Coupler for resonant cavity

Wave transmission lines and networks – Resonators – Coaxial or shielded

Reexamination Certificate

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Details

C333S223000, C333S230000

Reexamination Certificate

active

06466111

ABSTRACT:

BRIEF DESCRIPTION OF THE INVENTION
This invention relates to a coupler for coupling electromagnetic energy into or out of resonant cavities (herein I/O coupler).
BACKGROUND OF THE INVENTION
An RF resonant cavity (or multiple interconnected cavities) can be used to create an RF filter. The filter may either pass an RF signal over a limited frequency range (a bandpass filter) or exclude an RF signal over a limited frequency range (a notch or bandstop filter), depending upon how the resonator is connected to the overall system. A perfect single cavity resonant cavity would operate at a single, specific RF frequency (the resonant frequency), however due to material and other considerations all resonant frequency devices operate over a frequency range which encompasses the resonant frequency.
Referring to
FIG. 1
, an RF resonant cavity is shown having a conductive post or inner conductor
11
within a conductive cavity or housing
12
. In the illustrated example, the cavity is a tunable cavity of the type shown and described in co-pending application Ser. No. 60/169,189 filed Dec. 6, 1999 (FHTAH File No. P-68696). The housing
12
can be formed by machining or by casting aluminum or other metal. An alternative would be to mold the housing from plastic and provide the interior wall
14
With a conductive coating. The cavity illustrated is a tunable cavity whereby the post includes a central bore
16
adapted to receive an adjustment screw or bolt
17
. An enlarged well
18
is adapted to receive a spring
19
. The inner conductor or post may be integral to the housing or an added component as shown in
FIG. 1. A
bellows
21
has one end rigidly fixed to the top of the center conductor
11
and its other end rigidly fixed to a top
23
. The top contains a threaded bore (not shown) which receives an adjustment screw
17
which passes through the central bore
16
, spring
19
and bellows
21
, whereby rotation of the bolt adjusts the distance between the upper surface of the top
23
of the center post and the top surface of the cavity
14
, thereby controlling the frequency of operation.
The RF signal or energy is coupled into and out of the cavity by means of a coaxial line
28
or a waveguide (not shown) suitably attached to the cavity and which extends through a hole
29
in the cavity wall. The coaxial connector is shown with the outer conductor connected to the housing which forms the ground of the system. In this manner, the housing is at system ground potential. The input structure is connected to the center conductor of the coaxial cable and is terminated in one of several ways, depending upon the mechanism used to input the RF energy into the cavity.
If the mechanism for coupling energy into the cavity is by influencing the magnetic field, the center conductor
30
of the connector will be connected by means of a wire loop
31
to the side or bottom of the housing, FIG.
1
. This is an inductive coupling mechanism. Currents through the inner conductor
11
are terminated on the grounded housing. The current in the wire
31
generates a magnetic field within the housing that serves to excite the resonant cavity. By adjusting the area enclosed by the wire loop
31
it is possible to adjust the coupling of the structure for optimum system operation.
FIG. 2
, which bears like reference numerals, shows another method of coupling electromagnetic energy into the cavity. The coupling is an electric field coupling. The center conductor
30
of the coaxial connector is terminated in a disc
33
located near but spaced from the tip of the inner conductor
11
. In this case the disc
33
acts as an antenna. Currents in the inner conductor
11
create an electromagnetic field that excites the resonant cavity. By adjusting the location and orientation of the disc
33
relative to the tip of the inner conductor
11
it is possible to adjust the coupling to obtain optimum system operation.
In devices that couple the RF energy into the cavity using wire loop
31
, the wire must have a good physical and electrical connection to the housing or inner conductor. Typically this is accomplished by soldering the end of the wire to the housing. However, since the housing is made of conductive metal, it is a very good conductor of heat. Therefore it is necessary to use a soldering method that is capable of providing a large heat source, which is expensive and difficult to do in production.
In devices that excite the cavity by electric field excitation using a conductive disk attached to the center conductor of the connector, the input coupling is adjusted by changing the size of the disk and/or the distance of separation between the disk and the inner conductor. Practical devices of this type must have the conductive disk very close to the inner conductor. This limits the power handling capability of the device. The maximum voltage level permissible is proportional to the input power and inversely proportional to the distance of separation between the conductive disk and the inner conductor. Therefore a coupler with a disc which is located 3 mm, for example, from the inner conductor can sustain roughly one-half of the input power of a device in which the disc is located 6mm from the inner conductor.
OBJECTS AND SUMMARY OF THE INVENTION
It is an object of the present invention to provide a coupler for resonant cavities which can operate with high input power.
It is another object of the present invention to provide a coupler which is easily tunable.
The foregoing and other objects of the invention are achieved by a coupler which is in the form of a configurable loop which defines a surface which is substantially parallel to the axis of the center conductor of the resonant cavity to which it is coupled.


REFERENCES:
patent: 3187278 (1965-06-01), Wheeler
patent: 3577100 (1971-05-01), Askew et al.
patent: 4551694 (1985-11-01), Biehl et al.
patent: 4686494 (1987-08-01), Kaneko et al.
patent: 5119034 (1992-06-01), Ishikawa et al.
patent: 5604471 (1997-02-01), Rattila et al.
patent: 5608363 (1997-03-01), Cameron et al.
patent: 5625330 (1997-04-01), Wilson et al.
patent: 5708404 (1998-01-01), Kurisu et al.
patent: 5750473 (1998-05-01), Shen
patent: 5841330 (1998-11-01), Wenzel et al.
patent: 5942959 (1999-08-01), Kubo et al.
patent: 5945888 (1999-08-01), Weinert et al.

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