US2273432A - Electron discharge device circuits - Google Patents

Electron discharge device circuits Download PDF

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US2273432A
US2273432A US312236A US31223640A US2273432A US 2273432 A US2273432 A US 2273432A US 312236 A US312236 A US 312236A US 31223640 A US31223640 A US 31223640A US 2273432 A US2273432 A US 2273432A
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resistance
circuit
cathode
temperature
electron discharge
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US312236A
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Sherman T Brewer
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AT&T Corp
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Bell Telephone Laboratories Inc
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    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03FAMPLIFIERS
    • H03F1/00Details of amplifiers with only discharge tubes, only semiconductor devices or only unspecified devices as amplifying elements
    • H03F1/34Negative-feedback-circuit arrangements with or without positive feedback
    • H03F1/36Negative-feedback-circuit arrangements with or without positive feedback in discharge-tube amplifiers

Definitions

  • This invention relates to electron discharge device cir-cuits, and, more particularly, to circuits for expanding or compressing the volume range of a signal applied thereto.
  • An object of this invention is to cause the expansion or compression of the volume range of a signal applied to an electron discharge device, in a simple manner and with a minimum of circuit elements.
  • a feature of the invention comprises associating an element of high temperature coefllcient of resistance with a portion of the electron discharge device common to its input and output circuits.
  • Another feature comprises varying the temperature, and, consequently, the impedance, of such an element by passage of substantially only alternating current therethrough.
  • a temperature controlled, variable resistance element having, for example, a high positive or negative temperature coeflicient of resistance, is'connected in the cathode lead of the circuit of an electron-discharge device such that it is common to the input and output circuits of said device.
  • the gain of the device used as an amplifier will be a function of the temperature and of the current through the element. Since this current comprises the space current and the amplified signal current, the gain will be a function of the applied signal voltage; the amplifier is suitable for expansion or compression purposes. If it is desired to have the expansion or compression responsive only to changes in the applied signal, the resistance element may be provided with a shunt for direct current or be included in series with direct current blocking means.
  • the circuit may comprise two or more electron discharge devices in tandem, the circuit constituting an expander or a compressor of the volume range, dependent on thenumber of stages and on whether a positive or negative temperature coefilcient element is utilized.
  • the element of negative orpositive temperature coeflicient is of the type that evidences non-linear change in resistance with change in temperature, and that changes in temperature, .and, therefore, in resistance. with change in .the value of the current flow therethrough; silver sulphide resistance elements having such a characteristic may be utilized.
  • Fig. 1 shows an amplifying electron discharge devicecircuit embodying this invention
  • Fig. 2 shows another circuit embodiment of the invention in which a direct current by-pass is associated with the feedback variable resistance element
  • Figs. 3 and 4 show two-stage and three-stage electron discharge device circuits including the cathode lead arrangement of Fig. 2;
  • Fig. 5 shows a modificationlof the circuit arrangement of-Fl 1;
  • Fig. 6 shows a multistage circuit similar to that of Fig. 4 except that it includes the cathode lead arrangement of Fig. 5; and 1 Fig. 7 shows a modification of the circuit of Fig. 2 in which an electronic resistance is emplayed as the cathode lead variable resistance element.
  • Fig. 1 discloses the basic aspect of the invention in a single electron discharge device amplifying circuit.
  • the signal input terminals I, 2 are connected to the input control grid H and the low potential terminal of the cathode I! of the device or tube in, a grid biasing resistance R0 and a feedback element R1 being connected in series in the cathode lead.
  • the element R1, in accordance with the invention, is preferably of a substance or is a device having a high positive or negative temperature coeflicient of resistance,
  • anode or plate I3 is provided by source B, for example, a battery, through the load R2.
  • the gain of the amplifier is, therefore, a function of the temperature and, consequently, of the current flowing through R1.
  • the current flowing through R1 is composed of the cathode-anode direct or space current and the amplified'signal feedback responsive to the changes in the signal,
  • Fig, 2 may be used.
  • An inshown, a complex network could be used to accomplish the same purpose.
  • Whether the amplifier expands or compresses the volume range of an applied signal depends upon whether the element R1 has a positive or a negative temperature coeihcient of resistance, and whether the amplifier has an odd or an even number of stages. If the element R1 is of a material or is a device having a negative temperature coefficient of resistance, it will produce volume,
  • the element R1 is of a material or is a device having a positive temperature coefiicient of resistance, it will produce volume compression in an amplifying circuit with an odd number of stages, for example, Figs. 1, 2 and 4, and volume expansion when the number of stages is even, for example, as in Fig. 3. 1
  • R1 could be the plate resistance of a vacuum tube whose grid potential is varied in accordance with the signal to produce the desired expansion or compression.
  • the use of an electronic resistance for R1 possesses the advantage of making the time constant of the circuit more flexible.
  • the circuit could be arranged to accomplish the expansion or compression with any desired time lag. With zero time lag, R1 would respond to the instantaneous value of the impressed voltage.
  • the amplifier might be made more nearly linear, or, if desired, non-linear.
  • Fig. 7 shows a circuit embodying an electronic resistance for range expansion.
  • the vacuum tube M is connected in the grid-cathode and cathodeanode circuits with its anode or plate.
  • I 5 connected through condenser C1 to the junction of the biasingresistance R and inductance L1 and its cathode l6 connected through a biasing resistor l1 and by-pass condenser l8 to the junction of inductance L and the low potential terminal of the source B.
  • Potential for anode I is obtained from the highpotential terminal of source B through a coil l9.
  • a diode D is connected between the cathode end of biasing resistor R0 and the control grid of tube II.
  • the anodeZl of the diode is connected to the cathode I2 of tube l0 through a condenser 22, to the diode cathode 23 through a resistance 24, and to the control grid of tube I.
  • the junction of cathode 2 3 and resistance 24 is connected to the low potential terminal of the source B.
  • a biasing resistor R0 is connected in series with a network N, having high impedance to the frequency of the signal current to b transmitted between the input and output terminals, the resistor and network being connected between the cathode and the low potential terminal of source B of anode potential.
  • Seriesconnected condenser C2 and temperature-controlled variable resistance element R1 are connected in parallel with resistance R0 and network N.
  • the element R1 may be of a material or a device having a negative or a positive temperature coefiicient of resistance, and preferably, of the type that evidences non-linear changes in resistance with temperature change.
  • the circuit of Fig. 5 may be used to accomplish volume expansion.
  • Volume expansion may be accomplished in a multistage amplifier having an odd number of stages, for example, such as is shown in Fig. 6; volume compression is obtainable with a multistage circuit having an even number of stages.
  • expansion is obtainable with a circuit having an even number of stages, and compres-. sion with an odd number of stages.
  • condenser C2 insures that direct current, which would render it unstable, cannot flow through the element R1.
  • a circuit comprising a plurality of electron discharge devices connected in tandem, each of said devices comprising a cathode, an anode and a control grid, and a single feedback means common to the cathode-grid and cathode-anode circuits of each of said devices for causing a change in thesignal volume output of said circuit nonproportionate to a change in signal impressed on the input of said circuit, said means including a thermosensitive resistance element to be heated by current flow in said cathode-anode circuit and being of a substance having a non-linear temperature-resistance characteristic, and means in shunt with said resistance element and of high impedance to the signal current.
  • a circuit comprising a plurality of electric discharge devices, each device comprising a cathode, an anode and a control grid, the cathodes of said devices being connected directly together, input and output circuits for each of said devices, and impedance means common to said circuits and including a thermosensitive variable impedance to be heated by current flow in said output circuits and having one terminal common to said cathodes, said impedance being of a substance having a high temperature coefiicient of resistance.

Description

Feb. 17, 1942. s. 'r. BREWER 2,273,432
ELECTRON DISCHARGEYDEVICE' CIRCUITS Filed Jan. 5,- 1940 2 Sheets-Sheet -1 //v VENTOR S. 7. BREWER Feb. 17, "1942. s. 1-. BREWER ELECTRON DISCHARGE DEV ICE CIRCUITS Filed Jan. 3, 1940 2 Sheets-Sheet 2 v INVENTOR SJYBREWER er VATTOR EV Patented Feb. 17, 1942 ELECTRON DISCHARGE DEVICE CIRCUITS.
Sherman T. Brewer, New York, N. Y., assignor to Bell Telephone Laboratories,
Incorporated,
New York, N. Y,, a corporation of New York Application January 3, 1940, Serial No. 312,236
2 Claims.
This invention relates to electron discharge device cir-cuits, and, more particularly, to circuits for expanding or compressing the volume range of a signal applied thereto.
An object of this invention is to cause the expansion or compression of the volume range of a signal applied to an electron discharge device, in a simple manner and with a minimum of circuit elements.
A feature of the invention comprises associating an element of high temperature coefllcient of resistance with a portion of the electron discharge device common to its input and output circuits.
Another feature comprises varying the temperature, and, consequently, the impedance, of such an element by passage of substantially only alternating current therethrough. Y
ment of either positive or negative temperature coefllcient of resistance.
In accordance with the invention, a temperature controlled, variable resistance element having, for example, a high positive or negative temperature coeflicient of resistance, is'connected in the cathode lead of the circuit of an electron-discharge device such that it is common to the input and output circuits of said device. The gain of the device used as an amplifier will be a function of the temperature and of the current through the element. Since this current comprises the space current and the amplified signal current, the gain will be a function of the applied signal voltage; the amplifier is suitable for expansion or compression purposes. If it is desired to have the expansion or compression responsive only to changes in the applied signal, the resistance element may be provided with a shunt for direct current or be included in series with direct current blocking means. In accordance with the invention, also, the circuit may comprise two or more electron discharge devices in tandem, the circuit constituting an expander or a compressor of the volume range, dependent on thenumber of stages and on whether a positive or negative temperature coefilcient element is utilized. Preferably, the element of negative orpositive temperature coeflicient is of the type that evidences non-linear change in resistance with change in temperature, and that changes in temperature, .and, therefore, in resistance. with change in .the value of the current flow therethrough; silver sulphide resistance elements having such a characteristic may be utilized.
A more complete understanding of the inven- 1 'A further feature comprises utilizing an eletion will be obtained from the detailed description which follows, taken in conjunction with the appended drawings, wherein:
Fig. 1 shows an amplifying electron discharge devicecircuit embodying this invention;
Fig. 2 shows another circuit embodiment of the invention in which a direct current by-pass is associated with the feedback variable resistance element;
Figs. 3 and 4 show two-stage and three-stage electron discharge device circuits including the cathode lead arrangement of Fig. 2;
Fig. 5 shows a modificationlof the circuit arrangement of-Fl 1;
Fig. 6 shows a multistage circuit similar to that of Fig. 4 except that it includes the cathode lead arrangement of Fig. 5; and 1 Fig. 7 shows a modification of the circuit of Fig. 2 in which an electronic resistance is emplayed as the cathode lead variable resistance element.
Fig. 1 discloses the basic aspect of the invention in a single electron discharge device amplifying circuit. The signal input terminals I, 2 are connected to the input control grid H and the low potential terminal of the cathode I! of the device or tube in, a grid biasing resistance R0 and a feedback element R1 being connected in series in the cathode lead. The element R1, in accordance with the invention, is preferably of a substance or is a device having a high positive or negative temperature coeflicient of resistance,
and evidencing non-linear change in resistance with temperature change. Potential for the anode or plate I3 is provided by source B, for example, a battery, through the load R2.
An input voltage isapplied'to terminals l, 2-
and a voltage across R2 is developed which is greater than the applied voltage by the gain of the circuit, determined by the transconductance of the tube and the values of R0 and R1. The gain of the amplifier is, therefore, a function of the temperature and, consequently, of the current flowing through R1. The current flowing through R1, however, is composed of the cathode-anode direct or space current and the amplified'signal feedback responsive to the changes in the signal,
the arrangement of Fig, 2 may be used. An inshown, a complex network could be used to accomplish the same purpose.
The application of the cathode lead arrangement of Fig. 2 to a two-stage and a three-stage resistance-capacity coupled amplifier is shown in Figs. 3 and 4.
Whether the amplifier expands or compresses the volume range of an applied signal depends upon whether the element R1 has a positive or a negative temperature coeihcient of resistance, and whether the amplifier has an odd or an even number of stages. If the element R1 is of a material or is a device having a negative temperature coefficient of resistance, it will produce volume,
expansion when used in an amplifier having an odd number of stages, for example, that of Figs. 1, 2 and 4, and volume compression when used in an amplifying circuit having an even number of stages, for example, Fig. 3. If, on the other hand, the element R1 is of a material or is a device having a positive temperature coefiicient of resistance, it will produce volume compression in an amplifying circuit with an odd number of stages, for example, Figs. 1, 2 and 4, and volume expansion when the number of stages is even, for example, as in Fig. 3. 1
Although a directly or self-heated temperature-controlled resistance element has been described, other types of variable impedance might be used. For example, R1 could be the plate resistance of a vacuum tube whose grid potential is varied in accordance with the signal to produce the desired expansion or compression. The use of an electronic resistance for R1 possesses the advantage of making the time constant of the circuit more flexible. Thus the circuit could be arranged to accomplish the expansion or compression with any desired time lag. With zero time lag, R1 would respond to the instantaneous value of the impressed voltage. Thus the amplifier might be made more nearly linear, or, if desired, non-linear.
Fig. 7 shows a circuit embodying an electronic resistance for range expansion. The vacuum tube M is connected in the grid-cathode and cathodeanode circuits with its anode or plate. I 5 connected through condenser C1 to the junction of the biasingresistance R and inductance L1 and its cathode l6 connected through a biasing resistor l1 and by-pass condenser l8 to the junction of inductance L and the low potential terminal of the source B. Potential for anode I is obtained from the highpotential terminal of source B through a coil l9. A diode D is connected between the cathode end of biasing resistor R0 and the control grid of tube II. The anodeZl of the diode is connected to the cathode I2 of tube l0 through a condenser 22, to the diode cathode 23 through a resistance 24, and to the control grid of tube I. The junction of cathode 2 3 and resistance 24 is connected to the low potential terminal of the source B.
.Upon an increase in the magnitude of the signal impressed on termials I, 2, the increased current flow through tube l0 increases the diode current, drives the control grid of tube ll more positive, and reduces the plate resistance of tube II. The amount of degenerative 'feedback of signal to the control grid of tube I0 is decreased, and the output of the circuit is increased, but in ratio greater than the relative change in the magnitude of the signal impressed at the terminals l, 2.
In the circuit of Fig. 5, a biasing resistor R0 is connected in series with a network N, having high impedance to the frequency of the signal current to b transmitted between the input and output terminals, the resistor and network being connected between the cathode and the low potential terminal of source B of anode potential. Seriesconnected condenser C2 and temperature-controlled variable resistance element R1 are connected in parallel with resistance R0 and network N. The element R1 may be of a material or a device having a negative or a positive temperature coefiicient of resistance, and preferably, of the type that evidences non-linear changes in resistance with temperature change.
If element R1 is of the negative temperature 00-- eflicient type, the circuit of Fig. 5 may be used to accomplish volume expansion. Volume expansion may be accomplished in a multistage amplifier having an odd number of stages, for example, such as is shown in Fig. 6; volume compression is obtainable with a multistage circuit having an even number of stages. With an element R1 having a positive temperature coefficient, expansion is obtainable with a circuit having an even number of stages, and compres-. sion with an odd number of stages. If the-element R1 is of silver sulphide, condenser C2 insures that direct current, which would render it unstable, cannot flow through the element R1.
Although this invention has been disclosed with reference to certain specific embodiments, it is to be'understood that it is not limited in scope thereto, but by the appended claims only.
What is claimed is:
1. A circuit comprising a plurality of electron discharge devices connected in tandem, each of said devices comprising a cathode, an anode and a control grid, and a single feedback means common to the cathode-grid and cathode-anode circuits of each of said devices for causing a change in thesignal volume output of said circuit nonproportionate to a change in signal impressed on the input of said circuit, said means including a thermosensitive resistance element to be heated by current flow in said cathode-anode circuit and being of a substance having a non-linear temperature-resistance characteristic, and means in shunt with said resistance element and of high impedance to the signal current.
'2. A circuit comprising a plurality of electric discharge devices, each device comprising a cathode, an anode and a control grid, the cathodes of said devices being connected directly together, input and output circuits for each of said devices, and impedance means common to said circuits and including a thermosensitive variable impedance to be heated by current flow in said output circuits and having one terminal common to said cathodes, said impedance being of a substance having a high temperature coefiicient of resistance.
SHERMAN T. BREWER.
US312236A 1940-01-03 1940-01-03 Electron discharge device circuits Expired - Lifetime US2273432A (en)

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Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2504175A (en) * 1945-07-31 1950-04-18 Philco Corp Contrast control circuit for television systems
US2676300A (en) * 1951-12-06 1954-04-20 Gen Precision Lab Inc Vacuum tube voltmeter
US2691075A (en) * 1950-06-27 1954-10-05 Rca Corp Transistor amplifier with high undistorted output
US2749394A (en) * 1951-04-24 1956-06-05 Ericsson Telefon Ab L M Device for amplification of both voice and signalling voltages
DE950860C (en) * 1952-07-29 1956-10-18 Siemens & Halske Ges M B H Control amplifier with expander effect
DE1064112B (en) * 1956-01-28 1959-08-27 Telefonbau & Normalzeit Gmbh Push-pull B amplifier

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2504175A (en) * 1945-07-31 1950-04-18 Philco Corp Contrast control circuit for television systems
US2691075A (en) * 1950-06-27 1954-10-05 Rca Corp Transistor amplifier with high undistorted output
US2749394A (en) * 1951-04-24 1956-06-05 Ericsson Telefon Ab L M Device for amplification of both voice and signalling voltages
US2676300A (en) * 1951-12-06 1954-04-20 Gen Precision Lab Inc Vacuum tube voltmeter
DE950860C (en) * 1952-07-29 1956-10-18 Siemens & Halske Ges M B H Control amplifier with expander effect
DE1064112B (en) * 1956-01-28 1959-08-27 Telefonbau & Normalzeit Gmbh Push-pull B amplifier

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