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February 9, 192J,
R A D I O D F G E S T — Illustrated
Simple Explanation of Radio for Everybody
Chapter X — Part II — Loud Speakers
By M. W. Thompson
THE following article is the twentieth of a series for Radio beginners, written by Marvin W. Thompson, well known in airphone circles for his understandable style of approaching his subject. The remaining chapters will be:
Chapter XI— Dry Cells and Storage
Batteries. Chapter XII — Radio Frequency Amplification.
THE perfect diaphragm, or one that would be sufficiently good for most of us, would have an intensity curve like that shown in Figure 78. For notes below 50, the efficiency would be gradually rising and it would reach maximum on notes around 100. The intensity line would be flat to notes around 5,900. after which it would drop to zero at 6,000. True, some of the higher harmonics of the upper fundamentals would be lost, but reproduction would be most satisfactory. Unfortunately, due to the increasingly di
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FREGIUENCY
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Figure 79 — The diaphragm response is usually as shown here, the natural period being at 990 cycles.
other means of setting the air in vibration is essential.
The small chamber behind the diaphragm receives but little consideration in most loud speakers, although it can play quite an important part in the faith
1000 2O0O "3000 4000 5000
FREQUENCY
Figure 78 — The efficiency curve of a perfect loud speaker would show equal response at all frequencies.
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vided response on higher notes, the curve for even the best present-day loud speakers looks much like Figure 79. The peak at about 990 is due to the natural frequency of the diaphragm; those at 2,500 and 5,000 are due to certain harmonics at which the diaphragm vibrates well. The intensity, for the reasons given above, falls off and there is a pleasure-wrecking weakness of the high notes and a flat shrillness to them due to the elimination of their harmonics. The elimination of the diaphragm with the necessary substitution of some
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The new Thordarson Power Amplifying Transformers (push pull) are designed for use as third stage audio frequency amplifiers, to provide high power amplification for operating loud speaking devices.
With power amplification, not only is it possible to increase volume, but, since two tubes replace the usual one, the distortion and howling which usually accompany the overloading of a single tube on the third stage is done away with entirely.
The Thordarson Power Amplifying Transformers are well constructed electrically and are capable of indefinitely carrying the additional load without breaking down.
In tonal purity these transformers equal the Thordarson Super Audio Frequency transformer whose rich quality and even amplification has made it the popular transformer of the day.
JhordarsoN
ELECT. MFG. CO.
fulness of the reproduction. It is, as a rule, air-tight, and the air within it must expand and contract with the diaphragm. This air has a natural resonant point. Both of these factors react on the diaphragm, adding more bumps to the reproduction curve, which mean distortion. The Horn Part This brings us to the horn. Contrary to the general impression, the amplifying action on sound waves is not due to the horn vibrating and acting as a sounding board. The effect of the horn is to
CLEAR RECEPTION ASSURED,
A Crosley brings in distant Stations Easily.
Listen to Crosley Broadcas ting Station WLW.
500 W. Huron St.
CHICAGO
"N^TO MATTER which Crosley Receiver you choose, you can be assured of unexcelled performance at the lowest price. The Model X-J has proven especially popular. With it, Stations in all parts of the United States and Canada may be clearly heard. Even Honolulu has been frequently brought in from the eastern seaboard.
Compare These Prices
Crosley Model VI — a Two Tube Set $ 30
Crosley Model X-J — a Four Tube Set $65
Crosley Model X-L — a Four Tube Consolette $140
Special Mahogany Stand for Model X-X, $25
For Sale by Good Dealers Everywhere.
Write for free Catalog.
The Crosley Radio Corporation
Powel Crosley, Jr., President
Formerly The Precision Equipment Company and Crosley Manufacturing Company
2492 Alfred St., CINCINNATI, OHIO
The largest Manufacturers of Radio Receivers hi the World
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reinforce the vibrations which enter it due to the resonance properties of the body of air inclosed by it. The quantity and quality of this resonance depends mainly upon the volume of the inclosed air and somewhat upon its shape. Con
nant to any of the frequencies found in the musical scale, is not completely d and lifeless.
Unusually rigid material, such as stone or thick metal or compositions mad' wood fiber, gives the best results. If the walls of the horn are smooth and rigid, they produce no appreciable effect upon the tone. If, on the other hand, they .ugh or flexible (resonant), they may absorb or rapidly dissipate the energy of of the air vibration
and thus, by subtraction of certain harmonic overtones, have a marked influence upon tone quality. This would inject depressions or valleys into our curve of Figure 79 and make it appear as in Figure 80. A resonant point on the 1,750 notes will give the depression noted at that point and also a marked weakening on the first multiple, or 3,500. Shape of the Horn
The shape of the horn also affects that which comes out. Every curve and corner, twist and surface on the inner side
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FREQUENCY
Figure 80 — Many horns dissipate energy at certain frequencies, causing dips in the curve
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sideration of the speakers on the market gives one some idea of the divergence of opinion on the subject. The aim is to produce a horn that, while it is not reso
changes the direction of the outpouring
waves. The flare of the horn has a great
influence upon the response; widening the
(Continued on page 2*6)
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