US3536953A - Resonant cavity magnetron with mode suppressing short circuit connections - Google Patents
Resonant cavity magnetron with mode suppressing short circuit connections Download PDFInfo
- Publication number
- US3536953A US3536953A US775606A US3536953DA US3536953A US 3536953 A US3536953 A US 3536953A US 775606 A US775606 A US 775606A US 3536953D A US3536953D A US 3536953DA US 3536953 A US3536953 A US 3536953A
- Authority
- US
- United States
- Prior art keywords
- resonant cavity
- short circuit
- mode
- circuit connections
- connections
- 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
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J25/00—Transit-time tubes, e.g. klystrons, travelling-wave tubes, magnetrons
- H01J25/50—Magnetrons, i.e. tubes with a magnet system producing an H-field crossing the E-field
- H01J25/52—Magnetrons, 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
- H01J25/58—Magnetrons, 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 a number of resonators; having a composite resonator, e.g. a helix
- H01J25/587—Multi-cavity magnetrons
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J23/00—Details of transit-time tubes of the types covered by group H01J25/00
- H01J23/16—Circuit elements, having distributed capacitance and inductance, structurally associated with the tube and interacting with the discharge
- H01J23/18—Resonators
- H01J23/22—Connections between resonators, e.g. strapping for connecting resonators of a magnetron
Definitions
- the invention relates to a resonant cavity magnetron in which resonant cavities are formed by substantially flat anode vanes the end faces of which which face the oathode constitute the anode segments and in which annular equipotential connections which are located near to each other connect points located near the cathode on the axial end faces of alternate anode vanes in one or both end spaces.
- the (1r1) mode is the mode which in frequency is located nearest to the 1r-mode and which occurs in doublet.
- interruptions in equipotential connections which are distributed axially between the anode vanes.
- the parts of the interrupted connection adjoining the interruption are then both connected to an anode segment so that in addition to the interrupted connection a bridged resonant cavity is obtained.
- magnetrons for continuous operation for example, for high-frequency heating
- said measures are generally insufficient particularly in connection with the higher average powers and the high standing wave ratio which usually occurs.
- these magnetrons often have to operate with a supply having an unfiltered single phase or two-phase rectified mains voltage, so that, when the vr-mode does not occur immediately, the danger exists that the anode voltage increases to the higher value which is favourable for the (1r-1) mode.
- the edge steepness of the supply voltage is a few orders of magnitude 3,536,953 Patented Oct. 27, 1970 lower than in magnetrons for radar, these generally operate with a considerably lower standing wave ratio.
- a resonant cavity magnetron in which the resonant cavities are constituted by substantially flat anode vanes the end faces of which face the cathode constitute the anode segments and in which annular equipotential connections which are located near to each other connects points located near the cathode on the axial end faces of alternate anode vanes in one or both end spaces, short circuit connections are provided in the end spaces on the axial end faces of the anode segments of one or more resonant cavities which are located at an angle of approximately 45 or with the output line of the magnetron, said short circuit connections being located substantially centrally between the equipotential connections and the outside of the anode vanes.
- the angle between the coupling-out line and the bridged resonant cavities also determines the frequency of the doublet of the (1rl) mode and the radial position of the bridge determines whether the two doublets are coupled out to a more or less equal extent.
- the number of short circuit connections in one end space may be equal to one single or two connections located diametrically opposite to each other of four connections located 2 by 2 diametrically opposite to each other at diameters intersecting at right angles. If required, another four may be provided in the other space.
- Reference numeral 1 in the figure denotes the copper anode block in which 20 copper anode vanes 2 are soldered.
- the axial ends of the vanes are profiled so that they alternately contact the copper equipotential connections 3 and 4.
- the output line of the magnetron is a coaxial system 5, 6 the inner conductor 6 of which terminates on a transverse brace 7 which terminates on the outermost anode vanes of two adjacent resonant cavities.
- the resonant cavity 8 which is arranged at an angle of 45 with the output is bridged by a copper brace 9.
- a second brace 10 may also be provided or in addition two braces 11 and 12. If required, the system of the four braces may also be provided in the other end space.
- a resonant cavity magnetron comprising an annular block having a plurality of symmetrically positioned inwardly projecting spaced vanes defining resonant cavities therebetween, a concentrically positioned cathode within said annular block spaced from the ends of said vanes, means connecting alternate vanes adjacent their ends facing the cathode to provide equipotential connections thereto, output means connected to the ends of selected vanes at their ends remote from the cathode, and at least one short circuit connection between two adjacent vanes between the equipotential connections and the ends remote from the cathode positioned at an angle of substantially 45 or 135 with the output means.
- a resonant cavity magnetron as claimed in claim 1 References Cited characterized in that only one short circuit connection is UNITED STATES PATENTS provided at an angle of 45 with the output line.
Description
Oct. 27, 1970 v DE 500 3,536,953
7 RESONANT CAVITY MAGNETRON WITH MODE SUPPRESSING SHORT CIRCUIT CONNECTIONS Filed Nov. 14, 1968 W/ [m\\\\ 6 \mu INVENTOR.
JOHANNES A.VAN DE 600R AGENT United States Patent 3,536,953 RESONANT CAVITY MAGNETRON WITH MODE SUPPRESSING SHORT CIRCUIT CONNECTIONS Johannes Antonius van de Goor, Emmasingel, Eindhoven, Netherlands, assignor, by mesne assignments, to US. Phihps Corporation, New York, N.Y., a corporation of Delaware Filed Nov. 14, 1968, Ser. No. 775,606 Claims priority, application Netherlands, Nov. 24, 1967, 6715979 Int. Cl. H01j 23/22 U.S. Cl. 315-39.69 4 Claims ABSTRACT OF THE DISCLOSURE equipotential straps and the ends of the vanes remote from the cathode.
The invention relates to a resonant cavity magnetron in which resonant cavities are formed by substantially flat anode vanes the end faces of which which face the oathode constitute the anode segments and in which annular equipotential connections which are located near to each other connect points located near the cathode on the axial end faces of alternate anode vanes in one or both end spaces.
A problem which always presents itself in magnetrons is to realize that oscillating occurs only or mainly in the 1r-mode and that the higher modes, particularly the (1r1)-mode, do not occur. The (1r1) mode is the mode which in frequency is located nearest to the 1r-mode and which occurs in doublet.
In magnetrons for producing radar pulses bends in the equipotential connections are used, so as to orient the oscillation pattern of the two doublets of the (1r-1) mode in a particular manner with respect to the output coupling. Interruptions in the equipotential connections are also used sometimes.
It is also known to use interruptions in equipotential connections which are distributed axially between the anode vanes. The parts of the interrupted connection adjoining the interruption are then both connected to an anode segment so that in addition to the interrupted connection a bridged resonant cavity is obtained. Furthermore it is known to provide a coupling loop between two adjacent resonant cavities which does not influence the vr-mode but does influence the (1r1) mode.
In magnetrons for continuous operation, for example, for high-frequency heating, said measures are generally insufficient particularly in connection with the higher average powers and the high standing wave ratio which usually occurs. In addition, these magnetrons often have to operate with a supply having an unfiltered single phase or two-phase rectified mains voltage, so that, when the vr-mode does not occur immediately, the danger exists that the anode voltage increases to the higher value which is favourable for the (1r-1) mode. Although the edge steepness of the supply voltage is a few orders of magnitude 3,536,953 Patented Oct. 27, 1970 lower than in magnetrons for radar, these generally operate with a considerably lower standing wave ratio.
It is known to provide such continuously operating magnetrons with connection braces between anode vanes which bound an even number of resonant cavities, but this measure is not more than an extra equipotential connection which reduces the electronic efficiency.
According to the invention, in a resonant cavity magnetron in which the resonant cavities are constituted by substantially flat anode vanes the end faces of which face the cathode constitute the anode segments and in which annular equipotential connections which are located near to each other connects points located near the cathode on the axial end faces of alternate anode vanes in one or both end spaces, short circuit connections are provided in the end spaces on the axial end faces of the anode segments of one or more resonant cavities which are located at an angle of approximately 45 or with the output line of the magnetron, said short circuit connections being located substantially centrally between the equipotential connections and the outside of the anode vanes.
The angle between the coupling-out line and the bridged resonant cavities also determines the frequency of the doublet of the (1rl) mode and the radial position of the bridge determines whether the two doublets are coupled out to a more or less equal extent.
The number of short circuit connections in one end space may be equal to one single or two connections located diametrically opposite to each other of four connections located 2 by 2 diametrically opposite to each other at diameters intersecting at right angles. If required, another four may be provided in the other space.
In order that the invention may be readily carried into effect, one embodiment thereof will now be described in greater detail, by way of example, with reference to the accompanying drawing, the sole figure of which is an axial elevation on the anode system of a magnetron according to the invention.
Reference numeral 1 in the figure denotes the copper anode block in which 20 copper anode vanes 2 are soldered. The axial ends of the vanes are profiled so that they alternately contact the copper equipotential connections 3 and 4. The output line of the magnetron is a coaxial system 5, 6 the inner conductor 6 of which terminates on a transverse brace 7 which terminates on the outermost anode vanes of two adjacent resonant cavities. The resonant cavity 8 which is arranged at an angle of 45 with the output is bridged by a copper brace 9. A second brace 10 may also be provided or in addition two braces 11 and 12. If required, the system of the four braces may also be provided in the other end space.
Due to the braces it is realized that at a frequency of the 1r-mode of 2450 mc./s., the doublets of the (1r-1) mode which are then at 3000 and 3100 mc./s. are coupled out to substantially the same extent and with the same bandwidth.
What is claimed is:
1. A resonant cavity magnetron comprising an annular block having a plurality of symmetrically positioned inwardly projecting spaced vanes defining resonant cavities therebetween, a concentrically positioned cathode within said annular block spaced from the ends of said vanes, means connecting alternate vanes adjacent their ends facing the cathode to provide equipotential connections thereto, output means connected to the ends of selected vanes at their ends remote from the cathode, and at least one short circuit connection between two adjacent vanes between the equipotential connections and the ends remote from the cathode positioned at an angle of substantially 45 or 135 with the output means.
'7 a 4 2. A resonant cavity magnetron as claimed in claim 1, References Cited characterized in that only one short circuit connection is UNITED STATES PATENTS provided at an angle of 45 with the output line.
2,860,285 11/1958 Sm1th 31539.69 X
3. A resonant cavity magnetron as claimed in claim 1, characterized in that two short circuit connections are 5 provlded which are located diametrically opposite to each HERMAN KARL SAALBACH, Primary Examiner other.
4. A resonant cavity magnetron as claimed in claim 1, S. CHATMON, JR., Assistant Examiner characterized in that four short-circuit connections are provided in one or both end spaces and are located dia- 10 U5. Cl. X.R. metrically on two diameters intersecting each other at 315 39 51J 3953; 331 91 right angles.
3,121,822 2/1964 Boyd 31539.69
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
NL6715979A NL6715979A (en) | 1967-11-24 | 1967-11-24 |
Publications (1)
Publication Number | Publication Date |
---|---|
US3536953A true US3536953A (en) | 1970-10-27 |
Family
ID=19801807
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US775606A Expired - Lifetime US3536953A (en) | 1967-11-24 | 1968-11-14 | Resonant cavity magnetron with mode suppressing short circuit connections |
Country Status (5)
Country | Link |
---|---|
US (1) | US3536953A (en) |
DE (1) | DE1806058A1 (en) |
FR (1) | FR1592846A (en) |
GB (1) | GB1249893A (en) |
NL (1) | NL6715979A (en) |
Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3792306A (en) * | 1972-12-04 | 1974-02-12 | Raytheon Co | Multisignal magnetron having plural signal coupling means |
US4028583A (en) * | 1975-08-07 | 1977-06-07 | Atomic Energy Of Canada Limited | High power-double strapped vane type magnetron |
US4129834A (en) * | 1977-01-17 | 1978-12-12 | U.S. Philips Corporation | Resonant cavity magnetron with choke structure for reducing harmonics in output system |
US4365185A (en) * | 1979-07-14 | 1982-12-21 | English Electric Valve Company Limited | Magnetron having three alternatingly connected straps |
US5211776A (en) * | 1989-07-17 | 1993-05-18 | General Dynamics Corp., Air Defense Systems Division | Fabrication of metal and ceramic matrix composites |
US5216327A (en) * | 1991-12-19 | 1993-06-01 | Raytheon Company | Magnetron coaxial adaptor having a cap which fits over the magnetron output antenna |
US6384537B2 (en) * | 1999-08-25 | 2002-05-07 | Northrop Grumman Corporation | Double loop output system for magnetron |
Families Citing this family (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5030655U (en) * | 1973-07-16 | 1975-04-05 | ||
JPS50126159A (en) * | 1974-03-22 | 1975-10-03 |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2860285A (en) * | 1956-12-14 | 1958-11-11 | Raytheon Mfg Co | Electron discharge devices |
US3121822A (en) * | 1960-10-28 | 1964-02-18 | Gen Electric | Circuits for unimoding crossed field devices |
-
1967
- 1967-11-24 NL NL6715979A patent/NL6715979A/xx unknown
-
1968
- 1968-10-30 DE DE19681806058 patent/DE1806058A1/en active Pending
- 1968-11-14 US US775606A patent/US3536953A/en not_active Expired - Lifetime
- 1968-11-21 GB GB55255/68A patent/GB1249893A/en not_active Expired
- 1968-11-22 FR FR1592846D patent/FR1592846A/fr not_active Expired
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2860285A (en) * | 1956-12-14 | 1958-11-11 | Raytheon Mfg Co | Electron discharge devices |
US3121822A (en) * | 1960-10-28 | 1964-02-18 | Gen Electric | Circuits for unimoding crossed field devices |
Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3792306A (en) * | 1972-12-04 | 1974-02-12 | Raytheon Co | Multisignal magnetron having plural signal coupling means |
US4028583A (en) * | 1975-08-07 | 1977-06-07 | Atomic Energy Of Canada Limited | High power-double strapped vane type magnetron |
US4129834A (en) * | 1977-01-17 | 1978-12-12 | U.S. Philips Corporation | Resonant cavity magnetron with choke structure for reducing harmonics in output system |
US4365185A (en) * | 1979-07-14 | 1982-12-21 | English Electric Valve Company Limited | Magnetron having three alternatingly connected straps |
US5211776A (en) * | 1989-07-17 | 1993-05-18 | General Dynamics Corp., Air Defense Systems Division | Fabrication of metal and ceramic matrix composites |
US5216327A (en) * | 1991-12-19 | 1993-06-01 | Raytheon Company | Magnetron coaxial adaptor having a cap which fits over the magnetron output antenna |
US6384537B2 (en) * | 1999-08-25 | 2002-05-07 | Northrop Grumman Corporation | Double loop output system for magnetron |
Also Published As
Publication number | Publication date |
---|---|
FR1592846A (en) | 1970-05-19 |
GB1249893A (en) | 1971-10-13 |
NL6715979A (en) | 1969-05-28 |
DE1806058A1 (en) | 1969-07-31 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US2550614A (en) | High-efficiency magnetron | |
US3536953A (en) | Resonant cavity magnetron with mode suppressing short circuit connections | |
US2421725A (en) | Variable frequency cavity resonator oscillator | |
US3397339A (en) | Band edge oscillation suppression techniques for high frequency electron discharge devices incorporating slow wave circuits | |
US2323201A (en) | Tuned circuit and associated devices therefor | |
US2504329A (en) | Oscillation damping device | |
Boot et al. | The cavity magnetron | |
US2428612A (en) | Magnetron | |
US3360679A (en) | Electron discharge device having lossy resonant elements disposed within the electromagnetic field pattern of the slow-wave circuit | |
US2410396A (en) | High efficiency magnetron | |
US5084651A (en) | Microwave tube with directional coupling of an input locking signal | |
US3387168A (en) | Fin-supported helical slow wave circuit providing mode separation and suppression for traveling wave tubes | |
US2498720A (en) | High-frequency protective circuits | |
US2496500A (en) | Electron discharge device | |
US3223882A (en) | Traveling wave electric discharge oscillator with directional coupling connections to a traveling wave structure wherein the number of coupling connections times the phase shift between adjacent connections equal an integral number of wavelengths | |
GB650575A (en) | Improvements in and relating to magnetrons | |
US2450023A (en) | Electron discharge device of the magnetron type | |
US3361926A (en) | Interdigital stripline teeth forming shunt capacitive elements and an array of inductive stubs connected to adjacent teeth | |
US2473828A (en) | Electron discharge device of the magnetron type | |
US2597506A (en) | Ultra-short wave electron tube | |
US3289032A (en) | Microwave hybrid tube apparatus | |
USRE34863E (en) | High impedance circuit for injection locked magnetrons | |
US2432827A (en) | High efficiency magnetron | |
US3942066A (en) | Velocity modulation tube including a high resonance-frequency floating prebuncher having a q-value lower than a low resonance-frequency input cavity | |
US3646389A (en) | Reactively loaded interdigital slow wave circuits having increased interaction impedance and tubes using same |