US3289035A - Reverse magnetron having means to suppress undersired modes - Google Patents

Reverse magnetron having means to suppress undersired modes Download PDF

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US3289035A
US3289035A US216228A US21622862A US3289035A US 3289035 A US3289035 A US 3289035A US 216228 A US216228 A US 216228A US 21622862 A US21622862 A US 21622862A US 3289035 A US3289035 A US 3289035A
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cavity
circular electric
coupling
electric mode
modes
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US216228A
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Drexler Jerome
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SFD LAB Inc
S-F-D LABORATORIES Inc
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SFD LAB Inc
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Priority to US216227A priority Critical patent/US3290548A/en
Priority to US216228A priority patent/US3289035A/en
Priority to US219702A priority patent/US3255377A/en
Priority claimed from US221796A external-priority patent/US3223876A/en
Priority to US223499A priority patent/US3231781A/en
Priority to GB25074/66A priority patent/GB1061715A/en
Priority to JP38040875A priority patent/JPS4945617B1/ja
Priority to GB25073/66A priority patent/GB1061714A/en
Priority to GB31643/63A priority patent/GB1061711A/en
Priority to FR944394A priority patent/FR1372678A/en
Publication of US3289035A publication Critical patent/US3289035A/en
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J25/00Transit-time tubes, e.g. klystrons, travelling-wave tubes, magnetrons
    • H01J25/50Magnetrons, i.e. tubes with a magnet system producing an H-field crossing the E-field
    • H01J25/52Magnetrons, i.e. tubes with a magnet system producing an H-field crossing the E-field with an electron space having a shape that does not prevent any electron from moving completely around the cathode or guide electrode
    • H01J25/54Magnetrons, i.e. tubes with a magnet system producing an H-field crossing the E-field with an electron space having a shape that does not prevent any electron from moving completely around the cathode or guide electrode having only one cavity or other resonator, e.g. neutrode tubes
    • H01J25/55Coaxial cavity magnetrons
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J23/00Details of transit-time tubes of the types covered by group H01J25/00
    • H01J23/02Electrodes; Magnetic control means; Screens
    • H01J23/04Cathodes
    • H01J23/05Cathodes having a cylindrical emissive surface, e.g. cathodes for magnetrons
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J23/00Details of transit-time tubes of the types covered by group H01J25/00
    • H01J23/36Coupling devices having distributed capacitance and inductance, structurally associated with the tube, for introducing or removing wave energy

Definitions

  • the reverse magnetron tube of the present invention solves the aforementioned difiiculties associated with the prior art tube and provides a 32-35 gigacycle magnetron having a peak power output in the order of 290 kilowatts with average power output of approximately 50 watts while yielding overall efiiciencies of approximately 30% and a tunable bandwidth up to 12%.
  • This tube represents more than an order of magnitude increase in peak 3,289,035 Patented Nov. 29, 1966 lCC power output with approximately double the previously obtained efiiciency while having a long operating life in excess of 2,400 hours.
  • Another feature of the present invention is the provision of an axial rod centrally disposed of the circular electric mode cavity, said rod carrying the output coupling structure for facilitating axial translation of the coupling structure and tuning of the circular electric mode cavity.
  • FIG. 3 is a fragmentary view partly in cross-section and partly broken away of the portion of the structure of FIG. 2 taken along the line 33 in the direction of the arrows,
  • FIG. 5 is a cross-sectional mode diagram showing the TE circular electric mode of the cavity of FIG. 4,
  • FIG. 7 is a mode diagram showing the electric field lines for the TE mode in the cavity of FIG. 4.
  • a strong axial magetic field as of 12,000 to 15,000 gauss for the magnetron interaction region 8 is provided by a bowl shaped magnet '11, only partially shown in FIG. 2, enveloping the anode body portion 1 and having a re-entrant internal magnetic gap extending in the axial direction through the magnetron interaction region 8 between the magnetic pole pieces 12 disposed on opposite sides of the anode vanes 6.
  • the negative cathode potential of approximately 23 kv. is applied to the cathode emitter 9 via high voltage lead-in insulator assembly 4.
  • the cathode 9 uses a low voltage A.C. filament heater and therefore a dual wire cathode lead-in 10 is used.
  • the coupling disc 13 of FIGS. 2, 3 and 4 is replaced by a snowflake shape-d plate 25 :as shown in FIG. 6.
  • the elongated peripherally directed openings in the plate 25 between the radially directed members or points 26 of the snow-flake sha ed plate serve to couple the circular waveguide structure, and consequently the load, more (heavily to the non-circul-ar electric modes within the cavity, characterized by radially directed currents in the cavity end Walls 18 and This selective heavy coupling of the non-circular electric modes to the load serves to suppress these modes and prevent their sustained oscillation in the circular electric mode cavity 5.
  • the snowflake shaped coupling plate 25 has an odd number of connecting points 26. If the plate 25 has an even number of points 26, as for example six, then the undesired TE mode could align itself to minimize its coupling to the load.
  • a coupling device for wave energy communication between a hollow cavity resonator operating in a circular electric mode and a load including, a circular electric mode cavity resonator having an end wall, said end wall having an elongated coupling hole therethrough, a hollow circular electric mode wave supporting structure axially aligned with said coupling hole for wave communication between said cavity and the load, said elongated coupling hole being elongated in the circumferential direction of said cavity end wall to provide coupling to the desired circular electric mode while more heavily coupling the load to the undesired non-circular electric modesof said cavity having radial currents in said end wall to thereby load said undesired modes for suppression there of.

Description

Nov. 29, 1966 J. DREXLER 3,289,035-
REVERSE MAGNETRON HAVING MEANS TO SUPPRESS UNDESIRED MODES Filed Au 10,- 1962 2 Sheets-Sheet 1 JEROME DREXLER Y M aid;
' ATTORNEY .INVENT OR.
NOV. 29, 1966 XL R 3,289,035
HREVERSE QMAGNETRON HAVING MEANS To SUFIRESS UNDESIRED MODES Filed Aug 10, 1962 1 2 Sheets-Shed 2 INVENTOR. JEROME DREXLER ATTQRNEJY United States Patent REVERSE MAGNETRON HAVING MEANS TO SUPPRESS UNDESIRED MODES Jerome Drexler, New Providence, N..I., assignor to S-F-D Laboratories, Inc., Union, N.J., a corporation of New Jersey Filed Aug. 10, 1962, Ser. No. 216,228
11 Claims. (Cl. 31539.51)
The present invention relates in general to electron discharge devices of the crossed electric and magnetic field type and more specifically to a reverse magnetron useful for generating high power microwave energy at extremely high frequencies such as required in high power, high resolution radars.
A reverse magnetron tube typically comprises a circular electric mode cavity or circular electric mode wave propagating structure surrounded by a circumferential array of outwardly directed vane or cavity resonators coupled to the excited circular electric structure via a circular array of axial slots communicating with alternate anode resonators. The array of anode resonators is surrounded by a magnetron interaction region formed by an annular cathode emitter, emitting radially inwardly into the anode, in the presence of a strong axial magnetic field. Rotating spokes of electron space charge interact with the 1r mode fields of the anode resonators to excite the circular electric mode in the circular electric mode cavity. Since the energy stored in the circular electric mode cavity is much higher than that of the vane resonator circuit the anode vane resonator system is locked in the 1r mode to the circular electric cavity mode thereby stabilizing the magnetron. The reverse magnetron structure may be used as an oscillator or as an amplifier and microwave energy is extracted from the circular electric mode wave propagating structure or cavity and fed to a suitable load.
Heretofore a reverse magnetron of the above described type has been built operating at approximately 32 gigacycles and generating a peak power of approximately 15 kilowatts. When an attempt is made to push this prior art design to higher output levels of 300 kilowatts peak, 50 watts average, 30% efliciency and a tunable band of approximately 12% several severe problems are encountered which prevent attaining these late specifications.
Some of the problems associated with pushing the power output of the prior art reverse magnetron design to higher power levels are as follows:
In pulse operation, as of l microsecond, certain noncircular electric modes of the cavity are excited due to insufficient selective mode suppression, thereby causing the anode resonators to operate in an unstable non 1r mode resulting in pulse jitter and reduced efiiciency; during tuning of the circular electric mode cavity, parasitic modes associated with the back cavity spaces behind the noncontacting movable wall tuner results in dips in the power versus frequency curve over the operating band of the tube.
The reverse magnetron tube of the present invention solves the aforementioned difiiculties associated with the prior art tube and provides a 32-35 gigacycle magnetron having a peak power output in the order of 290 kilowatts with average power output of approximately 50 watts while yielding overall efiiciencies of approximately 30% and a tunable bandwidth up to 12%. This tube represents more than an order of magnitude increase in peak 3,289,035 Patented Nov. 29, 1966 lCC power output with approximately double the previously obtained efiiciency while having a long operating life in excess of 2,400 hours.
The principal object of the present invention is to provide an improved high power reverse magnetron tube yielding substantially enhanced peak power with increased etficiency and operating life.
One feature of the present invention is the provision of a novel output coupling method and apparatus for the circular electric mode cavity which more heavily and selectively couples the undesired non-circular electric modes of the cavity to the load thereby loading and suppressing the undesired non-circular electric modes, whereby when used in a reverse magnetron the result is stable operation of the tube and elimination of pulse jitter.
Another feature of the present invention is the provision of a novel tuner structure and method for the circular electric mode cavity wherein a structure is provided for tuning by producing axial translation of the output coupling structure, whereby dips in the power versus frequency curve over the band of the tube areeliminated, such dips being heretofore caused by parasitic resonance'associated with spaces behind the prior art non-contacting movable end wall tuners.
Another feature of the present invention is the provision of an axial rod centrally disposed of the circular electric mode cavity, said rod carrying the output coupling structure for facilitating axial translation of the coupling structure and tuning of the circular electric mode cavity.
Other features and advantages of the present invention will become apparent upon a perusal of the specification taken in connection with the accompanying drawings wherein:
FIG. 1 is an outside perspective view of the reverse magnetron tube of the present invention,
FIG. 2 is an enlarged fragmentary view partly broken away and partly in section of the structure of FIG. 1 taken along the line 22 in the direction of the arrows,
FIG. 3 is a fragmentary view partly in cross-section and partly broken away of the portion of the structure of FIG. 2 taken along the line 33 in the direction of the arrows,
FIG. 4 is an enlarged fragmentary cross-sectional view of the portion of the structure of FIG. 2 taken along the line 4-4 in the direction of the arrows,
FIG. 5 is a cross-sectional mode diagram showing the TE circular electric mode of the cavity of FIG. 4,
FIG. 6 is an alternative structure of that depicted in FIG. 4, and
FIG. 7 is a mode diagram showing the electric field lines for the TE mode in the cavity of FIG. 4.
Referring now to FIGS. 1, 2 and 3, character 1 represents the hollow tubular supporting body of the reverse magnetron, as of copper, to which other parts are brazed or otherwise suitably fastened to form a structure capable of being evacuated. On opposite sides of the body 1 in axial alignment there are brazed to the body 1 a tubular output waveguide assembly 2 and tuner assembly 3. Cathode lead-in insulator structure 4 extends outwardly from the main body section 1 in quadrature with the axially aligned output waveguide and tuner structures 2 and 3, respectively.
The term circular electric mode cavity, waveguide, or wave supporting structure as used herein is defined to mean a cavity, waveguide, or wave supporting structure formed, dimensioned, and excited in such a manner as to support at its certain preselected operating frequency a certain circular electric mode, of the general form TE to the exclusion of other modes. A circular electric mode cavity, waveguide, or wave supporting structure typically includes an outer cylindrical side wall and may or may not have an axially directed center conductor.
A hollow circular electric mode cavity resonator 5 is disposed centrally of the anode body 1 on the axis of the tube. In amplifier embodiments of the present invention, the circular electric mode cavity 5 is replaced by a circular electric wave supporting structure such as, for example, a hollow cylindrical pipe having an input port as well as an output port. A circumferential array of outwardly directed vanes 6 surround the circular electric mode cavity 5 and form an array of anode resonators by the spaces between adjacent vanes 6. Alternate anode resonators are electromagnetically coupled to the circular electric mode cavity 5 via an array of axially directed slots 7 communicating through the common wall between the anode resonators and the circular electric mode cavity 5. A magnetron interaction region 8 surrounds the outer tips of the vanes 6 and is defined by the space in-between the vanes 6 and a surrounding cathode emitter ring 9.
A strong axial magetic field as of 12,000 to 15,000 gauss for the magnetron interaction region 8 is provided by a bowl shaped magnet '11, only partially shown in FIG. 2, enveloping the anode body portion 1 and having a re-entrant internal magnetic gap extending in the axial direction through the magnetron interaction region 8 between the magnetic pole pieces 12 disposed on opposite sides of the anode vanes 6.
Tuning of the tube over its approximate 12% tuning band, centered at approximately 34 gigacycles, is obtained by means of axial translation of a combined cavity end wall and output coupling plate 13 carried upon the end of an axially directed and positioned rod 14 which is axially translatable via the intermediary of a captured nut 15 and bellows assembly 16, partially shown.
The negative cathode potential of approximately 23 kv. is applied to the cathode emitter 9 via high voltage lead-in insulator assembly 4. The cathode 9 uses a low voltage A.C. filament heater and therefore a dual wire cathode lead-in 10 is used.
In operation, the 1r mode of the anode resonator system adjacent the magnetron interaction region is locked to the circular electric mode resonator 5 via the intermediary of the coupling slots 7 serving to drive the resonator 5. An annular slot mode absorber 24, juxtapositioned the coupling plate end of the slots 7, suppresses the undesired slot mode. The slot mode absorber 24 and its support structure form the subject matter of and are claimed in copending US. application 223,499, filed September 13, 1962, now issued as 3,231,781 on January 25, 1966, and assigned to the same assignee as the present invention. Output energy from the resonator 5 is extracted via the coupling plate 13 and transmitted to the load, not shown, via the intermediary of the circular electric mode output waveguide structure 2 and an output vacuum tight wave permeable window 17.
The tube structure and mode of operation will now be described in greater detail as it specifically relates to each of the before mentioned features of the present invention.
The novel output coupling method and apparatus feature of the present invention can be seen by reference to FIGS. 2, 3 and 4. The circular electric mode cavity 5 is defined and bounded on one end by the fixed circular end wall 18 as of copper, and on the sides by the circular relatively thin anode wall 19, as of copper, and on the other end by axially translatable combined tuner and coupling plate 13, as of copper. The coupling plate 13 is carried upon the extremity of the axially directed centrally disposed rod 14 as of, for example, copper. The rod 14 is provided with an axially directed enlarged extension portion 20 as of molybdenum and is rectilinearly translatable axially of the tube for tuning of the circular electric cavity 5. The rod extension 20 is sealed in a vacuum tight manner to the tube body 1 via the intermediary of the axially extensible bellows 16. The rod extension portion 20 slides in an axial directed bore in an anode block 21 as of copper having an insert sleeve 22 as of molybdenum serving as a bearing support for the molybdenum extension 20.
A pair of axially spaced apart sapphire rings 23 of slightly smaller inside diameter than the molybdenum sleeve insert 22 are carried in the sleeve 22 and serve as the sliding bearing contact between the enlarged portion of the tuning rod 20 and the fixed sleeve insert 22. The rings 23 serve to facilitate axial movement of the tuning rod by minimizing sliding friction while at the same time providing a firm bearing support to minimize microphonics in use.
The circular electric mode cavity 5 is capable of supporting certain interfering non-circular electric modes such as, for example, the TE TE the TE etc. modes. These non-circular electric modes all have associated therewith certain radially directed currents in the end walls 13 and 18 of the circular electric mode cavity 5. The radial currents are exemplified by the TE electric field mode distribution as shown in FIG. 7.
The novel coupling plate 13 approximates a cavity end wall having an elongated peripherally directed coupling slot therethrough. Such a coupling slot heavily couples to those modes having radial currents in the end walls while much less heavily coupling to the circular electric mode currents. It is believed that the circular electric mode currents are perturbed slightly by the coupling plate 13 causing them to move radially inwardly toward the center of the cavity. This inward movement of the'desired circular electric mode field, see FIG. 5, is desirable since it tends to thereby move currents associated with the desired circular electric mode further away from the slot mode absorber 24 surrounding the coupling plate end of the axially directed coupling slots 7. The annular slot mode absorber 24 is used for suppressing certain undesired slot modes.
The elongated circumferential-1y directed coupling slot, formed by the annular space between the disc shaped coupling plate 13 and the inner side wall 19 of the circular electric mode cavity 5, performs the function of coupling out wave energy from the desired circular electric mode and also more heavily coupling the load, not shown, to the undesired non-circular electric modes thereby resulting in suppression of these undesired modes. This selective mode suppression stabilizes operation of the circular electric mode cavity 5 in the circular electric mode and locks the coupled system of anode resonators on the desired 1r mode in the magnetron interaction region 8.
Typical dimension for :a circular electric mode cavity 5, designed for operation at 34 gigacycles on the dominant TE mode are: the inside diameter of the cavity 5 is approximately 0.570", the height of the cavity is approximately /2 a wavelength, the axial thickness of the disc shaped coupling plate 13 is approximately 0.030", the disc 13 has a diameter of approximately 0.341", and the diameter of the tuning rod 14 is approximately the diameter of the cavity 5.
In a fixed tuned alternative output coupling embodiment of the present invention, the coupling disc 13 of FIGS. 2, 3 and 4 is replaced by a snowflake shape-d plate 25 :as shown in FIG. 6. The elongated peripherally directed openings in the plate 25 between the radially directed members or points 26 of the snow-flake sha ed plate serve to couple the circular waveguide structure, and consequently the load, more (heavily to the non-circul-ar electric modes within the cavity, characterized by radially directed currents in the cavity end Walls 18 and This selective heavy coupling of the non-circular electric modes to the load serves to suppress these modes and prevent their sustained oscillation in the circular electric mode cavity 5. The inwardly directed peripherally spaced apart notches 27 in the snowflake plate 25 serve to enhance coupling between the desired circular electric mode and the load for coupling output wave energy from the cavity to the load. As in the previous embodiment, the snowflake 25 may -be carried upon the extremity of the rod 14 for tuning or may be fixedly secured to the side walls 19 of the circular electric mode cavity 5 at the tips 26 of the snowflake plate 25, as by brazing.
In a preferred embodiment the snowflake shaped coupling plate 25 has an odd number of connecting points 26. If the plate 25 has an even number of points 26, as for example six, then the undesired TE mode could align itself to minimize its coupling to the load.
In operation, the combined tuning and coupling plate embodiments, as described above, readily permit tuning of the reverse magnetron oscillator over a 12% band centered at 34 gigacycles without encountering substantial dips in the power versus frequency curve as previously encountered due to back cavity resonances associated with prior art non-contacting movable wall tuners. In addition, the selective mode suppressing coupling plate readily permits enhanced efiiciencies of 30% while eliminating pulse jitter at power levels of 290 kw. peak power.
Since many changes could be made in the above construction and many apparently widely different embodiments or this invention could be made without departing from the scope thereof, it is intended that all matter contained in the above description or shown in the accompanying drawings shall be interpreted as illustrative and not in a limiting sense.
What is claimed is:
1. A coupling device for wave energy communication between a hollow cavity resonator operating in a circular electric mode and a load including, a circular electric mode cavity resonator having an end wall, said end wall having an elongated coupling hole therethrough, a hollow circular electric mode wave supporting structure axially aligned with said coupling hole for wave communication between said cavity and the load, said elongated coupling hole being elongated in the circumferential direction of said cavity end wall to provide coupling to the desired circular electric mode while more heavily coupling the load to the undesired non-circular electric modesof said cavity having radial currents in said end wall to thereby load said undesired modes for suppression there of.
2.. In an electronic circuit, means defining a first circular electric mode cavity resonator, means defining a second system of resonators, a common wall member separating said first cavity resonator from said second system of resonators, means communicating through said common Wall member for coupling said first and second resonators, coupling means for coupling wave energy zfrom said first circular electric mode cavity resonator to a load, said coupling means being formed and arranged to more heavily couple the load to non-circular electric modes of oscillation of said first cavity resonator than the circular electric mode of said first resonator for mode suppression of the non-circular electric modes in said first cavity resonator.
3. In a crossed field tube apparatus, a cathode, an anode wall with a plurality of anode resonators formed therein adjacent said cathode, means for defining with said anode wall a second cavity resonator, means for coupling certain ones of said anode resonators to said second cavity resonator and including a plurality of slots communicating through said anode wall between said anode resonators and said second cavity resonator, said second cavity resonator having an end wall, an elongated coupling hole provided in said end wall of said second cavity resonator, said elongated coupling hole being directed peripherally or said end wall for coupling wave energy from said second cavity resonator to a load, and :said peripherally directed coupling hole serving to more heavily couple modes of the said second cavity resonator having currents tending to flow radially across said elongated coupling hole than other modes having currents flowing in the peripheral direction of said coupling hole, whereby said certain modes having radially directed currents are more heavily coupled to the load for suppression thereof.
4. In a magnetron apparatus, a circular electric mode cavity having a pair of axially spaced apart energy reflective end wall members defining with a side wall said circular electric mode cavity, an array of resonant cavities, coupling means communicating through said side wall of said circular electric mode cavity for coupling said circular electric mode cavity to said array of resonant cavities, one of said end reflective wall members being .provided with a peripherally directed elongated coupling slot therethrough, circular electric mode waveguide disposed in registry with said elongated coupling slot for providing wave energy communication between said circular electric mode cavity and a load, and said elongated coupling slot being disposed in said end reflective wall member nearer to said circular electric cavity side wall than to the center of said end wall whereby the non-circular electric modes are more heavily coupled to the load than the circular electric mode and whereby the non-circular electric modes are selectively suppressed.
5. The apparatus according to claim 4 wherein said cavity end wall reflective member having the coupling hole therein is provided with a plurality of peripherally directed coupling iholes interrupted by radially directed conductive members, said radially directed conductive members serving to join said cavity side wall to said reflective end wall.
6. The apparatus according to claim 5 wherein there are an odd number of radially directed conductive members to heavily couple to the undesired TE mode for suppression thereof.
7. The apparatus according to claim 4 wherein said circular electric mode cavity includes, a centrally disposed axially directed member aflixed to said slotted end wall reflective member.
8. The apparatus according to claim 7 wherein said axially directed member aflixed to said slotted end wall is axially translatable for moving said slotted reflective end wall for tuning of said circular electric mode cavity.
9. The apparatus according to claim 8 wherein said axially directed centrally disposed member is made of an electrically conductive material.
10. A reverse magnetron tube apparatus including, an evacuable body portion, a cylindrical cavity resonator centrally disposed of said body portion for sustaining a TE mode of oscillation and having an outer cylindrical side wall, a circumferential array of anode resonators surrounding said cylindrical outer cavity wall, means for electrically locking the 11- mode of oscillation of said array of anode resonators to said TE mode of said central cavity resonator, said locking means including a circumferential array of axial slots extending through said outer cavity wall member at alternate ones of said anode resonators, a ring of glossy material disposed adjacent the ends of said slots on the outside of said outer cylindrical wall for loading certain unwanted modes of oscillation of said slots, said central cavity resonator having a fixed end closing wall with an axially directed bore therethrough, a centrally disposed axially directed rod extending axially through said central cavity resonator and movable through said bore, and said central cavity resonator having a movable end wall defined by a conductive disc carried upon said axially directed rod, said disc being spaced at its periphery from the outer side wall of said central cavity resonator for defining an annular coupling slot through said end wall, said annular coupling slot serving to selective-1y more heavily couple non-circular electric modes of said inner cavity to a load than the desired TE mode 7 of oscillation of said central cavity Whereby'said noncircular electric modes are suppressed.
11. A selective coupling apparatus for coupling to circular electric mode structures including, a circular electric mode cavity resonator having an end wall, said end wall having an elongated coupling hole the-rethrough, a hollow circular electric mode wave supporting structure axially aligned with said coupling hole for wave communication between said cavity and said w-ave supporting structure, said elongated coupling hole being elongated in the circumferential direction of said cavity end wall to provide coupling to the desired circular electric mode While more heavily and selectively coupling to the undesired noncircular electric modes of said cavity resonator characterized by radially directed currents in said end wall to thereby more heavily couple said undesired modes for suppression thereof.
References Cited by the Examiner UNITED STATES PATENTS HERMAN KARL sAALBAcHQrrimk Examiner;
GEORGE WESTBY, S. CHATMON, V 0 Assistant Examiners.

Claims (1)

1. A COUPLING DEVICE FOR WAVE ENERGY COMMUNICATION BETWEEN A HOLLOW CAVITY RESONATOR OPERATING IN A CIRCULAR ELECTRIC MODE AND A LOAD INCLUDING, A CIRCULAR ELECTRIC MODE CAVITY RESONATOR HAVING AN END WALL, SAID END WALL HAVING AN ELONGATED COUPLING HOLE THERETHROUGH, A HOLLOW CIRCULAR ELECTRIC MODE WAVE SUPPORTING STRUCTURE AXIALLY ALIGNED WITH SAID COUPLING HOLE FOR WAVE COMMUNICATION BETWEEN SAID CAVITY AND THE LOAD, SAID ELONGATED COUPLING HOLD BEING ELONGATED IN THE CIRCUMFERENTIAL DIRECTION OF SAID CAVITY END WALL TO PROVIDE COUPLING TO THE DISIRED CIRCULAR ELECTRIC MODE WHILD MORE HEAVILY COUPLING THE LOAD TO THE UNDESIRED NON-CIRCULAR ELECTRIC MODES OF SAID CAVITY HAVING RADIAL CURRENTS IN SAID WALL TO THEREBY LOAD SAID UNDESIRED MODES FOR SUPPRESSION THEREOF.
US216228A 1962-08-10 1962-08-10 Reverse magnetron having means to suppress undersired modes Expired - Lifetime US3289035A (en)

Priority Applications (9)

Application Number Priority Date Filing Date Title
US216227A US3290548A (en) 1962-08-10 1962-08-10 Reverse magnetron
US216228A US3289035A (en) 1962-08-10 1962-08-10 Reverse magnetron having means to suppress undersired modes
US219702A US3255377A (en) 1962-08-10 1962-08-27 Reverse magnetron with cathode support structure
US223499A US3231781A (en) 1962-08-10 1962-09-13 Reverse magnetron with slot mode absorber
GB25074/66A GB1061715A (en) 1962-08-10 1963-08-09 Electron-emitting cathode assemblies
JP38040875A JPS4945617B1 (en) 1962-08-10 1963-08-09
GB25073/66A GB1061714A (en) 1962-08-10 1963-08-09 Magnetrons
GB31643/63A GB1061711A (en) 1962-08-10 1963-08-09
FR944394A FR1372678A (en) 1962-08-10 1963-08-10 Inverted type magnetron

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FR1372678T
US216228A US3289035A (en) 1962-08-10 1962-08-10 Reverse magnetron having means to suppress undersired modes
US219702A US3255377A (en) 1962-08-10 1962-08-27 Reverse magnetron with cathode support structure
US221796A US3223876A (en) 1962-09-06 1962-09-06 Cathode heater assembly for use in strong d.c. magnetic fields

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Cited By (3)

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US3414761A (en) * 1965-09-16 1968-12-03 S F D Lab Dither tuner for a coaxial magnetron
US3458754A (en) * 1966-05-03 1969-07-29 Gen Electric Inverted cross field device having an arcuately segmented cathode
US8446096B1 (en) * 2009-10-02 2013-05-21 The United States Of America As Represented By The Secretary Of The Navy Terahertz (THz) reverse micromagnetron

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US3441792A (en) * 1966-07-08 1969-04-29 Sfd Lab Inc Reverse magnetron having a tie ring stiffening structure for its cathode support fingers
US3473072A (en) * 1967-03-01 1969-10-14 Nikolai Dmitrievich Ivano Mount for electric vacuum devices
US3805318A (en) * 1969-08-08 1974-04-23 R Marquette Brush cleaning device
US4620170A (en) * 1984-12-19 1986-10-28 Varian Associates, Inc. Means for liquid cooling a microwave window

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US2815469A (en) * 1951-01-08 1957-12-03 English Electric Valve Co Ltd Magnetron oscillators
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CH309019A (en) * 1952-12-30 1955-08-15 Patelhold Patentverwertung Tuning device for single-circuit magnetron.
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US2482495A (en) * 1943-11-27 1949-09-20 Westinghouse Electric Corp Magnetron
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US2951182A (en) * 1957-11-25 1960-08-30 Bell Telephone Labor Inc Magnetron

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3414761A (en) * 1965-09-16 1968-12-03 S F D Lab Dither tuner for a coaxial magnetron
US3458754A (en) * 1966-05-03 1969-07-29 Gen Electric Inverted cross field device having an arcuately segmented cathode
US8446096B1 (en) * 2009-10-02 2013-05-21 The United States Of America As Represented By The Secretary Of The Navy Terahertz (THz) reverse micromagnetron
US8624497B1 (en) 2009-10-02 2014-01-07 The United States Of America As Represented By The Secretary Of The Navy Terahertz (THz) reverse micromagnetron

Also Published As

Publication number Publication date
GB1061714A (en) 1967-03-15
GB1061715A (en) 1967-03-15
US3255377A (en) 1966-06-07
GB1061711A (en) 1967-03-15

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