US3063030A

US3063030A - Temperature compensated resonant cavities

Info

Publication number: US3063030A
Application number: US782522A
Authority: US
Inventors: John F Manahan; Edwin W Richter
Original assignee: Raytheon Co
Current assignee: Raytheon Co
Priority date: 1958-12-23
Filing date: 1958-12-23
Publication date: 1962-11-06
Anticipated expiration: 1979-11-06

Description

Nov. 6, 1962 J. F. MANAHAIN ETAL 3,063,030

TEMPERATURE `COMPENSATED RESONANT CAVITIES Filed Dec. 25, 1958 INVENTOS JOHN F. MA/VAHAN EDWIN W- RICHTER A TTOH/VEY United States Patent hfice Pam.,

3,063,030 TEMPERATURE CUMPENSATED RESONANT CAVTHJS .lohn F. Manahan, Chelmsford, and Edwin W. Richter,

This invention relates to resonant cavities, and more particularly, to means for compensating for the effects of thermal expansion on frequency in a resonant cavity.

It is well known that the resonant frequency of a resonant cavity fluctuates with dimensional changes caused by temperature variations. One known method employed to reduce this effect on frequency is to construct the cavity of an iron-nickel alloy, known as Invar, which has a very small coefficient of thermal expansion. Also', as is known, the cost of resonant cavities made of this material is quite expensive and, further, cavities of this type do not provide complete compensation especially where the cavity is subjected to extreme temperature variations. Another temperature compensating means which is utilized consists of' a resonant cavity made with quartz as the main frequency controlling element in order to take advantage of the very low linear coecient of expansion of quartz. However, when an attempt is made to hermetically seal a quartz cavity by normal soldering or brazing techniques, the solder has a different coefficient of expansion than the quartz and this changes the effective coecient of expansion of the cavity in a non-linear manner which is diilicult to compensate. This is particularly noticeable when the cavity is used as a reference for a source of oscillation in order to obtain a high degree of stability over extreme environmental conditions, such as wide changes in temperature, shock, humidity and atmospheric pressure. It is, therefore, desirable to provide a quartz reference cavity while is capable of uniform reproduction and at the same time is capable of being compensated by a material having a substantially linear coeilicient of expansion.

In accordance with the reference cavity of the invention, a cylindrical resonant structure or cavity is made of clear fuzed quartz having a low resistance metallic coated inner surface. A waveguide coupling member or flange is urged against one end of the quartz cylinder by a plurality of coupling springs mounted outside the Wall of the cavity. Surrounding the opposite end of the quartz cylinder is a cavity housing having a metal-lic re-entrant cylinder or cap which is adapted to expand within the quartz cavity in response to a change in temperature. This cap is compressed against the end of the quartz cylinder and is spring loaded to the waveguide coupling flange in order to provide a tightly sealed expandable cavity without soldering directly to the quartz. A single fluted bellows is soldered between the housing and waveguide ange to complete the hermetic seal of the cavity and to permit the housing and the waveguide flange to expand or contract with respect to each other. In addition, the center of the cavity housing is deformable by application of pressure to provide a fixed tuning mechanism. As the length and diameter of the quartz cylinder increases in response to heat or other environmental changes, the re-entrant cap, being spring anchored to the end of the quartz cylinder, expands at a different rate into the cavity to compensate for the increase in volume of the cylinder, resulting in substantially no change in the resonant frequency of the cavity. With this arrangement, the desirable linear expansion properties of the quartz are obtained, and, at the same time, no solder joints or similar sealing materials are bonded directly to the quartz to adversely affect its linear coefficient of expansion or mechanical dimensions.

Further objects and many of the attendant advantages of this invention will be readily appreciated as the description thereof progresses. In the accompanying drawing there is shown an isometric View of a resonant cavity 16 which can be used as an automatic frequency control of a microwave oscillator or as a tuned filter or like component for radio or other electrical circuits. Resonant cavity 10 comprises a cylindrical quartz structure 12 which is securely disposed between a waveguide coupling member or ilange 14 and a cavity housing 16.

The inner surface of the quartz structure 12 is coated with silver 17 or with a similar highly conductive material. The cavity housing 16 is formed of material having a higher coecient of thermal expansion than the quartz cavity and, in the present embodiment, is constructed of aluminum. The cavity housing extends around the outer portion of the quartz cavity and is compressed against the end of the quartz cylinder at 18'. The re-entrant portion 2i) of the cavity housing extends within the quartz cylinder a distance, l, and expands into the cavity at a rate of expansion determined by this distance. Thus, to compensate for the coeicient of linear expansion of quartz, the re-entrant material expands at a faster rate than the quartz. 'Il-1e distance which the compensating material projects into the cavity is a function of the ratio of the coelcient of expansion of the cavity and of the compensating material and is calculated in a well-known manner. Since the cavity housing 16 is compressed only against the end portion of the quartz cylinder, the expansion of the housing occurs into the cavity. In the center of the cavity housing is a cylindrical probe 22, which is slidably inserted into an aperture 23 in the cavity housing. A deformable metallic tuning cap 24 is integral with probe 22 and ts into the cavity housing. The metal tuning cap is deformable by application of pressure at its tapped portion to provide a fixed tuning mechanism which is permanently set to a desired resonant frequency and which expands with the re-entrant portion of the cavity housing into the cavity during temperature changes. Thus, for example, a 10,000 megacycle-per-second cavity can be tuned to any frequency within a forty megacycleper-second band by deforming the metal of the tuning cap. For example, at a given temperature, the cavity can be tuned within x50 kilocycles per second of a pre selected frequency.

Extending from the outer portion of the cavity housing 16 and integral therewith is an external mounting ange 26 which contains four equally spaced apertures to receive four mounting bolts 27 with steel springs 2S. The

mounting bolts 27 are inserted through the springs and then into the apertures of flange 26. Each spring is compressed between the head of the 'bolt 27 and the face of flange 26. The bolts are received by tapped apertures in the flange portion 29 of waveguide coupling 14. In this manner, the four springs 28 urge the cavity housing toward the waveguide coupling member and support the quartz cylinder in a manner which permits the cavity to expand in both length and diameter. In order to prevent air drafts on the compensator end of the cavity, a cover, not shown, preferably surrounds the entire cavity assembly and is bolted to an outer ange 29 on the waveguide coupling member 14. By means of this cover, the cavity parts are maintained in thermal equilibrium during rapid temperature changes.

In order that high frequency energy can be introduced and extracted from the cavity, the waveguide coupling member 14 is provided with an input section 34 and an oppositely disposed output section 36. Each section consists of a waveguide cavity having a resonant iris 38 coupling into the quartz structure 12 and a pair of

glass waveguide windows

42 and 44 to permit sealing of the cavity structure. These windows form part of the coupling ange portion 30 of the waveguide coupling member which is integral with ange portion 29 and provided with threaded tubes 32 to couple to input and output rectangular waveguide, not shown. The windows are located in the waveguide coupling member remote from the cavity Walls so that their physical variations with temperature and atmospheric changes have no effect upon the resonant frequency of the cavity.

In order to maintain a constant dielectric medium within the quartz cavity, evacuation of the cavity is achieved by means of an aperture 46 in the waveguide coupling member 14. This tubular portion extends radially outward from the waveguide coupling member and contains a metal exhaust tube 47 which is hermetically sealed to the waveguide coupling member 14 and pinched off after the cavity has been evacuated. An exhaust tube guard member 48 is attached to the waveguide coupling ange in order to protect the end portion of the exhaust tube. A single uted copper bellows 50 is soldered between the cavity housing 16 and the waveguide ilange 14 to complete the hermetic seal of the cavity. This bellows permits expansion and contraction of the cavity housing and waveguide ilange with respect to each other during temperature variations of the cavity. As noted, the cavity is tuned by deforming the annealed copper end cap 24 which is shaped in a manner to reduce microphonics and is hermetically sealed to cavity housing 16. In addition, apertures 25 permit the evacuation of the enclosed area formed by the copper end cap 24 and the cavity housing.

While the present embodiment of the invention utilizes a TEU mode cylindrical quartz cavity as its frequency controlling element, other materials such as plastics, ceramics or other metals can be substituted for quartz providing that a high conductive coating is applied to the inner surface of the cavity material. In each case, however, the distance, l, which the re-entrant compensating material protrudes within the cavity can be changed to compensate for the linear coeflicient of expansion of the substitute cavity material. In addition, the re-entrant portion of the cavity housing 16 can be constructed of materials other than aluminum and the required linear coefficient of expansion of the substituted material can be calculated in a wellknown manner.

For the foregoing reasons, it is to be understood that the above-described arrangements are illustrative of the application of the principles of the invention. Numerous other arrangements may be devised by those skilled in the art without departing from the spirit and scope of the invention. Accordingly, it is desired that the invention not be limited to the particular details of the embodimentsdisclosed herein except as defined in the appended claims.

What is claimed is:

l1. A temperature compensated resonant cavity comprising a hollow cylindrical quartz structure having a substantially linear coecient of expansion in response to changes in temperature, a waveguide coupling member in register with one end of said cylindrical structure to form a rst solder-free joint therewith, a re-entrant metallic cap extending into said cylindrical structure and enclosing the other end of said cylindrical structure to form a second solder-free joint therewith and adapted to expand into said resonant cavity at a diierent rate of expansion than that of said cylindrical structure, thereby to compensate for a change in volume of said resonant cavity in response to a change in temperature, and tension means extending out.

side said cylindrical structure urging said waveguide coupling member and said -reentrant metallic cap toward each other, thereby to provide a microwave seal for said resonant cavity.

2. A temperature compensated resonant cavity comprising a hollow cylindrical quartz structure having a substantially linear coeicient of expansion in response to changes in temperature, a waveguide coupling member in register with one end of said cylindrical structure to form a first solder-free joint therewith, a reentrant metallic cap extending into said cylindrical structure and enclosing the other end of said cylindrical structure to form a second solder-free joint therewith and adapted to expand into said resonant cavity at a diierent rate of expansion than that of said cylindrical structure, thereby to compensate for a change in volume of said resonant cavity in response to a change in temperature, the inner surface of said cylindrical structure having a metallic coating thereon, and tension means extending outside said cylindrical structure urging said waveguide coupling member and said reentrant metallic cap toward each other, thereby to provide a microwave seal for said resonant cavity.

3. A temperature compensating cavity resonator comprising a hollow cylindrical quartz structure having a substantially linear coefficient of expansion in response to changes in temperature, a waveguide coupling member positioned at one end of said cylindrical structure and adapted to couple energy to said cavity resonator to form a rst solder-free joint therewith, a lreentrant metallic cap extending into said cylindrical structure and enclosing the other end of said cylindrical structure to form a second solder-free joint therewith and adapted to expand into said resonant cavity at a diierent rate of expansion than that of said cylindrical structure, thereby to compensate for a change in volume of said resonant cavity in response to a change in temperature, and tension means extending outside said cylindrical structure urging said waveguide coupling member and said reentrant metallic cap toward each other, thereby to provide a microwave seal for said resonant cavity.

4. A temperature compensated resonant cavity comprising a hollow cylindrical quartz structure having a substantially linear coeicient of expansion in response to changes in temperature, a waveguide coupling member in register with one end of said cylindrical structure to form a first solder-free joint therewith, a reentrant metallic cap extending into said cylindrical structure and enclosing the other end of said cylindrical structure to form a second solder-free joint therewith and adapted to expand into said resonant cavity at a different rate than that of said cylindrical structure, thereby to compensate for a change in volume of said resonant cavity in yresponse to a change in temperature, an expandable bellows member connected between said waveguide coupling member and said reentrant metallic cap, and tension means extending outside said cylindrical structure urging said waveguide coupling member and said reentrant metallic cap toward each other, thereby to provide a microwave seal for said resonant cavity.

References Cited in the file of this patent UNITED STATES PATENTS 2,281,247 Peterson Apr. 28, 1942 2,439,908 Rigrod Apr. 20, 1948 2,553,811 Carnine May 22, 1951 2,883,630 Wheeler Apr. 21, 1959

Claims

2. A TEMPERATURE COMPENSATED RESONANT CAVITY COMPRISING A HALLOW CYLINDRIL QUARTZ STRUCTURE HAVING A SUBSTANTIALLY LINEAR COEFFICIENT OF EXPENDING IN RESPONSE TO CHANGES IN TEMPERATURE, A WAVEGUIDE COUPLING MEMBER IN REGISTER WITH ONE OF SAID CYLINDRICAL STRUCTURE TO FORM