US2343182A - Sound recording with supersonic modulator - Google Patents

Sound recording with supersonic modulator Download PDF

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US2343182A
US2343182A US469371A US46937142A US2343182A US 2343182 A US2343182 A US 2343182A US 469371 A US469371 A US 469371A US 46937142 A US46937142 A US 46937142A US 2343182 A US2343182 A US 2343182A
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voltage
carrier
supersonic
circuit
tubes
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US469371A
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Frank P Herrnfeld
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AT&T Corp
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Western Electric Co Inc
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    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor

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  • Terminals 5 and 6 of the windings SI and S2 are connected respectively to grids 1 and 8 of vacuum quency is low in level or altogether absent.
  • a feature of the invention is the provision of a pair of vacuum tubes by which is effected the final step of amplification of both the carrier frequency and the modulating signal frequency. These tubes are so arranged as to-p'ossess a net conductance varying with the level of the modulating signalbetween the maximum conductance of either tube alone and a minimum determined by the adjustment of the noise reduction control;
  • i is an oscillator tuned to a carrier frequency of, say, 8 megacycles per second.
  • Tuning coil 2 of this oscillator is linked as desired tubes Vi and V2 which are represented in the figthe as triodes but may, of course, be pentodes if desired.
  • link circuit 3 is adjustably linked at one end to oscillator tuning coil 2 and at the other end to primary 4 of transformer Ti.
  • the secondary circuits SI and S2 of transformer Tl are provided with trimmer condensers 9 and I0 whereby the transformer output circuits are accurately tuned to the carrier frequency generated by oscillator I.
  • Cathodes H and I2 of tubes Vi and V2, respectively, are maintained at the desired positive potentials with respect to grids 1 and 8, cathode H by a tap on potentiometer P2, cathode I2 by a tap on potentiometer P3. These potentiometers, in parallel, are in series with resistance 20 between,
  • By-pass condensers l4 and iii are provided in shunt between ground and cathodes Ii and i2, respectively. It is to be understood that the cathodes named are heated by the usual power supply, not shown.
  • inductance l6 and condenser ll constitute a filter for the anode current supply of'tubes VI and V2 which is obtained from battery l3 through inductances l6 and LI, the purpose of the latter inductance being stated below;
  • Anodes l8 and I 9 of tubes VI and V2 are joined together and to the terminal of inductance Ll remote from battery I 3.
  • the circuit functions as a class B amplifier of the carrier voltage received on grid 8. If a modulating signal voltage is now impressed across the terminals of resistance M, in series between ground and secondarywinding S2, output terminals X and .Y are capable of transmitting a modulated carrier wave to any I desired transmission line or terminal apparatus;
  • XY may lead to the crystal 22 of a supersonic valve 23 and the modulated carriervoltage so impressed on crystal 22 may be used to. modulate the light from source 24 transmitted through valve 23 to film 25 asdescribed in the prior art. Film 25 is driven by, conventional means not shown.
  • the portion of PI included between tap 30 and ground is in series between ground and secondary winding SI of transformer TI, and the indicated poling of rectifier 28 and connection of circuit B is such that as the level of the audio signal in circuit A varies, the conductance of tube VI is correspondingly varied, thereby providing a net conductance for tubes VI and V2 which varies with the level of the audio signal across resistor 2
  • Oscillator I is energized and tuned to the frequency of crystal 22 which is itself for this adjustment replaced by a dummy load, tube VI being removed from the circuit.
  • V2 is adjusted for class 3 operation.
  • the output circuits of transformer TI and circuit LI-C3 are tuned for maximum carrier output and link circuit 3 is adjusted to provide a carrier voltage on voltmeter VM suflicing to permit full modulation of the light transmitted by supersonic valve 23.
  • I Thereafter crystal 22 and tube VI are replaced and P2. is so adjusted that VI is just at cut-oil with the! carriervoltage applied.
  • Switches DI and D2 are provided so that in preliminary adjustment either circuit A or circuit B may, as desired, be replaced by a resistor 3
  • switches are in position as indicated in the figure and the operations just described "have been performed, conditions are such that the whole unit to the carrierv frequency derived from oscillator- I and by adjustment of the coupling of link cir-. cuit,3 to provide across terminals X and! a carrier voltage (tube VI being fully blocked for this purpose) of magnitude required ,to drive the" crystal 22.
  • a vacuum tube voltmeter VM is provided to measure the voltage between the terminals X and Y.
  • Tank circuit LI-C3' serves to provide a sine wave of carrier voltage derived from the class B output of tube VI.
  • a crystal modue lator'of the type here considered is sufllciently highly tuned so that nodetuning of oscillator I is to be feared as the conductances of tubes VI and V2 are varied.
  • secondary SI of transformer TI- is conductively connected to ground through a portion of potentiometer PI in the upper part of the figure.
  • a steady or slowly vary- .ing voltage across PI determines the control of the net conductance of tubes VI and V2 as this dependsupon the grid bias of tube VI.
  • cuit comprising microphone 26 sucaudio voltage is impressed across resistor 2
  • a portion of the output of amplifier 21 is rectified byv a full wave rectifier and'supplied through filter 29 so that a rectified voltage, the envelope of the audio signal, is 'var- 4 operates as a class B modulator wherein an input sound signal received by microphone 26 modulates the carrier voltage derived from oscillator I.
  • the output of rectifier 28 and filter 29 is so poled in conjunction with the initial adjustment of potentiometer P2 that tube VI is not conductive no matter how high the audio input signal may be.
  • a record of the microphone signal without The level of this signal is read on volume indicator VI.
  • the audio input is removed by suitably operating switch DI and potentiometer P2 is soadjustedthat the conductance of VI efiects partial cancellation of tube V2.
  • Voltmeter VM reads, say EI when VI is permitted a partial conductance and E2 when VI is blocked, so that noise reduction in decibels may be stated as I I [N 0i a--j
  • the setting of tap 30 on potentiometer PI is ,a
  • circuit B to grid J tacontrol such application and may be used wherever carrier transmission of low frequency signals is f required with or without the advantage'of suppressing to a desired extent the carrier frequency during periods .when theumidulating'signal is of low level or absent.
  • a carrier frequency oscillator an output circuit for said oscillator, power supply for said oscillator, a pair of vacuum tubes provided each at least with a control grid, a cathode and an anode, power supply for said tubes, a terminal connected to both of said anodes, a grounded terminal to which said cathodes are individually connected through adjustable resistances relatively adjusted to provide a net conductance for said vacuum tubes, individual input circuits between said control grids and said grounded terminal comprising each a resistor in series with inductive coupling to the output circuit of said oscillator, said input circuits being connected for push-pull coupling of said control grids to said output circuit, a source of audio frequency current, means for impressing across the resistor in one of said input circuits a voltage proportional to the instantaneous magnitude of said audio current, means for rectifying a portion of said audio current, and means for-impressing across the resistor in the other of said input circuits a voltage proportional to the magnitude of said rectified current.
  • a sound recording circuit including in combination a supersonic light valve having a pair of terminals, a source supplying supersonic voltage -to' said valve comprising a supersonic oscillator, a pair of vacuum tubes provided each at least with, a cathode, a control grid and an anode, said cathodes being individually connected to ground through variable resistances, said control grids being inductively'coupled m push-pull to said oscillator and said anodes being connected together and to the ungrounded terminal of said valve, a source of audio frequency current, means for supplying to one of said control grids a voltage proportional to the instantaneous value of said current, means for providing a voltage of supersonic frequency, power supply for said oscillator, a pair of amplifying tubes provided each at least with a control grid, a cathode and an anode, power supply for said tubes, a common connection of said anodes to an output terminal, adjustable biasing resisttors individually connecting said cathodes to a common
  • a supersonic frequency is modulated by a signal of audio frequency
  • the method which consists in generating a voltage of supersonic frequency, amplifying said supersonic voltage differentially and oppositely in phase in a pair of transmission paths, combining'said paths to produce a net amplified supersonic voltage, generating 2, voltage of audio frequency,.introducing said audio voltage in one only of said paths, rectifying a portion of said audio voltage, introducing said rectified voltage in the other only of said paths, and simultaneously controlling the level of said net supersonic voltage in accordance with the envelope of said rectified voltage] and modulating said net supersonic voltage by said audio voltrectifying a portion of, said current, and means for supplying to the other of said control grids a voltage proportional to said rectified current whereby the supersonic voltage-applied to said valve is varied in amplitude in accordance with the envelope of said rectified current.
  • a carrier signaling system in which a carrier frequency is modulated by signal frequency
  • the method which consists in generating a voltage of said carrier frequency, amplifying said carrier voltage differentially and in opposite phase in a pair of transmission paths, combining said paths to produce a net amplified supersonic voltage, generating a signal voltage

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Description

Feb. 29, 1944. F. P. HERRNFELD 2,343,182
SOUND RECORDING WITH SUPERSONIC MODULATOR Filed D66. 17, 1942 |H E w 3 INVENTOR f. I? HERRNFELD ATTORNEY 23, 1942, to G. W. Willard.
' to O. B. Blackwell and Patented Feb. 1944 UNITED s'rArEs PATENT OFFICE SOUND RECOBDIN G WITH S UPERSONIC MODULATOR Frank 1?. Herrnield, Los Angeies, Calif., assiznor to Western Electric Company, New York, N. Y., a corporation of Incorporated, New York Application December 17, 1942, Serial No. 469,371
6 Claims. (C1. 179-1003) through link circuit 3 to primary 4 of transformer Tl, the secondary winding of which is divided into two parts, Si and S2, joined bybypass condensers Cl and C2 in series, the junction of these condensers being connected to ground.
Terminals 5 and 6 of the windings SI and S2 are connected respectively to grids 1 and 8 of vacuum quency is low in level or altogether absent. A
preferred embodiment of the invention is described whereby noiseless photographic sound records of the variable. density type may be obtained in a recording system in which the modulator is'a supersonic valve such as that disclosed in United States Patent 2,287,587, granted June The use in photographic sound recording of a supersonic valve of this general description is described in United States Patent 2,084,201, granted June 15, 1937, to A. Karolua However, the disclosures of the prior'art show no method or circuit means whereby the advantages of noise reduction now universally demanded of sound records can be added. c
It is, therefore, an object of the present invention to provide means for photographic sound recording with noise reduction using a supersonic modulator. Reduction of noise in carrier transmission circuits during intervals of low or absent audio signals is taught. for example, in United States Patent 1,681,972, granted'August 28, 1928,
H. A. .Aflel. For the present purpose, however, the greatest'sixnplicity is desired in recording circuits and it is another object of the invention to provide a novel carrier transmission system of controlled carrier amplitude characterized by a minimum complexity of apparatus. r
A feature of the invention is the provision of a pair of vacuum tubes by which is effected the final step of amplification of both the carrier frequency and the modulating signal frequency. These tubes are so arranged as to-p'ossess a net conductance varying with the level of the modulating signalbetween the maximum conductance of either tube alone and a minimum determined by the adjustment of the noise reduction control;
Other objects and features of the invention will be apparent from the following description when 1 read with reference to the accompanying drawing in which the single figure schematically represents a circuit adaptedto achieve the objects above declared. I
In the figure, i is an oscillator tuned to a carrier frequency of, say, 8 megacycles per second.
Tuning coil 2 of this oscillator is linked as desired tubes Vi and V2 which are represented in the figthe as triodes but may, of course, be pentodes if desired. As, indicated, link circuit 3 is adjustably linked at one end to oscillator tuning coil 2 and at the other end to primary 4 of transformer Ti. The secondary circuits SI and S2 of transformer Tl are provided with trimmer condensers 9 and I0 whereby the transformer output circuits are accurately tuned to the carrier frequency generated by oscillator I.
Cathodes H and I2 of tubes Vi and V2, respectively, are maintained at the desired positive potentials with respect to grids 1 and 8, cathode H by a tap on potentiometer P2, cathode I2 by a tap on potentiometer P3. These potentiometers, in parallel, are in series with resistance 20 between,
the positive terminal of battery i3 and ground.
By-pass condensers l4 and iii are provided in shunt between ground and cathodes Ii and i2, respectively. It is to be understood that the cathodes named are heated by the usual power supply, not shown.
inductance l6 and condenser ll constitute a filter for the anode current supply of'tubes VI and V2 which is obtained from battery l3 through inductances l6 and LI, the purpose of the latter inductance being stated below; Anodes l8 and I 9 of tubes VI and V2 are joined together and to the terminal of inductance Ll remote from battery I 3.
It will at once be observed that the grid-cathode circuits of tubes VI and V2 are in push-pull connection while the corresponding anode circuits are in parallel. Therefore; if'the conductances of tubes VI and'V2 are equal, no carrier voltage will appear between ground and the junction of anodes IB and I9 whatever the input carrier voltage transmitted from oscillator I to the gridcathode circuits of tubes VI and V2. The conductances of these tubes are individually determined by adjustment of potentiometers P2 and P3.
The advantage in efliciency of operating a vacuum tube as a class B amplifier is well known and it is here preferred so to adjust P3 that tube V2 is just at cut-oil when there is no carrier voltage on grid 8. P2 may then be adjusted so that a push-pull alternating voltage on grids I and 8 results in no alternating current in the I output circuit or P2 may be adjusted to provide a still greater negative bias of grid 1 in which case there is a net conductance for tubes VI and V2 over the half-cycle of carrier voltage from oscillator I which V2 is permitted to pass. The value of this net conductance may be varied by suitably setting a tap on potentiometer P2 so that the opposition of tube VI to tube V2 is complete to any desired degree.
With the tap on P2 so placed that no conductance results in VI, the circuit functions as a class B amplifier of the carrier voltage received on grid 8. If a modulating signal voltage is now impressed across the terminals of resistance M, in series between ground and secondarywinding S2, output terminals X and .Y are capable of transmitting a modulated carrier wave to any I desired transmission line or terminal apparatus;
for example, XYmay lead to the crystal 22 of a supersonic valve 23 and the modulated carriervoltage so impressed on crystal 22 may be used to. modulate the light from source 24 transmitted through valve 23 to film 25 asdescribed in the prior art. Film 25 is driven by, conventional means not shown.
'Ii,'now in addition to the modulating signal voltage across resistor 2|, it is arranged to provide a control of the net conductance of tubes- VI and V2 in accordance with the envelope of the modulating signal, one may so arrange matters that the'net carrier voltage appearing across terminals X and 'Y is at all times only that which can be fully modulated by the audio frequency, thereby making possible a noiseless recording on film 25 of the variable density type.
Before providing audio signal and the noise control it is necessary to tune the tank circuit composed of inductance LI and condenser C3 lator I.
the conductance of tube VI. The portion of PI included between tap 30 and ground is in series between ground and secondary winding SI of transformer TI, and the indicated poling of rectifier 28 and connection of circuit B is such that as the level of the audio signal in circuit A varies, the conductance of tube VI is correspondingly varied, thereby providing a net conductance for tubes VI and V2 which varies with the level of the audio signal across resistor 2| which modulates the carrier voltage derived from oscil- It may be preferred, as insurance of greater freedom from distortion in circuit A, to provide for each of circuits A and B a separate amplifier succeeding amplifier 21.
The adjustment of the circuit prior to recording the-audio signal received by microphone 26 is as follows: Oscillator I is energized and tuned to the frequency of crystal 22 which is itself for this adjustment replaced by a dummy load, tube VI being removed from the circuit. V2 is adjusted for class 3 operation. The output circuits of transformer TI and circuit LI-C3 are tuned for maximum carrier output and link circuit 3 is adjusted to provide a carrier voltage on voltmeter VM suflicing to permit full modulation of the light transmitted by supersonic valve 23. I Thereafter crystal 22 and tube VI are replaced and P2. is so adjusted that VI is just at cut-oil with the! carriervoltage applied.
Switches DI and D2 are provided so that in preliminary adjustment either circuit A or circuit B may, as desired, be replaced by a resistor 3| or 32, respectively, without disturbing the adjustment of the companion circuit. If these,
switches are in position as indicated in the figure and the operations just described "have been performed, conditions are such that the whole unit to the carrierv frequency derived from oscillator- I and by adjustment of the coupling of link cir-. cuit,3 to provide across terminals X and! a carrier voltage (tube VI being fully blocked for this purpose) of magnitude required ,to drive the" crystal 22. A vacuum tube voltmeter VM is provided to measure the voltage between the terminals X and Y. Tank circuit LI-C3' serves to provide a sine wave of carrier voltage derived from the class B output of tube VI. A crystal modue lator'of the type here considered is sufllciently highly tuned so that nodetuning of oscillator I is to be feared as the conductances of tubes VI and V2 are varied. It will be noted that secondary SI of transformer TI- is conductively connected to ground through a portion of potentiometer PI in the upper part of the figure. A steady or slowly vary- .ing voltage across PI determines the control of the net conductance of tubes VI and V2 as this dependsupon the grid bias of tube VI.
For the carrier transmission circuit so far described, a modulating and noise controlling cirnoise reduction may now be-made on film 25.x
cuit is provided comprising microphone 26 sucaudio voltage is impressed across resistor 2|. simultaneously, a portion of the output of amplifier 21 is rectified byv a full wave rectifier and'supplied through filter 29 so that a rectified voltage, the envelope of the audio signal, is 'var- 4 operates as a class B modulator wherein an input sound signal received by microphone 26 modulates the carrier voltage derived from oscillator I. The output of rectifier 28 and filter 29 is so poled in conjunction with the initial adjustment of potentiometer P2 that tube VI is not conductive no matter how high the audio input signal may be. A record of the microphone signal without The level of this signal is read on volume indicator VI.
To apply noise reduction, the audio input is removed by suitably operating switch DI and potentiometer P2 is soadjustedthat the conductance of VI efiects partial cancellation of tube V2. Voltmeter VM reads, say EI when VI is permitted a partial conductance and E2 when VI is blocked, so that noise reduction in decibels may be stated as I I [N 0i a--j The setting of tap 30 on potentiometer PI is ,a
margin setting rovidedfor the accommodation of abrupt increasesin audio signal level. Y
In the foregoing description there has been set forth the application of the present invention tothe photographic recording ofsound, but it will be clear that the invention is in no way limited to iably selectedby tap so of potentiometer PI and applied through. circuit B to grid J tacontrol such application and may be used wherever carrier transmission of low frequency signals is f required with or without the advantage'of suppressing to a desired extent the carrier frequency during periods .when theumidulating'signal is of low level or absent.
What is claimed is: 4 l. Ina carrier transmission circuit. means for 2,843,182 generating a voltage of carrier frequency, meansfor simultaneously and differentially amplifying said carrier voltage in opposite phases in a pair of transmission paths, means for controlling the relative amplification in said paths, .means for uniting the opposite phases of said carrier voltage as differentially amplified, means for generating a voltage of signal frequency, means for rectifying a portion of said signal voltage, and means for simultaneously controlling in accordance with said rectified portion the amplification in one only of said paths and modulating said carrier voltage in the other only of said paths by said signal voltage.
2. In a carrier frequency transmission circuit,
.a carrier frequency oscillator, an output circuit for said oscillator, power supply for said oscillator, a pair of vacuum tubes provided each at least with a control grid, a cathode and an anode, power supply for said tubes, a terminal connected to both of said anodes, a grounded terminal to which said cathodes are individually connected through adjustable resistances relatively adjusted to provide a net conductance for said vacuum tubes, individual input circuits between said control grids and said grounded terminal comprising each a resistor in series with inductive coupling to the output circuit of said oscillator, said input circuits being connected for push-pull coupling of said control grids to said output circuit, a source of audio frequency current, means for impressing across the resistor in one of said input circuits a voltage proportional to the instantaneous magnitude of said audio current, means for rectifying a portion of said audio current, and means for-impressing across the resistor in the other of said input circuits a voltage proportional to the magnitude of said rectified current.
3 A sound recording circuit including in combination a supersonic light valve having a pair of terminals, a source supplying supersonic voltage -to' said valve comprising a supersonic oscillator, a pair of vacuum tubes provided each at least with, a cathode, a control grid and an anode, said cathodes being individually connected to ground through variable resistances, said control grids being inductively'coupled m push-pull to said oscillator and said anodes being connected together and to the ungrounded terminal of said valve, a source of audio frequency current, means for supplying to one of said control grids a voltage proportional to the instantaneous value of said current, means for providing a voltage of supersonic frequency, power supply for said oscillator, a pair of amplifying tubes provided each at least with a control grid, a cathode and an anode, power supply for said tubes, a common connection of said anodes to an output terminal, adjustable biasing resisttors individually connecting said cathodes to a common grounded output terminal, said biasing resistors being separately adjusted to provide unequal conductances for said tubes, input circuits individual to said tubes including each a series resistance connectedto said grounded terminal, inductive coupling between said oscillator and said input circuits in push-pull connection, a source of voltage of audio frequency, means for applying said audio frequency voltage across the series resistance in one of said input circuits,
- means for rectifyingca portion of said audio frequency voltage, and means for applying said rectified voltage across the series resistance in the other of said input circuits whereby there is produced between said output terminals a supersonic voltage modulated in accordance with the instantaneous value of said audio frequency voltage, and of average amplitude controlled by said rectified voltage;
5. In a signaling system in which a supersonic frequency is modulated by a signal of audio frequency, the method which consists in generating a voltage of supersonic frequency, amplifying said supersonic voltage differentially and oppositely in phase in a pair of transmission paths, combining'said paths to produce a net amplified supersonic voltage, generating 2, voltage of audio frequency,.introducing said audio voltage in one only of said paths, rectifying a portion of said audio voltage, introducing said rectified voltage in the other only of said paths, and simultaneously controlling the level of said net supersonic voltage in accordance with the envelope of said rectified voltage] and modulating said net supersonic voltage by said audio voltrectifying a portion of, said current, and means for supplying to the other of said control grids a voltage proportional to said rectified current whereby the supersonic voltage-applied to said valve is varied in amplitude in accordance with the envelope of said rectified current.
4. In a sound circuit in combination, an oscillator having an output circuit age.
6. In a carrier signaling system in which a carrier frequency is modulated by signal frequency, the method which consists in generating a voltage of said carrier frequency, amplifying said carrier voltage differentially and in opposite phase in a pair of transmission paths, combining said paths to produce a net amplified supersonic voltage, generating a signal voltage,
introducing said signal voltage in one only of said paths, rectifying a portion of said signal voltage, introducing said rectified voltage in the other only of said paths, and simultaneously controlling the level of said not carrier voltage in accordance with the envelope of said rectified portion and modulating said net carrier voltage by said signal envelope.
FRANK P. HERRNFELD.
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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2726131A (en) * 1952-12-18 1955-12-06 Exxon Research Engineering Co Modulated galvanometer recording of transient signals

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2726131A (en) * 1952-12-18 1955-12-06 Exxon Research Engineering Co Modulated galvanometer recording of transient signals

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