US2374000A - Phase modulator - Google Patents

Phase modulator Download PDF

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Publication number
US2374000A
US2374000A US478255A US47825543A US2374000A US 2374000 A US2374000 A US 2374000A US 478255 A US478255 A US 478255A US 47825543 A US47825543 A US 47825543A US 2374000 A US2374000 A US 2374000A
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phase
impedance
reactance
oscillations
source
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US478255A
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Murray G Crosby
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RCA Corp
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RCA Corp
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    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03CMODULATION
    • H03C3/00Angle modulation
    • H03C3/10Angle modulation by means of variable impedance
    • H03C3/24Angle modulation by means of variable impedance by means of a variable resistive element, e.g. tube
    • H03C3/26Angle modulation by means of variable impedance by means of a variable resistive element, e.g. tube comprising two elements controlled in push-pull by modulating signal

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  • This application concerns a new and improved phase modulation system.
  • phase modulation system In a known type of phase modulation system,
  • oscillations of carrier wave frequency are separated, relatively shifted in phase, differentially modulated in accordance with signals and combined to give resultant phase modulated oscillations.
  • An object of my invention is improved phase modulation of wave energy in accordance with signals.
  • I feed oscillations from a source thereof to a stage such as an amplifier or frequency multiplier by Way of a network, including at leasttwd elements the values of which are differentially modulated in accordance with signals to thereby correspondingly phase modulate the oscillations fed to the said stage.
  • Fig. 1 is a basic' simplified circuit illustrating the network, the manner in which the oscillations are fed thereto, the manner in which the phase shifted oscillations are derived therefrom and the means whereby the network elements are differentially modulated as to value to correspondingly pha modulate the oscillations clerived from the network.
  • Figs. 2 and 3 are modifications of the arrangement'of Fig. 1. l,
  • Fig. 1 an alternating current voltage is supplied to the leads marked I and 2.
  • X is shown as a condenser but may be a resistance or inductance and in my system X is adjusted to be large as compared to the reactance of condenser C or inductance L.
  • P is a potentiometer resistance the total value of which may be about three times the reactances of C or L.
  • this phase shifter is capable of providing about c phase shift without over 12 db. loss in amplitude of the alternating current from input terminals I, 2 to output terminals 3, 4, and about a 5 db. amplitude variation with phase change.
  • phase change range may be from 1350 to n instead of from 45 to 90.
  • potentiometer resistance P is replaced by the impedance between the anodes and cathodes of two tubes 20 and 30.
  • the grids of these tubes aregrounded and the cathod's thereofare raised above ground by biasing resistance 2
  • 40 is a source of oscillations such as, for eXample, a crystal oscillator and multipliers the output of which is impressed on a circuit 42 tuned to the output frequency.
  • the oscillations are fed from this circuit to the phase shifting network and the phase shifted oscillations are fed t0 additional circuits in 50, such as amplifiers, frequency increasers and amplitude limiters, and thence to a utilization circuit such as an antenna.
  • the frequency increasers in 50 may be frequency multipliers or hetero'dynes and mixers.
  • I modulate the grid potentials to vary the cathode to groun impedances of the tubes 20 and v3l), instead of the plate to cathode impedances, as in Fig. 2'.
  • cent degenerative feedback is used sistances are suitable ,cies
  • cathodes 25 and 35 are connected to grotmd through bias resistor 3l shunted by a radio frequency by-pass condenser. 'I'he anodes are tied together and connected to a source of potential through a radio frequency cholrel RFC. 39 is a radio frequency by-pass condenser.
  • tubes 20 and 30 connected as in Fig. 3 about 100 perand the cathode to ground impedancescan be modulated to very low values. Since the cathode to ground impedances go to lower values (of the order of a few hundred o hms) the range of phase variation obtainable by this modification of my system is greater than say the range obtainable in the modincation of Fig.
  • ZIc and Zlcl are two circuits used to tune out the cathode capacities of the tubes at the higher carrier frequencies.
  • the tuned circuits are used as shown to obtain astill wider phase variation obtainable in the phase shifting network.
  • Zic and Zkl may be replacedby resistances.
  • a pair of reactances of opposite sign connected together by an impedance having thereon a movable tap, a connection connecting the free terminals of said reactances together, a second value of which is large as compared to the value of either of said reactances connected to the terminals of said reactances tied together, connections for applying alternating current of substantially constant frequency to the other terminal of said second impedance and to said movable tap and connections to said movable tap and the terminals of said reactances tied together for deriving alternating current, the phase of which depends upon position of said tap on said impedance.
  • a source of alternating current of substantially constant carrier wave frequency a utilization circuit, connections one of which includes an impedance coupling said source to said utilization circuit, a first reactance and a rst dischargetube impedance in series across said utilization circuit, a second reactance of opposite sign and a second discharge tube impedance in series across said utilization circuit, said rst and second reactances being of small value relative to the value ofsaid impedance, and means for modulating the impedances of said tubes differentially in accordance with signals.
  • a source of alternating current ofsubstantially constant carrier wave frequency a utilization circuit, connections one of which includes an impedance couplingsaid source to said utilization circuit, a first reactance, and a iirst discharge ⁇ tube having its output impedance in series with the iirst reactance across said nections, a second reactance of opposite sign and a second discharge tube having its output impedance in series with the second reactance across said connections, said ilrst and second reactances being of small value relative to the value grid and an anode, 4second and third impedances coupling the cath- ,n
  • said utilization circuit a second reactance of opposite sign and a third impedance in shunt to said utilization circuit, a pair of electron discharge tubes each having a cathode, a control connections including said odes of said tubes to said first connection, a connection tying the anodesto said devices together and to a source of constant potential, andmeans for modulating the impedances of said tubes differentially in accordance with signals to thereby correspondingly vary the values of said second and third impedances.
  • two input terminals to which alternating current may be applied a pair of output terminals, a connection of low impedance between one input terminal and one output terminal, a second connection including an impedance coupling the other input terminal to the other output terminal, va first reactance having one terminal coupled to said other output terminal, a second reactance of opposite sign having one terminal coupledto said other output terminal, two differentially variable imone connecting the other terminal of one reactance to said one output terminal, the other diierential impedance connecting the other terminal of the other reactance to said one output terminal, saidiirst and second reactances being of small value relative to the value of said iirst impedance, and means for varying the impedances of said two differentially variable impedances differentially to thereby vary the phase of the current supplied to said output terminals.
  • a source of alternating current, output terminals a connection of low impedance to current of the frequency of said source coupling said source to one of said output terminals, a connection including an impedance between said source and the other of said output terminals, aiirst reactance and a tuned circuit in shunt to said output terminals, a second reactance oi opposite signsaid devices diierentially in accordance with signais.

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Description

April 17, 194s.
M. G. CROSBY PHASE MoDULAToR Filed Maron 6, 1945 -Hlllv qw w T m m. x v N 91u V m. f ,l zw. .mrlfkll Patented Apr. 17, 1945 PHASE MODULATOR Murray G. Crosby, Riverhead, N. Y., assigner to Radio Corporation of America, a corporation of Delaware Application March 6, 1943, Serial No. 478,255
6 Claims.
This application concerns a new and improved phase modulation system.
In a known type of phase modulation system,
oscillations of carrier wave frequency are separated, relatively shifted in phase, differentially modulated in accordance with signals and combined to give resultant phase modulated oscillations. I
An object of my invention is improved phase modulation of wave energy in accordance with signals.
In my present simplified and improved system I feed oscillations from a source thereof to a stage such as an amplifier or frequency multiplier by Way of a network, including at leasttwd elements the values of which are differentially modulated in accordance with signals to thereby correspondingly phase modulate the oscillations fed to the said stage.
In describing my invention reference will be made to the attached drawing, wherein Fig. 1 is a basic' simplified circuit illustrating the network, the manner in which the oscillations are fed thereto, the manner in which the phase shifted oscillations are derived therefrom and the means whereby the network elements are differentially modulated as to value to correspondingly pha modulate the oscillations clerived from the network.
Figs. 2 and 3 are modifications of the arrangement'of Fig. 1. l,
In Fig. 1 an alternating current voltage is supplied to the leads marked I and 2. X is shown as a condenser but may be a resistance or inductance and in my system X is adjusted to be large as compared to the reactance of condenser C or inductance L. P is a potentiometer resistance the total value of which may be about three times the reactances of C or L. With the adjustable arm of P on the point a there is no phase shift in the voltage supply from terminals l and 2 to terminals 3 and 4, if we assume that X is a condenser. This is because the impedance of L and the resistance of P will constitute a relatively negligible impedance across C so that X and condenser C act merely as a capacity potentiometer. arm moved to pointb the impedance of condenser C in series with the resistance of P becomes a relatively negligible impedance across inductance L, so that the current through inductance L will produce therein an inductive drop which leads the current. The phase of the current is determined by X since X Iis large. The drop across theinductance L can therefore With the potentiometer be made 180"J leading when the potentiometer arm is on point b. It will be apparent that for intermediate positions of the potentiometer arm phase shifts from zero to 180 are obtainable.
In the practicable case the full range of 18()3 is not obtainable because the shunting effect of inductance L in series with resistance P is not negligible across condenser C and likewise the shunting element of condenser C in series with resistance P is not negligible across the inductance L.
It was found experimentally that this phase shifter is capable of providing about c phase shift without over 12 db. loss in amplitude of the alternating current from input terminals I, 2 to output terminals 3, 4, and about a 5 db. amplitude variation with phase change.
It will be apparent that if elementX is inductance or capacity in place of resistance the range of phase change will be the same but the phase change at the extreme positions a and b will be different. For example, the phase change range may be from 1350 to n instead of from 45 to 90.
If oscillations of carrier wave frequency are applied at the terminals l and 2 and the army of potentiometer P is moved in accordance with signals, oscillations modulated in phase in accordance with saidsignals` will appear at the output terminals 3, 4.
In the modification of Fig. 2 the potentiometer resistance P is replaced by the impedance between the anodes and cathodes of two tubes 20 and 30. The grids of these tubes aregrounded and the cathod's thereofare raised above ground by biasing resistance 2| and differentially modulated to modulate the carrier phase in accordance with signals from a source v34 fed to a transformer 36 and thence to the cathodes differentially. 40 isa source of oscillations such as, for eXample, a crystal oscillator and multipliers the output of which is impressed on a circuit 42 tuned to the output frequency. The oscillations are fed from this circuit to the phase shifting network and the phase shifted oscillations are fed t0 additional circuits in 50, such as amplifiers, frequency increasers and amplitude limiters, and thence to a utilization circuit such as an antenna. The frequency increasers in 50 may be frequency multipliers or hetero'dynes and mixers.
In the modification of Fig. 3, I modulate the grid potentials to vary the cathode to groun impedances of the tubes 20 and v3l), instead of the plate to cathode impedances, as in Fig. 2'. The
, cent degenerative feedback is used sistances are suitable ,cies
cathodes 25 and 35 are connected to grotmd through bias resistor 3l shunted by a radio frequency by-pass condenser. 'I'he anodes are tied together and connected to a source of potential through a radio frequency cholrel RFC. 39 is a radio frequency by-pass condenser. With tubes 20 and 30 connected as in Fig. 3 about 100 perand the cathode to ground impedancescan be modulated to very low values. Since the cathode to ground impedances go to lower values (of the order of a few hundred o hms) the range of phase variation obtainable by this modification of my system is greater than say the range obtainable in the modincation of Fig. 2, wherein the anode to cathode impedances of the tubes 20 and 30 are modulated. In Fig. 3 ZIc and Zlcl are two circuits used to tune out the cathode capacities of the tubes at the higher carrier frequencies. In this preferred modification the tuned circuits are used as shown to obtain astill wider phase variation obtainable in the phase shifting network. In a modification Zic and Zkl may be replacedby resistances. Re-
I claim:
1. In a system of the class described, a pair of reactances of opposite sign connected together by an impedance having thereon a movable tap, a connection connecting the free terminals of said reactances together, a second value of which is large as compared to the value of either of said reactances connected to the terminals of said reactances tied together, connections for applying alternating current of substantially constant frequency to the other terminal of said second impedance and to said movable tap and connections to said movable tap and the terminals of said reactances tied together for deriving alternating current, the phase of which depends upon position of said tap on said impedance.
impedance the for lower carrier frequenpedances,
2. In a modulation system `of the nature described, a source of alternating current of substantially constant carrier wave frequency, a utilization circuit, connections one of which includes an impedance coupling said source to said utilization circuit, a first reactance and a rst dischargetube impedance in series across said utilization circuit, a second reactance of opposite sign and a second discharge tube impedance in series across said utilization circuit, said rst and second reactances being of small value relative to the value ofsaid impedance, and means for modulating the impedances of said tubes differentially in accordance with signals.
3. In a modulation/system of Ythe nature described, a source of alternating current ofsubstantially constant carrier wave frequency, a utilization circuit, connections one of which includes an impedance couplingsaid source to said utilization circuit, a first reactance, and a iirst discharge `tube having its output impedance in series with the iirst reactance across said nections, a second reactance of opposite sign and a second discharge tube having its output impedance in series with the second reactance across said connections, said ilrst and second reactances being of small value relative to the value grid and an anode, 4second and third impedances coupling the cath- ,n
said utilization circuit, a second reactance of opposite sign and a third impedance in shunt to said utilization circuit, a pair of electron discharge tubes each having a cathode, a control connections including said odes of said tubes to said first connection, a connection tying the anodesto said devices together and to a source of constant potential, andmeans for modulating the impedances of said tubes differentially in accordance with signals to thereby correspondingly vary the values of said second and third impedances.
5. In a current phase changing system, two input terminals to which alternating current may be applied, a pair of output terminals, a connection of low impedance between one input terminal and one output terminal, a second connection including an impedance coupling the other input terminal to the other output terminal, va first reactance having one terminal coupled to said other output terminal, a second reactance of opposite sign having one terminal coupledto said other output terminal, two differentially variable imone connecting the other terminal of one reactance to said one output terminal, the other diierential impedance connecting the other terminal of the other reactance to said one output terminal, saidiirst and second reactances being of small value relative to the value of said iirst impedance, and means for varying the impedances of said two differentially variable impedances differentially to thereby vary the phase of the current supplied to said output terminals.
6. In a current phase modulating system, a source of alternating current, output terminals, a connection of low impedance to current of the frequency of said source coupling said source to one of said output terminals, a connection including an impedance between said source and the other of said output terminals, aiirst reactance and a tuned circuit in shunt to said output terminals, a second reactance oi opposite signsaid devices diierentially in accordance with signais.
MURRAY G. CROSBY.
US478255A 1943-03-06 1943-03-06 Phase modulator Expired - Lifetime US2374000A (en)

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Cited By (12)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2502095A (en) * 1943-08-25 1950-03-28 Rca Corp Phase modulation
US2524992A (en) * 1947-03-27 1950-10-10 Ericsson Telefon Ab L M Frequency modulator
US2530937A (en) * 1946-06-25 1950-11-21 Westinghouse Electric Corp Frequency modulator
US2541650A (en) * 1943-05-06 1951-02-13 Hartford Nat Bank & Trust Co Wave length modulation
US2551802A (en) * 1948-01-05 1951-05-08 Rca Corp Phase modulator
US2559023A (en) * 1949-02-21 1951-07-03 United Geophysical Company Inc Phase modulation
US2579590A (en) * 1946-12-13 1951-12-25 Westinghouse Electric Corp Frequency modulator
US2588551A (en) * 1949-02-21 1952-03-11 United Geophysical Company Inc Frequency modulation
US2610318A (en) * 1947-12-03 1952-09-09 Int Standard Electric Corp Electronic frequency modulator
US2841769A (en) * 1953-07-08 1958-07-01 Marconi Wireless Telegraph Co Frequency modulated oscillation generators
US2956242A (en) * 1957-10-22 1960-10-11 Philamon Lab Inc Tuning fork oscillator
US2962671A (en) * 1956-02-23 1960-11-29 Bell Aerospace Corp Balanced frequency modulation for transmitters

Cited By (12)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2541650A (en) * 1943-05-06 1951-02-13 Hartford Nat Bank & Trust Co Wave length modulation
US2502095A (en) * 1943-08-25 1950-03-28 Rca Corp Phase modulation
US2530937A (en) * 1946-06-25 1950-11-21 Westinghouse Electric Corp Frequency modulator
US2579590A (en) * 1946-12-13 1951-12-25 Westinghouse Electric Corp Frequency modulator
US2524992A (en) * 1947-03-27 1950-10-10 Ericsson Telefon Ab L M Frequency modulator
US2610318A (en) * 1947-12-03 1952-09-09 Int Standard Electric Corp Electronic frequency modulator
US2551802A (en) * 1948-01-05 1951-05-08 Rca Corp Phase modulator
US2559023A (en) * 1949-02-21 1951-07-03 United Geophysical Company Inc Phase modulation
US2588551A (en) * 1949-02-21 1952-03-11 United Geophysical Company Inc Frequency modulation
US2841769A (en) * 1953-07-08 1958-07-01 Marconi Wireless Telegraph Co Frequency modulated oscillation generators
US2962671A (en) * 1956-02-23 1960-11-29 Bell Aerospace Corp Balanced frequency modulation for transmitters
US2956242A (en) * 1957-10-22 1960-10-11 Philamon Lab Inc Tuning fork oscillator

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