US234978A - Telephone - Google Patents

Description

J. GOODMAN. Telephope.

(No Model.)

No. 234,978. Patented Nov. 30,18-80 NVENTOR /6 mm,

@Q ATTORNEY JOHN GOODMAN, OF LOUISVILLE, KENTUCKY.

TELEPHONE.

SPECIFICATION forming part of Letters Patent No. 234,978, dated November 30, 1880,

, Application filed August 7, 1880.

To all whom it may concern:

Be it known that I, J OHN GOODMAN, of Louisville, in the county of J efl'erson and State of Kentucky, have invented a new and valuable Improvement in Telephones 5 and I do hereby declare that the following is a full, clear, and exact description of the construction and operation ofthe same, reference being had to the annexed drawings, making a part of this specificatiomand to the letters and figures of reference marked thereon.

Figure 1 of the drawings is a representation of a longitudinal section of telephone-receiver. Fig.2 is arepresentation of alongitudinal section taken at right angles to the first section. Fig. 3 is a representation of a cross-section.

This invention has relation to telephone-receivers; and it consists in the construction and novel arrangement, in combination, of a magnet or series of magnets and a flattened helix or coil of wire so related to each other that when a current of electricity is passed through the coil the magnet or magnets will have a tendency to assume a position at right angles to the direction of the current; and in connec- 'tion therewith it consists, also, of elastic devices exerting pressure on the magnets and tending to maintain them in a position approximating parallelism with the longitude of the helix, all as hereinafter shown and described.

In the accompanying drawings, the letterD represents the magnets, which, in this instance, are long and tongue-likein form, and are fastened at intervals, by one end, to the post H, which is located at the side of the case, near one end of the helix or helices O. In this construction two flattened helices are employed, their long sides being parallel with each other, and one being a left-hand, while the otheris a right-h and, helix. These helices are designed to affect the magnets situated between them in the same manner that a single coil would if it surrounded them, and asingle coil may therefore be employed with like effect. The magnets D extend between the coils O and parallel to the Wires thereof in the manner shown in the drawings, and the extremities of the magnets opposite to the post H are left free to move.

B indicates the resonator or sounding-diaphragm, made of thin metal or other suitable material.

(No model.)

A represents the ear-piece over the resonator, and E the cord extending from the resonator to the spring F, which is connected to the case at the opposite end from the resonator. The cord E is connected in its course to the middle portion of each of the magnets D, which are therefore, in a manner, strained or held in tension between two elastic devices-the resonator and the spring Fwhich tend to hold them parallel with the wires of the coils O. This tension may be regulated by means of an adjustable screw, G, to which the spring F is connected.

With this instrument sound is reproduced simply by variations in the force of the elec tric current, these variations varying from the full force thereof down to zero. If the instrument be applied to the ear and the circuit suddenly closed by metallic connections, the current in the coil will overcome the tension of the spring and the points of the magnets D will be deflected, and this movement being propagated to the diaphragm or resonator by means of the cord E, this diaphragm will be suddenly relaxed or retracted, (according to the direction of the current,) as if struck by a blow, and a short and sharp sound or click will be heard. If, however, one of the connections be a slightly-roughened surface and the other made of hard steel, when the latter is drawn slowly over the former a dull rasping sound will be heard; butif the passage of the one over the other be made by a quick movement the vibrations of the diaphragm will cause a continuous sound on a high key, resembling a shriek. These illustrations represent the extremes caused by making or breaking the circuit, and between them will be readily given forth by this instrument every degree of character and intensity of sound caused by the variations in the force of the current. Every variation in intonation and pitch in the sound depends upon the character and frequency of the vibrations of the diaphragm, and these, in turn, in this instrument, are due to variations in the force of the current which passes through the coils, by which the magnets are deflected.

In this instrument, instead of using two helices, a single coil may be employed and the magnet or magnets related to the external surface of one side of it; or the magnet or magnets may be placed within the coil longitudinally.

Instead of using an extraneous spring or elastic band to hold the magnets in parallel relation with the wires of the helices, the magnets themselves may be made in part flexible or elastic, so as to constitute asprin g and magnet in one piece.

When the magnets D are situated and restrained as above described, and a current of electricity is passed through the coils, the magnets will be deflected toward a position at right angles to thelength of the coils to an extent in proportion inversely to the strength of the springs and directly to the strength of the current. If the current is steady, the magnets will remain stationary at a point where the antagonizing forces exerted by the elastic pressure on the one hand and the electricity on the other are in cquilibrio but if the current be intermittent or variable in strength during the moments of its cessation or weakness, the elastic pressure will draw the magnets toward a parallelism with the conductor, and during its action or increment it will prevail over the elastic pressure and cause more or less departure of the magnets from this parallelism, thus throwing them into vibrations, which, if of proper frequency, and if imparted to a diaphragm or resonator, will produce sound.

In using this receiver any transmitter which varies the force of the electric current sufficiently will answer.

Having described this invention, what I claim, and desire to secure by Letters Patent,

1. In a telephonic receiver, the combination, with a helix or conductor and a vibratory magnet parallel therewith and tending to assume a position at right angles thereto when the conductor is electrified, of elastic connections designed to hold the magnets in a position approximating parallelism with the conductor, substantially as specified.

2. In a telephonic receiver, the combination, with the conductors or helices and the vibratory magnets arranged parallel therewith, of the resonator or diaphragm connected mechanically with the magnets, and the spring or elastic device tending to hold the magnets parallel with the helices and in strained connection with .the resonator, substantially as specified.

In testimony that I claim the abovel have hereunto subscribed my name in the presence of two witnesses.

JOHN GOODMAN.

Witnesses:

HAIDEN MILLER, GEORGE M. WARNER.

Images