US3448331A - Composite coaxial coupling device and coaxial window - Google Patents

Description

June 3, 1969 E. J. COOK 3,448,331

COMPOSITE COAXIAL COUPLING DEVICE AND COAXIAL WINDOW Filed July 19, 1966 Sheet of :5

FIG. 2 W4- I NVENTOR.

I2 EDWARD J. 000K- ATTORNEY June 3, 1969 E. 'J. COOK 3,448,331

COMPOSITE COAXIAL COUPLING DEVICE AND COAXIAL WINDOW Filed July 19, 1966 Sheet of s n, /2 A I FA w T v 4 l 7 L 7:100 pC J BEAM i/ 3 C E ,7 E I L 1 B 7G 4 FIG. 5

FIG. 7

/ J\ V I// I NVENTOR.

EDWARD J. 000K BY a ATTORNEY June 3; 1969 E. J. COOK 3,448,331

COMPOSITE COAXIAL COUPLING DEVICE AND COAXIAL WINDOW Filed July 19, 1966 Sheet of 3 FIG. 8

FIG. 9

FIG.|I

INVENTOR.

ATTORNEY United States Patent 3,448,331 COMPOSITE COAXIAL COUPLING DEVICE AND COAXIAL WINDOW Edward J. Cook, South Hamilton, Mass., assignors to Varian Associates, Palo Alto, Calif., a corporation of California Continuation-impart of application Ser. No. 525,455, Feb. 7, 1966. This application July 19, 1966, Ser. No. 574,271

Int. Cl. H01j /50; H0311 7/38;H01p 1/00 U.S. Cl. 315-3953 8 Claims ABSTRACT OF THE DISCLOSURE A composite coaxial coupling device and coaxial wave permeable Window for microwave structures including microwave tubes is disclosed. The coaxial coupling device and window includes an inner conductor portion which projects into a field containing a region of space defined between a pair of conductors. A dielectric wave permeable window member coaxially surrounds the inner conductor and projects into the field containing region of space. In one embodiment, the field containing region of space is defined by a wave supporting structure having a radial line portion and a coaxial portion with the outer wall of the coaxial portion apertured for passage of the center conductor of the coupler and wherein a portion of one wall of the radial portion of the line forms an overlying outer conductor extension portion for a coaxial coupling device to load the coaxial coupler to maintain the characteristic impedance to obtain a broadband match. In another embodiment of the present invention, a coupling capacitor structure is disposed at the inner end of the inner conductor of the coaxial line, whereby the capacitor structure balances out a small series inductive reactance of the inwardly projecting portion of the coaxial line to provide a refiectionless window.

The present invention is a continuation-in-part of parent application Ser. No. 525,455, filed Feb. 7, 1966 now abandoned and assigned to the same assignee as the present invention.

Heretofore, composite coaxial line coupling devices and RF. coaxial line windows have been used. However, in these prior devices, the window typically took the form of a ceramic or glass disk or bead disposed across the coaxial line at its entrance into the inductor of the circuit, usually a cavity resonator, to which the center conductor portion was connected or coupled. In such a device, the window introduces an impedance mismatch in the coaxial line which makes it unsuited for broadband coupling applications where wave reflections from the coupling device are to be avoided over a very broad frequencey range, for example, of 4 to 14 gc.

In the present invention, a composite coaxial coupling device and coaxial window is provided which is essentially refiectionless over the aforementioned frequency range. The broadband characteristic is attributable to utilizing a frame member and a portion of the window as integral portions of the coaxial line coupling device, whereby the distance betwen the anode circuit and the window are reduced to a minimum to obtain broadband operation.

The principal object of the present invention is to provide an improved composite coaxial coupling device and window for a coaxial line and tubes using same, whereby improved broadband performance characteristics are obtained.

One feature of the present invention is the provision of a composite coaxial line coupling means and cylindrical dielectric window wherein the window surrounds the cen- 3,448,331 Patented June 3, 1969 ter conductor of a coaxial line and projects with the center conductor into the region of the circuit to be coupled to the line with an extension of the outer conductor of the coaxial line disposed adjacent the inwardly projecting cylindrical window member to maintain its characteristic impedance whereby reflections are avoided over a broadband.

Another feature of the present invention is the same as the preceding feature including the provision of a disk shaped frame member portion sealing the center conductor of the coaxial line to the inwardly projecting cylindrical window at its inner end, and wherein the frame member is closely spaced and coupled to a conductor portion disposed Opposite to the conductor portion through which the coaxial line projects, whereby the impedance match is enhanced.

Another feature of the present invention is the same as one or more of the preceding features wherein the outer end of the cylindrical window is sealed over an axially coextensive region to a coaxially disposed cylindrical frame member which surrounds the cylindrical window, and which cylindrical frame forms a substantial length of the outer conductor of the coaxial line.

Another feature of the present invention is the same as any one or more of the preceding features wherein the composite window and coaxial coupling means is used for coupling wave energy from a voltage tunable magnetron to a load.

Another feature of the present invention is the same as any one or more of the preceding features wherein the center conductor of the coaxial line, which projects into the region of the circuit to be coupled, is capacitively coupled to the circuit at its inner end portion; whereby the capacitance serves to resonate a series inductance of the protruding center conductor of the coaxial line to better the impedance match between the coaxial line and the circuit being coupled.

Other features and advantages of the present invention will become apparent upon a perusal of the following specification taken in connection with the accompanying drawings wherein:

FIG. 1 is a schematic transverse sectional view of a magnetron oscillator coupled to a load,

FIG. 2 is an w-fl diagram showing the disperson characteristics for a voltage tunable magnetron,

FIG. 3 is a longitudinal sectional view of a magnetron incorporating features of the present invention. The view being similar to that as taken along line 3-3 in the direction of the arrows of FIG. 1.

FIG. 4 is an enlarged front view of an interdigital line magnetron interaction circuit similar to that as seen by a view taken along line 44 of FIG. 3 in the direction of the arrows,

FIG. 5 is a schematic equivalent circuit diagram for the interdigital magnetron interaction circuit of FIG. 3,

FIG. 6 is a transverse schematic circuit diagram for the tube of FIG. 3,

FIG. 7 is an enlarged sectional detailed view of an alternative embodiment of the present invention as delineated by lines 7-7 of FIG. 3,

FIG. 8 is an alternative embodiment of a portion of the structure of FIG. 3 delineated by line 8-8,

. FIG. 9 is a transverse sectional view of a portion of the structure of FIG. 8 taken along line 9-9 in the direction of the arrows,

FIG. 10 is a schematic equivalent circuit diagram for the output coupling circuit of FIGS. 8 and 9, and

FIG. 11 is an alternative embodiment of the structure of FIG. 7.

Referring now to FIG. 1 there is shown in schematic form a voltage tunable magnetron. More specifically, the magnetron includes ananode structure 1 coaxially surrounding acathode electrode 2 and defining, in an annular region therebetween, amagnetron interaction region 3. Theanode 1 is provided with a suitable fundamental backward waveperiodic wave circuit 4 formed therein facing thecathode 2 for interaction with the electrons of an electron stream in themagnetron interaction region 3. In operation suitable operating potentials are applied betweencathode 2 andanode 1 in the presence of an axially directed magnetic field B in themagnetron interaction region 3 for cumulative interaction with the electron stream to produce an output signal. The output signal is extracted from thecircuit 4 via suitable coupling means 5 and fed to a load 6. The voltage tunable magnetron will oscillate at a frequency determined by thecircuit 4 and by the voltage between thecathode 2 and theanode 1. The frequency range over which the tube may be tuned depends upon the loaded Q of theperiodic circuit 4.Circuit 4 may be loaded by heavily coupling thecircuit 4 to the load 6 or the circuit may be provided with internal resistance to lower its load Q.

Referring now to FIG. 2 there is shown a dispersion characteristic for a typical fundamental backward wave circuit. When thecircuit 4 is re-entrant, such that wave energy can travel in a continuous path around the circuit, the dispersion characteristic becomes discontinuous in the sense that a number of resonant modes of oscillation are produced corresponding to an integral number of full wavelengths of wave energy travel around thecircuit 4. Typically, there will be N/Znumber of resonant modes established where N is the number of periodic elements taken around thecircuit 4. Thus, if a circuit has 8 slot resonators as depicted in FIG. 1, there will be N/2 or 4 resonant modes of oscillation established at equal intervals of B or phase shift per period of the circuit. Heretofore, it has been the practice to operate on the 1r mode designated N/Z on the diagram. However, in the tube incorporating the output coupling feature of the present invention, the (N/2-1) mode is used, which, for a given operating frequency band, permits theanode circuit 4 to have larger dimensions and thus greater power handling capability than would be attainable if the tube was designed for operation on the 1r mode. Thus, the tube is operable over an electronic bandwidth from w to ta corresponding to synchronous beam voltages of V to V as shown in the diagram of FIG. 2. However, in order to obtain such a wide tuning range, thecircuit 4 must be heavily loaded such that the loaded Q of the anode circuit is on the order of to 20. If the coupling to the load does not provide a good match between the load and the tube, the tuning range of the tube will be drastically affected. Any reflection introduced in the coupling between the load and the tube diminishes the coupling thereby raising the Q of theanode circuit 4 and reducing its tunable bandwidth. Thus, a reflectionless match between theanode circuit 4 and the load is desired for maximum tunable bandwidth.

Referring now to FIG. 3, there is shown in longitudinal section a voltage tunable magnetron incorporating the output coupling circuit of the present invention. More specifically, the tube includes ananode 1 having a crown supported interdigitaltype anode circuit 4 essentially as shown in FIG. 4. Theinterdigital anode circuit 4 is crown supported by a pair of annular plates 11 which include radial portions followed by axial directed portions and which are closed at their outer ends byend wall 12. The anode circuit coaxially surrounds a coldcathode sole electrode 2 operated at cathode potential. An annularmagnetron interaction region 3 is defined between theinterdigital circuit 4 and the axially coextensive portion of thecathode electrode 2. Anelectron gun 13 is disposed at the opposite end of the tube from thecold cathode electrode 2 and includes ahelical filamentary emitter 14 surrounded by aninjector electrode 15 operating at a substantially lower potential than theanode circuit 4 whereby the electrons are axially injected into themagnetron interaction region 3 under the confining effect of the axial magnetic field B.

The vacuum envelope for the tube is defined by several annular members sealed together in a vacuum tight manner at their abutting surfaces. Thecathode sole 2 is sealed to an annularceramic insulator 16 which in turn is sealed to the lower conductor plate 11 of the anode. Lower plate 11 is also sealed in a vacuum tight manner to the other plate 11 via the intermediary of the coaxial axially extending wall portions and theend closing wall 12. The upper side of the upper annular anode plate 11 is sealed to another insulating ring 17 as of alumina which is in turn sealed to end enclosingplate member 18 as of ceramic.

The equivalent circuit for theanode circuit 4 is shown in FIG. 5. The circuit is essentially a two wire transmission line with series loading in the two conductors A and B formed by the quarter wave slot resonators formed between adjacent fingers in each of the lines. This can be readily seen by reference to FIG. 4 wherein one of the plates 11 is designated as A and the opposed plate 11 is designated as B. The upper cutoff frequency of the circuit is formed when the slot resonators formed in the interdigitated conductors A and B become resonant. This corresponds to alength 1 between successive interaction regions of a half wavelength and a finger length of nearly a half wavelength. On the w-fi diagram this upper cutoff frequency is :1 and for, the tube of FIG. 3 this frequency is selected to be approximately 70 gc. corresponding to a finger length of approximately 0.084".

The low frequency cutoff of this circuit 40;; corresponds to a resonance of the shunt elements L and C formed by the folded radial quarter wave cavity having a length designated 1 in FIG. 3 and capacitively loaded by the capacitance C between adjacent fingers of the interdigital line. In the tube of FIG. 3 I is selected such that the resonant frequency of the 11' mode corresponding to (0 is approximately 4 gc. With this low frequency cutoff, substantial mode separation is obtained between the (N/Z-l) operating mode at 856 to 9.6 gc. and

the adjacent 1r mode. The electron stream in themagnetron interaction region 3 successively cumulatively interacts with the electric field E between adjacent fingers which corresponds to the capacitive voltages developed across capacitors C in FIG. 5.

At the operating (N/Z-l) mode the shunt cavity resonator portion of the circuit formed by the shorted folded section of radial transmission line, defined by annular radial and axial plates 11 as closed byend wall 12, operates in the TM mode. This mode pattern is shown in FIG. 6.

The output signal is coupled out of the cavity via coaxial coupling means 21 which couples across a portion of the shunt inductor L More specifically, acoaxial line 22 is coupled to a load, not shown, and in the embodiments of FIGS. 3 and 7 has itscenter conductor 23 conductively connected to the inner conductor plate 11 of the crown supported interdigital line by passing through anaperture 24 in the outer wall 11. A cylindrical dielectric window member as ofalumina ceramic 25 coaxially surrounds theconductor 23 and projects inwardly of the vacuum envelope into the region ofspace 26 defined between the two conductor portions 11. A disk shapedmetallic frame member 27 as of copper plated molybdenum is brazed to the end of the inner end of thecylindrical window member 25 in a vacuum tight manner. Theframe member 27 is centrally apertured and is brazed to amolybdenum plug 28 which in turn is brazed to conductor portion B of the cavity.Plug 28 is centrally bored and tapped to receive thecenter conductor 23 threaded therein. The outer end of thecylindrical window 25 is brazed to acoaxially surrounding sleeve 29 as of nickel over an annular axially coextensive brazedregion 31 to form a vacuum tight seal therebetween. Sleeve 29 '5 forms the outer conductor of the coaxial line segment, which includes thewindow member 25 and thesleeve 29 and is in turn brazed in a vacuum tight manner at its inner end to theapertured wall 24 of conductor 11.

Thecylindrical window member 25 is closely spaced to the radial conductor portion 11 such as to maintain its characteristic S052 impedance for that portion of its length which projects into thecavity 26. This closely spaced outer conductor region is designated as 32 and assures a reflectionless coupling to the fields of the cavity by maintaining the characteristic impedance of theline 23 into the point of connection betweenplug 28 and conductor 11. An externally threaded miniaturecoaxial connector adapter 34 is soldered over the outer end of thesleeve 29 to facilitate connection of thecoaxial line 23 to a standard 509 miniature coaxial line.

By designing thewindow assembly 21 such that it presents substantially the same characteristic impedance, i.e. 509 as the miniature coaxial line into the point where it is connected to the inner conductor 11 there is assured a refiectionless connection between thecircuit 4 and the load resistance of the load 6, not shown in FIG. 3, whereby the circuit is heavily loaded by the load and its Q reduced to approximately -20 for broadband operation.

Referring now to FIG. 7 there is shown an alternative embodiment of the present invention wherein the closely spacedconductor region 32 has been replaced by a continuation formed by an inward extension of thesleeve 29 designated at 35. Thus, as in the embodiment of FIG. 3, the window segment maintains the characteristic 509 impedance into the point of connection of theinner conductor 23 to the axially directed portion of plate 11 via the intermediary offrame member 27.

Referring now to FIGS. 8-11 there is shown an alternative embodiment of the present invention. It has been found that in the output coupling arrangements of FIGS. 3 and 7, that the center conductor segment of thecoaxial line 21, which projects into the circuit being coupled to, has associated therewith a small amount of series inductance Ls, see FIG. 10. This inductance Ls presents a small reactance tothe slowwave circuit 4 which tends to shift the operating frequency of the tube and to slightly decouple the load from thetube 1.

This small series industance Ls is balanced out in the embodiments of FIGS. 811 by capacitively coupling the inner end of thecenter conductor 23 to conductor B of theslow wave circuit 4. The series capacitance of the coupling capacitor Cs is series resonated at the frequency of the tube with the series inductance Ls. Due to the heavy coupling of thecircuit 4 to the 50S load the Q of the series resonant coaxial coupling circuit, as coupled to theslow wave circuit 4, is so low that the pass band of the series resonant coupling circuit is much wider than the electrically tunable band of the tube on the operating (N/2-1) mode.

The apparatus of FIGS. 8-1l is essentially identical to the apparatus of FIGS. 3 and 7 except for the provision of the coupling capacitor Cs provided at the inner end of thecenter conductor 23. More particularly, in the structure of FIGS. 8 and 9 theplug 28 is terminated flush with a circumferentially enlargedwindow frame member 27. Aconductive tab 41 as of copper is brazed to conductor B such as to provide a portion facing theframe member 27 which is substantially of the same dimensions as thewindow frame member 27. Theframe member 27 is then slightly spaced from thetab 41 to form the series coupling capacitor structure Cs.

In a typical example of the capacitive coupling structure thetab 41 is made to have a circumferential extent of about 0.250", a thickness of 0.030", and a height h of about 0.100. The spacing s between the opposed faces of thetab 41 and the end of theframe 27 is dimensioned for series resonance at the center of the pass band of thetube 1 and typically falls within the range of 0.015" to 0.030".

Referring now to FIG. 11 this structure is essentially identical to the structure of FIG. 7 except that thewindow frame member 27 is terminated short of the opposed conductor B by a slight spacing s to form the series coupling capacitor Cs. The spacing s typically falls within the range of 0.015" to 0.030".

Since many changes could be made in the above construction and many apparently widely different embodiments of 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 composite coaxial line coupling device and gas tight wave permeable window assembly including, an evacuated wave supporting region of space defined be tween a pair of conductive portions defining a section of wave supporting structure having a radial line portion and a coaxial axially directed portion and containing fields to be coupled to a coaxial line, means forming a coaxial line having inner and outer conductor portions for coupling to the fields of said field containing region of space and having a certain characteristic impedance, the outer wall of said coaxial portion of said section of wave supporting structure being apertured for passage of said inner conductor of said coaxial line therethrough for coupling to the other conductor portion of said wave supporting structure, means forming a wave permeable dielectric window member coaxially surrounding said inner conductor and projecting into said field containing region of space, means at the inner end of said window for sealing said window member to said inner conductor, means forming an extension of said outer conductor of said coaxial line formed by a portion of one wall of said radial portion of said wave supporting structure disposed overlying an axially coextensive region of the inwardly projecting portion of said dielectric window member for loading same to maintain the characteristic impedance of the inwardly projecting portion of said coaxial line means, whereby reflections of wave energy from said window are minimized.

2. The apparatus according toclaim 1 wherein said wave supporting region of space is a portion of a microwave periodic circuit, and including means for producing a stream of charged particles adjacent said periodiccircuit for cumulative interaction with the fields thereof for producing an output signal which is coupled from said circuit to a load via said coaxial line.

3. The apparatus according toclaim 2 wherein said periodic circuit and said particle stream producing means are portions of a voltage tunable magnetron.

4. The apparatus according toclaim 4 wherein said periodic circuit is heavily coupled to the load for loading the periodic circuit and reducing the Q thereof for broadbanding said voltage tunable magnetron.

5. The apparatus according toclaim 1 wherein said dielectric window member is a ceramic cylinder.

6. The apparatus according toclaim 1 wherein said means for sealing the inner end of said window member to said center conductor comprises an annular metallic frame member.

7. The apparatus according toclaim 3 wherein said evacuated wave supporting region of space is contained withinin radial cavity resonator resonant in the TM mode at the output signal frequency.

8. A composite coaxial line coupling device gas tight wave permeable window assembly including, an evacuated wave supporting region of space defined between a pair of conductive portions and containing fields to be coupled to a coaxial line, means forming a coaxial line having an inner and outer conductor for coupling to the fields of said field containing region of space and having a certain characteristic impedance, said inner conductor passing through an aperture in one of said field supporting conductor portions and being coupled to the other conductor portion, means forming a wave permeable dielectric window member coaxially surrounding said inner conductor and projecting into said field containing region of space, means at the inner end of said window for sealing said window member to said inner conductor, means forming an extension of said outer conductor of said coaxial line disposed overlying an axially coextensixe region of the inwardly projecting portion of said dielectric window member for loading same to maintain the characteristic impedance of the inwardly projecting portion of said coaxial line means, and means forming a coupling capacitor structure disposed at the inner end of said inner conductor of said coaxial line means for coupling said inner conductor of said coaxial line means to said other conductor portion which is being coupled to said coaxial line, whereby said capacitor structure balances out a small series inductive reactance of the inwardly projecting portion of said coaxial line to provide a reflectionless window assembly.

References Cited UNITED STATES PATENTS 2,404,086 7/1946 Okress et a1. 33333 2,408,271 9/1946 Rigrod et al. 33333 2,557,391 6/1951 Okress et al. 333-33 3,195,010 7/1965 Lock 3l539.53 3,334,266 8/1967 Frutiger 3l539.53

HERMAN K. SAALBACH, Primary Examiner.

SAXFIELD CHATMAN, JR., Assistant Examiner.

US. Cl. X.R.

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