US717513A - Method of relaying space-telegraph signals. - Google Patents
Method of relaying space-telegraph signals. Download PDFInfo
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- US717513A US717513A US4439601A US1901044396A US717513A US 717513 A US717513 A US 717513A US 4439601 A US4439601 A US 4439601A US 1901044396 A US1901044396 A US 1901044396A US 717513 A US717513 A US 717513A
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- Prior art keywords
- conductors
- receiver
- elevated
- transmitter
- vibrations
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- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04L—TRANSMISSION OF DIGITAL INFORMATION, e.g. TELEGRAPHIC COMMUNICATION
- H04L25/00—Baseband systems
- H04L25/02—Details ; arrangements for supplying electrical power along data transmission lines
- H04L25/20—Repeater circuits; Relay circuits
- H04L25/24—Relay circuits using discharge tubes or semiconductor devices
- H04L25/242—Relay circuits using discharge tubes or semiconductor devices with retiming
Definitions
- the invention relates to the art of signaling electrically between stations not connected by a conducting-wire, sometimes called space telegraphy, and more particularly to the type of space telegraphy in which the signals are transmitted by unguided electromagnetic waves.
- the object of the present invention is to provide a method whereby space-telegraph messages may be automatically relayed.
- This object I attain by providing two space-telegraph systems of the elevated-conductor type, each comprising a transmitter .and receiver, with a relay adapted to be set in motion by the receiver of one system, and thereby to operate the transmitter of the other system and by so disposing the elevated conductor or conductors of the receiver of the first system and of the transmitter of the second, respectively,
- the elevated conductors of the transmitter of the second system are so placed that the Waves emanating from them produce planes or lines of interference, and the elevated conductor or conductors of the receiver ofthe first system are placed in these lines or planes of interference and are thereby rendered incapable of being aected by the Waves which emanate from the elevated conductors of the transmitter of the second system.
- the disposition of the elevated conductors in planes or lines of interference is described and claimed in an application 4.000d by me contemporaneously herewith, Serial No. 44,393, renewed February 24E, 1902, Serial No. 95,198.
- the elevated conductors of the receiver of the first system are so disposed relatively to those of the transmitter of the second that the electromagnetic waves emanating from the latter produce equal electric vibrations in the sev eral elevated conductors of the former; but the relay, which is set in motion by the receiver of the first system and which by its motion operates the transmitter of the second, is so associated with the elevated conductors of the receiver of the first system that the effects of the several equal electric vibrations conveyed to it from that transmitter are opposed to each other, and their resultant effect upon the relay is ml.
- the disposition of the elevated conductors last referred to is described and claimed in anapplication iled by me contemporaneously herewith, Serial No. 44,398.
- Figure l is a diagram illustrative of a disposition of apparatus in which the elevated conductor V of the receiver of one system is placed in the plane of interference of the Wavesfrom two elevated conductors V' V" of the transmitter of another system.
- Fig. 2 is adiagram illustrative of the disposition oli'Y apparatus in which the two elevated conductors V V of the receiver of one system are so disposed as to have equal electric vibrations developed in them by the electromagnectic waves emanating from the vertical wire V of the transmitter of another system and in which the effects of these Vibrations are opposed to each other at a relay associated with said receiver of the irst system.
- V V V are vertically-elevated conductors
- M M M are induction coils or transformers
- C C C, dre., are condensers
- B B are batteries
- K is a coherer
- R is a relay
- p is an automatic circuit-interrupter
- s is a spark-gap
- k is a contact which is normally open, but which is closed when the relay Ris set in motion
- F. is an earth connection.
- the operation of the coil M, Figs. 1 and 2 produces a spark at the spark-gap s, and electrical oscillations result in the primary of the coil M", Fig. 1, and M, Fig. 2, by virtue of the condensers C3, Fig. l, and C, Fig. 2.
- the primary coils of M are equal in every respect and are symmetrically disposed relative t-o the two secondary coils of M.
- the electrical oscillations in the primary coils of M therefore induce equal and opposite electrical vibrations in the two conductors V and V of Fig. l,owing to the fact that the two secondary coils of M are wound in the same direction and form virtually a continuous coil grounded at its neutral point.
- the vertical wire V is connected to the ground at this neutral point, so that it is unaected by the iiow of current through the coil.
- the electrical oscillations in the primary coil M develop electric vibrations in theconductorV. Beingsymmetricallydisposed with reference to the two vertical conductors V' and V, the electrical vibrations in it induce equal electrical vibrations in V' and V", and these Vibrations traversing the primary coils of lV in opposite directions their effect upon the secondary coil M" is mi.
- the electromagnetic signal-waves to be relayed are received from a distant transmitting-station upon the elevated conductor V and develop therein electric vibrations. These vibrations are conveyed to the coherer K through the intermediary of the inductioncoil M and cause it to set in motion the relay R in a well-understood manner.
- the relay R thus set in motion closes the circuit of the battery B at 7c through the interrupter p and the primary of the induction or spark coil M.
- a high potential is thereby developed in the secondary of the spark-coil M', and a series of sparks occur at the spark-gap s.
- Oscillations are thereby developed in the circuit containing the condenser C and the primary of the induction coil M", which in turn develop equal and opposite electric vibrations in the vertical conductors V and V.
- tric vibrations are equal and opposite, because the two halves of the secondary of M are equal, and the primary of M" is symmetrically disposed with respect to these two halves of the secondary.
- a decoherer restores the coherer to its normal state.
- the electromagnetic waves emanating from the two vertical conductors V Vll of the transmitter of the second system do not affect the vertical conductor V of the receiver of the first system, because the two conductors V V" are similar.
- the two oscillations developed in them are equal in amplitude and opposite in phase, and the vertical conductor V is symmetrically disposed with respect to V and V"-t'. e., it is in the plane of interference of the Waves which emanate from V' and V.
- the electromagnetic signal-waves to be relayed are received from a distant transmitting-station upon the elevated conductors Vl and V, which are in a plane approximately that including the distant transmitting-station and are preferably at a distance apart equal to one halt ⁇ a complete wave length of the electromagnetic waves to be received.
- the electric vibrations developed in the two conductors V and V will be equal in amplitude and opposite in phase.
- These vibrations are conveyed to the coherer K through the intermediary of the induction-coil or transformer lV and cause it to operate or set in motion the relay R in the usual manner.
- the relay R operates to close the circuit of the battery B at 7o through the interrupter p and the primary of the induction or spark coil M.
- a high potential is thereby induced in the secondary of M', and a rapid succession of sparks pass at the spark-gap at s, causing a highfrequency oscillation in the primary of the induction-coil M, and thereby developing high-frequency electric vibrations in the vertical wire V.
- a decoherer restores the coherer to its normal con- 'Ihe electromagnetic waves emanating from the vertical wire Vproduce equal electric vibrations in V and V; but owing to the fact that the two halves of the primary of the coil M are equal and symmetrically disposed with respect to the secondary these vibrations passing through the two halves of the primary in opposite directions have no resultant effect upon the coherer K, and therefore upon the relay R.
- the elevated conductor of either the transmitter or receiver, or both may be multiple.
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- Power Engineering (AREA)
- Computer Networks & Wireless Communication (AREA)
- Signal Processing (AREA)
- Train Traffic Observation, Control, And Security (AREA)
Description
No. 7|7,5|3. Patented nec. so', 1,902. J. s. sToNE.
` METHOD 0F RELAYING SPACE TELEGRAPH SIGNALS.
' (Application led Jan. 28', 1901;) (No Modei.)
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UNiTEE STATES PATENT OEEicE. e
JOI-IN STONE STONE, OF BOSTON, MASSACHUSETTS, ASSIGNOR TO LOUIS E. WI-IIOI-IER, ALEXANDER P. BROWNE, AND BRAINERD T. JUDKINS,
TRUSTEES.
METHOD OF RELAYING SPACE-TELEGRAPH SIGNALS.
SPECIFICATION forming part of Letters Patent No. 717,513, dated December 30, 1902.
Application filed January 23, 1901. Serial No. 44,396. (No model.)
T0 all whom t may concern.-
Be it known that I, JOHN STONE STONE, a citizen of the United States, residing at Boston,in the county of Suffolk and State of Massachusetts, have invented certain new and useful Improvements in Methods of Relaying Space-Telegraph Signals, of which the following is a specification.
The invention relates to the art of signaling electrically between stations not connected by a conducting-wire, sometimes called space telegraphy, and more particularly to the type of space telegraphy in which the signals are transmitted by unguided electromagnetic waves.
The distance to which it is at present practicable to signal by electromagnetic waves is limited to distances considerably less than those easily communicated over by the ordinary `telegraph and telephone of to-day. It is of the greatest importance, therefore, that suitable methods and means for automatically relaying space-telegraph signals be discovered and devised. So far as I am aware no method or apparatus for automatically relaying space-telegraph signals has heretofore been disclosed except such as depend for such efficiency as they may possess upon the use of a metallic screen as a material shield or barrier against the passage of the electromagnetic waves. Without considering in this connection the practical efficiency of such means,it seems suiiicient to point out that the present invention does not involve the idea of any material shield or barrier, but rather an electrical organization of the apparatus whereby the desired result may be Obtained.
The object of the present invention is to provide a method whereby space-telegraph messages may be automatically relayed. This object I attain by providing two space-telegraph systems of the elevated-conductor type, each comprising a transmitter .and receiver, with a relay adapted to be set in motion by the receiver of one system, and thereby to operate the transmitter of the other system and by so disposing the elevated conductor or conductors of the receiver of the first system and of the transmitter of the second, respectively,
that the former will not be operated by the latter. Several different forms of apparatus may within my invention be employed to accomplish this result. Two of these various forms shall hereinafter be fully described.. In one of the arrangements the elevated conductors of the transmitter of the second system are so placed that the Waves emanating from them produce planes or lines of interference, and the elevated conductor or conductors of the receiver ofthe first system are placed in these lines or planes of interference and are thereby rendered incapable of being aected by the Waves which emanate from the elevated conductors of the transmitter of the second system. The disposition of the elevated conductors in planes or lines of interference is described and claimed in an application iiled by me contemporaneously herewith, Serial No. 44,393, renewed February 24E, 1902, Serial No. 95,198. In another arrangement the elevated conductors of the receiver of the first system are so disposed relatively to those of the transmitter of the second that the electromagnetic waves emanating from the latter produce equal electric vibrations in the sev eral elevated conductors of the former; but the relay, which is set in motion by the receiver of the first system and which by its motion operates the transmitter of the second, is so associated with the elevated conductors of the receiver of the first system that the effects of the several equal electric vibrations conveyed to it from that transmitter are opposed to each other, and their resultant effect upon the relay is ml. The disposition of the elevated conductors last referred to is described and claimed in anapplication iled by me contemporaneously herewith, Serial No. 44,398.
The nature of theinvention and the manner in which it operates may best be understood by having reference to the drawingswhich accompany and form a part of this specification.
Figure l is a diagram illustrative of a disposition of apparatus in which the elevated conductor V of the receiver of one system is placed in the plane of interference of the Wavesfrom two elevated conductors V' V" of the transmitter of another system. Fig. 2 is adiagram illustrative of the disposition oli'Y apparatus in which the two elevated conductors V V of the receiver of one system are so disposed as to have equal electric vibrations developed in them by the electromagnectic waves emanating from the vertical wire V of the transmitter of another system and in which the effects of these Vibrations are opposed to each other at a relay associated with said receiver of the irst system.
In the figures, V V V are vertically-elevated conductors, M M M are induction coils or transformers, C C C, dre., are condensers, B B are batteries, K is a coherer, R is a relay, p is an automatic circuit-interrupter, s is a spark-gap, k is a contact which is normally open, but which is closed when the relay Ris set in motion, and F. is an earth connection.
The operation of the coil M, Figs. 1 and 2, produces a spark at the spark-gap s, and electrical oscillations result in the primary of the coil M", Fig. 1, and M, Fig. 2, by virtue of the condensers C3, Fig. l, and C, Fig. 2. The primary coils of M are equal in every respect and are symmetrically disposed relative t-o the two secondary coils of M. The electrical oscillations in the primary coils of M therefore induce equal and opposite electrical vibrations in the two conductors V and V of Fig. l,owing to the fact that the two secondary coils of M are wound in the same direction and form virtually a continuous coil grounded at its neutral point.
The vertical wire V is connected to the ground at this neutral point, so that it is unaected by the iiow of current through the coil. In Fig. 2 the electrical oscillations in the primary coil M develop electric vibrations in theconductorV. Beingsymmetricallydisposed with reference to the two vertical conductors V' and V, the electrical vibrations in it induce equal electrical vibrations in V' and V", and these Vibrations traversing the primary coils of lV in opposite directions their effect upon the secondary coil M" is mi.
In the operation of the organization shown in Fig. l the electromagnetic signal-waves to be relayed are received from a distant transmitting-station upon the elevated conductor V and develop therein electric vibrations. These vibrations are conveyed to the coherer K through the intermediary of the inductioncoil M and cause it to set in motion the relay R in a well-understood manner. The relay R thus set in motion closes the circuit of the battery B at 7c through the interrupter p and the primary of the induction or spark coil M. A high potential is thereby developed in the secondary of the spark-coil M', and a series of sparks occur at the spark-gap s. Oscillations are thereby developed in the circuit containing the condenser C and the primary of the induction coil M", which in turn develop equal and opposite electric vibrations in the vertical conductors V and V. These elecdition.
tric vibrations are equal and opposite, because the two halves of the secondary of M are equal, and the primary of M" is symmetrically disposed with respect to these two halves of the secondary. When a given electromagnetic signal-wave has passed the receiver, a decoherer (not shown in the drawings) restores the coherer to its normal state. The electromagnetic waves emanating from the two vertical conductors V Vll of the transmitter of the second system do not affect the vertical conductor V of the receiver of the first system, because the two conductors V V" are similar. The two oscillations developed in them are equal in amplitude and opposite in phase, and the vertical conductor V is symmetrically disposed with respect to V and V"-t'. e., it is in the plane of interference of the Waves which emanate from V' and V.
In the operation of the organization shown in Fig. 2 the electromagnetic signal-waves to be relayed are received from a distant transmitting-station upon the elevated conductors Vl and V, which are in a plane approximately that including the distant transmitting-station and are preferably at a distance apart equal to one halt` a complete wave length of the electromagnetic waves to be received. Under these circumstances the electric vibrations developed in the two conductors V and V will be equal in amplitude and opposite in phase. These vibrations are conveyed to the coherer K through the intermediary of the induction-coil or transformer lV and cause it to operate or set in motion the relay R in the usual manner. The relay R operates to close the circuit of the battery B at 7o through the interrupter p and the primary of the induction or spark coil M. A high potential is thereby induced in the secondary of M', and a rapid succession of sparks pass at the spark-gap at s, causing a highfrequency oscillation in the primary of the induction-coil M, and thereby developing high-frequency electric vibrations in the vertical wire V. When the electromagnetic waves of a given signal have passed the receiver, a decoherer (not shown in the drawings) restores the coherer to its normal con- 'Ihe electromagnetic waves emanating from the vertical wire Vproduce equal electric vibrations in V and V; but owing to the fact that the two halves of the primary of the coil M are equal and symmetrically disposed with respect to the secondary these vibrations passing through the two halves of the primary in opposite directions have no resultant effect upon the coherer K, and therefore upon the relay R.
As has been above shown, the elevated conductor of either the transmitter or receiver, or both, may be multiple.
I-Iaving fully described my invention, I claim- The method of relaying space-telegraph signals, which consists in receiving the sig- IOO IIO
nais to be relayed in the receiver of one spaceteiegraph system of the elevated-conductor type; causing this receiver to thereby oper` ate the transmitter of a second system of the same type, and so respectively electrically organizing and disposing the said receiver and transmitter conductors that the receiver will not be operated by signals sent by the transmitter.
JOHN STONE STONE.
In presence of- ALEX. P. BROWNE,
ELLEN B. TOMLINSON.
Priority Applications (1)
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US4439601A US717513A (en) | 1901-01-23 | 1901-01-23 | Method of relaying space-telegraph signals. |
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US4439601A US717513A (en) | 1901-01-23 | 1901-01-23 | Method of relaying space-telegraph signals. |
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US717513A true US717513A (en) | 1902-12-30 |
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