This invention relates to collectors for electron beam tubes.
Linear electron beam tubes are used for the amplification of rf signals. They incorporate an electron gun for the generation of an electron beam of the appropriate power. The electron gun has a cathode heated to a high temperature so that the application of an electric field results in the emission of electrons, the electric field being produced by spacing an anode in front of and some distance from the cathode. Typically, the anode is held at around potential and the cathode at a large, for example, several tens of kilovolts, negative potential.
In one type of linear beam tube called an Inductive Output Tube (IOT), a grid is placed close to and in front of the cathode and an rf signal to be amplified is applied between the cathode and grid so that the electron beam generated in the gun region is density modulated. The density modulated electron beam is directed through an rf interaction region which includes one or more resonant cavities. The beam may be focussed by magnetic means, to ensure that it passes through the rf region, and delivers power at an output section where the amplified rf signal is extracted.
After passing through the output section the beam enters a collector where it is collected and the remaining power on it is dissipated. The amount of power needing to be dissipated depends upon the efficiency of the linear beam tube, this being the difference between the power of the beam generated at the electron gun region and the rf power extracted in the output coupling of the rf region.
A collector may consist of a single conductive component, usually of copper, which operates at ground potential or close to ground potential. It is known to improve the overall efficiency of an amplifier tube by using a collector consisting of a number of electrically isolated stages each operating at a respective potential at or between ground and cathode potential. In one such typical arrangement for a high power klystron used for the amplification of television signals at uhf frequencies the collector has 5 stages, the difference in potential between the various stages being 25% of the beam voltage. By using such a multi-stage collector, the electrons in the beam are slowed down before impacting on the electrode surfaces thus leading to greater recovery of energy. Collectors may of course have a different number of stages operating at different potentials to effect an energy saving.
According to a first aspect of the invention, a multi-stage collector for an electron beam tube comprises: at least two electrode stages with a dielectric ring located between them, the ring having a respective metal plate on each of its end faces electrically connected to respective different stages such that they act together with the ring to define a high frequency distributed bypass capacitor.
The ring is an annulus, the radial distance between its outer and inner peripheries being equal to or greater than the axial distance between its end faces. This is in contrast to a conventional arrangement in which electrical insulation between adjacent electrode stages is provided by a dielectric cylinder having a significant axial length compared to the thickness of its wall. By using the invention, the ring enables a high capacitance to be achieved as the distance between the plates is small compared to their surface area. Thus the combination of the ring and the metal plates is able to perform as a bypass capacitor which is effective as a low impedance at high frequencies. The electron beam entering the collector is modulated by rf current components, generating rf voltages in the collector region. This can result in rf leakage occurring from the inside of the collector to the outside of the collector through insulators separating collector stages. Use of the invention permits rf leakage through the insulators to be reduced or eliminated compared to a conventional construction. Preferably the ring is of a ceramic material, but other forms of insulator may be suitable.
In a preferred embodiment, at least one of the metal plates consists of a metallisation layer, which may be laid down accurately using well known techniques. However, the metal plates could instead comprise separately fabricated components which are then fixed to the surface of the ring.
Advantageously, at least one of the metal plates does not extend to the inner and outer peripheries of the face on which it is located. Thus, in addition to the axial thickness of the ring providing a certain path length between components at different electrical potentials, there is also the distance between the edge of the metal plate and the periphery. It is therefore possible to obtain the same voltage hold-off with the dielectric ring as would be possible with a dielectric cylinder of greater axial length. This also provides a more compact collector in the axial direction.
The invention maybe applied to a collector formed as a single piece, with the dielectric ring being located between the collector and the body of the tube to which it is fixed. The distributed bypass capacitor is thus defined by the collector body, ring and tube body. Thus, a further aspect of the invention provides an electron beam tube comprising two stages, one of which is a collector, with a dielectric ring between them, the ring having a respective metal plate on each of its end faces electrically connected to the respective stages such that, together with the ring, they define a high-frequency bypass capacitor. This arrangement may be advantageous where the collector is operated at depressed voltage to give improved energy efficiency.
One way in which the invention may be performed is now described by way of example in which:
With reference to
A ceramic annular ring 5 is located between the first stage 1 and second stage 2 and another annular ceramic ring 6 between stages 2 and 3. As can be seen in
The ring 5 has an axial extent a which is significantly shorter than the distance h in a radial direction between the inner periphery 11 and the outer periphery 12. The other ring 6 has similar dimensions. The axial extent a is chosen to be great enough to provide sufficient dielectric material to withstand the voltage between collector stages 1 and 2.
As can be seen in
In this embodiment, the layers of metallisation 7 and 9 together with the thickness a of ceramic material between them together act as a distributed bypass capacitor to prevent leakage of high frequency energy from the interior of the collector and withstand the inter collector voltage while minimizing the axial extent of the collector.
As can be seen in
During use, the stages 1, 2 and 3 are operated at different electrical potentials and any rf energy appearing within the collector is prevented from leaving that region by the distributed by-pass capacitors formed by the ceramic rings 5 and 6 and associated metal plates.
The collector may be used with an IOT, klystron, travelling wave tube or any other electron beam tube device in which it is necessary to collect an electron beam such as a high frequency amplifier, as can be seen in
Number | Date | Country | Kind |
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0002523 | Feb 2000 | GB | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCTGB01/00452 | 2/5/2001 | WO | 00 | 11/18/2002 |
Publishing Document | Publishing Date | Country | Kind |
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WO0157906 | 8/9/2001 | WO | A |
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3993925 | Achter et al. | Nov 1976 | A |
4480210 | Preist et al. | Oct 1984 | A |
5536992 | Crompton | Jul 1996 | A |
5684364 | Heppinstall et al. | Nov 1997 | A |
Number | Date | Country |
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1024517 | Aug 2000 | EP |
2771215 | May 1999 | FR |
Number | Date | Country | |
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20030090208 A1 | May 2003 | US |