This invention relates to magnetron arrangements and more particularly to magnetron outputs.
According to the invention, there is provided a magnetron arrangement comprising a magnetron having a coaxial output which is coupled in an endfire configuration to a rectangular waveguide.
The present inventors have realised that the traditional technique for coupling the output of a magnetron into a rectangular waveguide need not be used. By employing the invention, a much more compact arrangement may be realised which also gives weight savings and a reduction in materials required. The endfire configuration is also particularly convenient for coupling to other parts of an r.f. system for which the magnetron supplies the power, for example. A particularly significant advantage of the invention is that it avoids the need to accurately locate a probe with respect to a backstop, reducing manufacturing time.
By “endfire configuration” it is meant that the coaxial output extends in the same direction as the direction in which energy is transmitted along the waveguide.
Preferably, the coaxial output is coupled directly to the rectangular waveguide, that is, there are no intervening transitional sections for converting a circular waveguide mode to a rectangular waveguide mode. Possibly a transition could be included but this would tend to undesirably increase the complexity and bulk of the arrangment without necessarily giving a significantly improved coupling between the coaxial output and the rectangular waveguide.
Preferably, the central conductor of the coaxial output is aligned with the edge of a broad wall of the rectangular waveguide and at its mid-point. This location gives optimum coupling between the two components.
The coaxial output may be located flush in a surrounding wall but preferably is surrounded by a cylindrical wall. This may be arranged to act as a harmonic choke around the coaxial output, presenting one quarter wavelength at the second or third harmonic of the operating frequency to filter power coupled from the magnetron at the undesired harmonic frequencies. Where a harmonic choke is included in the coaxial to waveguide transition, other dimensions used to match the coaxial output to the waveguide are modified so as to incorporate the inductance of the choke at the operating frequency.
One way in which the invention may be performed is now described by way of example with reference to the accompanying drawings, in which:
With reference to
The probe 14 is located adjacent to the end of a rectangular waveguide 17 into which the energy from the magnetron is to be coupled for transmission in the direction shown by the arrow. As can be seen more clearly in
In this embodiment, a harmonic choke 19 which is one quarter wavelength long at the second or third harmonic of the operating frequency is included around the probe 14. This acts to filter undesirable output frequencies.
Number | Date | Country | Kind |
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9930110 | Dec 1999 | GB | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/GB00/04931 | 12/21/2000 | WO | 00 | 11/4/2002 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO01/46985 | 6/28/2001 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
3334266 | Frutiger | Aug 1967 | A |
3641389 | Leidigh | Feb 1972 | A |
3739225 | Mims | Jun 1973 | A |
3758886 | Landry et al. | Sep 1973 | A |
4139828 | Commault et al. | Feb 1979 | A |
4673783 | Igarashi et al. | Jun 1987 | A |
5216327 | Myers et al. | Jun 1993 | A |
5461283 | Thornber et al. | Oct 1995 | A |
5525865 | Simpson | Jun 1996 | A |
5838212 | Pettit et al. | Nov 1998 | A |
5894198 | Miki et al. | Apr 1999 | A |
6097018 | Kim et al. | Aug 2000 | A |
6097154 | Choi | Aug 2000 | A |
6114676 | Jerby et al. | Sep 2000 | A |
Number | Date | Country |
---|---|---|
777485 | Jun 1957 | GB |
2 280 541 | Feb 1995 | GB |
59-103340 | Jun 1984 | JP |
Number | Date | Country | |
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20030121911 A1 | Jul 2003 | US |