US1583826A - Method and apparatus for balancing out radiointerference on wire lines - Google Patents

Method and apparatus for balancing out radiointerference on wire lines Download PDF

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US1583826A
US1583826A US537050A US53705022A US1583826A US 1583826 A US1583826 A US 1583826A US 537050 A US537050 A US 537050A US 53705022 A US53705022 A US 53705022A US 1583826 A US1583826 A US 1583826A
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frequency
radio
line
receiving
interference
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US537050A
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Ralph W Deardorff
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AT&T Corp
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American Telephone and Telegraph Co Inc
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    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B3/00Line transmission systems
    • H04B3/02Details
    • H04B3/32Reducing cross-talk, e.g. by compensating

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  • the principal obj ect of my invention is to provide a new and improved system to overcome the interference on signaling conductors due to radio transmission.
  • my invention relates to balancing out the interference in a carrier current channel caused by radio signaling with a frequency a lying within the range of that channel.
  • Figure 1 is a diagram for a case in which a'balance is effected in a high frequency receiving circuit
  • -Fig. 2 is a diagram for a case in which a balance is effected ina low frequency receiving circuit.
  • carrier currents of high frequency and lymg in a plurality of carrier current channel ranges of frequency are transmitted both ways on the line
  • this line L passes through the composite set C to the hybrid coil transformer T with the balancing network N. From the composite set C the low frequency conductors LF are led away and only the high frequencies go into the transformer T.
  • the high frequency sending currents are impressed upon the line L at the station shown in Fig. 1 through the conductors S at the transformer T.
  • the arrangemerft is such that the sending currents are balanced 0 in their'effect on the receiving conductors R and these last mentioned conductors receive only the high frequency currents that come into the station over the line L.
  • I These received high frequency currents lie in a number of frequency ranges corresponding to different channels of transmission, for example, one channel may comprise frequencies from 7000.to 10000 cycles per second, another from 17000 to 20000 cycles per second, etc.
  • radio waves due to some long distance radio transmitting station. and having a frequency within one of these ranges, say a frequency of 18,200 cycles per second. Since the radio wave trains of this frequency lie within the carrier current band from 17000 to 20000 cycles per second, they may produce objectionable interference in a telephone conversation employing that channel.
  • I select 7 low frequency transmission on the line L shall not be affected.
  • conductors go through a potentiometer P and phase shifter whose output is connected in series in the circuit of the high frequency receiving conductors R.
  • This circuit R passes in series through the inputs of the several band filters F, each corresponding to a frequency range channel, and in particular, one of these filters passes the frequencies from 17000 to 20000 cycles per second, received from the transformer T, and this quencies lying outside that'range.
  • the interfering frequency E. M. R which in the example is assumed to be of a frequency 18,200 cycles per second, ..is superposed in the line L and thus enters the receiving circuit B through transformer T.
  • this same frequency E. M. E which is of course received in the line L, is introduced in the receiving circuit B so as to be equal in magnitude and opposite in phase to the superposed E. M. F. of that frequency received from the line L, and hence to neutralize it.
  • a troublesome interfering radio frequency can be neutralized in a wire signaling system.
  • any one of a large number of overhead transmission lines such as L can be utilized, selecting the line L from among those in which the radio frequency is not objectionable. so far as the normal use of that line is concerned. Indeed, it is simply desirable to obtain the radio frequency from any source different from the line L and by throwing the switches S, the neutralizing radio frequency currents may .be drawn from the antenna A if desired.
  • Fig. 2 I have shown a modification in which the high frequency currents are first line and as received for the purpose of balancing, and are then combined to produce a null effect.
  • the wire signaling system is the same as in Fig. 1 to the receiving circuit R, from which the band filters F for the respective frequency ranges lead to the branch receiving circuits as shown.
  • One of these band filters passes the frequency range which includes the interfering radio frequency which, for example, we have mentioned as 18,200.
  • the received currents of this frequency range pass throughthe detector D and detecting amplifier DA'to the low frequency receiving circuit R.
  • the high frequency currents tapped from the line L go through a composite set C and a potentiometer P, as in Fig. 1, but the phase shifter of Fig. 1 is omitted, and the radio frequency currents of Fig. 2 pass through a detector D and detecting amplifier DA, whose output is connected in series inthe receiving circuit R.
  • the interference in the receiving circuit R due to the radio currents received in the line L, is superposed on the currents that are properly and desirably received in the circuit R.
  • This superposed electromotive 'force is matched oppositely by an electromotive force in the output of the detecting amplifier DA, determined by the radio reception in the line L.
  • a pole changer PC is provided to insure that the output shall be series opposing instead of series aiding, and
  • phase shifter may be interposed here if needed.
  • Some radio telegraph systems employ the method of sending which involves shortcircuiting a part of the inductance of the antenna circuit with the sending key.
  • the part of the inductance is short-circuited and the frequency is say 18,800 cycles per second, but when the key is pressed to marking position,
  • two or more lines L may each be tapped to obtain balancing electromotive forces for the several interfering frequencies ;,and these may be applied through suitable phase. shifters and amplifiers or potenin the same way as the line L, thus illus-' trating the foregoing statement about how to proceed to balance out more than one interfering frequency.
  • the method of overcoming interference at a receiving station of said system due to radio signaling which consists in intercepting some of t e radio wave power at said receiving station and applying the electromotive forces obtained thereby at said receiving station to oppose the interfering electromotive forces in a receiving circuit of the said system.
  • tem subject to radio interference a conductor that is exposed to the same radiation as said system, receiving branch circuits con nected to said system and said conductor and means to apply electromotive forces in opposition corresponding to the radio re ception in the said system and the said overhead conductor.
  • the method of overcoming interference at a receiving station of that system due to radio signaling which consists in obtaining electromotive forces of the interfering frequency from radiation near the said receiving station and applying such electromotive forces to oppose the interfering electromotive forces in a receiving circuit. at the said station.
  • said system comprlsmg a receiving stationfa conductor exposed to radiation from said source
  • a high frequencv transmission line a three-winding transformer associated therewith for simultaneous transmit-ting and receiving, receiving conductors connected with said transformer, a plurality of filters having their input terminals connected in series with said receiving conductor, a conductor exposed to interfering radiation, and a connection from said conductor interposed in series with the inputs of said filters, said connection comprising an amplifier and a phase shifter.
  • cuits connected with at least one of the other lines to draw ofi' therefrom energy of frequency determined by said radio interference, an amplifier and a phase shifter to modify the energy drawn off in this way, the output from the amplifier and base shifterbeing connected with the receiving system for the other conductor to neutralize the interference therein.

Description

May 11 1926.- 1,583,826
7 R. W. DEARDORFF METHOD AND APPARATUS FOR BALANCING OUT RADIOINTERFERENCE 0N WIRE LINES Filed Feb. 16, 1922 IN V EN TOR.
ATTORNEY Patented May 11, 1926.
UNITED STATES PATENT OFFICE- RALPH w. DEAEDORFF, OF BROOKLYN, NEW YORK, ASSIGNOR TO AMERICAN PHONE AND TELEGRAPH COMPANY, A CORPORATION OF NEW YORK.
TELE- METHOD AND APPARATUS FOR BALANCING OUT RADIOINTERFERENCE ONWIRE LINES.
Application filed February 16, 1922. Serial No. 537,050.
The principal obj ect of my invention is to provide a new and improved system to overcome the interference on signaling conductors due to radio transmission. In another aspect, my invention relates to balancing out the interference in a carrier current channel caused by radio signaling with a frequency a lying within the range of that channel. These and other objects of my invention will be made apparent upon conslderatlon of a few specific examples of pract1ce 1n accordance therewith. In the accompanying drawings, the apparatus for these examples is shown in diagram and I will now proceed to a specific description with the understanding that the invention is defined 1n the appended claims.
In the drawings, Figure 1 is a diagram for a case in which a'balance is effected in a high frequency receiving circuit, and -Fig. 2 is a diagram for a case in which a balance is effected ina low frequency receiving circuit.
Referring to Fig. 1, carrier currents of high frequency and lymg in a plurality of carrier current channel ranges of frequency are transmitted both ways on the line At the station shown in the diagram, this line L passes through the composite set C to the hybrid coil transformer T with the balancing network N. From the composite set C the low frequency conductors LF are led away and only the high frequencies go into the transformer T.
The high frequency sending currents are impressed upon the line L at the station shown in Fig. 1 through the conductors S at the transformer T. The arrangemerft is such that the sending currents are balanced 0 in their'effect on the receiving conductors R and these last mentioned conductors receive only the high frequency currents that come into the station over the line L. I These received high frequency currents lie in a number of frequency ranges corresponding to different channels of transmission, for example, one channel may comprise frequencies from 7000.to 10000 cycles per second, another from 17000 to 20000 cycles per second, etc.
It may happen that in the geographical region through which the line L extends,
there are radio waves due to some long distance radio transmitting station. and having a frequency within one of these ranges, say a frequency of 18,200 cycles per second. Since the radio wave trains of this frequency lie within the carrier current band from 17000 to 20000 cycles per second, they may produce objectionable interference in a telephone conversation employing that channel.
To balance out such interference, I select 7 low frequency transmission on the line L shall not be affected.
From the composite set C, conductors go through a potentiometer P and phase shifter whose output is connected in series in the circuit of the high frequency receiving conductors R.
This circuit R passes in series through the inputs of the several band filters F, each corresponding to a frequency range channel, and in particular, one of these filters passes the frequencies from 17000 to 20000 cycles per second, received from the transformer T, and this quencies lying outside that'range.
The interfering frequency E. M. R, which in the example is assumed to be of a frequency 18,200 cycles per second, ..is superposed in the line L and thus enters the receiving circuit B through transformer T. By proper adjustment of the potentiometer P and phase shifter this same frequency E. M. E, which is of course received in the line L, is introduced in the receiving circuit B so as to be equal in magnitude and opposite in phase to the superposed E. M. F. of that frequency received from the line L, and hence to neutralize it. This allows the transmitted frequencies within the range 17000 to 20000 cycles or second that are received over the line to enter the receiving circuit same band filter F excludes fre- 3 demodulated, both as received over the wire R and pass to the output of the'band filter F without the presence of superposed currents due to the radio frequency of 18,200.
In the manner indicated in the foregoing description a troublesome interfering radio frequency can be neutralized in a wire signaling system. For this purpose, any one of a large number of overhead transmission lines such as L can be utilized, selecting the line L from among those in which the radio frequency is not objectionable. so far as the normal use of that line is concerned. Indeed, it is simply desirable to obtain the radio frequency from any source different from the line L and by throwing the switches S, the neutralizing radio frequency currents may .be drawn from the antenna A if desired.
In Fig. 2, I have shown a modification in which the high frequency currents are first line and as received for the purpose of balancing, and are then combined to produce a null effect. The wire signaling system is the same as in Fig. 1 to the receiving circuit R, from which the band filters F for the respective frequency ranges lead to the branch receiving circuits as shown. One of these band filters passes the frequency range which includes the interfering radio frequency which, for example, we have mentioned as 18,200. In the usual manner for carrier current reception, the received currents of this frequency range pass throughthe detector D and detecting amplifier DA'to the low frequency receiving circuit R. p
The high frequency currents tapped from the line L go through a composite set C and a potentiometer P, as in Fig. 1, but the phase shifter of Fig. 1 is omitted, and the radio frequency currents of Fig. 2 pass through a detector D and detecting amplifier DA, whose output is connected in series inthe receiving circuit R.
The interference in the receiving circuit R, due to the radio currents received in the line L, is superposed on the currents that are properly and desirably received in the circuit R. This superposed electromotive 'force is matched oppositely by an electromotive force in the output of the detecting amplifier DA, determined by the radio reception in the line L. A pole changer PC is provided to insure that the output shall be series opposing instead of series aiding, and
a phase shifter may be interposed here if needed.
Some radio telegraph systems employ the method of sending which involves shortcircuiting a part of the inductance of the antenna circuit with the sending key. Thus, when the key is in spacing position, the part of the inductance is short-circuited and the frequency is say 18,800 cycles per second, but when the key is pressed to marking position,
be adjusted to balance out that frequency.
Again, it may happen that both frequencies Will be equally Within a single carrier cur-' rent range and equally troublesome, in which case the system that I have proposed will balance out both of them, provided the line L picks up both frequencies in the same ratio as the line L.
If thereis more than one interfering frequency to be balanced out which cannot satisfactorily be cared for by one equipment such as I have shown as associated with the line L, then two or more lines L may each be tapped to obtain balancing electromotive forces for the several interfering frequencies ;,and these may be applied through suitable phase. shifters and amplifiers or potenin the same way as the line L, thus illus-' trating the foregoing statement about how to proceed to balance out more than one interfering frequency.
What is claimed is:
1. In the operation of a high frequency Wire signaling system, the method of overcoming interference at a receiving station of said system due to radio signaling, which consists in intercepting some of t e radio wave power at said receiving station and applying the electromotive forces obtained thereby at said receiving station to oppose the interfering electromotive forces in a receiving circuit of the said system.
2. In the operation of a carrier current wire signaling system, the method of overcoming interference at a receiving station of said system due to radio signaling at a fre: I
consists in obtaining electromotive forces from radiation of the interfering frequency in the neighborhood of the receiving station, deriving therefrom electromotive forces of proper amplitude and phase relation and applying them at the receiving station in opposition to the interfering electromotive I forces ina rece v ng circuit at said s ation.
. tem subject to radio interference, a conductor that is exposed to the same radiation as said system, receiving branch circuits con nected to said system and said conductor and means to apply electromotive forces in opposition corresponding to the radio re ception in the said system and the said overhead conductor. v
5. In the operation of a high frequency wire signaling system, the method of overcoming interference at a receiving station of that system due to radio signaling, which consists in obtaining electromotive forces of the interfering frequency from radiation near the said receiving station and applying such electromotive forces to oppose the interfering electromotive forces in a receiving circuit. at the said station.
6. In the operation of a high frequency carrier current wire signaling system which is sub-'ect to interference by radio of the same requency, the method of overcoming such interference at a receiving station of said system which consists in gathering radiated energy from the same interfering source, adjusting the amplitude and phase of this energy and applying the modified energy to the said wire system at said receiving station to neutralize the interference therein.
7. In combination, a high frequency wire signaling system subject to radlo interfer-.
ence from a certain source, said system comprlsmg a receiving stationfa conductor exposed to radiation from said source, and
means at said station connecting from-said conductor to said station to ap 1y electromotive forces from said exposed. conductor so as to neutralize the interference in said system.
8. In combination, a high frequencv transmission line, a three-winding transformer associated therewith for simultaneous transmit-ting and receiving, receiving conductors connected with said transformer, a plurality of filters having their input terminals connected in series with said receiving conductor, a conductor exposed to interfering radiation, and a connection from said conductor interposed in series with the inputs of said filters, said connection comprising an amplifier and a phase shifter.
9. In combination, a plurality of wire transmission lines all subject. to the same radio interference, a receiving station for carrier currents of the same frequency as said rad1o interference said station belng connected with one of said lines, branch cir-.
cuits connected with at least one of the other lines to draw ofi' therefrom energy of frequency determined by said radio interference, an amplifier and a phase shifter to modify the energy drawn off in this way, the output from the amplifier and base shifterbeing connected with the receiving system for the other conductor to neutralize the interference therein.
" In testimony whereof, I have signed my name to this specification this 14th day of February, 1922.
RALPH W. DEABDORFE.
US537050A 1922-02-16 1922-02-16 Method and apparatus for balancing out radiointerference on wire lines Expired - Lifetime US1583826A (en)

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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE1102921B (en) * 1955-07-01 1961-03-23 Sueddeutsche Telefon App Kabel Sieve arrangement for two-wire lines

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE1102921B (en) * 1955-07-01 1961-03-23 Sueddeutsche Telefon App Kabel Sieve arrangement for two-wire lines

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