US2338237A - High-frequency electron discharge apparatus - Google Patents
High-frequency electron discharge apparatus Download PDFInfo
- Publication number
- US2338237A US2338237A US369431A US36943140A US2338237A US 2338237 A US2338237 A US 2338237A US 369431 A US369431 A US 369431A US 36943140 A US36943140 A US 36943140A US 2338237 A US2338237 A US 2338237A
- Authority
- US
- United States
- Prior art keywords
- resonator
- electrons
- stream
- discharge apparatus
- frequency
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
Links
- 230000010355 oscillation Effects 0.000 description 8
- 238000010894 electron beam technology Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 1
- 230000005284 excitation Effects 0.000 description 1
- 238000012423 maintenance Methods 0.000 description 1
- 230000000979 retarding effect Effects 0.000 description 1
Images
Classifications
-
- D—TEXTILES; PAPER
- D01—NATURAL OR MAN-MADE THREADS OR FIBRES; SPINNING
- D01G—PRELIMINARY TREATMENT OF FIBRES, e.g. FOR SPINNING
- D01G23/00—Feeding fibres to machines; Conveying fibres between machines
- D01G23/02—Hoppers; Delivery shoots
- D01G23/04—Hoppers; Delivery shoots with means for controlling the feed
- D01G23/045—Hoppers; Delivery shoots with means for controlling the feed by successive weighing; Weighing hoppers
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01G—WEIGHING
- G01G13/00—Weighing apparatus with automatic feed or discharge for weighing-out batches of material
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J25/00—Transit-time tubes, e.g. klystrons, travelling-wave tubes, magnetrons
- H01J25/02—Tubes with electron stream modulated in velocity or density in a modulator zone and thereafter giving up energy in an inducing zone, the zones being associated with one or more resonators
- H01J25/06—Tubes having only one resonator, without reflection of the electron stream, and in which the modulation produced in the modulator zone is mainly velocity modulation, e.g. Lüdi-Klystron
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J25/00—Transit-time tubes, e.g. klystrons, travelling-wave tubes, magnetrons
- H01J25/02—Tubes with electron stream modulated in velocity or density in a modulator zone and thereafter giving up energy in an inducing zone, the zones being associated with one or more resonators
- H01J25/10—Klystrons, i.e. tubes having two or more resonators, without reflection of the electron stream, and in which the stream is modulated mainly by velocity in the zone of the input resonator
- H01J25/12—Klystrons, i.e. tubes having two or more resonators, without reflection of the electron stream, and in which the stream is modulated mainly by velocity in the zone of the input resonator with pencil-like electron stream in the axis of the resonators
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P7/00—Resonators of the waveguide type
- H01P7/04—Coaxial resonators
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03C—MODULATION
- H03C3/00—Angle modulation
- H03C3/30—Angle modulation by means of transit-time tube
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03C—MODULATION
- H03C7/00—Modulating electromagnetic waves
- H03C7/02—Modulating electromagnetic waves in transmission lines, waveguides, cavity resonators or radiation fields of antennas
Definitions
- This invention relates to ultra-high frequency apparatus comprising resonators of the cavity type.
- the invention is primarily applicable to electron discharge apparatus using the principles of velocity modulation of electrons for the excitation of a resonator effective at very high frequencies.
- Such apparatus usually comprises a single resonator or a pair of coupled resonators of cavity type, electrons being passed through two successive gaps therein to be modulated in velocity in the first gap and to yield energy at the second gap for the maintenance or oscillations.
- an auxiliary electron beam may be fired across some part of one of the resonators.
- This auxiliary beam if of suitable velocity will change the dielectric constant and hence the natural frequency of the resonator.
- modulation of the auxiliary beam will give a frequency modulation of the high frequency output, while in a double resonator it will give an amplitude modulation (owing to the detuning of one resonator with respect to the other), probably combined with some degree of frequency modulation.
- Fig. 1 shows a single cavity arrangement
- Fig. 2 a double cavity arrangement
- an electron emitting cathode l0 emits electrons which are accelerated by accelerator electrode I l and centered by the control electrode l2 to produce a cathode beam shown in dotted lines at l3.
- This beam is transmitted through a pair of grids l4, l5, located in the wall of resonant cavity l6 and tube ll, respectively, after which it is again subject to the effect of a control potential between grid l8 and the end wall of chamber it.
- Such a tube is known in the prior art and energy may be extracted from the tube due to the retarding effect caused between l8 and the end wall.
- modulation of the signal beam is provided by means of a second beam traversing the cavity through which the beam passes so as to change the dielectric constant effective in this area.
- Thi is accomplished by a cathode 20, an accelerating electrode 2
- serve to vary the concentration of the beam emitted from cathod 20 and so to vary the tures shown invFig. 2 may, if desired, be applied to Fig. 1 and similarly the features of Fig. 1 which differ from Fig. 2 may be applied to this other arrangement.
- High frequency discharge apparatus including a tube, means coaxial with and surrounding said tube, forming a hollow resonant chamber, a plurality of aligned grids, one in one end of said means, a second in one end of said tube and adjacent said first grid, and a. third at the other end of said tube, a source of electrons aligned with said grids and adapted to discharge and-direct electrons along ,a path through all of said grids, and means for varying the dielectric constant of said chamber, comprising a second source of electrons and a target positioned within said chamber, forming an electron discharge path across said chamber between said third grid and the other end of said resonant chamber forming means.
- Modulated high frequency discharge apparatus comprising a hollow resonator having a predetermined dielectric constant, means for maintaining oscillations in the resonator including means for directing a stream of electrons along a main discharge path through the resonator, and means for modulating said oscillations including means for directing a second stream of electrons along a second discharge path through the resonator and means for modulating said second stream.
- Modulated high frequency discharge apparatus as set forth in claim 2, including means for velocity modulating the first stream of electrons in one part of the resonator, and means for transferring energy from said stream to the oscillating field in a second part of the resonator, and in which the second stream of electrons passes through said second part of the resonator.
- Frequency modulated high frequency discharge apparatus comprising a hollow resonator having a predetermined dielectric constant and an oscillation frequency determined by said constant, means for maintaining oscillations in the resonator including means for directing a stream of electrons along a main discharge path through the resonator, and means for modulating the frequency of said oscillations including mean for directing a second stream of electrons along a 20 second discharge path through the resonator and means for modulating said second stream.
- Amplitude modulated high frequency discharge apparatus comprising a hollow resonator having a predetermined dielectric constant and formed with two resonant cavities, means for maintaining oscillations in the resonator including means for directing a stream of electrons along a main discharge path passing through both cavities of the resonator, and means for amplitude modulating the frequency of said oscillations including means for directing a second stream of electrons along a second discharge path through the second cavity of the resonator, located adjacent the discharge end of the first stream of electrons, and modulating said second stream, said detuning action of one cavity with respect to the other producing amplitude modulation.
Description
Jan. 4; 1944. FREMLlN 2,338,237
HIGH FREQUENCY ELECTRON DISCHARGE APPARATUS Filed Dec. 10, 1940 TO SIGNAL MODl/M 7' IIVG Sou/r65 T0 JIGML MODl/LA TING SOURCE IN VEN TOR JOHN HEAVEI? FfiEMU/V ATTORNEY Patented Jan. 4, 1944 UNITED STATES v PATENT- Fl=lCE azaazs'z HIGH-FREQUENCY ELECTRON DISCHARGE John Beaver Fremlin, London, England, asaignor to International Standard Electric Corporation,
New York, N. Y.
Application December 10, 1940, Serial No. 369,431
In Great Britain December 22, 1939 Claims. (CL 250-275) This invention relates to ultra-high frequency apparatus comprising resonators of the cavity type.
It is proposed, in accordance with the invention, to modulate or change the frequency of a resonator of the cavity type by varying the dielectric constant withina portion of the reso-v nator, by varying an electronic space charge or by varying the intensity or velocity of an electron beam traversing that portion.
The invention is primarily applicable to electron discharge apparatus using the principles of velocity modulation of electrons for the excitation of a resonator effective at very high frequencies.
Briefly such apparatus usually comprises a single resonator or a pair of coupled resonators of cavity type, electrons being passed through two successive gaps therein to be modulated in velocity in the first gap and to yield energy at the second gap for the maintenance or oscillations.
In either single or double resonator apparatus utilising velocity modulation of electrons, an auxiliary electron beam may be fired across some part of one of the resonators. This auxiliary beam, if of suitable velocity will change the dielectric constant and hence the natural frequency of the resonator. In the case of a single resonator, therefore, modulation of the auxiliary beam will give a frequency modulation of the high frequency output, while in a double resonator it will give an amplitude modulation (owing to the detuning of one resonator with respect to the other), probably combined with some degree of frequency modulation.
The illustration of the single cavity and double cavity tubes in accordance with this invention are shown in the drawing in which, Fig. 1 shows a single cavity arrangement, and Fig. 2 a double cavity arrangement.
In the drawing the illustrations are made diagrammatically.
In Fig. 1 an electron emitting cathode l0 emits electrons which are accelerated by accelerator electrode I l and centered by the control electrode l2 to produce a cathode beam shown in dotted lines at l3. This beam is transmitted through a pair of grids l4, l5, located in the wall of resonant cavity l6 and tube ll, respectively, after which it is again subject to the effect of a control potential between grid l8 and the end wall of chamber it. Such a tube is known in the prior art and energy may be extracted from the tube due to the retarding effect caused between l8 and the end wall.
In accordance with my invention modulation of the signal beam is provided by means of a second beam traversing the cavity through which the beam passes so as to change the dielectric constant effective in this area. Thi is accomplished by a cathode 20, an accelerating electrode 2| to which a signal modulating source is coupled, a concentrating electrode 22 to form the electrons emitted from cathode 20 into a beam,
and a target electrode 23 which serves to prevent electrons from the beam from returning into the space. The signal modulations applied to electrode 2| serve to vary the concentration of the beam emitted from cathod 20 and so to vary the tures shown invFig. 2 may, if desired, be applied to Fig. 1 and similarly the features of Fig. 1 which differ from Fig. 2 may be applied to this other arrangement.
What is claimed is:
1. High frequency discharge apparatus including a tube, means coaxial with and surrounding said tube, forming a hollow resonant chamber, a plurality of aligned grids, one in one end of said means, a second in one end of said tube and adjacent said first grid, and a. third at the other end of said tube, a source of electrons aligned with said grids and adapted to discharge and-direct electrons along ,a path through all of said grids, and means for varying the dielectric constant of said chamber, comprising a second source of electrons and a target positioned within said chamber, forming an electron discharge path across said chamber between said third grid and the other end of said resonant chamber forming means.
2. Modulated high frequency discharge apparatus comprising a hollow resonator having a predetermined dielectric constant, means for maintaining oscillations in the resonator including means for directing a stream of electrons along a main discharge path through the resonator, and means for modulating said oscillations including means for directing a second stream of electrons along a second discharge path through the resonator and means for modulating said second stream.
3. Modulated high frequency discharge apparatus as set forth in claim 2, including means for velocity modulating the first stream of electrons in one part of the resonator, and means for transferring energy from said stream to the oscillating field in a second part of the resonator, and in which the second stream of electrons passes through said second part of the resonator.
4. Frequency modulated high frequency discharge apparatus comprising a hollow resonator having a predetermined dielectric constant and an oscillation frequency determined by said constant, means for maintaining oscillations in the resonator including means for directing a stream of electrons along a main discharge path through the resonator, and means for modulating the frequency of said oscillations including mean for directing a second stream of electrons along a 20 second discharge path through the resonator and means for modulating said second stream.
5. Amplitude modulated high frequency discharge apparatus comprising a hollow resonator having a predetermined dielectric constant and formed with two resonant cavities, means for maintaining oscillations in the resonator including means for directing a stream of electrons along a main discharge path passing through both cavities of the resonator, and means for amplitude modulating the frequency of said oscillations including means for directing a second stream of electrons along a second discharge path through the second cavity of the resonator, located adjacent the discharge end of the first stream of electrons, and modulating said second stream, said detuning action of one cavity with respect to the other producing amplitude modulation.
JOHN HEAVER FREMLIN.
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
GB32816/39A GB537491A (en) | 1939-12-22 | 1939-12-22 | Improvements in or relating to high frequency electron discharge apparatus |
Publications (1)
Publication Number | Publication Date |
---|---|
US2338237A true US2338237A (en) | 1944-01-04 |
Family
ID=120265
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US369431A Expired - Lifetime US2338237A (en) | 1939-12-22 | 1940-12-10 | High-frequency electron discharge apparatus |
Country Status (5)
Country | Link |
---|---|
US (1) | US2338237A (en) |
BE (1) | BE469969A (en) |
CH (1) | CH265037A (en) |
GB (1) | GB537491A (en) |
NL (1) | NL65060C (en) |
Cited By (29)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2416283A (en) * | 1942-07-03 | 1947-02-25 | Bell Telephone Labor Inc | Ultra high frequency electronic device |
US2438954A (en) * | 1941-11-12 | 1948-04-06 | Bell Telephone Labor Inc | Electronic oscillator of the cavity resonator type |
US2439387A (en) * | 1941-11-28 | 1948-04-13 | Sperry Corp | Electronic tuning control |
US2454306A (en) * | 1948-11-23 | clifford et au | ||
US2468145A (en) * | 1943-11-25 | 1949-04-26 | Sperry Corp | Cavity resonator apparatus, including frequency control means |
US2482768A (en) * | 1942-12-30 | 1949-09-27 | Sperry Corp | High-frequency modulating system |
US2482766A (en) * | 1942-07-01 | 1949-09-27 | Sperry Corp | High-frequency modulating system |
US2484643A (en) * | 1945-03-06 | 1949-10-11 | Bell Telephone Labor Inc | High-frequency electronic device |
US2500945A (en) * | 1943-11-08 | 1950-03-21 | Sperry Corp | Modulator and frequency changer |
US2504739A (en) * | 1944-09-27 | 1950-04-18 | Westinghouse Electric Corp | Electron discharge device having a cavity resonator provided with a tuning electrode |
US2519826A (en) * | 1945-04-30 | 1950-08-22 | Raytheon Mfg Co | Electron discharge device |
US2537112A (en) * | 1945-08-20 | 1951-01-09 | Sperry Corp | High-frequency tube structure |
US2538087A (en) * | 1944-12-26 | 1951-01-16 | Raytheon Mfg Co | Electron discharge device of the magnetron type |
US2556747A (en) * | 1946-03-19 | 1951-06-12 | Raytheon Mfg Co | Electron discharge device of the magnetron type |
US2560859A (en) * | 1944-03-02 | 1951-07-17 | Csf | Method for modulating the highfrequency energy transmitted in hollow dielectric guides |
US2576696A (en) * | 1945-03-15 | 1951-11-27 | Gen Electric | Generation of electromagnetic waves by doppler effects |
US2586816A (en) * | 1945-03-24 | 1952-02-26 | Sperry Corp | High-frequency modulating system |
US2607861A (en) * | 1951-01-25 | 1952-08-19 | Herbert M Wagner | Space charge reaction device |
US2614234A (en) * | 1946-02-02 | 1952-10-14 | Voge Jean Paul | Oscillating and amplifying vacuum tube for very short waves |
US2617079A (en) * | 1944-08-08 | 1952-11-04 | Westinghouse Electric Corp | Tunable magnetron |
US2695373A (en) * | 1944-11-16 | 1954-11-23 | Rca Corp | Cavity resonator high-frequency apparatus |
US2730647A (en) * | 1949-06-22 | 1956-01-10 | Bell Telephone Labor Inc | Microwave amplifier |
US2772377A (en) * | 1951-08-29 | 1956-11-27 | Kazan Benjamin | Device for electronically controlling the propagation of radio frequency power |
US2781476A (en) * | 1944-11-16 | 1957-02-12 | Rca Corp | Magnetron |
US2806976A (en) * | 1952-11-26 | 1957-09-17 | Karl G Hernqvist | Impedance matching device |
US2902615A (en) * | 1954-04-01 | 1959-09-01 | Zenith Radio Corp | Beam internation devices |
US3046492A (en) * | 1958-04-30 | 1962-07-24 | English Electric Valve Co Ltd | Klystron microwave oscillator with particular keying means |
US3350566A (en) * | 1964-10-06 | 1967-10-31 | Gen Dynamics Corp | Laser mixer and if amplifier |
US3801854A (en) * | 1972-08-24 | 1974-04-02 | Varian Associates | Modulator circuit for high power linear beam tube |
-
1939
- 1939-12-22 GB GB32816/39A patent/GB537491A/en not_active Expired
-
1940
- 1940-12-10 US US369431A patent/US2338237A/en not_active Expired - Lifetime
-
1946
- 1946-12-06 BE BE469969A patent/BE469969A/fr unknown
- 1946-12-11 CH CH265037D patent/CH265037A/en unknown
-
1947
- 1947-02-25 NL NL130567A patent/NL65060C/nl active
Cited By (29)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2454306A (en) * | 1948-11-23 | clifford et au | ||
US2438954A (en) * | 1941-11-12 | 1948-04-06 | Bell Telephone Labor Inc | Electronic oscillator of the cavity resonator type |
US2439387A (en) * | 1941-11-28 | 1948-04-13 | Sperry Corp | Electronic tuning control |
US2482766A (en) * | 1942-07-01 | 1949-09-27 | Sperry Corp | High-frequency modulating system |
US2416283A (en) * | 1942-07-03 | 1947-02-25 | Bell Telephone Labor Inc | Ultra high frequency electronic device |
US2482768A (en) * | 1942-12-30 | 1949-09-27 | Sperry Corp | High-frequency modulating system |
US2500945A (en) * | 1943-11-08 | 1950-03-21 | Sperry Corp | Modulator and frequency changer |
US2468145A (en) * | 1943-11-25 | 1949-04-26 | Sperry Corp | Cavity resonator apparatus, including frequency control means |
US2560859A (en) * | 1944-03-02 | 1951-07-17 | Csf | Method for modulating the highfrequency energy transmitted in hollow dielectric guides |
US2617079A (en) * | 1944-08-08 | 1952-11-04 | Westinghouse Electric Corp | Tunable magnetron |
US2504739A (en) * | 1944-09-27 | 1950-04-18 | Westinghouse Electric Corp | Electron discharge device having a cavity resonator provided with a tuning electrode |
US2781476A (en) * | 1944-11-16 | 1957-02-12 | Rca Corp | Magnetron |
US2695373A (en) * | 1944-11-16 | 1954-11-23 | Rca Corp | Cavity resonator high-frequency apparatus |
US2538087A (en) * | 1944-12-26 | 1951-01-16 | Raytheon Mfg Co | Electron discharge device of the magnetron type |
US2484643A (en) * | 1945-03-06 | 1949-10-11 | Bell Telephone Labor Inc | High-frequency electronic device |
US2576696A (en) * | 1945-03-15 | 1951-11-27 | Gen Electric | Generation of electromagnetic waves by doppler effects |
US2586816A (en) * | 1945-03-24 | 1952-02-26 | Sperry Corp | High-frequency modulating system |
US2519826A (en) * | 1945-04-30 | 1950-08-22 | Raytheon Mfg Co | Electron discharge device |
US2537112A (en) * | 1945-08-20 | 1951-01-09 | Sperry Corp | High-frequency tube structure |
US2614234A (en) * | 1946-02-02 | 1952-10-14 | Voge Jean Paul | Oscillating and amplifying vacuum tube for very short waves |
US2556747A (en) * | 1946-03-19 | 1951-06-12 | Raytheon Mfg Co | Electron discharge device of the magnetron type |
US2730647A (en) * | 1949-06-22 | 1956-01-10 | Bell Telephone Labor Inc | Microwave amplifier |
US2607861A (en) * | 1951-01-25 | 1952-08-19 | Herbert M Wagner | Space charge reaction device |
US2772377A (en) * | 1951-08-29 | 1956-11-27 | Kazan Benjamin | Device for electronically controlling the propagation of radio frequency power |
US2806976A (en) * | 1952-11-26 | 1957-09-17 | Karl G Hernqvist | Impedance matching device |
US2902615A (en) * | 1954-04-01 | 1959-09-01 | Zenith Radio Corp | Beam internation devices |
US3046492A (en) * | 1958-04-30 | 1962-07-24 | English Electric Valve Co Ltd | Klystron microwave oscillator with particular keying means |
US3350566A (en) * | 1964-10-06 | 1967-10-31 | Gen Dynamics Corp | Laser mixer and if amplifier |
US3801854A (en) * | 1972-08-24 | 1974-04-02 | Varian Associates | Modulator circuit for high power linear beam tube |
Also Published As
Publication number | Publication date |
---|---|
BE469969A (en) | 1946-10-30 |
CH265037A (en) | 1949-11-15 |
GB537491A (en) | 1941-06-24 |
NL65060C (en) | 1949-12-16 |
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