JP2808938B2 - High power microwave tube - Google Patents
High power microwave tubeInfo
- Publication number
- JP2808938B2 JP2808938B2 JP22379191A JP22379191A JP2808938B2 JP 2808938 B2 JP2808938 B2 JP 2808938B2 JP 22379191 A JP22379191 A JP 22379191A JP 22379191 A JP22379191 A JP 22379191A JP 2808938 B2 JP2808938 B2 JP 2808938B2
- Authority
- JP
- Japan
- Prior art keywords
- electron gun
- electron beam
- collector
- power microwave
- microwave tube
- 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.)
- Expired - Fee Related
Links
- 238000010894 electron beam technology Methods 0.000 claims description 19
- 230000004907 flux Effects 0.000 description 14
- 125000006850 spacer group Chemical group 0.000 description 5
- 238000001816 cooling Methods 0.000 description 2
- 230000005684 electric field Effects 0.000 description 2
- 239000004575 stone Substances 0.000 description 2
- 238000010586 diagram Methods 0.000 description 1
- 239000000696 magnetic material Substances 0.000 description 1
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 1
Landscapes
- Microwave Tubes (AREA)
Description
【0001】[0001]
【産業上の利用分野】本発明は、電磁石を集束装置とす
る大電力マイクロ波管に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a high power microwave tube using an electromagnet as a focusing device.
【0002】[0002]
【従来の技術】従来の、電磁石を集束装置に使用する大
電力マイクロ波管は、図3に示すように、電子ビームを
射出する電子銃部と、この電子銃部からの電子ビームを
捕捉するコレクタ部と、電子銃部とコレクタ部との間に
配置された高周波回路部と、電子ビームを集束させる集
束回路部とを基本的に具備している。2. Description of the Related Art As shown in FIG. 3, a conventional high-power microwave tube using an electromagnet as a focusing device captures an electron beam from an electron gun and captures the electron beam from the electron gun. It basically comprises a collector, a high-frequency circuit disposed between the electron gun and the collector, and a focusing circuit for focusing the electron beam.
【0003】次に各部の動作を説明する。電子銃部は、
電子ビームを射出するカソード5と、カソード5を支持
するカソード支持体2、電子ビームを集束及び加速する
ための電界を形成するウエネルト電極3とアノード電極
6、そして各電極間を電気的に絶縁する絶縁石4及び電
子銃部を支持する電子銃支持体1で構成される。コレク
タ部は、電子銃部から射出された電子ビームを捕捉する
コレクタ14で構成される。Next, the operation of each section will be described. The electron gun section
A cathode 5 for emitting an electron beam, a cathode support 2 for supporting the cathode 5, a Wehnelt electrode 3 and an anode electrode 6 for forming an electric field for converging and accelerating the electron beam, and electrically insulating between the electrodes. It is composed of an insulating stone 4 and an electron gun support 1 that supports an electron gun section. The collector section includes a collector 14 for capturing an electron beam emitted from the electron gun section.
【0004】高周波回路部は、電子銃部から射出された
電子ビームを高周波信号により速度変調し電子ビームを
集群し、電子ビームのエネルギーを高周波信号に変換す
る高周波回路部11で構成される。集束回路部は、電子
銃部から射出された電子ビームを集束させたまま高周波
回路部を通過させるために必要な磁界を形成するもの
で、電磁石コイル10と、磁性体である電子銃側ポール
ピース7、下ヨーク8、上ヨーク12、コレクタ側ポー
ルピース13と電磁石コイル10の位置出しに使用され
るスペーサ9で構成される。The high-frequency circuit section includes a high-frequency circuit section 11 that modulates the speed of an electron beam emitted from an electron gun by a high-frequency signal, collects the electron beams, and converts the energy of the electron beam into a high-frequency signal. The focusing circuit unit forms a magnetic field necessary for passing the electron beam emitted from the electron gun unit through the high-frequency circuit unit while keeping the electron beam focused. The focusing circuit unit includes an electromagnet coil 10 and an electron gun-side pole piece that is a magnetic material. 7, a lower yoke 8, an upper yoke 12, a collector-side pole piece 13, and a spacer 9 used for positioning the electromagnet coil 10.
【0005】この従来の大電力マイクロ波間の電子銃部
の中心軸上の磁束密度分布を図2において実線で示す。
この磁束密度分布は高周波回路を通過する電子ビームの
直径及びリップル率を左右するので、集束回路部の形状
を実験的に変えて最適な磁束密度分布を得るようにして
いる。この時同時に、必要なパービアンスと耐電圧的安
定が求められるので、設計上の制約となる。The conventional magnetic flux density distribution on the central axis of the electron gun between high power microwaves is shown by a solid line in FIG.
Since the magnetic flux density distribution affects the diameter and the ripple rate of the electron beam passing through the high-frequency circuit, the shape of the focusing circuit is experimentally changed to obtain the optimum magnetic flux density distribution. At this time, the required perforance and withstand voltage stability are required at the same time, which is a design constraint.
【0006】[0006]
【発明が解決しようとする課題】この従来の大電力マイ
クロ波管では、電磁石のスペーサ9が存在するため径方
向へのもれ磁束が多くなり図3のA部の磁束密度が比較
的小さくなる。ところが、必要な電子ビームの直径,リ
ップル率,パービアンス及び耐電圧的安定性を得るため
に図3のA部での磁束密度を更に大きくしたい場合、実
現不可能となることがある。スペーサ9を取り除けば径
方向へのもれ磁束が少なくなり図3のA部の磁束密度が
大きくなるが、電磁石コイル10の位置出しと電磁石コ
イル冷却用の水冷パイプの配管に必要であるため取り除
くことができない。In this conventional high-power microwave tube, the presence of the electromagnet spacers 9 increases the leakage flux in the radial direction, and the flux density in the portion A in FIG. 3 becomes relatively small. . However, if it is desired to further increase the magnetic flux density at the portion A in FIG. 3 in order to obtain the required electron beam diameter, ripple rate, perforance, and withstand voltage stability, it may not be possible to realize this. If the spacer 9 is removed, the magnetic flux leaking in the radial direction is reduced and the magnetic flux density of the portion A in FIG. 3 is increased. However, since it is necessary for the positioning of the electromagnet coil 10 and the piping of the water cooling pipe for cooling the electromagnet coil, it is removed. Can not do.
【0007】[0007]
【課題を解決するための手段】本発明は、電子ビームを
射出する電子銃部と、電子銃部からの電子ビームを捕捉
するコレクタ部と、電子銃部とコレクタ部との間に配置
された高周波回路部と、高周波回路部の外周に配設され
た電磁石よりなる集束回路部とを有する大電力マイクロ
波管において、前記集束回路部の電子銃部側の磁性体ポ
ールピースは、管軸に沿ってコレクタ部方向へ凹んだ凹
状構造を有することを特徴とする。SUMMARY OF THE INVENTION The present invention provides an electron beam.
Captures the electron gun and the electron beam from the electron gun
To be placed between the electron gun section and the collector section
The high-frequency circuit part and the outer periphery of the high-frequency circuit part
In high power microwave tube and a focusing circuit portion made of electromagnets, magnetic pole pieces of the electron gun side of the focusing circuit is recessed into the collector section along the tube axis concave
It is characterized by having a like-shaped structure .
【0008】[0008]
【作用】本発明では、もれ磁束が径方向に広がる前の位
置にA部を移すことによりA部での磁束密度を大きくす
ることができた。According to the present invention, the magnetic flux density in the portion A can be increased by moving the portion A to a position before the leakage magnetic flux spreads in the radial direction.
【0009】[0009]
【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大電力マイクロ波管の
断面図である。カソード5から射出された電子ビームは
ウエネルト電極3とアノード電極6の間の電界により集
束される。アノード電極6を通過した電子ビームは電磁
石コイル10,コレクタ側ポールピース13,上ヨーク
12,下ヨーク8,スペーサ9及び電子銃側ポールピー
ス7による磁気回路系による磁界により集束されたまま
高周波回路部11を通り、コレクタ部で捕捉される。DESCRIPTION OF THE PREFERRED EMBODIMENTS Next, the present invention will be described with reference to the drawings. FIG. 1 is a sectional view of a high power microwave tube according to one embodiment of the present invention. The electron beam emitted from the cathode 5 is focused by an electric field between the Wehnelt electrode 3 and the anode electrode 6. The electron beam that has passed through the anode electrode 6 remains focused by the magnetic field of the magnetic circuit system including the electromagnet coil 10, the collector-side pole piece 13, the upper yoke 12, the lower yoke 8, the spacer 9, and the electron gun-side pole piece 7. 11 and is captured by the collector.
【0010】本実施例では、電子銃側ポールピース7は
電磁石コイル内の方向へ突き出しており、電子銃部の磁
束密度分布は図2の破線のようになり、A部での磁束密
度を従来より大きくすることができた。また、これによ
り従来実現できなかった電子銃構造が可能となり、本実
施例ではアノード電極6と電子銃側ポールピース7の間
の距離を従来より広くとれ、耐電圧的に更に余裕のある
構造にできた。In this embodiment, the electron gun side pole piece 7 protrudes in the direction of the electromagnet coil, and the magnetic flux density distribution of the electron gun portion is as shown by the broken line in FIG. Could be larger. In addition, this enables an electron gun structure that could not be realized conventionally. In the present embodiment, the distance between the anode electrode 6 and the electron gun-side pole piece 7 can be made wider than in the past, and the structure has more margin in terms of withstand voltage. did it.
【0011】[0011]
【発明の効果】以上説明したように本発明は、電子銃側
ポールピースを電磁石コイル内の方向へ突き出すこと
で、電子銃部の磁束密度分布を図2の実線から図2の破
線のようにできA部での磁束密度を従来より大きくする
ことができた。また、電磁石コイル内の方向へ電子銃ポ
ールピースを突き出すほどA部での磁束密度は上げるこ
とができるので、本発明を用いれば、電子銃の設計自由
度を広げることができる。As described above, according to the present invention, the magnetic pole density distribution of the electron gun portion is changed from the solid line in FIG. 2 to the broken line in FIG. As a result, the magnetic flux density at the portion A could be made larger than before. Further, the more the electron gun pole piece protrudes in the direction inside the electromagnet coil, the higher the magnetic flux density in the portion A can be. Therefore, if the present invention is used, the degree of freedom in designing the electron gun can be increased.
【図1】本発明の一実施例の断面図である。FIG. 1 is a sectional view of one embodiment of the present invention.
【図2】本発明と従来例の電子銃部の磁束密度分布を示
す図である。FIG. 2 is a diagram showing a magnetic flux density distribution of an electron gun unit according to the present invention and a conventional example.
【図3】従来技術の一例の断面図である。FIG. 3 is a cross-sectional view of an example of the related art.
1 電子銃支持体 2 カソード支持体 3 ウエネルト電極 4 絶縁石 5 カソード 6 アノード電極 7 電子銃側ポールピース 8 下ヨーク 9 スペーサ 10 電磁石コイル 11 高周波回路部 12 上ヨーク 13 コレクタ側ポールピース 14 コレクタ Reference Signs List 1 electron gun support 2 cathode support 3 Wehnelt electrode 4 insulating stone 5 cathode 6 anode electrode 7 electron gun side pole piece 8 lower yoke 9 spacer 10 electromagnet coil 11 high frequency circuit section 12 upper yoke 13 collector side pole piece 14 collector
Claims (1)
銃部からの電子ビームを捕捉するコレクタ部と、電子銃
部とコレクタ部との間に配置された高周波回路部と、高
周波回路部の外周に配設された電磁石よりなる集束回路
部とを有する大電力マイクロ波管において、前記集束回
路部の電子銃部側の磁性体ポールピースは、管軸に沿っ
てコレクタ部方向へ凹んだ凹状構造を有することを特徴
とする大電力マイクロ波管。 An electron gun for emitting an electron beam;
A collector for capturing the electron beam from the gun, and an electron gun
High-frequency circuit section between the
Focusing circuit consisting of electromagnets arranged on the outer periphery of the frequency circuit
In high power microwave tube having a section, the converging times
Magnetic pole pieces of the electron gun side of the road section, along the tube axis
A high-power microwave tube having a concave structure recessed toward the collector .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP22379191A JP2808938B2 (en) | 1991-09-04 | 1991-09-04 | High power microwave tube |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP22379191A JP2808938B2 (en) | 1991-09-04 | 1991-09-04 | High power microwave tube |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0562603A JPH0562603A (en) | 1993-03-12 |
| JP2808938B2 true JP2808938B2 (en) | 1998-10-08 |
Family
ID=16803772
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP22379191A Expired - Fee Related JP2808938B2 (en) | 1991-09-04 | 1991-09-04 | High power microwave tube |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2808938B2 (en) |
-
1991
- 1991-09-04 JP JP22379191A patent/JP2808938B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0562603A (en) | 1993-03-12 |
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|---|---|---|---|
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| R250 | Receipt of annual fees |
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