JPS6028137A - Microwave tube - Google Patents
Microwave tubeInfo
- Publication number
- JPS6028137A JPS6028137A JP13611283A JP13611283A JPS6028137A JP S6028137 A JPS6028137 A JP S6028137A JP 13611283 A JP13611283 A JP 13611283A JP 13611283 A JP13611283 A JP 13611283A JP S6028137 A JPS6028137 A JP S6028137A
- Authority
- JP
- Japan
- Prior art keywords
- grid
- control grid
- potential
- cathode
- electron
- 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
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J23/00—Details of transit-time tubes of the types covered by group H01J25/00
- H01J23/02—Electrodes; Magnetic control means; Screens
Landscapes
- Microwave Tubes (AREA)
Abstract
Description
【発明の詳細な説明】
この発明は、マイクロ波電子管の格子付電子銃における
格子電極の構造に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a structure of a grid electrode in a grid-equipped electron gun of a microwave electron tube.
マイクロ波電子管は、電・子ビームを射出し形成する電
子銃部、電子ビームと相互作用し高周波電力を増幅する
高周波回路部、相互作用後の電子ビーム全捕捉するコレ
クタ部、そして電子ビームの集束を保つ集束装置を大き
な構成要素としている。A microwave electron tube consists of an electron gun section that injects and forms an electron/electron beam, a high-frequency circuit section that interacts with the electron beam and amplifies high-frequency power, a collector section that captures all of the electron beams after interaction, and a focusing section for the electron beam. A major component is the focusing device that maintains the
マイクロ波電子管をパルス動作させたう2種類の出力動
作(デュアルモード)を行なうには2通常。2 Normal to perform two types of output operation (dual mode) in which the microwave electron tube is operated in pulses.
カソードの前面に格子電極を設はカソードからの放射電
流全制御する方式が採られる。近年、マイクロ波管電子
管は、高出力、高効率の高周波電カケ得る事が要求され
、そのため、高電流密度の電子ビームが必要であフこれ
はプーアルモード動作のものも例外ではない。格子付電
子銃では、カソードの電子放射面に近接した位置に配置
されたカソード面上を制御する格子篭@全カソードに対
して正電位を印加すると、カソードからの放射電子の一
部が格子に衝突し熱損失となる。この格子電極の熱損失
低減のため電流制御格子とカソード間にもう一つ格子金
膜け、動作状態ではカソードと同電位にして電子が直接
電流制御格子に流入するのケしゃへいしている。また、
これらの格子を絶縁体で被唆しカソード面上に直接配置
する方法もある。A method is adopted in which a grid electrode is installed in front of the cathode to completely control the radiation current from the cathode. In recent years, microwave tubes and electron tubes have been required to obtain high-power, high-efficiency high-frequency electric radiation, and therefore require electron beams with high current density.Puerh mode operation type tubes are no exception to this. In an electron gun with a grid, when a positive potential is applied to the grid cage that controls the cathode surface placed close to the electron emitting surface of the cathode (all cathodes), some of the emitted electrons from the cathode are transferred to the grid. Collision results in heat loss. In order to reduce heat loss in this grid electrode, another grid gold film is placed between the current control grid and the cathode, which is kept at the same potential as the cathode in the operating state to prevent electrons from directly flowing into the current control grid. Also,
There is also a method in which these grids are covered with an insulator and placed directly on the cathode surface.
プーアルモード電子管の設計は、高出力動作時の場合全
基準にビーム電圧、ビーム電流、格子電位などの動作条
件を決め、次に各電極形状を決めるのが普通である。そ
して通常のプーアルモード動作は、カソード格子間の電
位を変化させカソードからの電流1変えることによシ実
現している。When designing a Puar mode electron tube, it is common practice to determine operating conditions such as beam voltage, beam current, and grid potential based on all standards for high-power operation, and then to determine the shape of each electrode. Normal Puar mode operation is realized by changing the potential between the cathode lattices and changing the current from the cathode by 1.
従って、設計時に基準とした動作モード以外の動作状態
では、格子電極の電位による静電レンズが形成され、電
子軌道の乱れる原因となる。この電子軌道の乱れは、高
周波回路人口付近のボディ電極や高周波回路へ衝突する
ことで熱的問題となりさらには管球の安定性にも影響を
与える。Therefore, in an operating state other than the operating mode set as a reference at the time of design, an electrostatic lens is formed due to the potential of the grid electrode, causing disturbance of electron trajectories. This disturbance in the electron trajectory causes a thermal problem when it collides with the body electrode and the high-frequency circuit near the high-frequency circuit, which also affects the stability of the tube.
本発明の目的は、デュアルモード動作マイクロ波管の格
子付電子銃の格子を任意に分割しそれぞれに異なる電位
の印加を可能とじカソードの電子放射面積を分割した格
子ごとに制御する電極構造を提供することである。An object of the present invention is to provide an electrode structure in which the grid of a grid-equipped electron gun of a dual-mode microwave tube can be arbitrarily divided and different potentials can be applied to each grid, and the electron emission area of the cathode can be controlled for each divided grid. It is to be.
不発明によれば、電流制御格子を異なる電位の印加を可
能とする複数個に分割し、同一球面上に配置した事を特
徴とする電子銃を具備したマイクロ波電子管が得られる
。According to the present invention, there is obtained a microwave electron tube equipped with an electron gun characterized in that the current control grid is divided into a plurality of parts that can apply different potentials and are arranged on the same spherical surface.
以下実施例を図で説明する。Examples will be explained below using figures.
第1図がじゃへい・格子と電流制御格子を一体化した格
子付電子銃の構造である。また第1図のカソードと格子
の部分全拡大したものが第2図である。電流制御格子3
とじゃへい格子2は、パイロリティックグラファイトで
形成し、それを絶縁体ポロンナイトライド・8で制御格
子3とじゃへい格子2の間隔寸法を採シさらにカソード
1としゃへい格子間も同様にポロンナイトライド9で絶
縁し間隔も保っている。またじゃへい格子2と制御格子
3の表面上の絶縁層lOは、格子からの2次電子を減ら
す働きをする。この時の制御格子3の横断面図を第3図
に示す。Figure 1 shows the structure of a grid-equipped electron gun that integrates a jamb/grid and a current control grid. Further, FIG. 2 is a partially enlarged view of the cathode and grid in FIG. 1. Current control grid 3
The shield lattice 2 is made of pyrolytic graphite, and the spacing between the control grid 3 and the shield lattice 2 is made of polon nitride, which is an insulator. Ride 9 insulates and maintains spacing. Also, the insulating layer lO on the surfaces of the jamming grating 2 and the control grating 3 serves to reduce secondary electrons from the grating. A cross-sectional view of the control grid 3 at this time is shown in FIG.
第1図の電極構造で高周波出力を変えるにはh1制御格
子3の電位を変化させ1例えばカソード1と制御格子3
間室位を下げビーム電流全少なくする。In order to change the high frequency output with the electrode structure shown in Fig. 1, the potential of h1 control grid 3 is changed.
Lower the chamber height and reduce the beam current.
しかし、この場合しゃへい格子2と制御格子3の形状は
高出力時を基にして設計されるのが普通で。However, in this case, the shapes of the shielding grid 2 and the control grid 3 are usually designed based on high output.
IJII力時の電子ビームはカソード1と制御格子3間
に形成される静電レンズで軌道が乱されてしまう。この
乱れた電子ビームは、ボディー電極5や高周波回路7に
衝突し熱損失となシ熱的問題を引き越こし、管球の安定
性や効率が低下する事にもなる。特に高周波Ial路が
ヘリックス7の場合には。The trajectory of the electron beam during the IJII force is disturbed by the electrostatic lens formed between the cathode 1 and the control grid 3. This turbulent electron beam collides with the body electrode 5 and the high frequency circuit 7, causing thermal problems such as heat loss and reducing the stability and efficiency of the tube. Especially when the high frequency Ial path is helix 7.
熱損失によりヘリックスの溶断があり、絶対に電子ビー
ムの高周波回路への衝突を避けなければならない。The helix may melt due to heat loss, so collision of the electron beam with the high-frequency circuit must be avoided at all costs.
従来、この乱れた電子ビームがへソックス回路へ衝突す
るのを防ぐためヘリックス回路の入口に乱れた電子ビー
ムを整形する電極6を設けていた。Conventionally, in order to prevent this disordered electron beam from colliding with the Hesox circuit, an electrode 6 for shaping the disordered electron beam has been provided at the entrance of the helix circuit.
ビーム整形電極6は、ヘリ、yクス7の内径よりも小さ
い内径金持ち長さはビームの乱れの程度で決める事にな
る。ビームの乱れが大きい場合、ビーム整形電極6は当
然長くな9管球の長さも長くなり、また熱対策も十分に
行なう必要がある。The beam shaping electrode 6 has an inner diameter smaller than the inner diameter of the helical and y-axis 7, and its length is determined by the degree of beam disturbance. If the beam disturbance is large, the length of the beam shaping electrode 6 and the tube 9 will naturally be long, and sufficient heat countermeasures must be taken.
本発明による電流制御格子3の実施例全第4図に示す。An entire embodiment of a current control grid 3 according to the invention is shown in FIG.
電流制御格子3は周方向に3aと3bの2分割されてお
シそれぞれ独立して電位を印加できるようになっている
。プーアルモード動作は。The current control grid 3 is divided into two parts 3a and 3b in the circumferential direction so that a potential can be applied independently to each part. Puar mode operation.
この分割した制御格子電位を変えて実現する。すなわち
高出力動作時は、2つの制御格子3a、3’b共同−電
位を印加す−る。一方低出力動作時は、内側の制御格子
3bの電位を吐くシ、外側の制御格子3aの電位は高出
力時と変えないようにする。This is achieved by changing the divided control grid potential. That is, during high output operation, a common potential is applied to the two control grids 3a and 3'b. On the other hand, during low output operation, the potential of the inner control grid 3b is discharged, and the potential of the outer control grid 3a is kept unchanged from that during high output.
従って低出力動作時の電子ビームは、カソード表面上で
中空の抜けたホロービームとなる。この方法によれば、
カソードからの電流の取り出しを内側の制御格子電位だ
けで制御可能となり、電子軌道の大きな乱れを防ぎプー
アルモード動作に安定したビームを得ることができる格
子付電子銃全提供できる。制御格子3の分割は、低出力
の大きさに応じて設計する。Therefore, the electron beam during low power operation becomes a hollow beam on the cathode surface. According to this method,
The extraction of current from the cathode can be controlled only by the inner control grid potential, and a complete electron gun with a grid can be provided that can prevent large disturbances in electron trajectories and obtain a stable beam in Puar mode operation. The division of the control grid 3 is designed according to the magnitude of the low output.
そして、不発明により各制御格子3には、異なる電位を
印加することが可能でビーム形状やビーム径、ビーム電
流の微調が容易となる。By virtue of the invention, different potentials can be applied to each control grid 3, making it easy to finely adjust the beam shape, beam diameter, and beam current.
なお、実施例として高周波回路がヘリックスのものを示
したが、不発明はこれに限る事なく他の高周波回路の場
合にも適用できる。また格子の分割数や分割法も制御格
子の基の形状に応じて任意の分割数9分割法を採る事も
可能である。In addition, although the high frequency circuit is shown as a helix as an example, the invention is not limited to this and can be applied to other high frequency circuits. Furthermore, the number of grid divisions and the division method may be any number of divisions, such as nine divisions, depending on the shape of the base of the control grid.
第1]シ1は、格子付電子銃の軸方向断面図、第2図は
、格子付電子銃の格子をパイロリティックグラファイト
で構成した時のカソードと格子の軸方向断面斜視図、第
3図は、従来形格子の横断面図。
第4図は1本発明による一実施例の横断血肉である。
1・・・・・・カソード、2・・・・・・しゃへい格子
、3・・・・・・制御格子、4・・・・・・ビーム形成
電極、5・・・・・ボディーを極、6・−・・・・ビー
ム整形電極、7−・・・・・ヘリックス、8・・・・・
・しゃへい格子と制御格子の絶縁ボロンナイトライド、
9・・・・・・カソードとしゃへい格子の絶縁ボロンナ
イトライド、10・・・・・・制御格子絶縁ボロンナイ
トライド。
h?−圀
一17ζ−1] Fig. 1 is an axial sectional view of the electron gun with a grating, Fig. 2 is a perspective axial sectional view of the cathode and the lattice when the lattice of the electron gun with a lattice is made of pyrolytic graphite, and Fig. 3 is a cross-sectional view of a conventional lattice. FIG. 4 is a cross-section of blood and meat according to an embodiment of the present invention. 1... Cathode, 2... Shielding grating, 3... Control grid, 4... Beam forming electrode, 5... Body as pole, 6... Beam shaping electrode, 7-... Helix, 8...
・Insulating boron nitride for shielding grid and control grid,
9...Insulating boron nitride for cathode and shielding grid, 10...Insulating boron nitride for control grid. h? -Kuniichi 17ζ-
Claims (1)
ら構成されるマイクロ波管において、前記電子銃のカソ
ード面上カソードからの放射電流を制御する格子を異な
る電位の印加が可能な複数個に分割したもの全同一球面
上に配置した事をt¥f@とするマイクロ波管。Electron gun, high frequency circuit, collector. In a microwave tube composed of an electron beam focusing device, a grid on the cathode surface of the electron gun that controls the radiation current from the cathode is divided into a plurality of parts to which different potentials can be applied, all of which are arranged on the same spherical surface. A microwave tube that makes things t¥f@.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP13611283A JPS6028137A (en) | 1983-07-26 | 1983-07-26 | Microwave tube |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP13611283A JPS6028137A (en) | 1983-07-26 | 1983-07-26 | Microwave tube |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6028137A true JPS6028137A (en) | 1985-02-13 |
Family
ID=15167571
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP13611283A Pending JPS6028137A (en) | 1983-07-26 | 1983-07-26 | Microwave tube |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6028137A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH027849U (en) * | 1988-06-28 | 1990-01-18 | ||
WO2002086936A1 (en) * | 2001-04-23 | 2002-10-31 | Litton Systems, Inc. | Linear beam sevices with a gridded electron gun |
JP5835822B1 (en) * | 2014-06-30 | 2015-12-24 | Necネットワーク・センサ株式会社 | High frequency circuit system |
-
1983
- 1983-07-26 JP JP13611283A patent/JPS6028137A/en active Pending
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH027849U (en) * | 1988-06-28 | 1990-01-18 | ||
WO2002086936A1 (en) * | 2001-04-23 | 2002-10-31 | Litton Systems, Inc. | Linear beam sevices with a gridded electron gun |
US6664720B2 (en) | 2001-04-23 | 2003-12-16 | L-3 Communications Corporation | Temperature compensated gun |
JP5835822B1 (en) * | 2014-06-30 | 2015-12-24 | Necネットワーク・センサ株式会社 | High frequency circuit system |
WO2016002183A1 (en) * | 2014-06-30 | 2016-01-07 | Necネットワーク・センサ株式会社 | Traveling wave tube and high-frequency circuit system |
US10068738B2 (en) | 2014-06-30 | 2018-09-04 | Nec Network And Sensor Systems, Ltd. | Traveling wave tube and high-frequency circuit system |
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