JPH04255642A - Microwave tube - Google Patents
Microwave tubeInfo
- Publication number
- JPH04255642A JPH04255642A JP1622391A JP1622391A JPH04255642A JP H04255642 A JPH04255642 A JP H04255642A JP 1622391 A JP1622391 A JP 1622391A JP 1622391 A JP1622391 A JP 1622391A JP H04255642 A JPH04255642 A JP H04255642A
- Authority
- JP
- Japan
- Prior art keywords
- microwave tube
- cylindrical ceramic
- cathode
- electrode
- wehnelt
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 239000000919 ceramic Substances 0.000 claims abstract description 21
- 239000002184 metal Substances 0.000 claims abstract description 8
- 238000009413 insulation Methods 0.000 claims description 3
- 230000002093 peripheral effect Effects 0.000 abstract 1
- 230000000694 effects Effects 0.000 description 4
- 230000005684 electric field Effects 0.000 description 3
- 238000005219 brazing Methods 0.000 description 2
- 239000012212 insulator Substances 0.000 description 1
Landscapes
- Microwave Tubes (AREA)
Abstract
Description
【0001】0001
【産業上の利用分野】本発明はマイクロ波管に関し、特
にスタック型電子銃の絶縁部の構造に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a microwave tube, and more particularly to the structure of an insulating part of a stacked electron gun.
【0002】0002
【従来の技術】従来のマイクロ波管のスタック型電子銃
に於ては、図4に示すように高電圧側の電極としてアノ
ード電極4、低電圧側としてカソード・ウェネルト電極
5、真空外囲器と絶縁を兼ねる円筒形セラミックス部品
11とがろう付けにより接合され真空外囲器の一部を構
成している。2. Description of the Related Art In a conventional microwave tube stack type electron gun, as shown in FIG. and a cylindrical ceramic component 11 which also serves as an insulator are joined by brazing and constitute a part of the vacuum envelope.
【0003】円筒形セラミックス部品11の真空側壁面
には図に示すように円周上に突き出しが設けられている
。この突き出しは、円筒形セラミックス部品11の沿面
長を長くすることによりセラミック表面に沿って発生す
る沿面放電を制御するものであり、本図では3個の付き
出しを設けているが、アノード,カソード間の電位差に
よって突き出しの寸法、個数は当然変化する。[0003] The vacuum side wall surface of the cylindrical ceramic component 11 is provided with a protrusion on the circumference as shown in the figure. These protrusions are used to control creeping discharge that occurs along the ceramic surface by increasing the creeping length of the cylindrical ceramic component 11. In this figure, three protrusions are provided; Naturally, the dimensions and number of protrusions change depending on the potential difference between them.
【0004】0004
【発明が解決しようとする課題】このような従来構造に
於いては、アノード電極4とカソード・ウエネルト電極
5の間の電位差が大きくなるに従って、円筒形セラミッ
クス部品11の突き出しの長さlを大きくするか、突き
出しの数を増やすことにより、沿面長を大きく取ってや
る必要があった。よって、マイクロ波管の大電力化に伴
い大きなカソード電流を取るために、アノード電圧が増
大するのにつれて、円筒形セラミックス部品11の寸法
が大形化するという問題点があった。[Problems to be Solved by the Invention] In such a conventional structure, as the potential difference between the anode electrode 4 and the cathode-Wehnelt electrode 5 increases, the protrusion length l of the cylindrical ceramic component 11 is increased. Alternatively, it was necessary to increase the creepage length by increasing the number of protrusions. Therefore, there is a problem in that the size of the cylindrical ceramic component 11 increases as the anode voltage increases due to the large cathode current required as the power of the microwave tube increases.
【0005】[0005]
【課題を解決するための手段】本発明のマイクロ波管の
スタック型電子銃は、電極間の絶縁と真空外囲器を兼ね
る円筒形セラミックスの真空側壁面にその円周上に沿っ
て少くとも1個の突き出しを有し、かつ、その突き出し
の高電圧側の面に対して対向する面を有する金属製のシ
ールド部品を少なくとも1個低電圧側の電極上に設置し
た構造を有する。[Means for Solving the Problems] The microwave tube stack type electron gun of the present invention has a vacuum side wall surface of a cylindrical ceramic which serves as insulation between electrodes and a vacuum envelope at least along the circumference. It has a structure in which at least one metal shield component having one protrusion and a surface opposite to the high voltage side surface of the protrusion is installed on the low voltage side electrode.
【0006】[0006]
【実施例】次に本発明について図面を参照して説明する
。図1は本発明の第1の実施例の断面図である。円筒形
セラミックス1,2,3とアノード電極4,カソード・
ウエネルト電極5が交互に積み重ねられ、ろう付けによ
り接合されている。特に円筒形セラミックス2の真空側
壁面には円周上に1個の突き出しが設けられている。
この突き出しの高電圧側すなわちアノード電極4の側の
面に対して対向する面を有する金属製のシールド部品8
がウエネルト支持体9にろう付け又は溶接されている。
この結果、シールド部品8はカソード・ウエネルト電極
5と同電位となる。DESCRIPTION OF THE PREFERRED EMBODIMENTS Next, the present invention will be explained with reference to the drawings. FIG. 1 is a sectional view of a first embodiment of the invention. Cylindrical ceramics 1, 2, 3, anode electrode 4, cathode
Wehnelt electrodes 5 are alternately stacked and joined by brazing. In particular, one protrusion is provided on the circumference of the vacuum side wall surface of the cylindrical ceramic 2. A metal shield component 8 having a surface opposite to the high voltage side of this protrusion, that is, the surface on the anode electrode 4 side.
is brazed or welded to the Wehnelt support 9. As a result, the shield component 8 has the same potential as the cathode Wehnelt electrode 5.
【0007】従って、円筒形セラミックス2の突き出し
の表面付近はカソード電位に非常に近い値となるため、
円筒形セラミックス2とカソード・ウエネルト電極5と
のろう付部分と突き出し部の電界強度はシールド部品8
が無い場合に比べて非常に小さくなる。このため、シー
ルド部品8が無い場合には沿面放電が生じるような電位
差がカソード,アノード間に印加された場合でも、沿面
放電の種となる電子がろう付け部から電界放出されるの
を大幅に抑制することができる。[0007] Therefore, since the vicinity of the protruding surface of the cylindrical ceramic 2 has a value very close to the cathode potential,
The electric field strength at the brazed portion and the protruding portion between the cylindrical ceramic 2 and the cathode/Wehnelt electrode 5 is determined by the shield component 8.
It is much smaller than without it. Therefore, even if a potential difference that would cause a creeping discharge is applied between the cathode and the anode in the absence of the shield component 8, the electric field emission of electrons, which would cause the creeping discharge, from the brazed part is greatly reduced. Can be suppressed.
【0008】また、たとえ電子がろう付け部から電界放
出されたとしても円筒形セラミックス2の突き出しの表
面に沿って進む電子は、加速電界が十分弱いためにエネ
ルギーが小さく、セラミック表面に衝突したときに発生
する2次電子の放出比は1以下となり、電子は突き出し
部表面を進むうちに自然消滅するために沿面放電に発展
することはない。Furthermore, even if electrons are field-emitted from the brazed part, the electrons traveling along the protruding surface of the cylindrical ceramic 2 have low energy because the accelerating electric field is sufficiently weak, and when they collide with the ceramic surface, The emission ratio of the secondary electrons generated is less than 1, and the electrons spontaneously disappear as they travel along the surface of the protrusion, so they do not develop into creeping discharge.
【0009】図2は、本発明の第2の実施例を示す断面
図である。この実施例では、金属製のシールド部品10
をカソード・ウエネルト電極5にろう付けまたは溶接し
ており、作用効果は図1の第1の実施例と同じである。FIG. 2 is a sectional view showing a second embodiment of the present invention. In this embodiment, a metal shield component 10
is brazed or welded to the cathode/Wehnelt electrode 5, and the effect is the same as that of the first embodiment shown in FIG.
【0010】図3は、本発明の第3の実施例の断面図で
ある。この実施例では、円筒形セラミックス11の突き
出しが3個あり、その突き出しと突き出しの間の2ケ所
の凹部に金属製のシールド部品8が1個ずつ対応して、
ウエネルト支持体9にろう付けまたは溶接されている。
この実施例の構造は、第1および第2の実施例に比べて
セラミック表面の突きだしの個性が増加したことと、シ
ールド部品8の個数が増えたことの両方の効果により、
更に高い電位差まで使用が可能である。FIG. 3 is a cross-sectional view of a third embodiment of the invention. In this embodiment, there are three protrusions of the cylindrical ceramic 11, and one metal shield component 8 corresponds to each of the two recesses between the protrusions.
It is brazed or welded to the Wehnelt support 9. The structure of this embodiment has the effect of increasing the individuality of the protrusion of the ceramic surface and increasing the number of shield parts 8 compared to the first and second embodiments.
It can be used up to even higher potential differences.
【0011】[0011]
【発明の効果】以上説明したように本発明は、マイクロ
波管のスタック型電子銃の絶縁と真空外囲器を兼ねる円
筒形セラミックスの真空側壁面の突き出しと低電圧電極
に接続された金属製シールド部品を組み合わせることに
より、セラミックス表面の突き出しのみで、シールド部
品を有していない従来例に比べて沿面放電の開始電圧を
数十%以上高くすることができるという効果がある。Effects of the Invention As explained above, the present invention has a protrusion of the vacuum side wall surface of a cylindrical ceramic which serves as insulation and a vacuum envelope of a stacked electron gun of a microwave tube, and a metal structure connected to a low voltage electrode. By combining shield components, there is an effect that the starting voltage of creeping discharge can be increased by several tens of percent or more compared to a conventional example without a shield component, just by protruding the ceramic surface.
【図1】本発明の第1の実施例の断面図である。FIG. 1 is a sectional view of a first embodiment of the invention.
【図2】本発明の第2の実施例の断面図である。FIG. 2 is a sectional view of a second embodiment of the invention.
【図3】本発明の第3の実施例の断面図である。FIG. 3 is a sectional view of a third embodiment of the invention.
【図4】従来例の断面図である。FIG. 4 is a sectional view of a conventional example.
【符号の説明】
1,2,3,11 円筒形セラミックス4
アノード電極
5 カソード・ウエネルト電極
6 ウエネルト
7 カソード
8,10 シールド部品
9 ウエネルト支持体[Explanation of symbols] 1, 2, 3, 11 Cylindrical ceramics 4
Anode electrode 5 Cathode/Wehnelt electrode 6 Wehnelt 7 Cathode 8, 10 Shield part 9 Wehnelt support
Claims (1)
外囲器を兼ねる円筒形セラッミックスを交互に積み重ね
、ろう付けしてなるスタック型電気銃を有するマイクロ
波管において、円筒形セラミックスの真空側壁面にその
円周上に沿って少くとも1個の突き出しを有し、かつ、
その突き出しの高電圧側の面に対して対向する面を有す
る金属製のシールド部品を少くとも1個低電圧側の電極
上に固着して設けたことを特徴とするマイクロ波管。Claim 1: In a microwave tube having a stacked electric gun in which metal electrodes and cylindrical ceramics, which serve as insulation between the electrodes and a vacuum envelope, are alternately stacked and brazed, The vacuum side wall surface has at least one protrusion along its circumference, and
A microwave tube characterized in that at least one metal shield component having a surface opposite to the protruding high voltage side surface is fixedly provided on the low voltage side electrode.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1622391A JPH04255642A (en) | 1991-02-07 | 1991-02-07 | Microwave tube |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1622391A JPH04255642A (en) | 1991-02-07 | 1991-02-07 | Microwave tube |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH04255642A true JPH04255642A (en) | 1992-09-10 |
Family
ID=11910538
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP1622391A Pending JPH04255642A (en) | 1991-02-07 | 1991-02-07 | Microwave tube |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH04255642A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5637957A (en) * | 1995-03-20 | 1997-06-10 | Nec Corporation | Cathode-anode spacer comprising a projection of a length limited relative to its distance to the cathode |
US20120307978A1 (en) * | 2011-06-01 | 2012-12-06 | Canon Kabushiki Kaisha | Radiation generating tube |
JP2016021408A (en) * | 2015-08-24 | 2016-02-04 | キヤノン株式会社 | X-ray tube |
-
1991
- 1991-02-07 JP JP1622391A patent/JPH04255642A/en active Pending
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5637957A (en) * | 1995-03-20 | 1997-06-10 | Nec Corporation | Cathode-anode spacer comprising a projection of a length limited relative to its distance to the cathode |
US20120307978A1 (en) * | 2011-06-01 | 2012-12-06 | Canon Kabushiki Kaisha | Radiation generating tube |
US9159525B2 (en) * | 2011-06-01 | 2015-10-13 | Canon Kabushiki Kaisha | Radiation generating tube |
JP2016021408A (en) * | 2015-08-24 | 2016-02-04 | キヤノン株式会社 | X-ray tube |
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