JPH0541171A - Linear beam microwave tube - Google Patents
Linear beam microwave tubeInfo
- Publication number
- JPH0541171A JPH0541171A JP19563791A JP19563791A JPH0541171A JP H0541171 A JPH0541171 A JP H0541171A JP 19563791 A JP19563791 A JP 19563791A JP 19563791 A JP19563791 A JP 19563791A JP H0541171 A JPH0541171 A JP H0541171A
- Authority
- JP
- Japan
- Prior art keywords
- electron
- cathode
- emission surface
- electrons
- electron emission
- 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
Landscapes
- Microwave Tubes (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は、マイクロ波の増幅器等
として使用される進行波管などの直線ビームマイクロ波
管に関し、特に直線ビームマイクロ波管の電子銃部の陰
極形状に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a linear beam microwave tube such as a traveling wave tube used as a microwave amplifier, and more particularly to a cathode shape of an electron gun portion of the linear beam microwave tube.
【0002】[0002]
【従来の技術】進行波管などの直線ビームマイクロ波管
は、周知のように電子流を発生する電子銃部と、電子銃
で作られた電子流とマイクロ波の相互作用によりマイク
ロ波の増幅を行なう高周波回路部と、高周波回路部を通
過した電子流を捕捉し、熱エネルギに変換するコレクタ
部と、電子流を集束させる磁界を発生する磁極及び磁石
などで構成されている。これらのうち電子銃部には、図
3に示すように電子を放出する陰極1,陰極1を加熱す
るためのヒータ4,陰極1から放出された電子を集束す
るためのウェーネルト2,電子を加速するためのアノー
ド3などで構成されるピアース形電子銃が用いられる。
また、この直線ビームマイクロ波管用のピアース形電子
銃では通常、らせん等によって構成される高周波回路部
において、細くかつ大きな電流の電子流5を得るために
陰極1の電子放出面6は、その曲率中心が管軸上に位置
する球面形状を成し、放出された電子流が無理なく集束
され、アノード3の中心孔を通過し、さらに下流に位置
するらせん等によって構成される高周波回路部へ導かれ
る。このように、大きな陰極1から細い電子流5を発生
するピアース電子銃は集束形ピアース電子銃と呼ばれ
る。陰極1の曲率半径は、電子流5の集束比、アノード
3の加速電位,電子流5の電流値などから最適な値が決
められる。2. Description of the Related Art As is well known, a straight-beam microwave tube such as a traveling wave tube amplifies a microwave by an electron gun section that generates an electron stream and an interaction between the electron stream created by the electron gun and the microwave. It comprises a high frequency circuit part for performing the above, a collector part for capturing the electron flow passing through the high frequency circuit part and converting it into heat energy, a magnetic pole and a magnet for generating a magnetic field for converging the electron flow. As shown in FIG. 3, the electron gun portion includes a cathode 1 for emitting electrons, a heater 4 for heating the cathode 1, a Wehnelt 2 for focusing the electrons emitted from the cathode 1, and an electron acceleration. A Pierce-type electron gun including an anode 3 and the like is used.
Further, in this Pierce type electron gun for a linear beam microwave tube, in the high frequency circuit section which is usually constituted by a spiral or the like, the electron emission surface 6 of the cathode 1 has a curvature in order to obtain an electron flow 5 of a thin and large current. It has a spherical shape with its center located on the tube axis, the emitted electron flow is reasonably focused, passes through the central hole of the anode 3, and is guided to a high-frequency circuit section composed of a spiral located further downstream. Get burned. Thus, the pierce electron gun that produces the thin electron stream 5 from the large cathode 1 is called a focused pierce electron gun. An optimum value for the radius of curvature of the cathode 1 is determined from the focusing ratio of the electron flow 5, the acceleration potential of the anode 3, the current value of the electron flow 5, and the like.
【0003】[0003]
【発明が解決しようとする課題】上述のように直線ビー
ムマイクロ波管の電子を放出する陰極1の電子放出面6
の形状は、球面形状を成している。このような球面形状
の加工は、通常旋盤を用いて行われるが、球面の曲率に
は極めて高い精度が要求されるため加工費用は高価なも
のとなる。また、旋盤によって球面を加工するため、表
面粗さは通常5μm程度が限界であり、この表面の粗さ
に起因する電子軌道の微小な乱れは直線ビームマイクロ
波管の雑音となって特性に悪影響を及ぼしている。As described above, the electron emission surface 6 of the cathode 1 for emitting electrons of the linear beam microwave tube.
The shape of is a spherical shape. The processing of such a spherical shape is usually performed by using a lathe, but the processing cost becomes expensive because the curvature of the spherical surface requires extremely high accuracy. Further, since the spherical surface is processed by the lathe, the surface roughness is usually limited to about 5 μm, and the minute disturbance of the electron orbit due to this surface roughness becomes noise of the linear beam microwave tube and adversely affects the characteristics. Is affecting.
【0004】さらに、電子放出面6は球面形を成してい
るため、特に球面の曲率半径が小さい場合には、電子放
出面6の最外径部はナイフエッジ状となり直線ビームマ
イクロ波管の組立途中等でのエッジの欠けを生じる原因
となるなどの問題点があった。Further, since the electron emission surface 6 has a spherical shape, the outermost diameter portion of the electron emission surface 6 has a knife edge shape especially when the radius of curvature of the spherical surface is small. There was a problem such as a cause of chipping of an edge during assembling.
【0005】[0005]
【課題を解決するための手段】本発明は、電子流を発生
する電子銃部と、電子流とマイクロ波の相互作用を行な
う高周波回路部と、相互作用を終えた電子流を捕捉し熱
エネルギーに変換するコレクタ部と、電子流を集束させ
る磁気回路などからなる直線ビームマイクロ波管におい
て、電子流源である電子銃部を構成する陰極1の電子放
出面6が従来の様に球面ではなく平面であることを特徴
としている。SUMMARY OF THE INVENTION According to the present invention, an electron gun section for generating an electron flow, a high frequency circuit section for interacting an electron flow with a microwave, and an electron stream after the interaction are captured to obtain thermal energy. In a linear beam microwave tube composed of a collector part for converting into an electron stream and a magnetic circuit for converging an electron flow, the electron emission surface 6 of the cathode 1 constituting the electron gun part which is the electron flow source is not a spherical surface as in the conventional case. It is characterized by being a plane.
【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は本発明の一実施例の直線ビームマイクロ波管
の電子銃部の断面図である。図1において、陰極1はヒ
ータ4によって900℃〜1100℃に加熱され、その
電子放出面6から電子が放出される。放出された電子
は、ウェーネルト2によって集束されると共にアノード
3に印加された高電圧によって加速され電子流5を形成
し、さらに下流に位置する高周波回路部に導かれる、い
わゆる集束形ピアース電子銃である。ここで陰極1の電
子放出面6は平面形状をしており電子が陰極から飛び出
した瞬間の電子の運動方向は、管軸と平行な方向とな
る。しかし、集束電極であるウェーネルト2が存在する
ため、陰極1とアノード3の間の空間において等電位面
14は図1の中に示したような形となり電界は等電位面
14と直角な方向となり陰極から出た電子は電界方向の
集束する力を受け、アノード3の中心孔を通過し、高周
波回路部に導かれる。この様に、電子放出面6の形状は
必らずしも球面である必要はなく、平面であっても電子
は充分集束され所要の電子流5を形成することが可能と
なる。The present invention will be described below with reference to the drawings. FIG. 1 is a sectional view of an electron gun portion of a linear beam microwave tube according to an embodiment of the present invention. In FIG. 1, the cathode 1 is heated to 900 ° C. to 1100 ° C. by the heater 4, and electrons are emitted from its electron emission surface 6. The emitted electrons are focused by the Wehnelt 2 and are accelerated by the high voltage applied to the anode 3 to form an electron stream 5, which is guided to a high frequency circuit located further downstream by a so-called focused pierce electron gun. is there. Here, the electron emission surface 6 of the cathode 1 has a planar shape, and the movement direction of the electron at the moment when the electron jumps out from the cathode is parallel to the tube axis. However, due to the presence of the Wehnelt 2 which is a focusing electrode, the equipotential surface 14 has the shape shown in FIG. 1 in the space between the cathode 1 and the anode 3, and the electric field is in the direction perpendicular to the equipotential surface 14. The electrons emitted from the cathode receive a force of focusing in the direction of the electric field, pass through the central hole of the anode 3, and are guided to the high frequency circuit section. As described above, the shape of the electron emission surface 6 does not necessarily have to be a spherical surface, and even if it is a flat surface, the electrons are sufficiently focused and the required electron flow 5 can be formed.
【0007】種々の実験の結果では、電子流5の直径と
陰極1の電子放出面6の外径の比が1対3程度以下であ
れば、電子放出面6の形状が平面であっても球面の場合
とほとんど差がなく、電子は集束され所要の電子流5が
得られることが確認されている。As a result of various experiments, if the ratio of the diameter of the electron flow 5 to the outer diameter of the electron emission surface 6 of the cathode 1 is about 1: 3 or less, even if the shape of the electron emission surface 6 is flat. It is confirmed that there is almost no difference from the case of the spherical surface and the electrons are focused and the required electron flow 5 is obtained.
【0008】図2は本発明による直線ビームマイクロ波
管の一種であるらせん型進行波管の一例の縦断面図であ
る。図2において、陰極1の電子放出面6は平面形状を
しており、上述したように陰極1から出た電子は集束さ
れアノード3を通過した後、高周波回路を形成するらせ
ん7の中に導かれ、らせん7上に存在するマイクロ波と
の相互作用によりマイクロ波を増幅させる。さらに、ら
せん7を通過した電子はコレクタ10に捕捉される。FIG. 2 is a longitudinal sectional view of an example of a spiral traveling wave tube which is a kind of the linear beam microwave tube according to the present invention. In FIG. 2, the electron emission surface 6 of the cathode 1 has a flat shape, and as described above, the electrons emitted from the cathode 1 are focused and passed through the anode 3, and then guided into the spiral 7 forming a high frequency circuit. Then, the microwave is amplified by the interaction with the microwave existing on the helix 7. Further, the electrons that have passed through the helix 7 are captured by the collector 10.
【0009】[0009]
【発明の効果】以上説明したように本発明は、直線ビー
ムマイクロ波管の電子源である陰極1の電子放出面6を
平面したことを特徴としており、その結果、陰極1の外
形形状の加工を容易にすることが可能となる。このこと
は、直線ビームマイクロ波管の高価な部品の一つである
陰極の価格を低減することを可能にし、従って直線ビー
ムマイクロ波管のコストを下げる効果を有している。As described above, the present invention is characterized in that the electron emission surface 6 of the cathode 1 which is the electron source of the linear beam microwave tube is flat, and as a result, the outer shape of the cathode 1 is processed. Can be facilitated. This makes it possible to reduce the cost of the cathode, which is one of the expensive parts of the linear beam microwave tube, and has the effect of reducing the cost of the linear beam microwave tube.
【0010】さらに、陰極1の電子放出面6の形状を平
面にすることにより、従来、球面の電子放出面6を加工
する場合には旋盤により切削を行っていたため、電子放
出面6の表面粗さには限界があったが平面とすることに
より旋盤加工後、さらに研磨により表面精度を高くする
ことができる。このことは、電子放出面6の表面粗さに
起因する電子軌道の乱れをなくすことができ、層流性の
良い電子流5を得ることを可能にし、直線ビームマイク
ロ波管の雑音等の特性向上に結びつく効果を有する。Further, by making the shape of the electron emission surface 6 of the cathode 1 to be a flat surface, the surface roughness of the electron emission surface 6 is conventionally cut by lathe when processing the spherical electron emission surface 6. Although there is a limit to this, by using a flat surface, it is possible to further improve the surface accuracy by lathing after polishing. This can eliminate the disturbance of the electron orbit due to the surface roughness of the electron emission surface 6, makes it possible to obtain the electron flow 5 having a good laminar flow property, and the characteristics such as noise of the linear beam microwave tube. It has the effect of improving.
【図1】本発明の直線ビームマイクロ波管の電子銃部の
主要電極部分を示す縦断面図である。FIG. 1 is a vertical sectional view showing a main electrode portion of an electron gun section of a linear beam microwave tube according to the present invention.
【図2】本発明の直線ビームマイクロ波管の一例である
らせん型進行波管の縦断面図である。FIG. 2 is a vertical cross-sectional view of a spiral traveling wave tube which is an example of the linear beam microwave tube of the present invention.
【図3】従来の直線ビームマイクロ波管の電子銃部の主
要電極部分を示す縦断面図である。FIG. 3 is a vertical cross-sectional view showing a main electrode portion of an electron gun section of a conventional linear beam microwave tube.
1 陰極 2 ウェーネルト 3 アノード 4 ヒータ 5 電子流 6 電子放出面 7 らせん 8 磁極 9 磁石 10 コレクタ 11 誘電体支持棒 12 入力部 13 出力部 14 等電位面 1 Cathode 2 Wehnelt 3 Anode 4 Heater 5 Electron flow 6 Electron emission surface 7 Helix 8 Magnetic pole 9 Magnet 10 Collector 11 Dielectric support rod 12 Input section 13 Output section 14 Equipotential surface
Claims (1)
マイクロ波の相互作用を行なう高周波回路部と、相互作
用を終えた電子流を捕捉し熱エネルギーに変換するコレ
クタ部と、電子流を集束させる磁気回路などからなる直
線ビームマイクロ波管において、前記電子銃部は集束形
ピアース電子銃であり、かつ電子銃を構成する陰極の電
子放出面が平面であることを特徴とする直線ビームマイ
クロ波管。1. An electron gun section for generating an electron stream, a high-frequency circuit section for interacting the electron stream with a microwave, a collector section for capturing the electron stream after the interaction and converting it into heat energy, and an electron. In a linear beam microwave tube including a magnetic circuit for focusing a flow, the electron gun unit is a focused pierce electron gun, and the electron emission surface of a cathode constituting the electron gun is a flat line. Beam microwave tube.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19563791A JPH0541171A (en) | 1991-08-06 | 1991-08-06 | Linear beam microwave tube |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19563791A JPH0541171A (en) | 1991-08-06 | 1991-08-06 | Linear beam microwave tube |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0541171A true JPH0541171A (en) | 1993-02-19 |
Family
ID=16344482
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP19563791A Pending JPH0541171A (en) | 1991-08-06 | 1991-08-06 | Linear beam microwave tube |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0541171A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR100281393B1 (en) * | 1997-01-09 | 2001-02-01 | 니시무로 타이죠 | Multipolar electron tube |
US7655869B2 (en) | 2003-04-18 | 2010-02-02 | Ibiden Co., Ltd. | Flex-rigid wiring board |
US7968798B2 (en) | 2006-11-14 | 2011-06-28 | Toshiba Matsushita Display Technology Co., Ltd. | Flexible printed board |
US8093502B2 (en) | 2004-06-10 | 2012-01-10 | Ibiden Co., Ltd. | Flex-rigid wiring board and manufacturing method thereof |
-
1991
- 1991-08-06 JP JP19563791A patent/JPH0541171A/en active Pending
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR100281393B1 (en) * | 1997-01-09 | 2001-02-01 | 니시무로 타이죠 | Multipolar electron tube |
US7655869B2 (en) | 2003-04-18 | 2010-02-02 | Ibiden Co., Ltd. | Flex-rigid wiring board |
US8093502B2 (en) | 2004-06-10 | 2012-01-10 | Ibiden Co., Ltd. | Flex-rigid wiring board and manufacturing method thereof |
US7968798B2 (en) | 2006-11-14 | 2011-06-28 | Toshiba Matsushita Display Technology Co., Ltd. | Flexible printed board |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US2306875A (en) | Electron discharge apparatus | |
US2312723A (en) | Electron discharge device | |
Ruess et al. | An inverse magnetron injection gun for the KIT 2-MW coaxial-cavity gyrotron | |
US2949558A (en) | High efficiency velocity modulation devices | |
US2852715A (en) | High frequency structure | |
US5461282A (en) | Advanced center post electron gun | |
US2991391A (en) | Electron beam discharge apparatus | |
US2802135A (en) | Traveling wave electron tube | |
US3832596A (en) | Magnetic structure for focusing of linear beams | |
JPH0541171A (en) | Linear beam microwave tube | |
US2888591A (en) | Charged particle emitter apparatus | |
JPH0613822A (en) | High frequency amplifier | |
JPS6318297B2 (en) | ||
US2955229A (en) | Secondary emission suppression in electron beam tubes | |
US2886738A (en) | Electron beam system | |
US4445070A (en) | Electron gun for producing spiral electron beams and gyrotron devices including same | |
JPS594819B2 (en) | ion source | |
US3214632A (en) | Low noise electron gun | |
CA1224873A (en) | Linear beam tube with reflected electron trap | |
JPS6219017B2 (en) | ||
JP2000215820A (en) | Helix type slow-wave circuit | |
JP3411196B2 (en) | Linear electron accelerator | |
JP2830608B2 (en) | High power microwave tube | |
US3271731A (en) | Electron beam parametric amplifier with positive ion elimination | |
US3140420A (en) | Electron tube generating oppositely directed radially-displaced beams |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
A02 | Decision of refusal |
Free format text: JAPANESE INTERMEDIATE CODE: A02 Effective date: 20000905 |