machinery. It is equal to + 746 watts. + </p> + <p> + The <i>kilowatt</i> is 1,000 watts. + </p> + <p> + The units of capacitance actually used in wireless work are the <i>microfarad</i>, + which is the millionth part of a farad, because the farad is too large a + unit; and the <i>C. G. S. electrostatic unit of capacitance</i>, which is + often called the <i>centimeter of capacitance</i>, which is about equal to + 1.11 microfarads. + </p> + <p> + The units of inductance commonly used in radio work are the <i>millihenry</i>, + which is the thousandth part of a henry; and the <i>centimeter of + inductance</i>, which is one one-thousandth part of a microhenry. + </p> + <p> + <i>Note</i>.--For further information about electric and magnetic units + get the <i>Bureau of Standards Circular No. 60</i>, called <i>Electric + Units and Standards</i>, the price of which is 15 cents; also get <i>Scientific + Paper No. 292</i>, called <i>International System of Electric and Magnetic + Units</i>, price 10 cents. These and other informative papers can be had + from the <i>Superintendent of Documents, Government Printing Office</i>, + Washington, D. C. + </p> + <h3> + WIRELESS BOOKS + </h3> + <p> + <i>The Admiralty Manual of Wireless Telegraphy</i>. 1920. Published by His + Majesty's Stationery Office, London. + </p> + <p> + Ralph E. Batcher.--<i>Prepared Radio Measurements</i>. 1921. Wireless + Press, Inc., New York City. + </p> + <p> + Elmer E. Bucher.--<i>Practical Wireless Telegraphy</i>. 1918. Wireless + Press, Inc., New York City. + </p> + <p> + Elmer E. Bucher.--<i>Vacuum Tubes in Wireless Communication</i>. 1919. + Wireless Press, Inc., New York City. + </p> + <p> + Elmer E. Bucher.--<i>The Wireless Experimenter's Manual</i>. 1920. + Wireless Press, Inc., New York City. + </p> + <ol> + <li> + Frederick Collins.--<i>Wireless Telegraphy, Its History, Theory, and + Practice</i>. 1905. McGraw Pub. Co., New York City. + </li> + <li> + H. Dellinger.--<i>Principles Underlying Radio Communication</i>. + </li> + <li> + Signal Corps, U. S. Army, Washington, D. C. + </li> + <li> + M. Dorsett.--<i>Wireless Telegraphy and Telephony</i>. 1920. Wireless + Press, Ltd., London. + </li> + <li> + A. Fleming.--<i>Principles of Electric Wave Telegraphy</i>. 1919. + Longmans, Green and Co., London. + </li> + </ol> + <p> + Charles B. Hayward.--<i>How to Become a Wireless Operator</i>. 1918. + American Technical Society, Chicago, Ill. + </p> + <p> + G. D. Robinson.--<i>Manual of Radio Telegraphy and Telephony</i>. 1920. + United States Naval Institute, Annapolis, Md. + </p> + <p> + Rupert Stanley.--<i>Textbook of Wireless Telegraphy</i>. 1919. Longmans, + Green and Co., London. + </p> + <p> + E. W. Stone.--<i>Elements of Radio Telegraphy</i>. 1919. D, Van Nostrand + Co., New York City. + </p> + <p> + L. B. Turner.--<i>Wireless Telegraphy and Telephony</i>. 1921. Cambridge + University Press. Cambridge, England. + </p> + <p> + Send to the <i>Superintendent of Documents, Government Printing Office</i>, + Washington, D. C., for a copy of <i>Price List No. 64</i> which lists the + Government's books and pamphlets on wireless. It will be sent to you free + of charge. + </p> + <p> + The Government publishes; (1) <i>A List of Commercial Government and + Special Wireless Stations</i>, every year, price 15 cents; (2) <i>A List + of Amateur Wireless Stations</i>, yearly, price 15 cents; (3) <i>A + Wireless Service Bulletin</i> is published monthly, price 5 cents a copy, + or 25 cents yearly; and (4) <i>Wireless Communication Laws of the United + States</i>, the <i>International Wireless Telegraphic Convention and + Regulations Governing Wireless Operators and the Use of Wireless on Ships + and Land Stations</i>, price 15 cents a copy. Orders for the above + publications should be addressed to the <i>Superintendent of Documents, + Government Printing Office, Washington, D. C.</i> + </p> + <h3> + Manufacturers and Dealers in Wireless Apparatus and Supplies: + </h3> + <p> + Adams-Morgan Co., Upper Montclair, N. J. + </p> + <p> + American Hard Rubber Co., 11 Mercer Street, New York City. + </p> + <p> + American Radio and Research Corporation, Medford Hillside, Mass. + </p> + <p> + Brach (L. S.) Mfg. Co., 127 Sussex Ave., Newark, N. J. + </p> + <p> + Brandes (C.) Inc., 237 Lafayette St., New York City. + </p> + <p> + Bunnell (J. H.) Company, Park Place, New York City. + </p> + <p> + Burgess Battery Company, Harris Trust Co. Bldg., Chicago, Ill. + </p> + <p> + Clapp-Eastman Co., 120 Main St., Cambridge, Mass. + </p> + <p> + Connecticut Telephone and Telegraph Co., Meriden, Conn. + </p> + <p> + Continental Fiber Co., Newark, Del. + </p> + <p> + Coto-Coil Co., Providence, R. I. + </p> + <p> + Crosley Mfg. Co., Cincinnati, Ohio. + </p> + <p> + Doolittle (F. M.), 817 Chapel St., New Haven, Conn. + </p> + <p> + Edelman (Philip E.), 9 Cortlandt St., New York City. + </p> + <p> + Edison Storage Battery Co., Orange, N. J. + </p> + <p> + Electric Specialty Co., Stamford, Conn. + </p> + <p> + Electrose Mfg. Co., 60 Washington St., Brooklyn, N. Y. + </p> + <p> + General Electric Co., Schenectady, N. Y. + </p> + <p> + Grebe (A. H.) and Co., Inc., Richmond Hill, N. Y. C. + </p> + <p> + International Brass and Electric Co., 176 Beekman St., New York City. + </p> + <p> + International Insulating Co., 25 West 45th St., New York City. + </p> + <p> + King Amplitone Co., 82 Church St., New York City. + </p> + <p> + Kennedy (Colin B.) Co., Rialto Bldg., San Francisco, Cal. + </p> + <p> + Magnavox Co., Oakland, Cal. + </p> + <p> + Manhattan Electrical Supply Co., Park Place, N. Y. + </p> + <p> + Marshall-Gerken Co., Toledo, Ohio. + </p> + <p> + Michigan Paper Tube and Can Co., 2536 Grand River Ave., Detroit, Mich. + </p> + <p> + Murdock (Wm. J.) Co., Chelsea, Mass. + </p> + <p> + National Carbon Co., Inc., Long Island City, N. Y. + </p> + <p> + Pittsburgh Radio and Appliance Co., 112 Diamond St., Pittsburgh, Pa, + </p> + <p> + Radio Corporation of America, 233 Broadway, New York City. + </p> + <p> + Riley-Klotz Mfg. Co., 17-19 Mulberry St., Newark, N. J. + </p> + <p> + Radio Specialty Co., 96 Park Place, New York City. + </p> + <p> + Roller-Smith Co., 15 Barclay St., New York City. + </p> + <p> + Tuska (C. D.) Co., Hartford, Conn. + </p> + <p> + Western Electric Co., Chicago, Ill. + </p> + <p> + Westinghouse Electric Co., Pittsburgh, Pa. + </p> + <p> + Weston Electrical Instrument Co., 173 Weston Ave., Newark, N. J. + </p> + <p> + Westfield Machine Co., Westfield, Mass. + </p> + <h3> + ABBREVIATIONS OF COMMON TERMS + </h3> +<pre xml:space="preserve"> +A. ..............Aerial + +A.C. ............Alternating Current + +A.F. ............Audio Frequency + +B. and S. .......Brown & Sharpe Wire Gauge + +C. ..............Capacity or Capacitance + +C.G.S. ..........Centimeter-Grain-Second + +Cond. ...........Condenser + +Coup. ...........Coupler + +C.W. ............Continuous Waves + +D.C. ............Direct Current + +D.P.D.T. ........Double Point Double Throw + +D.P.S.T. ........Double Point Single Throw + +D.X. ............Distance + +E. ..............Short for Electromotive Force (Volt) + +E.M.F. ..........Electromotive Force + +F. ..............Filament or Frequency + +G. ..............Grid + +Gnd. ............Ground + +I. ..............Current Strength (Ampere) + +I.C.W. ..........Interrupted Continuous Waves + +KW. .............Kilowatt + +L. ..............Inductance + +L.C. ............Loose Coupler + +Litz. ...........Litzendraht + +Mfd. ............Microfarad + +Neg. ............Negative + +O.T. ............Oscillation Transformer + +P. ..............Plate + +Prim. ...........Primary + +Pos. ............Positive + +R. ..............Resistance + +R.F. ............Radio Frequency + +Sec. ............Secondary + +S.P.D.T. ........Single Point Double Throw + +S.P.S.T. ........Single Point Single Throw + +S.R. ............Self Rectifying + +T. ..............Telephone or Period (time) of Complete + Oscillation + +Tick. ...........Tickler + +V. ..............Potential Difference + +Var. ............Variometer + +Var. Cond. ......Variable Condenser + +V.T. ............Vacuum Tube + +W.L. ............Wave Length + +X. ..............Reactance +</pre> + <h2> + <a name="glossary" id="glossary">GLOSSARY</a> + </h2> + <p> + <i>A</i> BATTERY.--<i>See Battery A</i>. + </p> + <p> + ABBREVIATIONS, CODE.--Abbreviations of questions and answers used in + wireless communication. The abbreviation <i>of a question</i> is usually + in three letters of which the first is Q. Thus Q R B is the code + abbreviation of "<i>what is your distance?</i>" and the answer "<i>My + distance is</i>..." See <i>Page 306</i> [Appendix: List of Abbreviations]. + </p> + <p> + ABBREVIATIONS, UNITS.--Abbreviations of various units used in wireless + electricity. These abbreviations are usually lower case letters of the + Roman alphabet, but occasionally Greek letters are used and other signs. + Thus <i>amperes</i> is abbreviated <i>amp., micro</i>, which means <i>one + millionth</i>, [Greek: mu], etc. See <i>Page 301</i> [Appendix: Useful + Abbreviations]. + </p> + <p> + ABBREVIATIONS OF WORDS AND TERMS.--Letters used instead of words and terms + for shortening them up where there is a constant repetition of them, as <i>A.C.</i> + for <i>alternating current; C.W.</i> for <i>continuous waves; V.T.</i> for + <i>vacuum tube</i>, etc. See <i>Page 312</i> [Appendix: Abbreviations of + Common Terms]. + </p> + <p> + AERIAL.--Also called <i>antenna</i>. An aerial wire. One or more wires + suspended in the air and insulated from its supports. It is the aerial + that sends out the waves and receives them. + </p> + <p> + AERIAL, AMATEUR.--An aerial suitable for sending out 200 meter wave + lengths. Such an aerial wire system must not exceed 120 feet in length + from the ground up to the aerial switch and from this through the + leading-in wire to the end of the aerial. + </p> + <p> + AERIAL AMMETER.--See <i>Ammeter, Hot Wire</i>. + </p> + <p> + AERIAL, BED-SPRINGS.--Where an outdoor aerial is not practicable <i>bed-springs</i> + are often made to serve the purpose. + </p> + <p> + AERIAL CAPACITY.--See <i>Capacity, Aerial.</i> + </p> + <p> + AERIAL COUNTERPOISE.--Where it is not possible to get a good ground an <i>aerial + counterpoise</i> or <i>earth capacity</i> can be used to advantage. The + counterpoise is made like the aerial and is supported directly under it + close to the ground but insulated from it. + </p> + <p> + AERIAL, DIRECTIONAL.--A flat-top or other aerial that will transmit and + receive over greater distances to and from one direction than to and from + another. + </p> + <p> + AERIAL, GROUND.--Signals can be received on a single long wire when it is + placed on or buried in the earth or immersed in water. It is also called a + <i>ground antenna</i> and an <i>underground aerial.</i> + </p> + <p> + AERIAL, LOOP.--Also called a <i>coil aerial, coil antenna, loop aerial, + loop antenna</i> and when used for the purpose a <i>direction finder</i>. + A coil of wire wound on a vertical frame. + </p> + <p> + AERIAL RESISTANCE.--See <i>Resistance, Aerial.</i> + </p> + <p> + AERIAL SWITCH.--See <i>Switch Aerial.</i> + </p> + <p> + AERIAL WIRE.--(1) A wire or wires that form the aerial. (2) Wire that is + used for aerials; this is usually copper or copper alloy. + </p> + <p> + AERIAL WIRE SYSTEM.--An aerial and ground wire and that part of the + inductance coil which connects them. The open oscillation circuit of a + sending or a receiving station. + </p> + <p> + AIR CORE TRANSFORMER.--See <i>Transformer, Air Core.</i> + </p> + <p> + AMATEUR AERIAL OR ANTENNA.--See <i>Aerial, Amateur.</i> + </p> + <p> + ALTERNATOR.--An electric machine that generates alternating current. + </p> + <p> + ALPHABET, INTERNATIONAL CODE.--A modified Morse alphabet of dots and + dashes originally used in Continental Europe and, hence, called the <i>Continental + Code</i>. It is now used for all general public service wireless + communication all over the world and, hence, it is called the <i>International + Code</i>. See <i>page 305</i> [Appendix: International Morse Code]. + </p> + <p> + ALTERNATING CURRENT (<i>A.C.</i>)--See <i>Current.</i> + </p> + <p> + ALTERNATING CURRENT TRANSFORMER.--See <i>Transformer</i>. + </p> + <p> + AMATEUR GROUND.--See <i>Ground, Amateur</i>. + </p> + <p> + AMMETER.--An instrument used for measuring the current strength, in terms + of amperes, that flows in a circuit. Ammeters used for measuring direct + and alternating currents make use of the <i>magnetic effects</i> of the + currents. High frequency currents make use of the <i>heating effects</i> + of the currents. + </p> + <p> + AMMETER, HOT-WIRE.--High frequency currents are usually measured by means + of an instrument which depends on heating a wire or metal strip by the + oscillations. Such an instrument is often called a <i>thermal ammeter</i>, + <i>radio ammeter</i> and <i>aerial ammeter</i>. + </p> + <p> + AMMETER, AERIAL.--See <i>Ammeter, Hot Wire</i>. + </p> + <p> + AMMETER, RADIO.--See <i>Ammeter, Hot Wire</i>. + </p> + <p> + AMPERE.--The current which when passed through a solution of nitrate of + silver in water according to certain specifications, deposits silver at + the rate of 0.00111800 of a gram per second. + </p> + <p> + AMPERE-HOUR.--The quantity of electricity transferred by a current of 1 + ampere in 1 hour and is, therefore, equal to 3600 coulombs. + </p> + <p> + AMPERE-TURNS.--When a coil is wound up with a number of turns of wire and + a current is made to flow through it, it behaves like a magnet. B The + strength of the magnetic field inside of the coil depends on (1) the + strength of the current and (2) the number of turns of wire on the coil. + Thus a feeble current flowing through a large number of turns will produce + as strong a magnetic field as a strong current flowing through a few turns + of wire. This product of the current in amperes times the number of turns + of wire on the coil is called the <i>ampere-turns</i>. + </p> + <p> + AMPLIFICATION, AUDIO FREQUENCY.--A current of audio frequency that is + amplified by an amplifier tube or other means. + </p> + <p> + AMPLIFICATION, CASCADE.--See <i>Cascade Amplification</i>. + </p> + <p> + AMPLIFICATION, RADIO FREQUENCY.--A current of radio frequency that is + amplified by an amplifier tube or other means before it reaches the + detector. + </p> + <p> + AMPLIFICATION, REGENERATIVE.--A scheme that uses a third circuit to feed + back part of the oscillations through a vacuum tube and which increases + its sensitiveness when used as a detector and multiplies its action as an + amplifier and an oscillator. + </p> + <p> + AMPLIFIER, AUDIO FREQUENCY.--A vacuum tube or other device that amplifies + the signals after passing through the detector. + </p> + <p> + AMPLIFIER, MAGNETIC.--A device used for controlling radio frequency + currents either by means of a telegraph key or a microphone transmitter. + The controlling current flows through a separate circuit from that of the + radio current and a fraction of an ampere will control several amperes in + the aerial wire. + </p> + <p> + AMPLIFIERS, MULTI-STAGE.--A receiving set using two or more amplifiers. + Also called <i>cascade amplification</i>. + </p> + <p> + AMPLIFIER, VACUUM TUBE.--A vacuum tube that is used either to amplify the + radio frequency currents or the audio frequency currents. + </p> + <p> + AMPLITUDE OF WAVE.--The greatest distance that a point moves from its + position of rest. + </p> + <p> + AMPLIFYING TRANSFORMER, AUDIO.--See <i>Transformer, Audio Amplifying</i>. + </p> + <p> + AMPLIFYING MODULATOR VACUUM TUBE.--See <i>Vacuum Tube, Amplifying + Modulator</i>. + </p> + <p> + AMPLIFYING TRANSFORMER RADIO.--See <i>Transformer, Radio Amplifying</i>. + </p> + <p> + ANTENNA, AMATEUR.--See <i>Aerial, Amateur</i>. + </p> + <p> + ANTENNA SWITCH.--See <i>Switch, Aerial</i>. + </p> + <p> + APPARATUS SYMBOLS.--See <i>Symbols, Apparatus</i>. + </p> + <p> + ARMSTRONG CIRCUIT.--See <i>Circuit, Armstrong</i>. + </p> + <p> + ATMOSPHERICS.--Same as <i>Static</i>, which see. + </p> + <p> + ATTENUATION.--In Sending wireless telegraph and telephone messages the + amplitude of the electric waves is damped out as the distance increases. + This is called <i>attenuation</i> and it increases as the frequency is + increased. This is the reason why short wave lengths will not carry as far + as long wave lengths. + </p> + <p> + AUDIO FREQUENCY AMPLIFIER.--See <i>Amplifier, Audio Frequency</i>. + </p> + <p> + AUDIO FREQUENCY AMPLIFICATION.--See <i>Amplification, Audio Frequency</i>. + </p> + <p> + AUDIBILITY METER.--See <i>Meter, Audibility</i>. + </p> + <p> + AUDIO FREQUENCY.--See <i>Frequency, Audio</i>. + </p> + <p> + AUDIO FREQUENCY CURRENT.--See <i>Current, Audio Frequency</i>. + </p> + <p> + AUDION.--An early trade name given to the vacuum tube detector. + </p> + <p> + AUTODYNE RECEPTOR.--See <i>Receptor, Autodyne</i>. + </p> + <p> + AUTO TRANSFORMER.--See <i>Transformer, Auto</i>. + </p> + <p> + BAKELITE.--A manufactured insulating compound. + </p> + <p> + B BATTERY.--See <i>Battery B</i>. + </p> + <p> + BAND, WAVE LENGTH.--See <i>Wave Length Band</i>. + </p> + <p> + BASKET WOUND COILS.--See <i>Coils, Inductance</i>. + </p> + <p> + BATTERY, A.--The 6-volt storage battery used to heat the filament of a + vacuum tube, detector or amplifier. + </p> + <p> + BATTERY, B.--The 22-1/2-volt dry cell battery used to energize the plate + of a vacuum tube detector or amplifier. + </p> + <p> + BATTERY, BOOSTER.--This is the battery that is connected in series with + the crystal detector. + </p> + <p> + BATTERY, C.--A small dry cell battery sometimes used to give the grid of a + vacuum tube detector a bias potential. + </p> + <p> + BATTERY, EDISON STORAGE.--A storage battery in which the elements are made + of nickel and iron and immersed in an alkaline <i>electrolyte</i>. + </p> + <p> + BATTERY, LEAD STORAGE.--A storage battery in which the elements are made + of lead and immersed in an acid electrolyte. + </p> + <p> + BATTERY POLES.--See <i>Poles, Battery</i>. + </p> + <p> + BATTERY, PRIMARY.--A battery that generates current by chemical action. + </p> + <p> + BATTERY, STORAGE.--A battery that develops a current after it has been + charged. + </p> + <p> + BEAT RECEPTION.--See <i>Heterodyne Reception</i>. + </p> + <p> + BED SPRINGS AERIAL.--See <i>Aerial, Bed Springs</i>. + </p> + <p> + BLUB BLUB.--Over modulation in wireless telephony. + </p> + <p> + BROAD WAVE.--See <i>Wave, Broad</i>. + </p> + <p> + BRUSH DISCHARGE.--See <i>Discharge</i>. + </p> + <p> + BUZZER MODULATION.--See <i>Modulation, Buzzer</i>. + </p> + <p> + BLUE GLOW DISCHARGE.--See <i>Discharge</i>. + </p> + <p> + BOOSTER BATTERY.--See <i>Battery, Booster</i>. + </p> + <p> + BROADCASTING.--Sending out intelligence and music from a central station + for the benefit of all who live within range of it and who have receiving + sets. + </p> + <p> + CAPACITANCE.--Also called by the older name of <i>capacity</i>. The + capacity of a condenser, inductance coil or other device capable of + retaining a charge of electricity. Capacitance is measured in terms of the + <i>microfarad</i>. + </p> + <p> + CAPACITIVE COUPLING.--See <i>Coupling, Capacitive</i>. + </p> + <p> + CAPACITY.--Any object that will retain a charge of electricity; hence an + aerial wire, a condenser or a metal plate is sometimes called a <i>capacity</i>. + </p> + <p> + CAPACITY, AERIAL.--The amount to which an aerial wire system can be + charged. The <i>capacitance</i> of a small amateur aerial is from 0.0002 + to 0.0005 microfarad. + </p> + <p> + CAPACITY, DISTRIBUTED.--A coil of wire not only has inductance, but also a + certain small capacitance. Coils wound with their turns parallel and + having a number of layers have a <i>bunched capacitance</i> which produces + untoward effects in oscillation circuits. In honeycomb and other stagger + wound coils the capacitance is more evenly distributed. + </p> + <p> + CAPACITY REACTANCE.--See <i>Reactance, Capacity</i>. + </p> + <p> + CAPACITY UNIT.--See <i>Farad</i>. + </p> + <p> + CARBON RHEOSTATS.--See <i>Rheostat, Carbon</i>. + </p> + <p> + CARBORUNDUM DETECTOR.--See <i>Detector</i>. + </p> + <p> + CARRIER CURRENT TELEPHONY.--See <i>Wired-Wireless</i>. + </p> + <p> + CARRIER FREQUENCY.--See <i>Frequency, Carrier</i>. + </p> + <p> + CARRIER FREQUENCY TELEPHONY.--See <i>Wired-Wireless</i>. + </p> + <p> + CASCADE AMPLIFICATION.--Two or more amplifying tubes hooked up in a + receiving set. + </p> + <p> + CAT WHISKER CONTACT.--A long, thin wire which makes contact with the + crystal of a detector. + </p> + <p> + CENTIMETER OF CAPACITANCE.--Equal to 1.11 <i>microfarads</i>. + </p> + <p> + CENTIMETER OF INDUCTANCE.--Equal to one one-thousandth part of a <i>microhenry</i>. + </p> + <p> + CELLULAR COILS.--See <i>Coils, Inductance</i>. + </p> + <p> + C.G.S. ELECTROSTATIC UNIT OF CAPACITANCE.--See <i>Centimeter of + Capacitance</i>. + </p> + <p> + CHARACTERISTICS.--The special behavior of a device, such as an aerial, a + detector tube, etc. + </p> + <p> + CHARACTERISTICS, GRID.--See <i>Grid Characteristics</i>. + </p> + <p> + CHOKE COILS.--Coils that prevent the high voltage oscillations from + surging back into the transformer and breaking down the insulation. + </p> + <p> + CHOPPER MODULATION.--See <i>Modulation, Chopper</i>. + </p> + <p> + CIRCUIT.--Any electrical conductor through which a current can flow. A low + voltage current requires a loop of wire or other conductor both ends of + which are connected to the source of current before it can flow. A high + frequency current will surge in a wire which is open at both ends like the + aerial. + </p> + <ul> + <li> + <i>Closed Circuit</i>.--A circuit that is continuous. + </li> + <li> + <i>Open Circuit</i>.--A conductor that is not continuous. + </li> + <li> + <i>Coupled Circuits</i>.--Open and closed circuits connected together by + inductance coils, condensers or resistances. See <i>coupling</i>. + </li> + <li> + <i>Close Coupled Circuits</i>.--Open and closed circuits connected + directly together with a single inductance coil. + </li> + <li> + <i>Loose Coupled Circuits</i>.--Opened and closed currents connected + together inductively by means of a transformer. + </li> + <li> + <i>Stand-by Circuits</i>.--Also called <i>pick-up</i> circuits. When + listening-in for possible calls from a number of stations, a receiver is + used which will respond to a wide band of wave lengths. + </li> + <li> + <i>Armstrong Circuits</i>.--The regenerative circuit invented by Major + E. H. Armstrong. + </li> + </ul> + <p> + CLOSE COUPLED CIRCUITS.--See <i>Currents, Close Coupled</i>. + </p> + <p> + CLOSED CIRCUIT.--See <i>Circuit, Closed</i>. + </p> + <p> + CLOSED CORE TRANSFORMER.--See <i>Transformer, Closed Core</i>. + </p> + <p> + CODE.-- + </p> + <ul> + <li> + <i>Continental</i>.--Same as <i>International</i>. + </li> + <li> + <i>International</i>.--On the continent of Europe land lines use the <i>Continental + Morse</i> alphabetic code. This code has come to be used throughout the + world for wireless telegraphy and hence it is now called the <i>International + code</i>. It is given on Page <i>305</i>. [Appendix: International Morse + Code]. + </li> + <li> + <i>Morse</i>.--The code devised by Samuel F. B. Morse and which is used + on the land lines in the U. S. + </li> + <li> + <i>National Electric</i>.--A set of rules and requirements devised by + the <i>National Board of Fire Underwriters</i> for the electrical + installations in buildings on which insurance companies carry risks. + This code also covers the requirements for wireless installations. A + copy may be had from the <i>National Board of Fire Underwriters</i>, New + York City, or from your insurance agent. + </li> + <li> + <i>National Electric Safety</i>.--<i>The Bureau of Standards</i>, + Washington, D. C., have investigated the precautions which should be + taken for the safe operation of all electric equipment. A copy of the <i>Bureau + of Standards Handbook No. 3</i> can be had for 40 cents from the <i>Superintendent + of Documents</i>. + </li> + </ul> + <p> + COEFFICIENT OF COUPLING.--See <i>Coupling, Coefficient of</i>. + </p> + <p> + COIL AERIAL.--See <i>Aerial, Loop</i>. + </p> + <p> + COIL ANTENNA.--See <i>Aerial, Loop</i>. + </p> + <p> + COIL, INDUCTION.--An apparatus for changing low voltage direct currents + into high voltage, low frequency alternating currents. When fitted with a + spark gap the high voltage, low frequency currents are converted into high + voltage, high frequency currents. It is then also called a <i>spark coil</i> + and a <i>Ruhmkorff coil</i>. + </p> + <p> + COIL, LOADING.--A coil connected in the aerial or closed oscillation + circuit so that longer wave lengths can be received. + </p> + <p> + COIL, REPEATING.--See <i>Repeating Coil</i>. + </p> + <p> + COIL, ROTATING.--One which rotates on a shaft instead of sliding as in a + <i>loose coupler</i>. The rotor of a <i>variometer</i> or <i>variocoupler</i> + is a <i>rotating coil</i>. + </p> + <p> + COILS, INDUCTANCE.--These are the tuning coils used for sending and + receiving sets. For sending sets they are formed of one and two coils, a + single sending coil is generally called a <i>tuning inductance coil</i>, + while a two-coil tuner is called an <i>oscillation transformer</i>. + Receiving tuning coils are made with a single layer, single coil, or a + pair of coils, when it is called an oscillation <i>transformer</i>. Some + tuning inductance coils have more than one layer, they are then called <i>lattice + wound</i>, <i>cellular</i>, <i>basket wound</i>, <i>honeycomb</i>, <i>duo-lateral</i>, + <i>stagger wound</i>, <i>spider-web</i> and <i>slab</i> coils. + </p> + <p> + COMMERCIAL FREQUENCY.--See <i>Frequency, Commercial</i>. + </p> + <p> + CONDENSER, AERIAL SERIES.--A condenser placed in the aerial wire system to + cut down the wave length. + </p> + <p> + CONDENSER, VERNIER.--A small variable condenser used for receiving + continuous waves where very sharp tuning is desired. + </p> + <p> + CONDENSER.--All conducting objects with their insulation form capacities, + but a <i>condenser</i> is understood to mean two sheets or plates of metal + placed closely together but separated by some insulating material. + </p> + <ul> + <li> + <i>Adjustable Condenser</i>.--Where two or more condensers can be + coupled together by means of plugs, switches or other devices. + </li> + <li> + <i>Aerial Condenser</i>.--A condenser connected in the aerial. + </li> + <li> + <i>Air Condenser</i>.--Where air only separates the sheets of metal. + </li> + <li> + <i>By-Pass Condenser</i>.--A condenser connected in the transmitting + currents so that the high frequency currents cannot flow back through + the power circuit. + </li> + <li> + <i>Filter Condenser</i>.--A condenser of large capacitance used in + combination with a filter reactor for smoothing out the pulsating direct + currents as they come from the rectifier. + </li> + <li> + <i>Fixed Condenser</i>.--Where the plates are fixed relatively to one + another. + </li> + <li> + <i>Grid Condenser</i>.--A condenser connected in series with the grid + lead. + </li> + <li> + <i>Leyden Jar Condenser</i>.--Where glass jars are used. + </li> + <li> + <i>Mica Condenser</i>.--Where mica is used. + </li> + <li> + <i>Oil Condenser</i>.--Where the plates are immersed in oil. + </li> + <li> + <i>Paper Condenser</i>.--Where paper is used as the insulating material. + </li> + <li> + <i>Protective</i>.--A condenser of large capacity connected across the + low voltage supply circuit of a transmitter to form a by-path of + kick-back oscillations. + </li> + <li> + <i>Variable Condenser</i>.--Where alternate plates can be moved and so + made to interleave more or less with a set of fixed plates. + </li> + <li> + <i>Vernier</i>.--A small condenser with a vernier on it so that it can + be very accurately varied. It is connected in parallel with the variable + condenser used in the primary circuit and is used for the reception of + continuous waves where sharp tuning is essential. + </li> + </ul> + <p> + CONDENSITE.--A manufactured insulating compound. + </p> + <p> + CONDUCTIVITY.--The conductance of a given length of wire of uniform cross + section. The reciprocal of <i>resistivity</i>. + </p> + <p> + CONTACT DETECTORS.--See <i>Detectors, Contact</i>. + </p> + <p> + CONTINENTAL CODE.--See <i>Code, Continental</i>. + </p> + <p> + COULOMB.--The quantity of electricity transferred by a current of 1 ampere + in 1 second. + </p> + <p> + CONVECTIVE DISCHARGE.--See <i>Discharge</i>. + </p> + <p> + CONVENTIONAL SIGNALS.--See <i>Signals, Conventional</i>. + </p> + <p> + COUNTER ELECTROMOTIVE FORCE.--See <i>Electromotive Force, Counter</i>. + </p> + <p> + COUNTERPOISE. A duplicate of the aerial wire that is raised a few feet + above the earth and insulated from it. Usually no connection is made with + the earth itself. + </p> + <p> + COUPLED CIRCUITS.--See <i>Circuit, Coupled</i>. + </p> + <p> + COUPLING.--When two oscillation circuits are connected together either by + the magnetic field of an inductance coil, or by the electrostatic field of + a condenser. + </p> + <p> + COUPLING, CAPACITIVE.--Oscillation circuits when connected together by + condensers instead of inductance coils. + </p> + <p> + COUPLING, COEFFICIENT OF.--The measure of the closeness of the coupling + between two coils. + </p> + <p> + COUPLING, INDUCTIVE.--Oscillation circuits when connected together by + inductance coils. + </p> + <p> + COUPLING, RESISTANCE.--Oscillation circuits connected together by a + resistance. + </p> + <p> + CRYSTAL RECTIFIER.--A crystal detector. + </p> + <p> + CURRENT, ALTERNATING (<i>A.C.</i>).--A low frequency current that surges + to and fro in a circuit. + </p> + <p> + CURRENT, AUDIO FREQUENCY.--A current whose frequency is low enough to be + heard in a telephone receiver. Such a current usually has a frequency of + between 200 and 2,000 cycles per second. + </p> + <p> + CURRENT, PLATE.--The current which flows between the filament and the + plate of a vacuum tube. + </p> + <p> + CURRENT, PULSATING.--A direct current whose voltage varies from moment to + moment. + </p> + <p> + CURRENT, RADIO FREQUENCY.--A current whose frequency is so high it cannot + be heard in a telephone receiver. Such a current may have a frequency of + from 20,000 to 10,000,000 per second. + </p> + <p> + CURRENTS, HIGH FREQUENCY.--(1) Currents that oscillate from 10,000 to + 300,000,000 times per second. (2) Electric oscillations. + </p> + <p> + CURRENTS, HIGH POTENTIAL.--(1) Currents that have a potential of more than + 10,000 volts. (2) High voltage currents. + </p> + <p> + CYCLE.--(1) A series of changes which when completed are again at the + starting point. (2) A period of time at the end of which an alternating or + oscillating current repeats its original direction of flow. + </p> + <p> + DAMPING.--The degree to which the energy of an electric oscillation is + reduced. In an open circuit the energy of an oscillation set up by a spark + gap is damped out in a few swings, while in a closed circuit it is greatly + prolonged, the current oscillating 20 times or more before the energy is + dissipated by the sum of the resistances of the circuit. + </p> + <p> + DECREMENT.--The act or process of gradually becoming less. + </p> + <p> + DETECTOR.--Any device that will (1) change the oscillations set up by the + incoming waves into direct current, that is which will rectify them, or + (2) that will act as a relay. + </p> + <ul> + <li> + <i>Carborundum</i>.--One that uses a <i>carborundum</i> crystal for the + sensitive element. Carborundum is a crystalline silicon carbide formed + in the electric furnace. + </li> + <li> + <i>Cat Whisker Contact</i>.--See <i>Cat Whisker Contact</i>. + </li> + <li> + <i>Chalcopyrite</i>.--Copper pyrites. A brass colored mineral used as a + crystal for detectors. See <i>Zincite</i>. + </li> + <li> + <i>Contact</i>.--A crystal detector. Any kind of a detector in which two + dissimilar but suitable solids make contact. + </li> + <li> + <i>Ferron</i>.--A detector in which iron pyrites are used as the + sensitive element. + </li> + <li> + <i>Galena</i>.--A detector that uses a galena crystal for the rectifying + element. + </li> + <li> + <i>Iron Pyrites</i>.--A detector that uses a crystal of iron pyrites for + its sensitive element. + </li> + <li> + <i>Molybdenite</i>.--A detector that uses a crystal of <i>sulphide of + molybdenum</i> for the sensitive element. + </li> + <li> + <i>Perikon</i>.--A detector in which a <i>bornite</i> crystal makes + contact with a <i>zincite</i> crystal. + </li> + <li> + <i>Silicon</i>.--A detector that uses a crystal of silicon for its + sensitive element. + </li> + <li> + <i>Vacuum Tube</i>.--A vacuum tube (which see) used as a detector. + </li> + <li> + <i>Zincite</i>.--A detector in which a crystal of <i>zincite</i> is used + as the sensitive element. + </li> + </ul> + <p> + DE TUNING.--A method of signaling by sustained oscillations in which the + key when pressed down cuts out either some of the inductance or some of + the capacity and hence greatly changes the wave length. + </p> + <p> + DIELECTRIC.--An insulating material between two electrically charged + plates in which there is set up an <i>electric strain</i>, or + displacement. + </p> + <p> + DIELECTRIC STRAIN.--The electric displacement in a dielectric. + </p> + <p> + DIRECTIONAL AERIAL.--See <i>Aerial, Directional</i>. + </p> + <p> + DIRECTION FINDER.--See <i>Aerial, Loop</i>. + </p> + <p> + DISCHARGE.--(1) A faintly luminous discharge that takes place from the + positive pointed terminal of an induction coil, or other high potential + apparatus; is termed a <i>brush discharge</i>. (2) A continuous discharge + between the terminals of a high potential apparatus is termed a <i>convective + discharge</i>. (3) The sudden breaking-down of the air between the balls + forming the spark gap is termed a <i>disruptive discharge</i>; also called + an <i>electric spark</i>, or just <i>spark</i> for short. (4) When a tube + has a poor vacuum, or too large a battery voltage, it glows with a blue + light and this is called a <i>blue glow discharge</i>. + </p> + <p> + DISRUPTIVE DISCHARGE.--See <i>Discharge</i>. + </p> + <p> + DISTRESS CALL. [Morse code:] ...---... (SOS). + </p> + <p> + DISTRIBUTED CAPACITY.--See <i>Capacity, Distributed</i>. + </p> + <p> + DOUBLE HUMP RESONANCE CURVE.--A resonance curve that has two peaks or + humps which show that the oscillating currents which are set up when the + primary and secondary of a tuning coil are closely coupled have two + frequencies. + </p> + <p> + DUO-LATERAL COILS.--See <i>Coils, Inductance</i>. + </p> + <p> + DUPLEX COMMUNICATION.--A wireless telephone system with which it is + possible to talk between both stations in either direction without the use + of switches. This is known as the <i>duplex system</i>. + </p> + <p> + EARTH CAPACITY.--An aerial counterpoise. + </p> + <p> + EARTH CONNECTION.--Metal plates or wires buried in the ground or immersed + in water. Any kind of means by which the sending and receiving apparatus + can be connected with the earth. + </p> + <p> + EDISON STORAGE BATTERY.--See <i>Storage Battery, Edison</i>. + </p> + <p> + ELECTRIC ENERGY.--The power of an electric current. + </p> + <p> + ELECTRIC OSCILLATIONS.--See <i>Oscillations, Electric</i>. + </p> + <p> + ELECTRIC SPARK.--See <i>Discharge, Spark</i>. + </p> + <p> + ELECTRICITY, NEGATIVE.--The opposite of <i>positive electricity</i>. + Negative electricity is formed of negative electrons which make up the + outside particles of an atom. + </p> + <p> + ELECTRICITY, POSITIVE.--The opposite of <i>negative electricity</i>. + Positive electricity is formed of positive electrons which make up the + inside particles of an atom. + </p> + <p> + ELECTRODES.--Usually the parts of an apparatus which dip into a liquid and + carry a current. The electrodes of a dry battery are the zinc and carbon + elements. The electrodes of an Edison storage battery are the iron and + nickel elements, and the electrodes of a lead storage battery are the lead + elements. + </p> + <p> + ELECTROLYTES.--The acid or alkaline solutions used in batteries. + </p> + <p> + ELECTROMAGNETIC WAVES.--See <i>Waves, Electric</i>. + </p> + <p> + ELECTROMOTIVE FORCE.--Abbreviated <i>emf</i>. The force that drives an + electric current along a conductor. Also loosely called <i>voltage</i>. + </p> + <p> + ELECTROMOTIVE FORCE, COUNTER.--The emf. that is set up in a direction + opposite to that in which the current is flowing in a conductor. + </p> + <p> + ELECTRON.--(1) A negative particle of electricity that is detached from an + atom. (2) A negative particle of electricity thrown off from the + incandescent filament of a vacuum tube. + </p> + <p> + ELECTRON FLOW.--The passage of electrons between the incandescent filament + and the cold positively charged plate of a vacuum tube. + </p> + <p> + ELECTRON RELAY.--See <i>Relay, Electron</i>. + </p> + <p> + ELECTRON TUBE.--A vacuum tube or a gas-content tube used for any purpose + in wireless work. See <i>Vacuum Tube</i>. + </p> + <p> + ELECTROSE INSULATORS.--Insulators made of a composition material the trade + name of which is <i>Electrose</i>. + </p> + <p> + ENERGY, ELECTRIC.--See <i>Electric Energy</i>. + </p> + <p> + ENERGY UNIT.--The <i>joule</i>, which see, <i>Page 308</i> [Appendix: + Definitions of Electric and Magnetic Units]. + </p> + <p> + FADING.--The sudden variation in strength of signals received from a + transmitting station when all the adjustments of both sending and + receiving apparatus remain the same. Also called <i>swinging</i>. + </p> + <p> + FARAD.--The capacitance of a condenser in which a potential difference of + 1 volt causes it to have a charge of 1 coulomb of electricity. + </p> + <p> + FEED-BACK ACTION.--Feeding back the oscillating currents in a vacuum tube + to amplify its power. Also called <i>regenerative action</i>. + </p> + <p> + FERROMAGNETIC CONTROL.--See <i>Magnetic Amplifier</i>. + </p> + <p> + FILAMENT.--The wire in a vacuum tube that is heated to incandescence and + which throws off electrons. + </p> + <p> + FILAMENT RHEOSTAT.--See <i>Rheostat, Filament</i>. + </p> + <p> + FILTER.--Inductance coils or condensers or both which (1) prevent + troublesome voltages from acting on the different circuits, and (2) smooth + out alternating currents after they have been rectified. + </p> + <p> + FILTER REACTOR.--See <i>Reactor, Filter</i>. + </p> + <p> + FIRE UNDERWRITERS.--See <i>Code, National Electric</i>. + </p> + <p> + FIXED GAP.--See <i>Gap</i>. + </p> + <p> + FLEMING VALVE.--A two-electrode vacuum tube. + </p> + <p> + FORCED OSCILLATIONS.--See <i>Oscillations, Forced</i>. + </p> + <p> + FREE OSCILLATIONS.--See <i>Oscillations, Free</i>. + </p> + <p> + FREQUENCY, AUDIO.--(1) An alternating current whose frequency is low + enough to operate a telephone receiver and, hence, which can be heard by + the ear. (2) Audio frequencies are usually around 500 or 1,000 cycles per + second, but may be as low as 200 and as high as 10,000 cycles per second. + </p> + <ul> + <li> + <i>Carrier</i>.--A radio frequency wave modulated by an audio frequency + wave which results in setting of <i>three</i> radio frequency waves. The + principal radio frequency is called the carrier frequency, since it + carries or transmits the audio frequency wave. + </li> + <li> + <i>Commercial</i>.--(1) Alternating current that is used for commercial + purposes, namely, light, heat and power. (2) Commercial frequencies now + in general use are from 25 to 50 cycles per second. + </li> + <li> + <i>Natural</i>.--The pendulum and vibrating spring have a <i>natural + frequency</i> which depends on the size, material of which it is made, + and the friction which it has to overcome. Likewise an oscillation + circuit has a natural frequency which depends upon its <i>inductance</i>, + <i>capacitance</i> and <i>resistance</i>. + </li> + <li> + <i>Radio</i>.--(1) An oscillating current whose frequency is too high to + affect a telephone receiver and, hence, cannot be heard by the ear. (2) + Radio frequencies are usually between 20,000 and 2,000,000 cycles per + second but may be as low as 10,000 and as high as 300,000,000 cycles per + second. + </li> + <li> + <i>Spark.--</i>The number of sparks per second produced by the discharge + of a condenser. + </li> + </ul> + <p> + GAP, FIXED.--One with fixed electrodes. + </p> + <p> + GAP, NON-SYNCHRONOUS.--A rotary spark gap run by a separate motor which + may be widely different from that of the speed of the alternator. + </p> + <p> + GAP, QUENCHED.--(1) A spark gap for the impulse production of oscillating + currents. (2) This method can be likened to one where a spring is struck a + single sharp blow and then continues to set up vibrations. + </p> + <p> + GAP, ROTARY.--One having fixed and rotating electrodes. + </p> + <p> + GAP, SYNCHRONOUS.--A rotary spark gap run at the same speed as the + alternator which supplies the power transformer. Such a gap usually has as + many teeth as there are poles on the generator. Hence one spark occurs per + half cycle. + </p> + <p> + GAS-CONTENT TUBE.--See <i>Vacuum Tube.</i> + </p> + <p> + GENERATOR TUBE.--A vacuum tube used to set up oscillations. As a matter of + fact it does not <i>generate</i> oscillations, but changes the initial low + voltage current that flows through it into oscillations. Also called an <i>oscillator + tube</i> and a <i>power tube.</i> + </p> + <p> + GRID BATTERY.--See <i>Battery C.</i> + </p> + <p> + GRID CHARACTERISTICS.--The various relations that could exist between the + voltages and currents of the grid of a vacuum tube, and the values which + do exist between them when the tube is in operation. These characteristics + are generally shown by curves. + </p> + <p> + GRID CONDENSER.--See <i>Condenser, Grid.</i> + </p> + <p> + GRID LEAK.--A high resistance unit connected in the grid lead of both + sending and receiving sets. In a sending set it keeps the voltage of the + grid at a constant value and so controls the output of the aerial. In a + receiving set it controls the current flowing between the plate and + filament. + </p> + <p> + GRID MODULATION.--See <i>Modulation, Grid.</i> + </p> + <p> + GRID POTENTIAL.--The negative or positive voltage of the grid of a vacuum + tube. + </p> + <p> + GRID VOLTAGE.--See <i>Grid Potential.</i> + </p> + <p> + GRINDERS.--The most common form of <i>Static,</i> which see. They make a + grinding noise in the headphones. + </p> + <p> + GROUND.--See <i>Earth Connection.</i> + </p> + <p> + GROUND, AMATEUR.--A water-pipe ground. + </p> + <p> + GROUND, WATERPIPE.--A common method of grounding by amateurs is to use the + waterpipe, gaspipe or radiator. + </p> + <p> + GUIDED WAVE TELEPHONY.--See <i>Wired Wireless.</i> + </p> + <p> + HARD TUBE.--A vacuum tube in which the vacuum is <i>high,</i> that is, + exhausted to a high degree. + </p> + <p> + HELIX.--(1) Any coil of wire. (2) Specifically a transmitter tuning + inductance coil. + </p> + <p> + HENRY.--The inductance in a circuit in which the electromotive force + induced is 1 volt when the inducing current varies at the rate of 1 ampere + per second. + </p> + <p> + HETERODYNE RECEPTION.--(1) Receiving by the <i>beat</i> method. (2) + Receiving by means of superposing oscillations generated at the receiving + station on the oscillations set up in the aerial by the incoming waves. + </p> + <p> + HETERODYNE RECEPTOR.--See <i>Receptor, Heterodyne.</i> + </p> + <p> + HIGH FREQUENCY CURRENTS.--See <i>Currents, High Frequency.</i> + </p> + <p> + HIGH FREQUENCY RESISTANCE.--See <i>Resistance, High Frequency.</i> + </p> + <p> + HIGH POTENTIAL CURRENTS.--See <i>Currents, High Potential.</i> + </p> + <p> + HIGH VOLTAGE CURRENTS.--See <i>Currents, High Potential.</i> + </p> + <p> + HONEYCOMB COILS.--See <i>Coils, Inductance.</i> + </p> + <p> + HORSE-POWER.--Used in rating steam machinery. It is equal to 746 watts. + </p> + <p> + HOT WIRE AMMETER.--See <i>Ammeter, Hot Wire.</i> + </p> + <p> + HOWLING.--Where more than three stages of radio amplification, or more + than two stages of audio amplification, are used howling noises are apt to + occur in the telephone receivers. + </p> + <p> + IMPEDANCE.--An oscillation circuit has <i>reactance</i> and also <i>resistance,</i> + and when these are combined the total opposition to the current is called + <i>impedance.</i> + </p> + <p> + INDUCTANCE COILS.--See <i>Coils, Inductance.</i> + </p> + <p> + INDUCTANCE COIL, LOADING.--See <i>Coil, Loading Inductance.</i> + </p> + <p> + INDUCTIVE COUPLING.--See <i>Coupling, Inductive.</i> + </p> + <p> + INDUCTIVE REACTANCE.--See <i>Reactance, Inductive.</i> + </p> + <p> + INDUCTION COIL.--See <i>Coil, Induction.</i> + </p> + <p> + INDUCTION, MUTUAL.--Induction produced between two circuits or coils close + to each other by the mutual interaction of their magnetic fields. + </p> + <p> + INSULATION.--Materials used on and around wires and other conductors to + keep the current from leaking away. + </p> + <p> + INSPECTOR, RADIO.--A U. S. inspector whose business it is to issue both + station and operators' licenses in the district of which he is in charge. + </p> + <p> + INTERFERENCE.--The crossing or superposing of two sets of electric waves + of the same or slightly different lengths which tend to oppose each other. + It is the untoward interference between electric waves from different + stations that makes selective signaling so difficult a problem. + </p> + <p> + INTERMEDIATE WAVES.--See <i>Waves.</i> + </p> + <p> + IONIC TUBES.--See <i>Vacuum Tubes.</i> + </p> + <p> + INTERNATIONAL CODE.--See Code, International. + </p> + <p> + JAMMING.--Waves that are of such length and strength that when they + interfere with incoming waves they drown them out. + </p> + <p> + JOULE.--The energy spent in 1 second by a flow of 1 ampere in 1 ohm. + </p> + <p> + JOULE'S LAW.--The relation between the heat produced in seconds to the + resistance of the circuit, to the current flowing in it. + </p> + <p> + KENOTRON.--The trade name of a vacuum tube rectifier made by the <i>Radio + Corporation of America.</i> + </p> + <p> + KICK-BACK.--Oscillating currents that rise in voltage and tend to flow + back through the circuit that is supplying the transmitter with low + voltage current. + </p> + <p> + KICK-BACK PREVENTION.--See <i>Prevention, Kick-Back.</i> + </p> + <p> + KILOWATT.--1,000 watts. + </p> + <p> + LAMBDA.--See <i>Pages 301, 302.</i> [Appendix: Useful Abbreviations]. + </p> + <p> + LATTICE WOUND COILS.--See <i>Coils, Inductance.</i> + </p> + <p> + LIGHTNING SWITCH.--See <i>Switch, Lightning.</i> + </p> + <p> + LINE RADIO COMMUNICATION.--See <i>Wired Wireless.</i> + </p> + <p> + LINE RADIO TELEPHONY.--See <i>Telephony, Line Radio.</i> + </p> + <p> + LITZENDRAHT.--A conductor formed of a number of fine copper wires either + twisted or braided together. It is used to reduce the <i>skin effect.</i> + See <i>Resistance, High Frequency.</i> + </p> + <p> + LOAD FLICKER.--The flickering of electric lights on lines that supply + wireless transmitting sets due to variations of the voltage on opening and + closing the key. + </p> + <p> + LOADING COIL.--See <i>Coil, Loading.</i> + </p> + <p> + LONG WAVES.--See <i>Waves.</i> + </p> + <p> + LOOP AERIAL.--See <i>Aerial, Loop.</i> + </p> + <p> + LOOSE COUPLED CIRCUITS.--See <i>Circuits, Loose Coupled.</i> + </p> + <p> + LOUD SPEAKER.--A telephone receiver connected to a horn, or a specially + made one, that reproduces the incoming signals, words or music loud enough + to be heard by a room or an auditorium full of people, or by large crowds + out-doors. + </p> + <p> + MAGNETIC POLES.--See <i>Poles, Magnetic.</i> + </p> + <p> + MEGOHM.--One million ohms. + </p> + <p> + METER, AUDIBILITY.--An instrument for measuring the loudness of a signal + by comparison with another signal. It consists of a pair of headphones and + a variable resistance which have been calibrated. + </p> + <p> + MHO.--The unit of conductance. As conductance is the reciprocal of + resistance it is measured by the <i>reciprocal ohm</i> or <i>mho.</i> + </p> + <p> + MICA.--A transparent mineral having a high insulating value and which can + be split into very thin sheets. It is largely used in making condensers + both for transmitting and receiving sets. + </p> + <p> + MICROFARAD.--The millionth part of a <i>farad.</i> + </p> + <p> + MICROHENRY.--The millionth part of a <i>farad.</i> + </p> + <p> + MICROMICROFARAD.--The millionth part of a <i>microfarad.</i> + </p> + <p> + MICROHM.--The millionth part of an <i>ohm.</i> + </p> + <p> + MICROPHONE TRANSFORMER.--See <i>Transformer, Microphone.</i> + </p> + <p> + MICROPHONE TRANSMITTER.--See <i>Transmitter, Microphone.</i> + </p> + <p> + MILLI-AMMETER.--An ammeter that measures a current by the one-thousandth + of an ampere. + </p> + <p> + MODULATION.--(1) Inflection or varying the voice. (2) Varying the + amplitude of oscillations by means of the voice. + </p> + <p> + MODULATION, BUZZER.--The modulation of radio frequency oscillations by a + buzzer which breaks up the sustained oscillations of a transmitter into + audio frequency impulses. + </p> + <p> + MILLIHENRY.--The thousandth part of a <i>henry.</i> + </p> + <p> + MODULATION, CHOPPER.--The modulation of radio frequency oscillations by a + chopper which breaks up the sustained oscillations of a transmitter into + audio frequency impulses. + </p> + <p> + MODULATION, GRID.--The scheme of modulating an oscillator tube by + connecting the secondary of a transformer, the primary of which is + connected with a battery and a microphone transmitter, in the grid lead. + </p> + <p> + MODULATION, OVER.--See <i>Blub Blub.</i> + </p> + <p> + MODULATION, PLATE.--Modulating the oscillations set up by a vacuum tube by + varying the current impressed on the plate. + </p> + <p> + MODULATOR TUBE.--A vacuum tube used as a modulator. + </p> + <p> + MOTION, WAVE.--(1) The to and fro motion of water at sea. (2) Waves + transmitted by, in and through the air, or sound waves. (3) Waves + transmitted by, in and through the <i>ether,</i> or <i>electromagnetic + waves,</i> or <i>electric waves</i> for short. + </p> + <p> + MOTOR-GENERATOR.--A motor and a dynamo built to run at the same speed and + mounted on a common base, the shafts being coupled together. In wireless + it is used for changing commercial direct current into direct current of + higher voltages for energizing the plate of a vacuum tube oscillator. + </p> + <p> + MULTI-STAGE AMPLIFIERS.--See <i>Amplifiers, Multi-Stage.</i> + </p> + <p> + MUTUAL INDUCTION.--See <i>Induction, Mutual.</i> + </p> + <p> + MUSH.--Irregular intermediate frequencies set up by arc transmitters which + interfere with the fundamental wave lengths. + </p> + <p> + MUSHY NOTE.--A note that is not clear cut, and hence hard to read, which + is received by the <i>heterodyne method</i> when damped waves or modulated + continuous waves are being received. + </p> + <p> + NATIONAL ELECTRIC CODE.--See <i>Code, National Electric.</i> + </p> + <p> + NATIONAL ELECTRIC SAFETY CODE.--See <i>Code, National Electric Safety.</i> + </p> + <p> + NEGATIVE ELECTRICITY.--See <i>Electricity, Negative.</i> + </p> + <p> + NON-SYNCHRONOUS GAP.--See <i>Gap, Non-Synchronous.</i> + </p> + <p> + OHM.--The resistance of a thread of mercury at the temperature of melting + ice, 14.4521 grams in mass, of uniform cross-section and a length of + 106.300 centimeters. + </p> + <p> + OHM'S LAW.--The important fixed relation between the electric current, its + electromotive force and the resistance of the conductor in which it flows. + </p> + <p> + OPEN CIRCUIT.--See <i>Circuit, Open.</i> + </p> + <p> + OPEN CORE TRANSFORMER.--See <i>Transformer, Open Core.</i> + </p> + <p> + OSCILLATION TRANSFORMER.--See <i>Transformer, Oscillation.</i> + </p> + <p> + OSCILLATIONS, ELECTRIC.--A current of high frequency that surges through + an open or a closed circuit. (1) Electric oscillations may be set up by a + spark gap, electric arc or a vacuum tube, when they have not only a high + frequency but a high potential, or voltage. (2) When electric waves + impinge on an aerial wire they are transformed into electric oscillations + of a frequency equal to those which emitted the waves, but since a very + small amount of energy is received their potential or voltage is likewise + very small. + </p> + <ul> + <li> + <i>Sustained.--</i>Oscillations in which the damping factor is small. + </li> + <li> + <i>Damped.--</i>Oscillations in which the damping factor is large. + </li> + <li> + <i>Free.--</i>When a condenser discharges through an oscillation + circuit, where there is no outside electromotive force acting on it, the + oscillations are said to be <i>free.</i> + </li> + <li> + <i>Forced.--</i>Oscillations that are made to surge in a circuit whose + natural period is different from that of the oscillations set up in it. + </li> + </ul> + <p> + OSCILLATION TRANSFORMER.--See <i>Transformer.</i> + </p> + <p> + OSCILLATION VALVE.--See <i>Vacuum Tube.</i> + </p> + <p> + OSCILLATOR TUBE.--A vacuum tube which is used to produce electric + oscillations. + </p> + <p> + OVER MODULATION.--See <i>Blub Blub.</i> + </p> + <p> + PANCAKE OSCILLATION TRANSFORMER.--Disk-shaped coils that are used for + receiving tuning inductances. + </p> + <p> + PERMEABILITY, MAGNETIC.--The degree to which a substance can be + magnetized. Iron has a greater magnetic permeability than air. + </p> + <p> + PHASE.--A characteristic aspect or appearance that takes place at the same + point or part of a cycle. + </p> + <p> + PICK-UP CIRCUITS.--See <i>Circuits, Stand-by.</i> + </p> + <p> + PLATE CIRCUIT REACTOR.--See <i>Reactor, Plate Circuit.</i> + </p> + <p> + PLATE CURRENT.--See <i>Current, Plate.</i> + </p> + <p> + PLATE MODULATION.--See <i>Modulation, Plate.</i> + </p> + <p> + PLATE VOLTAGE.--See <i>Foliage, Plate.</i> + </p> + <p> + POLES, BATTERY.--The positive and negative terminals of the elements of a + battery. On a storage battery these poles are marked + and - respectively. + </p> + <p> + POLES, MAGNETIC.--The ends of a magnet. + </p> + <p> + POSITIVE ELECTRICITY.--See <i>Electricity, Positive.</i> + </p> + <p> + POTENTIAL DIFFERENCE.--The electric pressure between two charged + conductors or surfaces. + </p> + <p> + POTENTIOMETER.--A variable resistance used for subdividing the voltage of + a current. A <i>voltage divider.</i> + </p> + <p> + POWER TRANSFORMER.--See <i>Transformer, Power.</i> + </p> + <p> + POWER TUBE.--See <i>Generator Tube.</i> + </p> + <p> + PRIMARY BATTERY.--See <i>Battery, Primary.</i> + </p> + <p> + PREVENTION, KICK-BACK.--A choke coil placed in the power circuit to + prevent the high frequency currents from getting into the transformer and + breaking down the insulation. + </p> + <p> + Q S T.--An abbreviation used in wireless communication for (1) the + question "Have you received the general call?" and (2) the notice, + "General call to all stations." + </p> + <p> + QUENCHED GAP.--See <i>Gap, Quenched.</i> + </p> + <p> + RADIATION.--The emission, or throwing off, of electric waves by an aerial + wire system. + </p> + <p> + RADIO AMMETER.--See <i>Ammeter, Hot Wire.</i> + </p> + <p> + RADIO FREQUENCY.--See <i>Frequency, Radio.</i> + </p> + <p> + RADIO FREQUENCY AMPLIFICATION.--See <i>Amplification, Radio Frequency.</i> + </p> + <p> + RADIO FREQUENCY CURRENT.--See <i>Current, Radio Frequency.</i> + </p> + <p> + RADIO INSPECTOR.--See <i>Inspector, Radio</i>. + </p> + <p> + RADIOTRON.--The trade name of vacuum tube detectors, amplifiers, + oscillators and modulators made by the <i>Radio Corporation of America</i>. + </p> + <p> + RADIO WAVES.--See <i>Waves, Radio</i>. + </p> + <p> + REACTANCE.--When a circuit has inductance and the current changes in + value, it is opposed by the voltage induced by the variation of the + current. + </p> + <p> + REACTANCE, CAPACITY.--The capacity reactance is the opposition offered to + a current by a capacity. It is measured as a resistance, that is, in <i>ohms</i>. + </p> + <p> + RECEIVING TUNING COILS.--See <i>Coils, Inductance</i>. + </p> + <p> + RECEIVER, LOUD SPEAKING.--See <i>Loud Speakers</i>. + </p> + <p> + RECEIVER, WATCH CASE.--A compact telephone receiver used for wireless + reception. + </p> + <p> + REACTANCE, INDUCTIVE.--The inductive reactance is the opposition offered + to the current by an inductance coil. It is measured as a resistance, that + is, in <i>ohms</i>. + </p> + <p> + REACTOR, FILTER.--A reactance coil for smoothing out the pulsating direct + currents as they come from the rectifier. + </p> + <p> + REACTOR, PLATE CIRCUIT.--A reactance coil used in the plate circuit of a + wireless telephone to keep the direct current supply at a constant + voltage. + </p> + <p> + RECEIVER.--(1) A telephone receiver. (2) An apparatus for receiving + signals, speech or music. (3) Better called a <i>receptor</i> to + distinguish it from a telephone receiver. + </p> + <p> + RECTIFIER.--(1) An apparatus for changing alternating current into + pulsating direct current. (2) Specifically in wireless (<i>a</i>) a + crystal or vacuum tube detector, and (<i>b</i>) a two-electrode vacuum + tube used for changing commercial alternating current into direct current + for wireless telephony. + </p> + <p> + REGENERATIVE AMPLIFICATION.--See <i>Amplification, Regenerative</i>. + </p> + <p> + RECEPTOR.--A receiving set. + </p> + <p> + RECEPTOR, AUTODYNE.--A receptor that has a regenerative circuit and the + same tube is used as a detector and as a generator of local oscillations. + </p> + <p> + RECEPTOR, BEAT.--A heterodyne receptor. + </p> + <p> + RECEPTOR, HETERODYNE.--A receiving set that uses a separate vacuum tube to + set up the second series of waves for beat reception. + </p> + <p> + REGENERATIVE ACTION.--See <i>Feed-Back Action.</i> + </p> + <p> + REGENERATIVE AMPLIFICATION.--See <i>Amplification, Regenerative.</i> + </p> + <p> + RELAY, ELECTRON.--A vacuum tube when used as a detector or an amplifier. + </p> + <p> + REPEATING COIL.--A transformer used in connecting up a wireless receiver + with a wire transmitter. + </p> + <p> + RESISTANCE.--The opposition offered by a wire or other conductor to the + passage of a current. + </p> + <p> + RESISTANCE, AERIAL.--The resistance of the aerial wire to oscillating + currents. This is greater than its ordinary ohmic resistance due to the + skin effect. See <i>Resistance, High Frequency.</i> + </p> + <p> + RESISTANCE BOX.--See <i>Resistor.</i> + </p> + <p> + RESISTANCE COUPLING.--See <i>Coupling, Resistance.</i> + </p> + <p> + RESISTANCE, HIGH FREQUENCY.--When a high frequency current oscillates on a + wire two things take place that are different than when a direct or + alternating current flows through it, and these are (1) the current inside + of the wire lags behind that of the current on the surface, and (2) the + amplitude of the current is largest on the surface and grows smaller as + the center of the wire is reached. This uneven distribution of the current + is known as the <i>skin effect</i> and it amounts to the same thing as + reducing the size of the wire, hence the resistance is increased. + </p> + <p> + RESISTIVITY.--The resistance of a given length of wire of uniform cross + section. The reciprocal of <i>conductivity.</i> + </p> + <p> + RESISTOR.--A fixed or variable resistance unit or a group of such units. + Variable resistors are also called <i>resistance boxes</i> and more often + <i>rheostats.</i> + </p> + <p> + RESONANCE.--(1) Simple resonance of sound is its increase set up by one + body by the sympathetic vibration of a second body. (2) By extension the + increase in the amplitude of electric oscillations when the circuit in + which they surge has a <i>natural</i> period that is the same, or nearly + the same, as the period of the first oscillation circuit. + </p> + <p> + RHEOSTAT.--A variable resistance unit. See <i>Resistor.</i> + </p> + <p> + RHEOSTAT, CARBON.--A carbon rod, or carbon plates or blocks, when used as + variable resistances. + </p> + <p> + RHEOSTAT, FILAMENT.--A variable resistance used for keeping the current of + the storage battery which heats the filament of a vacuum tube at a + constant voltage. + </p> + <p> + ROTATING COIL.--See <i>Coil.</i> + </p> + <p> + ROTARY GAP.--See <i>Gap.</i> + </p> + <p> + ROTOR.--The rotating coil of a variometer or a variocoupler. + </p> + <p> + RUHMKORFF COIL.--See <i>Coil, Induction.</i> + </p> + <p> + SATURATION.--The maximum plate current that a vacuum tube will take. + </p> + <p> + SENSITIVE SPOTS.--Spots on detector crystals that are sensitive to the + action of electric oscillations. + </p> + <p> + SHORT WAVES.--See <i>Waves.</i> + </p> + <p> + SIDE WAVES.--See <i>Wave Length Band.</i> + </p> + <p> + SIGNALS, CONVENTIONAL.--(1) The International Morse alphabet and numeral + code, punctuation marks, and a few important abbreviations used in + wireless telegraphy. (2) Dot and dash signals for distress call, + invitation to transmit, etc. Now used for all general public service + wireless communication. + </p> + <p> + SKIN EFFECT.--See <i>Resistance, High Frequency.</i> + </p> + <p> + SOFT TUBE.--A vacuum tube in which the vacuum is low, that is, it is not + highly exhausted. + </p> + <p> + SPACE CHARGE EFFECT.--The electric field intensity due to the pressure of + the negative electrons in the space between the filament and plate which + at last equals and neutralizes that due to the positive potential of the + plate so that there is no force acting on the electrons near the filament. + </p> + <p> + SPARK.--See <i>Discharge.</i> + </p> + <p> + SPARK COIL.--See <i>Coil, Induction.</i> + </p> + <p> + SPARK DISCHARGE.--See <i>Spark, Electric.</i> + </p> + <p> + SPARK FREQUENCY.--See <i>Frequency, Spark.</i> + </p> + <p> + SPARK GAP.--(1) A <i>spark gap,</i> without the hyphen, means the + apparatus in which sparks take place; it is also called a <i>spark + discharger.</i> (2) <i>Spark-gap,</i> with the hyphen, means the air-gap + between the opposed faces of the electrodes in which sparks are produced. + </p> + <ul> + <li> + <i>Plain.--</i>A spark gap with fixed electrodes. + </li> + <li> + <i>Rotary.--</i>A spark gap with a pair of fixed electrodes and a number + of electrodes mounted on a rotating element. + </li> + <li> + <i>Quenched.--</i>A spark gap formed of a number of metal plates placed + closely together and insulated from each other. + </li> + </ul> + <p> + SPIDER WEB INDUCTANCE COIL.--See <i>Coil, Spider Web Inductance.</i> + </p> + <p> + SPREADER.--A stick of wood, or spar, that holds the wires of the aerial + apart. + </p> + <p> + STAGGER WOUND COILS.--See <i>Coils, Inductance.</i> + </p> + <p> + STAND-BY CIRCUITS.--See <i>Circuits, Stand-By.</i> + </p> + <p> + STATIC.--Also called <i>atmospherics, grinders, strays, X's,</i> and, when + bad enough, by other names. It is an electrical disturbance in the + atmosphere which makes noises in the telephone receiver. + </p> + <p> + STATOR.--The fixed or stationary coil of a variometer or a variocoupler. + </p> + <p> + STORAGE BATTERY.--See <i>Battery, Storage.</i> + </p> + <p> + STRAY ELIMINATION.--A method for increasing the strength of the signals as + against the strength of the strays. See <i>Static.</i> + </p> + <p> + STRAYS.--See <i>Static</i>. + </p> + <p> + STRANDED WIRE.--See <i>Wire, Stranded</i>. + </p> + <p> + SUPER-HETERODYNE RECEPTOR.--See <i>Heterodyne, Super</i>. + </p> + <p> + SWINGING.--See <i>Fading</i>. + </p> + <p> + SWITCH, AERIAL.--A switch used to change over from the sending to the + receiving set, and the other way about, and connect them with the aerial. + </p> + <p> + SWITCH, LIGHTNING.--The switch that connects the aerial with the outside + ground when the apparatus is not in use. + </p> + <p> + SYMBOLS, APPARATUS.--Also called <i>conventional symbols</i>. These are + diagrammatic lines representing various parts of apparatus so that when a + wiring diagram of a transmitter or a receptor is to be made it is only + necessary to connect them together. They are easy to make and easy to + read. See <i>Page 307</i> [Appendix: Symbols Used for Apparatus]. + </p> + <p> + SYNCHRONOUS GAP.--See <i>Gap, Synchronous</i>. + </p> + <p> + TELEPHONY, LINE RADIO.--See <i>Wired Wireless</i>. + </p> + <p> + THERMAL AMMETER.--See <i>Ammeter, Hot Wire</i>. + </p> + <p> + THREE ELECTRODE VACUUM TUBE.--<i>See Vacuum Tube, Three Electrode</i>. + </p> + <p> + TIKKER.--A slipping contact device that breaks up the sustained + oscillations at the receiving end into groups so that the signals can be + heard in the head phones. The device usually consists of a fine steel or + gold wire slipping in the smooth groove of a rotating brass wheel. + </p> + <p> + TRANSFORMER.--A primary and a secondary coil for stepping up or down a + primary alternating or oscillating current. + </p> + <ul> + <li> + <i>A. C.</i>--See <i>Power Transformer</i>. + </li> + <li> + <i>Air Cooled</i>.--A transformer in which the coils are exposed to the + air. + </li> + <li> + <i>Air Core</i>.--With high frequency currents it is the general + practice not to use iron cores as these tend to choke off the + oscillations. Hence the core consists of the air inside of the coils. + </li> + <li> + <i>Auto.--</i>A single coil of wire in which one part forms the primary + and the other part the secondary by bringing out an intermediate tap. + </li> + <li> + <i>Audio Amplifying.--</i>This is a transformer with an iron core and is + used for frequencies up to say 3,000. + </li> + <li> + <i>Closed Core.--</i>A transformer in which the path of the magnetic + flux is entirely through iron. Power transformers have closed cores. + </li> + <li> + <i>Microphone.--</i>A small transformer for modulating the oscillations + set up by an arc or a vacuum tube oscillator. + </li> + <li> + <i>Oil Cooled.--</i>A transformer in which the coils are immersed in + oil. + </li> + <li> + <i>Open Core.--</i>A transformer in which the path of the magnetic flux + is partly through iron and partly through air. Induction coils have open + cores. + </li> + <li> + <i>Oscillation.--</i>A coil or coils for transforming or stepping down + or up oscillating currents. Oscillation transformers usually have no + iron cores when they are also called <i>air core transformers.</i> + </li> + <li> + <i>Power.--</i>A transformer for stepping down a commercial alternating + current for lighting and heating the filament and for stepping up the + commercial a.c., for charging the plate of a vacuum tube oscillator. + </li> + <li> + <i>Radio Amplifying.--</i>This is a transformer with an air core. It + does not in itself amplify but is so called because it is used in + connection with an amplifying tube. + </li> + </ul> + <p> + TRANSMITTER, MICROPHONE.--A telephone transmitter of the kind that is used + in the Bell telephone system. + </p> + <p> + TRANSMITTING TUNING COILS.--See <i>Coils, Inductance.</i> + </p> + <p> + TUNING.--When the open and closed oscillation circuits of a transmitter or + a receptor are adjusted so that both of the former will permit electric + oscillations to surge through them with the same frequency, they are said + to be tuned. Likewise, when the sending and receiving stations are + adjusted to the same wave length they are said to be <i>tuned.</i> + </p> + <ul> + <li> + <i>Coarse Tuning.--</i>The first adjustment in the tuning oscillation + circuits of a receptor is made with the inductance coil and this tunes + them coarse, or roughly. + </li> + <li> + <i>Fine Tuning.--</i>After the oscillation circuits have been roughly + tuned with the inductance coil the exact adjustment is obtained with the + variable condenser and this is <i>fine tuning.</i> + </li> + <li> + <i>Sharp.--</i>When a sending set will transmit or a receiving set will + receive a wave of given length only it is said to be sharply tuned. The + smaller the decrement the sharper the tuning. + </li> + </ul> + <p> + TUNING COILS.--See <i>Coils, Inductance.</i> + </p> + <p> + TWO ELECTRODE VACUUM TUBE.--See <i>Vacuum Tube, Two Electrode.</i> + </p> + <p> + VACUUM TUBE.--A tube with two or three electrodes from which the air has + been exhausted, or which is filled with an inert gas, and used as a + detector, an amplifier, an oscillator or a modulator in wireless + telegraphy and telephony. + </p> + <ul> + <li> + <i>Amplifier.--</i>See <i>Amplifier, Vacuum Tube.</i> + </li> + <li> + <i>Amplifying Modulator.--</i>A vacuum tube used for modulating and + amplifying the oscillations set up by the sending set. + </li> + <li> + <i>Gas Content.--</i>A tube made like a vacuum tube and used as a + detector but which contains an inert gas instead of being exhausted. + </li> + <li> + <i>Hard.--</i>See <i>Hard Tube.</i> + </li> + <li> + <i>Rectifier.--</i>(1) A vacuum tube detector. (2) a two-electrode + vacuum tube used for changing commercial alternating current into direct + current for wireless telephony. + </li> + <li> + <i>Soft.--</i>See <i>Soft Tube.</i> + </li> + <li> + <i>Three Electrode.--</i>A vacuum tube with three electrodes, namely a + filament, a grid and a plate. + </li> + <li> + <i>Two Electrode.--</i>A vacuum tube with two electrodes, namely the + filament and the plate. + </li> + </ul> + <p> + VALVE.--See <i>Vacuum Tube.</i> + </p> + <p> + VALVE, FLEMING.--See <i>Fleming Valve.</i> + </p> + <p> + VARIABLE CONDENSER.--See <i>Condenser, Variable.</i> + </p> + <p> + VARIABLE INDUCTANCE.--See <i>Inductance, Variable.</i> + </p> + <p> + VARIABLE RESISTANCE.--See <i>Resistance, Variable.</i> + </p> + <p> + VARIOCOUPLER.--A tuning device for varying the inductance of the receiving + oscillation circuits. It consists of a fixed and a rotatable coil whose + windings are not connected with each other. + </p> + <p> + VARIOMETER.--A tuning device for varying the inductance of the receiving + oscillation currents. It consists of a fixed and a rotatable coil with the + coils connected in series. + </p> + <p> + VERNIER CONDENSER.--See <i>Condenser, Vernier.</i> + </p> + <p> + VOLT.--The electromotive force which produces a current of 1 ampere when + steadily applied to a conductor the resistance of which is one ohm. + </p> + <p> + VOLTAGE DIVIDER.--See <i>Potentiometer.</i> + </p> + <p> + VOLTAGE, PLATE.--The voltage of the current that is used to energize the + plate of a vacuum tube. + </p> + <p> + VOLTMETER.--An instrument for measuring the voltage of an electric + current. + </p> + <p> + WATCH CASE RECEIVER.--See <i>Receiver, Watch Case.</i> + </p> + <p> + WATER-PIPE GROUND.--See <i>Ground, Water-Pipe.</i> + </p> + <p> + WATT.--The power spent by a current of 1 ampere in a resistance of 1 ohm. + </p> + <p> + WAVE, BROAD.--A wave having a high decrement, when the strength of the + signals is nearly the same over a wide range of wave lengths. + </p> + <p> + WAVE LENGTH.--Every wave of whatever kind has a length. The wave length is + usually taken to mean the distance between the crests of two successive + waves. + </p> + <p> + WAVE LENGTH BAND.--In wireless reception when continuous waves are being + sent out and these are modulated by a microphone transmitter the different + audio frequencies set up corresponding radio frequencies and the energy of + these are emitted by the aerial; this results in waves of different + lengths, or a band of waves as it is called. + </p> + <p> + WAVE METER.--An apparatus for measuring the lengths of electric waves set + up in the oscillation circuits of sending and receiving sets. + </p> + <p> + WAVE MOTION.--Disturbances set up in the surrounding medium as water waves + in and on the water, sound waves in the air and electric waves in the + ether. + </p> + <p> + WAVES.--See <i>Wave Motion</i>. + </p> + <p> + WAVES, ELECTRIC.--Electromagnetic waves set up in and transmitted by and + through the ether. + </p> + <ul> + <li> + <i>Continuous</i>. <i>Abbreviated C.W.</i>--Waves that are emitted + without a break from the aerial. Also called <i>undamped waves</i>. + </li> + <li> + <i>Discontinuous</i>.--Waves that are emitted periodically from the + aerial. Also called <i>damped waves</i>. <i>Damped</i>.--See <i>Discontinuous + Waves</i>. + </li> + <li> + <i>Intermediate</i>.--Waves from 600 to 2,000 meters in length. + </li> + <li> + <i>Long</i>.--Waves over 2,000 meters in length. <i>Radio</i>.--Electric + waves used in wireless telegraphy and telephony. + </li> + <li> + <i>Short</i>.--Waves up to 600 meters in length. + </li> + <li> + <i>Wireless</i>.--Electric waves used in wireless telegraphy and + telephony. + </li> + <li> + <i>Undamped</i>.--See <i>Continuous Waves</i>. + </li> + </ul> + <p> + WIRELESS TELEGRAPH CODE.--See <i>Code, International</i>. + </p> + <p> + WIRE, ENAMELLED.--Wire that is given a thin coat of enamel which insulates + it. + </p> + <p> + WIRE, PHOSPHOR BRONZE.--A very strong wire made of an alloy of copper and + containing a trace of phosphorus. + </p> + <p> + WIRED WIRELESS.--Continuous waves of high frequency that are sent over + telephone wires instead of through space. Also called <i>line radio + communication; carrier frequency telephony, carrier current telephony; + guided wave telephony</i> and <i>wired wireless.</i> + </p> + <p> + X'S.--See <i>Static.</i> + </p> + <p> + ZINCITE.--See <i>Detector.</i> + </p> + <h2> + <a name="donts" id="donts">WIRELESS DON'TS</a> + </h2> + <h3> + AERIAL WIRE DON'TS + </h3> + <p> + <i>Don't</i> use iron wire for your aerial. + </p> + <p> + <i>Don't</i> fail to insulate it well at both ends. + </p> + <p> + <i>Don't</i> have it longer than 75 feet for sending out a 200-meter wave. + </p> + <p> + <i>Don't</i> fail to use a lightning arrester, or better, a lightning + switch, for your receiving set. + </p> + <p> + <i>Don't</i> fail to use a lightning switch with your transmitting set. + </p> + <p> + <i>Don't</i> forget you must have an outside ground. + </p> + <p> + <i>Don't</i> fail to have the resistance of your aerial as small as + possible. Use stranded wire. + </p> + <p> + <i>Don't</i> fail to solder the leading-in wire to the aerial. + </p> + <p> + <i>Don't</i> fail to properly insulate the leading-in wire where it goes + through the window or wall. + </p> + <p> + <i>Don't</i> let your aerial or leading-in wire touch trees or other + objects. + </p> + <p> + <i>Don't</i> let your aerial come too close to overhead wires of any kind. + </p> + <p> + <i>Don't</i> run your aerial directly under, or over, or parallel with + electric light or other wires. + </p> + <p> + <i>Don't</i> fail to make a good ground connection with the water pipe + inside. + </p> + <h3> + TRANSMITTING DON'TS + </h3> + <p> + <i>Don't</i> attempt to send until you get your license. + </p> + <p> + <i>Don't</i> fail to live up to every rule and regulation. + </p> + <p> + <i>Don't</i> use an input of more than 1/2 a kilowatt if you live within 5 + nautical miles of a naval station. + </p> + <p> + <i>Don't</i> send on more than a 200-meter wave if you have a restricted + or general amateur license. + </p> + <p> + <i>Don't</i> use spark gap electrodes that are too small or they will get + hot. + </p> + <p> + <i>Don't</i> use too long or too short a spark gap. The right length can + be found by trying it out. + </p> + <p> + <i>Don't</i> fail to use a safety spark gap between the grid and the + filament terminals where the plate potential is above 2,000 volts. + </p> + <p> + <i>Don't</i> buy a motor-generator set if you have commercial alternating + current in your home. + </p> + <p> + <i>Don't</i> overload an oscillation vacuum tube as it will greatly + shorten its life. Use two in parallel. + </p> + <p> + <i>Don't</i> operate a transmitting set without a hot-wire ammeter in the + aerial. + </p> + <p> + <i>Don't</i> use solid wire for connecting up the parts of transmitters. + Use stranded or braided wire. + </p> + <p> + <i>Don't</i> fail to solder each connection. + </p> + <p> + <i>Don't</i> use soldering fluid, use rosin. + </p> + <p> + <i>Don't</i> think that all of the energy of an oscillation tube cannot be + used for wave lengths of 200 meters and under. It can be if the + transmitting set and aerial are properly designed. + </p> + <p> + <i>Don't</i> run the wires of oscillation circuits too close together. + </p> + <p> + <i>Don't</i> cross the wires of oscillation circuits except at right + angles. + </p> + <p> + <i>Don't</i> set the transformer of a transmitting set nearer than 3 feet + to the condenser and tuning coil. + </p> + <p> + <i>Don't</i> use a rotary gap in which the wheel runs out of true. + </p> + <h3> + RECEIVING DON'TS + </h3> + <p> + <i>Don't</i> expect to get as good results with a crystal detector as with + a vacuum tube detector. + </p> + <p> + <i>Don't</i> be discouraged if you fail to hit the sensitive spot of a + crystal detector the first time--or several times thereafter. + </p> + <p> + <i>Don't</i> use a wire larger than <i>No. 80</i> for the wire electrode + of a crystal detector. + </p> + <p> + <i>Don't</i> try to use a loud speaker with a crystal detector receiving + set. + </p> + <p> + <i>Don't</i> expect a loop aerial to give worthwhile results with a + crystal detector. + </p> + <p> + <i>Don't</i> handle crystals with your fingers as this destroys their + sensitivity. Use tweezers or a cloth. + </p> + <p> + <i>Don't</i> imbed the crystal in solder as the heat destroys its + sensitivity. Use <i>Wood's metal,</i> or some other alloy which melts at + or near the temperature of boiling water. + </p> + <p> + <i>Don't</i> forget that strong static and strong signals sometimes + destroy the sensitivity of crystals. + </p> + <p> + <i>Don't</i> heat the filament of a vacuum tube to greater brilliancy than + is necessary to secure the sensitiveness required. + </p> + <p> + <i>Don't</i> use a plate voltage that is less or more than it is rated + for. + </p> + <p> + <i>Don't</i> connect the filament to a lighting circuit. + </p> + <p> + <i>Don't</i> use dry cells for heating the filament except in a pinch. + </p> + <p> + <i>Don't</i> use a constant current to heat the filament, use a constant + voltage. + </p> + <p> + <i>Don't</i> use a vacuum tube in a horizontal position unless it is made + to be so used. + </p> + <p> + <i>Don't</i> fail to properly insulate the grid and plate leads. + </p> + <p> + <i>Don't</i> use more than 1/3 of the rated voltage on the filament and on + the plate when trying it out for the first time. + </p> + <p> + <i>Don't</i> fail to use alternating current for heating the filament + where this is possible. + </p> + <p> + <i>Don't</i> fail to use a voltmeter to find the proper temperature of the + filament. + </p> + <p> + <i>Don't</i> expect to get results with a loud speaker when using a single + vacuum tube. + </p> + <p> + <i>Don't</i> fail to protect your vacuum tubes from mechanical shocks and + vibration. + </p> + <p> + <i>Don't</i> fail to cut off the <i>A</i> battery entirely from the + filament when you are through receiving. + </p> + <p> + <i>Don't</i> switch on the <i>A</i> battery current all at once through + the filament when you start to receive. + </p> + <p> + <i>Don't</i> expect to get the best results with a gas-content detector + tube without using a potentiometer. + </p> + <p> + <i>Don't</i> connect a potentiometer across the <i>B</i> battery or it + will speedily run down. + </p> + <p> + <i>Don't</i> expect to get as good results with a single coil tuner as you + would with a loose coupler. + </p> + <p> + <i>Don't</i> expect to get as good results with a two-coil tuner as with + one having a third, or <i>tickler</i>, coil. + </p> + <p> + <i>Don't</i> think you have to use a regenerative circuit, that is, one + with a tickler coil, to receive with a vacuum tube detector. + </p> + <p> + <i>Don't</i> think you are the only amateur who is troubled with static. + </p> + <p> + <i>Don't</i> expect to eliminate interference if the amateurs around you + are sending with spark sets. + </p> + <p> + <i>Don't</i> lay out or assemble your set on a panel first. Connect it up + on a board and find out if everything is right. + </p> + <p> + <i>Don't</i> try to connect up your set without a wiring diagram in front + of you. + </p> + <p> + <i>Don't</i> fail to shield radio frequency amplifiers. + </p> + <p> + <i>Don't</i> set the axes of the cores of radio frequency transformers in + a line. Set them at right angles to each other. + </p> + <p> + <i>Don't</i> use wire smaller than <i>No. 14</i> for connecting up the + various parts. + </p> + <p> + <i>Don't</i> fail to adjust the <i>B</i> battery after putting in a fresh + vacuum tube, as its sensitivity depends largely on the voltage. + </p> + <p> + <i>Don't</i> fail to properly space the parts where you use variometers. + </p> + <p> + <i>Don't</i> fail to put a copper shield between the variometer and the + variocoupler. + </p> + <p> + <i>Don't</i> fail to keep the leads to the vacuum tube as short as + possible. + </p> + <p> + <i>Don't</i> throw your receiving set out of the window if it <i>howls</i>. + Try placing the audio-frequency transformers farther apart and the cores + of them at right angles to each other. + </p> + <p> + <i>Don't</i> use condensers with paper dielectrics for an amplifier + receiving set or it will be noisy. + </p> + <p> + <i>Don't</i> expect as good results with a loop aerial, or when? using the + bed springs, as an out-door aerial will give you. + </p> + <p> + <i>Don't</i> use an amplifier having a plate potential of less than 100 + volts for the last step where a loud speaker is to be used. + </p> + <p> + <i>Don't</i> try to assemble a set if you don't know the difference + between a binding post and a blue print. Buy a set ready to use. + </p> + <p> + <i>Don't</i> expect to get Arlington time signals and the big cableless + stations if your receiver is made for short wave lengths. + </p> + <p> + <i>Don't</i> take your headphones apart. You are just as apt to spoil them + as you would a watch. + </p> + <p> + <i>Don't</i> expect to get results with a Bell telephone receiver. + </p> + <p> + <i>Don't</i> forget that there are other operators using the ether besides + yourself. + </p> + <p> + <i>Don't</i> let your <i>B</i> battery get damp and don't let it freeze. + </p> + <p> + <i>Don't</i> try to recharge your <i>B</i> battery unless it is + constructed for the purpose. + </p> + <h3> + STORAGE BATTERY DON'TS + </h3> + <p> + <i>Don't</i> connect a source of alternating current direct to your + storage battery. You have to use a rectifier. + </p> + <p> + <i>Don't</i> connect the positive lead of the charging circuit with the + negative terminal of your storage battery. + </p> + <p> + <i>Don't</i> let the electrolyte get lower than the tops of the plates of + your storage battery. + </p> + <p> + <i>Don't</i> fail to look after the condition of your storage battery once + in a while. + </p> + <p> + <i>Don't</i> buy a storage battery that gives less than 6 volts for + heating the filament. + </p> + <p> + <i>Don't</i> fail to keep the specific gravity of the electrolyte of your + storage battery between 1.225 and 1.300 Baume. This you can do with a + hydrometer. + </p> + <p> + <i>Don't</i> fail to recharge your storage battery when the hydrometer + shows that the specific gravity of the electrolyte is close to 1.225. + </p> + <p> + <i>Don't</i> keep charging the battery after the hydrometer shows that the + specific gravity is 1.285. + </p> + <p> + <i>Don't</i> let the storage battery freeze. + </p> + <p> + <i>Don't</i> let it stand for longer than a month without using unless you + charge it. + </p> + <p> + <i>Don't</i> monkey with the storage battery except to add a little + sulphuric acid to the electrolyte from time to time. If anything goes + wrong with it better take it to a service station and let the expert do + it. + </p> + <h3> + EXTRA DON'TS + </h3> + <p> + <i>Don't</i> think you have an up-to-date transmitting station unless you + are using C.W. + </p> + <p> + <i>Don't</i> use a wire from your lightning switch down to the outside + ground that is smaller than No. <i>4</i>. + </p> + <p> + <i>Don't</i> try to operate your spark coil with 110-volt direct lighting + current without connecting in a rheostat. + </p> + <p> + <i>Don't</i> try to operate your spark coil with 110-volt alternating + lighting current without connecting in an electrolytic interrupter. + </p> + <p> + <i>Don't</i> try to operate an alternating current power transformer with + 110-volt direct current without connecting in an electrolytic interruptor. + </p> + <p> + <i>Don't</i>--no never--connect one side of the spark gap to the aerial + wire and the other side of the spark gap to the ground. The Government + won't have it--that's all. + </p> + <p> + <i>Don't</i> try to tune your transmitter to send out waves of given + length by guesswork. Use a wavemeter. + </p> + <p> + <i>Don't</i> use <i>hard fiber</i> for panels. It is a very poor insulator + where high frequency currents are used. + </p> + <p> + <i>Don't</i> think you are the only one who doesn't know all about + wireless. Wireless is a very complex art and there are many things that + those experienced have still to learn. + </p> + <h3> + THE END. + </h3> + <p> + <br /> <br /> <br /> <br /> + </p> +<pre xml:space="preserve"> +*** END OF THE PROJECT GUTENBERG EBOOK, THE RADIO AMATEUR'S HAND BOOK *** + +This file should be named 6935-h.htm or 6935-h.zip + +Project Gutenberg eBooks are often created from several printed +editions, all of which are confirmed as Public Domain in the US +unless a copyright notice is included. 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