US3087124A - Feedback system for reed modulated magnetrons - Google Patents

Feedback system for reed modulated magnetrons Download PDF

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US3087124A
US3087124A US738892A US73889258A US3087124A US 3087124 A US3087124 A US 3087124A US 738892 A US738892 A US 738892A US 73889258 A US73889258 A US 73889258A US 3087124 A US3087124 A US 3087124A
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anode
reed
plate
feedback
frequency
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Jr Willard W Mcleod
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Raytheon Co
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J23/00Details of transit-time tubes of the types covered by group H01J25/00
    • H01J23/16Circuit elements, having distributed capacitance and inductance, structurally associated with the tube and interacting with the discharge
    • H01J23/18Resonators
    • H01J23/20Cavity resonators; Adjustment or tuning thereof
    • H01J23/207Tuning of single resonator
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03CMODULATION
    • H03C3/00Angle modulation
    • H03C3/30Angle modulation by means of transit-time tube
    • H03C3/32Angle modulation by means of transit-time tube the tube being a magnetron

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  • This invention relates to electron ldischarge devices, and more particularly, to feedback means for stabilizing the frequency modulation characteristics of tunable election discharge devices of the frequency modulated megnetron type.
  • the vibratory reed or tunable element In an electron discharge device of the vibratory reed megnetron type, in which the frequency of the megnetron is a function of the capacity Ibetween the anode straps, the vibratory reed or tunable element usually supports a sensing coil and .a drive coil adjacent to the anode and is movable with respect to the anode straps for tuning the device.
  • the sensing or pick-up coil senses the motion of the vibratory reed or tunable element and produces a feedback voltage which is combined with a modulating input signal and amplified in ⁇ a feedback amplifier.
  • the output of this amplifier is connected to the drive coil to produce an electromagnetic field which interacts with the magnetic field of the magnetron to impart motion to the reed.
  • the drive coil operates to damp and control the motion of the reed to conform more accurately to the input frequency modulating signal.
  • the magnetron frequency is a function of the spacing between the reed or tunable element and the anode
  • a two coil system of this type does not directly compensate for variations in Spacing between the reed and the anode.
  • the feedback voltage so developed controls only the motion of the reed and not the capacity between the reed and the anode straps.
  • a capacity plate is insulatedly supported by the vibratory reed or tunable element and positioned adjacent to the straps of a frequency modulated magnetron in order to form a capacity pick-off to develop a feedback voltage.
  • This feedback voltage is fed to the input stage of a feedback amplier connected to a drive coil supported by the vibratory reed element.
  • the capacity plate is insulated from and biased with respect to the anode of the magnetron by means of a high impedance input circuit which introduces the frequency modulated input signal and the feedback voltage into the feedback amplier.
  • the time constant of this input circuit is made short relative to the input modulating frequency to permit the feedback voltage signal to be proportional -to the rate of change of capacitance between the capacity plate and the anode straps.
  • This feedback then provides frequency modulation Which is proportional and linear with the input modulating signal.
  • the voltage derived by the capacity pick-olf plate Will be a function of one over the reed to anode spacing, which is the same as the frequency modulating characteristics of the vibratory reed element.
  • the effective capacity between the straps of the magnetron is controlled Aby a capacity feedback system of this type and, thus, compensation is introduced for the non-linearity of the reed modulation element.
  • the rate of change of frequency of the magnetron is proportional to and linear with the input signal to the amplifier.
  • the direct coupling between the drive and pick-up elements and the resulting limitation on frequency response is substantially eliminated.
  • the system of this invention constitutes an improvement over the system disclosed in U.S. Patent No. 2,750,565 of William R. Mercer et al., issued June 12, 1956.
  • FIG. l is la fragmentary longitudinal sectional view taken through the center of the magnetron of the vibrating reed type showing the capacity plate and driving coil on the tunable reed element;
  • FIG. 2 is a simplified schematic of the magnetron feedback circuit of the subject invention in which the capacity feedback plate is connected in a manner to affect the input signal to the driving coil, hereinafter referred to as a closed loop circuit; and
  • FIG 3 is an enlarged, fragmentary View of a portion of FiG. 1 showing the vibratory reed element and the capacity plate.
  • FIG. 1 illustrates a frequency modulated magnetron, generally indicated by reference numeral 10, which utilizes a vibrating reed assembly upon which a driving coil and a capacity plate are mounted.
  • Magnetron 10 comprises an anode structure 11, a cathode structure 12 (only partially shown), magnetic means including pole pieces 13 and 14 for establishing a magnetic eld in a direction perpendicular to the path of theI electron flow between said cathode and anode structures, and a vibratory reed assembly or tunable element 15.
  • anode structure 11 includes a cylindrical body 16 made of highly conductive material, such as copper, and having a plurality of radially extending anode vanes 17, as is Well known in the magnetron art. Surrounding ⁇ the cylindrical body 16 is a cover assembly 18 which functions as a magnetic return path for pole pieces 13 and 14. Anode structure 11 is closed at the ends, for example, by end plates 19 and 20 hermetically sealed at the junction between said plates and cylindrical body 16, as shown at 21.
  • the cathode structure 12 is coaxially arranged with respect to the anode structure and comprises a cathode heating filament 22 which passes through a recess in the pole piece 14 in the usual manner.
  • the cathode may be supported and insulated ⁇ from the anode structure in the manner shown by Becker in U.S. Patent No. 2,566,478, dated September 4, 1951.
  • pole pieces 13 is hermetically sealed, as at 25, into the end plate 19.
  • the other pole piece 14 is broken ⁇ away at 26 and shows a centrally located bore which allows for entry of cathode assembly 12.
  • This pole piece may be hermetically sealed as at 27 into the end plate 2li.
  • Pole pieces 13 and 14- are adapted to be fixed to the opposite ends of a magnet, such as bar magnets (not shown) for producing an appropriate magnetic field, as noted, in a direction normal to the path of electrons flowing from cathode to anode.
  • a coupling device 28 connected to one of the anode vanes ⁇ 17 serves to couple energy out of the magnetron and 3 is brought out through outlet pipe 30 ⁇ which engages cylindrical body ⁇ lla of anode structure il and extends through the cover assembly 18.
  • the anode -vanes 17 are each provided With a slot 31 f or receiving ⁇ a pair'of concentric conducting straps 32 and 33 which contact alternate anode vanes. As is well known in the magnetron art, the aforesaid straps present a capacitance therebetween which partially determines the natural resonant frequency of the magnetron.
  • a vibrating reed assembly 15 includes a capacity plate 34 which is moved with respect to anode vanes 17, that is with respect to straps 32 and 33, whereby the distributed capacitance may be altered so that the magnetron may be Ivaried in frequency.
  • the capacitance or capacity plate 34 takes the form of a metalized coating on an annular ceramic diaphragm 40 which is secured to the lower flanged portion of a hollow cylindrical core 36.
  • the core 36 forming part of the tunable reed element 15 is secured, as by soldering, to a ring or fiange portion 37 of the tunable element which, in turn, is secured at its periphery, to a supporting ledge 38 of Ycylindrical body d6 of anode structure 1l.
  • the capacitive plate 34 as shown in FIG. 3, consists of a metalized surface on the ceramic insert ttl secured to reed-like flange 46 partially surrounded by an extension of corre 36 and adjacent to core bracket 39.
  • the ceramic support 40 insulates the capacitive plate 34 from the tuning assembly 15 and, in particular, from the core or metallic support 3bl for a drive coil 5t).
  • the output lead il then passes through an opening 4 4 in cover assembly 18 and, together with a lead i5 connected to the anode assembly, provides a means for introducing the feedback voltage into the input circuitry of the feedback amplifier.
  • the drive coil 50 ⁇ as shown in FiG. 3, preferably consists of approximate-1y 20y turns of insulated wire which is wound upon the hollow core 36 and firmly attached thereto.
  • the ends of drive coil 50 are led out of the magnetron through an aperture in the ring or flange portion 37 of the tunable element and through a glass seal 52 fused into the upper end plate i9.
  • Output leads 54 and 55 are connected to the ends of coil 5t? extending beyond the glass seal 52.
  • the tunable reed assembly i5 and the driving coil Sil carried lthereon are disposed relative to the pole pieces 13 and 14 so that the drive coil 5G is in the leakage field existing between said pole pieces.
  • a square wave applied to the input terminals 6'9, 60 is coupled to feedback amplifier 6i by way of an input circuit 62.
  • This circuit comprises a .5 megohm input resistor 63, and a .l microfared coupling capacitor 54 which isolates the negative bias voltage from the input of amplifier 61.
  • the insulated capacitive plate 34g isl biased at a negative voltage of minus 400 vo'rts with respect -to the grounded anode structure 17 by means of a bias source 65 and .5 megohm bias resistor 66.
  • the out put of amplifier all is coupled through an output transformer 68 ⁇ to the driving coil Si? shown in HG. l.
  • the core about which the drive coil 50 is securely wound is adapted to move to and fro between the magnetic pole pieces )i3 and 14;- as shown by the arrows.
  • the feedback voltage which is developed by the capacity plate 34 is fed to the input circuit of the amplifier, the time constant of which is made short relative to the square wave input modulating lvoltage at terminals 6i), 60.
  • the feedback voltage and input signal become proportional to the rate of change of capacitance between the capacity plate 34 and the anode straps 32 and 33.
  • This feedback circuit therefore, provides a rate of change of frequency which is proportional to the input modulating signal.
  • the capacity plate provides that the feedback voltage is a function of one over the reed to anode spacing which is the same as the modulation characteristics of the vibrating tunable e1e ment.
  • the feedback voltage is a function of one over the reed to anode spacing which is the same as the modulation characteristics of the vibrating tunable e1e ment.
  • the error or feedback voltage derived across the capacitive plate is fed to the amplifier input circuit7 combined with the input signal voltage and reamplified in phase opposition so as to tend to cancel out the error originally generated by irregularities in the drive coil motion.
  • the electrically insulated capacity plate may be used to regulate the frequency response of other than electron discharge device-s.
  • the non-linear response of, for example, a driving coil applied to a magnetic transducer, in an arrangement as shown in FG. 3, may be compensated by the feedback voltage developed in this closed loop feedback system, or other non-linear electromechanical vibrating assemblies may attain similar advantages.
  • a frequency modulation circuit comprising an electron discharge device including a cathode, an anode, means for producing a magnetic field and a tunable element positioned in said magnetic field, said tunable element including a conductive plate insulatedly supported thereon and 'adjacent to said anode in a manner adapted to vary the frequency of said electron discharge device in response to movement of said plate, means for varying the position of said plate including a driving element mounted on said tunable element, means for applying an input voltage to said driving coil, means for developing a feedback voltage in response to variations in electrical charge on said plate due to changes of capacitance between said plate and said anode, and means for combining said feedback voltage with said input Voltage to apply a modulating voltage to said driving element.
  • a frequency modulation circuit comprising means for establishing a flow of electrons in a given direction, means for establishing a magnetic field in a direction substantially perpendicular to such direction of electron flow, and means mounted for movement within such magnetic field and adjacent such electron fiow to both frequencymodulate such electron flow in accordance with such movement and provide a capacitive pick-off the amplitude of which varies in linear relationship with such movement, whereby the variable capacitance of said pick-off may be employed to control feedback circuitry the output of which is combined with drive signals applied to said frequency modulating means to stabilize the operation of such lastmentioned means.
  • a frequency modulation circuit comprising means for establishing a iiow of electrons in a given direction, means for establishing a magnetic field in a direction substantially perpendicular to such direction of electron iiow, means mounted for movement within such magnetic field and adjacent such electron flow to both frequency-modulate such electron flow in accordance with such movement and provide a capacitive pick-olf the amplitude of which varies in linear relationship with such movement, means for effecting movement of said frequency modulating means in accordance with a modulating signal, and means connected in feedback relationship between said capacitive pick-off means and said means for effecting movement.
  • a frequency modulation circuit comprising an electron discharge device including a cathode, an anode, and means for establishing a magnetic field in a direction substantially perpendicular to the path of the electron flow between said cathode and said anode, a mechanical tuning means positioned in said magnetic iield, and a conductive plate insulatedly supported -by said tuning means within said device in capacitive relationship with said anode, said tuning means being mounted for movement relative to said anode to vary the distance between said conductive plate and said anode and thereby vary such capacitive ⁇ relationship linearly with respect to such movement, whereby the movement of said conductive plate serves both to frequency-modulate the electron ow from said cathode to said anode and to provide -a capacitive pickoff which varies linearly with such movement.
  • a frequency modulation circuit comprising an electron discharge device having a cathode, an anode yand a magnetic circuit having a field portion substantially perpendicular to a ow of electrons between said cathode and said anode, a vibratory member mounted for movement within such magnetic eld adjacent such electron flow, a drive coil mounted on said vibratory member, an input circuit for said drive coil for applying modulating signals thereto to cause corresponding movement of said coil and vibratory member as la result of interaction between the magnetic fields of said coil and said magnetic circuit, a conductive plate member mounted on and insulated from said vibratory member for movement toward -and away from said anode in capacitive relationship therewith, and a feedback circuit connected between said insulated conductive plate member and said input circuit, whereby such movement of said conductive plate member serves both to frequency-modulate the electron flow from said cathode to said anode and to provide a variable capacitance control for such feedback circuit which varies linearly with the movement of said conductive plate member.

Description

April 23, 1963 w. w. MCLEOD, JR 3,0875124 FEEDBACK SYSTEM FOR REED MODULATED MAGNETRONS Filed May 29, 195e M//u/Wo W Mdsoa, J2
,4 rroe/vgy 3,087,124 Patented Apr. 23, 1963 ice 3,087,124 FEEDBACK SYSTEM FOR REED MODULATED MAGNETRQNS Willard W. McLeod, fr., Lexington, Mass., assigner to Raytheon Company, Lexington, Mass., a corporation of Delaware Filed May 29, 1958, Ser. No. 738,892 Qlaizns. (Cl. 332-16) This invention relates to electron ldischarge devices, and more particularly, to feedback means for stabilizing the frequency modulation characteristics of tunable election discharge devices of the frequency modulated megnetron type.
In an electron discharge device of the vibratory reed megnetron type, in which the frequency of the megnetron is a function of the capacity Ibetween the anode straps, the vibratory reed or tunable element usually supports a sensing coil and .a drive coil adjacent to the anode and is movable with respect to the anode straps for tuning the device. As is known, the sensing or pick-up coil senses the motion of the vibratory reed or tunable element and produces a feedback voltage which is combined with a modulating input signal and amplified in `a feedback amplifier. The output of this amplifier is connected to the drive coil to produce an electromagnetic field which interacts with the magnetic field of the magnetron to impart motion to the reed. In this manner, the drive coil operates to damp and control the motion of the reed to conform more accurately to the input frequency modulating signal. However, since the magnetron frequency is a function of the spacing between the reed or tunable element and the anode, a two coil system of this type does not directly compensate for variations in Spacing between the reed and the anode. As a result, the feedback voltage so developed controls only the motion of the reed and not the capacity between the reed and the anode straps.
In addition, undesirable transformer coupling between the drive and the pick-up coils tends to cancel out the feedback voltage and limit the frequency response of the feedback system so that it is difficult, if not inrpossible, to control the motion of the reed at high frequencies. As a result, the frequency response of the tunable element or reed modulator is Seriously limited in the region in which the feedback voltage is impaired. It is therefore desirable to provide a feedback system in which the capacity between the anode straps of a frequency modulated magnetron is varied in a linear manner in order to improve the frequency response of the reed modulator and, thereby, obtain linear frequency modulation.
In accordance with the reed modulated feedback system of this invention, a capacity plate is insulatedly supported by the vibratory reed or tunable element and positioned adjacent to the straps of a frequency modulated magnetron in order to form a capacity pick-off to develop a feedback voltage. This feedback voltage is fed to the input stage of a feedback amplier connected to a drive coil supported by the vibratory reed element. The capacity plate is insulated from and biased with respect to the anode of the magnetron by means of a high impedance input circuit which introduces the frequency modulated input signal and the feedback voltage into the feedback amplier. The time constant of this input circuit is made short relative to the input modulating frequency to permit the feedback voltage signal to be proportional -to the rate of change of capacitance between the capacity plate and the anode straps. This feedback then provides frequency modulation Which is proportional and linear with the input modulating signal. In addition, the voltage derived by the capacity pick-olf plate Will be a function of one over the reed to anode spacing, which is the same as the frequency modulating characteristics of the vibratory reed element. In this manner, the effective capacity between the straps of the magnetron is controlled Aby a capacity feedback system of this type and, thus, compensation is introduced for the non-linearity of the reed modulation element. With this arrangement, the rate of change of frequency of the magnetron is proportional to and linear with the input signal to the amplifier. In addition, the direct coupling between the drive and pick-up elements and the resulting limitation on frequency response is substantially eliminated.
The system of this invention constitutes an improvement over the system disclosed in U.S. Patent No. 2,750,565 of William R. Mercer et al., issued June 12, 1956.
Other and further advantages of this invention will be apparent as the description thereof progresses, reference being had to the accompanying drawings, wherein:
FIG. l is la fragmentary longitudinal sectional view taken through the center of the magnetron of the vibrating reed type showing the capacity plate and driving coil on the tunable reed element;
FIG. 2 is a simplified schematic of the magnetron feedback circuit of the subject invention in which the capacity feedback plate is connected in a manner to affect the input signal to the driving coil, hereinafter referred to as a closed loop circuit; and
FIG 3 is an enlarged, fragmentary View of a portion of FiG. 1 showing the vibratory reed element and the capacity plate.
FIG. 1 illustrates a frequency modulated magnetron, generally indicated by reference numeral 10, which utilizes a vibrating reed assembly upon which a driving coil and a capacity plate are mounted. Magnetron 10 comprises an anode structure 11, a cathode structure 12 (only partially shown), magnetic means including pole pieces 13 and 14 for establishing a magnetic eld in a direction perpendicular to the path of theI electron flow between said cathode and anode structures, and a vibratory reed assembly or tunable element 15.
As shown in FIG. 1, anode structure 11 includes a cylindrical body 16 made of highly conductive material, such as copper, and having a plurality of radially extending anode vanes 17, as is Well known in the magnetron art. Surrounding `the cylindrical body 16 is a cover assembly 18 which functions as a magnetic return path for pole pieces 13 and 14. Anode structure 11 is closed at the ends, for example, by end plates 19 and 20 hermetically sealed at the junction between said plates and cylindrical body 16, as shown at 21. The cathode structure 12 is coaxially arranged with respect to the anode structure and comprises a cathode heating filament 22 which passes through a recess in the pole piece 14 in the usual manner. The cathode may be supported and insulated `from the anode structure in the manner shown by Becker in U.S. Patent No. 2,566,478, dated September 4, 1951.
One of the pole pieces 13 is hermetically sealed, as at 25, into the end plate 19. The other pole piece 14 is broken `away at 26 and shows a centrally located bore which allows for entry of cathode assembly 12. This pole piece may be hermetically sealed as at 27 into the end plate 2li. Pole pieces 13 and 14- are adapted to be fixed to the opposite ends of a magnet, such as bar magnets (not shown) for producing an appropriate magnetic field, as noted, in a direction normal to the path of electrons flowing from cathode to anode.
A coupling device 28 connected to one of the anode vanes `17 serves to couple energy out of the magnetron and 3 is brought out through outlet pipe 30 `which engages cylindrical body `lla of anode structure il and extends through the cover assembly 18.
The anode -vanes 17 are each provided With a slot 31 f or receiving `a pair'of concentric conducting straps 32 and 33 which contact alternate anode vanes. As is well known in the magnetron art, the aforesaid straps present a capacitance therebetween which partially determines the natural resonant frequency of the magnetron.
Referring now to FIGS. l and 3, a vibrating reed assembly 15 includes a capacity plate 34 which is moved with respect to anode vanes 17, that is with respect to straps 32 and 33, whereby the distributed capacitance may be altered so that the magnetron may be Ivaried in frequency. vThe capacitance or capacity plate 34 takes the form of a metalized coating on an annular ceramic diaphragm 40 which is secured to the lower flanged portion of a hollow cylindrical core 36. The core 36 forming part of the tunable reed element 15 is secured, as by soldering, to a ring or fiange portion 37 of the tunable element which, in turn, is secured at its periphery, to a supporting ledge 38 of Ycylindrical body d6 of anode structure 1l.
The capacitive plate 34, as shown in FIG. 3, consists of a metalized surface on the ceramic insert ttl secured to reed-like flange 46 partially surrounded by an extension of corre 36 and adjacent to core bracket 39. The end of core 36 opposite from core bracket 39, is braced by means of support 4S extending diagonally to the vibrator portion 49 of the reed-like ange 46. The ceramic support 40 insulates the capacitive plate 34 from the tuning assembly 15 and, in particular, from the core or metallic support 3bl for a drive coil 5t). Connected to the metallic capacitive plate is =a wire output lead 41 which passes through an opening 4Z in anode ring or fiange 37 and out yof the magnetron through la glass seal i3 in the end plate 19. The output lead il then passes through an opening 4 4 in cover assembly 18 and, together with a lead i5 connected to the anode assembly, provides a means for introducing the feedback voltage into the input circuitry of the feedback amplifier.
The drive coil 50, `as shown in FiG. 3, preferably consists of approximate-1y 20y turns of insulated wire which is wound upon the hollow core 36 and firmly attached thereto. The ends of drive coil 50 are led out of the magnetron through an aperture in the ring or flange portion 37 of the tunable element and through a glass seal 52 fused into the upper end plate i9. Output leads 54 and 55 are connected to the ends of coil 5t? extending beyond the glass seal 52. The tunable reed assembly i5 and the driving coil Sil carried lthereon are disposed relative to the pole pieces 13 and 14 so that the drive coil 5G is in the leakage field existing between said pole pieces. When an external modulating voltage is applied to leads 54 and 55, the electromagnetic field set up between the current flowing in driving coil 5f) and the leakage magnetic field of the magnetron interact to produce motion of core 36 and is accompanying capacitive plate 34 with respect to the anode straps 32 and 33. in this manner, the distributed capacitance ofthe magnetron is varied and frequency modulation obtained. As the tuning element vibrates to and fro in response to the drive coil input, a capacitive pick-off voltage is generated on the capacitive plate 34 which is fed by way of lead di to the input terminals of a feedback amplifier 6l.
Referring to FIG. 2, a square wave applied to the input terminals 6'9, 60 is coupled to feedback amplifier 6i by way of an input circuit 62. This circuit comprises a .5 megohm input resistor 63, and a .l microfared coupling capacitor 54 which isolates the negative bias voltage from the input of amplifier 61. The insulated capacitive plate 34g isl biased at a negative voltage of minus 400 vo'rts with respect -to the grounded anode structure 17 by means of a bias source 65 and .5 megohm bias resistor 66. The out put of amplifier all is coupled through an output transformer 68` to the driving coil Si? shown in HG. l. The core about which the drive coil 50 is securely wound is adapted to move to and fro between the magnetic pole pieces )i3 and 14;- as shown by the arrows. The feedback voltage which is developed by the capacity plate 34 is fed to the input circuit of the amplifier, the time constant of which is made short relative to the square wave input modulating lvoltage at terminals 6i), 60. In this closed loop circuit, the feedback voltage and input signal become proportional to the rate of change of capacitance between the capacity plate 34 and the anode straps 32 and 33. This feedback circuit, therefore, provides a rate of change of frequency which is proportional to the input modulating signal. At the same time, the capacity plate provides that the feedback voltage is a function of one over the reed to anode spacing which is the same as the modulation characteristics of the vibrating tunable e1e ment. Thus, any variation of the reed modulation ele ment due to non-linearity is compensated for by the arnplified feedback and signal voltages. The voltage out put from the capacitor plate will thus be constant while the motion of the core is in one direction, changes polarity when the coil reverses direction, and remains constant at the new polarity until the cycle reoccurs. If for any reason, Ithe motion of the drive coil is not linear, the error or feedback voltage derived across the capacitive plate is fed to the amplifier input circuit7 combined with the input signal voltage and reamplified in phase opposition so as to tend to cancel out the error originally generated by irregularities in the drive coil motion.
It should be understood that this invention is not limited to the particular details of construction, materials and processes described, as many equivale-nts will suggest themselves to those skilled in the art. For example, the electrically insulated capacity plate may be used to regulate the frequency response of other than electron discharge device-s. The non-linear response of, for example, a driving coil applied to a magnetic transducer, in an arrangement as shown in FG. 3, may be compensated by the feedback voltage developed in this closed loop feedback system, or other non-linear electromechanical vibrating assemblies may attain similar advantages.
It is accordingly desired that this invention not be limited to the particular details of the embodiment disclosed herein except as defined by the appended claims.
What is claimed is:
1. A frequency modulation circuit comprising an electron discharge device including a cathode, an anode, means for producing a magnetic field and a tunable element positioned in said magnetic field, said tunable element including a conductive plate insulatedly supported thereon and 'adjacent to said anode in a manner adapted to vary the frequency of said electron discharge device in response to movement of said plate, means for varying the position of said plate including a driving element mounted on said tunable element, means for applying an input voltage to said driving coil, means for developing a feedback voltage in response to variations in electrical charge on said plate due to changes of capacitance between said plate and said anode, and means for combining said feedback voltage with said input Voltage to apply a modulating voltage to said driving element.
2. A frequency modulation circuit comprising means for establishing a flow of electrons in a given direction, means for establishing a magnetic field in a direction substantially perpendicular to such direction of electron flow, and means mounted for movement within such magnetic field and adjacent such electron fiow to both frequencymodulate such electron flow in accordance with such movement and provide a capacitive pick-off the amplitude of which varies in linear relationship with such movement, whereby the variable capacitance of said pick-off may be employed to control feedback circuitry the output of which is combined with drive signals applied to said frequency modulating means to stabilize the operation of such lastmentioned means.
3. A frequency modulation circuit comprising means for establishing a iiow of electrons in a given direction, means for establishing a magnetic field in a direction substantially perpendicular to such direction of electron iiow, means mounted for movement within such magnetic field and adjacent such electron flow to both frequency-modulate such electron flow in accordance with such movement and provide a capacitive pick-olf the amplitude of which varies in linear relationship with such movement, means for effecting movement of said frequency modulating means in accordance with a modulating signal, and means connected in feedback relationship between said capacitive pick-off means and said means for effecting movement.
4. A frequency modulation circuit, comprising an electron discharge device including a cathode, an anode, and means for establishing a magnetic field in a direction substantially perpendicular to the path of the electron flow between said cathode and said anode, a mechanical tuning means positioned in said magnetic iield, and a conductive plate insulatedly supported -by said tuning means within said device in capacitive relationship with said anode, said tuning means being mounted for movement relative to said anode to vary the distance between said conductive plate and said anode and thereby vary such capacitive `relationship linearly with respect to such movement, whereby the movement of said conductive plate serves both to frequency-modulate the electron ow from said cathode to said anode and to provide -a capacitive pickoff which varies linearly with such movement.
5. A frequency modulation circuit comprising an electron discharge device having a cathode, an anode yand a magnetic circuit having a field portion substantially perpendicular to a ow of electrons between said cathode and said anode, a vibratory member mounted for movement within such magnetic eld adjacent such electron flow, a drive coil mounted on said vibratory member, an input circuit for said drive coil for applying modulating signals thereto to cause corresponding movement of said coil and vibratory member as la result of interaction between the magnetic fields of said coil and said magnetic circuit, a conductive plate member mounted on and insulated from said vibratory member for movement toward -and away from said anode in capacitive relationship therewith, and a feedback circuit connected between said insulated conductive plate member and said input circuit, whereby such movement of said conductive plate member serves both to frequency-modulate the electron flow from said cathode to said anode and to provide a variable capacitance control for such feedback circuit which varies linearly with the movement of said conductive plate member.
References Cited in the le of this patent UNITED STATES PATENTS 2,114,086 Smith et al Apr. 12, 1938 2,269,041 Schussler Jan. 6, 1942 2,444,435 Fisk July 6, 1948 2,493,819 Harry Jan. 10i, 195o 2,615,156 Smith Oct. 2l, 1952 2,750,565 Mercer June 12, 1956 2,784,345 Spencer Mar. 5, 1957 2,802,178 Shafer Aug. 6, 1957

Claims (1)

1. A FREQUENCY MODULATION CIRCUIT COMPRISING AN ELECTRON DISCHARGE DEVICE INCLUDING A CATHODE, AN ANODE, MEANS FOR PRODUCING A MAGNETIC FIELD AND A TUNABLE ELEMENT POSITIONED IN SAID MAGNETIC FIELD, SAID TUNABLE ELEMENT INCLUDING A CONDUCTIVE PLATE INSULATEDLY SUPPORTED THEREON AND ADJACENT TO SAID ANODE IN A MANNER ADAPTED TO VARY THE FREQUENCY OF SAID ELECTRON DISCHARGE DEVICE IN RESPONSE TO MOVEMENT OF SAID PLATE, MEANS FOR VARYING THE POSITION OF SAID PLATE INCLUDING A DRIVING ELEMENT
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Cited By (12)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3149292A (en) * 1962-07-10 1964-09-15 Joseph H Gamble Frequency modulator for magnetron pulses utilizing variably phase shifted reflectionfrom mismatch to pull magnetron frequency
US3365609A (en) * 1964-09-01 1968-01-23 Philips Corp Transducer for use with variable frequency magnetrons
US3379925A (en) * 1962-12-24 1968-04-23 Raytheon Co Tunable magnetron having a capacitive transducer magnetically coupled to the tuning member
US3414760A (en) * 1965-10-15 1968-12-03 Westinghouse Electric Corp A frequency diversity coaxial magnetron
US3440565A (en) * 1966-03-17 1969-04-22 Westinghouse Electric Corp Sensor for detection of frequency of a reed modulated magnetron
US3478246A (en) * 1967-05-05 1969-11-11 Litton Precision Prod Inc Piezoelectric bimorph driven tuners for electron discharge devices
US3478247A (en) * 1967-06-12 1969-11-11 Litton Precision Prod Inc Microwave tuner having a rapid tuning rate
US3727097A (en) * 1970-08-06 1973-04-10 English Electric Valve Co Ltd Magnetrons
US3727099A (en) * 1963-02-04 1973-04-10 Westinghouse Electric Corp Tuned cavity device
US3729646A (en) * 1970-07-01 1973-04-24 English Electric Valve Co Ltd Magnetron tunable by piezo-electric means over a wide range in discrete steps
US4311968A (en) * 1978-12-05 1982-01-19 English Electric Valve Company Limited Magnetron having cavity wall vibrated by tuning fork
US4518932A (en) * 1981-09-08 1985-05-21 English Electric Valve Company, Ltd. Coaxial magnetron having cavity walls vibrated by tuning fork

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US2114036A (en) * 1936-10-17 1938-04-12 Bell Telephone Labor Inc Frequency stabilization system
US2269041A (en) * 1938-10-21 1942-01-06 Telefunken Gmbh Automatic frequency control system
US2444435A (en) * 1942-05-01 1948-07-06 Bell Telephone Labor Inc Frequency control of magnetron oscillators
US2493819A (en) * 1947-11-25 1950-01-10 Bell Telephone Labor Inc Stabilized feed-back condenser microphone
US2615156A (en) * 1948-02-14 1952-10-21 Rca Corp Frequency modulation of electron discharge devices
US2750565A (en) * 1952-09-13 1956-06-12 Raytheon Mfg Co Altimeter modulators
US2784345A (en) * 1951-06-26 1957-03-05 Raytheon Mfg Co Electron-discharge devices
US2802178A (en) * 1954-09-22 1957-08-06 Gen Electric Motion detecting device

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US2114036A (en) * 1936-10-17 1938-04-12 Bell Telephone Labor Inc Frequency stabilization system
US2269041A (en) * 1938-10-21 1942-01-06 Telefunken Gmbh Automatic frequency control system
US2444435A (en) * 1942-05-01 1948-07-06 Bell Telephone Labor Inc Frequency control of magnetron oscillators
US2493819A (en) * 1947-11-25 1950-01-10 Bell Telephone Labor Inc Stabilized feed-back condenser microphone
US2615156A (en) * 1948-02-14 1952-10-21 Rca Corp Frequency modulation of electron discharge devices
US2784345A (en) * 1951-06-26 1957-03-05 Raytheon Mfg Co Electron-discharge devices
US2750565A (en) * 1952-09-13 1956-06-12 Raytheon Mfg Co Altimeter modulators
US2802178A (en) * 1954-09-22 1957-08-06 Gen Electric Motion detecting device

Cited By (12)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3149292A (en) * 1962-07-10 1964-09-15 Joseph H Gamble Frequency modulator for magnetron pulses utilizing variably phase shifted reflectionfrom mismatch to pull magnetron frequency
US3379925A (en) * 1962-12-24 1968-04-23 Raytheon Co Tunable magnetron having a capacitive transducer magnetically coupled to the tuning member
US3727099A (en) * 1963-02-04 1973-04-10 Westinghouse Electric Corp Tuned cavity device
US3365609A (en) * 1964-09-01 1968-01-23 Philips Corp Transducer for use with variable frequency magnetrons
US3414760A (en) * 1965-10-15 1968-12-03 Westinghouse Electric Corp A frequency diversity coaxial magnetron
US3440565A (en) * 1966-03-17 1969-04-22 Westinghouse Electric Corp Sensor for detection of frequency of a reed modulated magnetron
US3478246A (en) * 1967-05-05 1969-11-11 Litton Precision Prod Inc Piezoelectric bimorph driven tuners for electron discharge devices
US3478247A (en) * 1967-06-12 1969-11-11 Litton Precision Prod Inc Microwave tuner having a rapid tuning rate
US3729646A (en) * 1970-07-01 1973-04-24 English Electric Valve Co Ltd Magnetron tunable by piezo-electric means over a wide range in discrete steps
US3727097A (en) * 1970-08-06 1973-04-10 English Electric Valve Co Ltd Magnetrons
US4311968A (en) * 1978-12-05 1982-01-19 English Electric Valve Company Limited Magnetron having cavity wall vibrated by tuning fork
US4518932A (en) * 1981-09-08 1985-05-21 English Electric Valve Company, Ltd. Coaxial magnetron having cavity walls vibrated by tuning fork

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