JPH0711938B2 - Microwave tube - Google Patents
Microwave tubeInfo
- Publication number
- JPH0711938B2 JPH0711938B2 JP29112887A JP29112887A JPH0711938B2 JP H0711938 B2 JPH0711938 B2 JP H0711938B2 JP 29112887 A JP29112887 A JP 29112887A JP 29112887 A JP29112887 A JP 29112887A JP H0711938 B2 JPH0711938 B2 JP H0711938B2
- Authority
- JP
- Japan
- Prior art keywords
- collector
- section
- high frequency
- electron beam
- frequency circuit
- 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 - Lifetime
Links
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- Microwave Tubes (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、クライストロンや進行波管などのマイクロ波
管のコレクタに関し、特にコレクタ電圧を高周波回路の
電位より低くして高効率化したマイクロ波管のコレクタ
構造に関する。Description: TECHNICAL FIELD The present invention relates to a collector of a microwave tube such as a klystron or a traveling wave tube, and more particularly to a microwave whose efficiency is improved by lowering the collector voltage below the potential of a high frequency circuit. Regarding the collector structure of the tube.
一般にマイクロ波無線通信回線の中継局、衛星通信地上
局などの送信機に用いられるマイクロ波管においては、
装置設計や経済性の面から低消費電力であること、つま
り高効率であることが要求される。効率改善の手段とし
ては、コレクタ電位を高周波回路電位より低くして、コ
レクタ消費電力を低減した電位低下コレクタが広く用い
られる。In the microwave tube generally used for the transmitter of the microwave radio communication line relay station, satellite communication ground station, etc.,
Low power consumption, that is, high efficiency is required in terms of device design and economy. As a means for improving efficiency, a potential-decreased collector in which collector power is reduced by lowering the collector potential below the high-frequency circuit potential is widely used.
電子ビームは高周波回路と相互作用を行なう際、その結
合状態が各々異なり速度変調を受けるので相互作用後の
電子ビームのもつ運動エネルギーに速度分散を生じる。
従って最も遅い電子ビーム群を捕捉し得る電位まで低下
することが可能である。しかしこれ以上に電位を低下し
てより一層の効率改善を図ろうとすると、コレクタに捕
捉されるに十分な速度を持たない一次電子ビーム群の一
部や、コレクタ内面から発生した2次電子がより高電位
の高周波回路部へ逆行し、高周波回路に作用して、振幅
歪,位相歪など伝送特性に悪影響を及ぼし、また異常発
振,動作不安定などの要因となるなど、十分な電位低下
が行なえず、効率改善に支障をきたす。そこで、逆行電
子防止のためコレクタ外部に偏向用マグネットを取付け
ることによってコレクタ内部に管軸に垂直な面に磁界を
印加し電子に作用するローレンツカによって電子軌道を
曲げて高周波回路への逆行を防止する方策がとられてい
る。When the electron beam interacts with the high-frequency circuit, the coupling states thereof are different from each other and the velocity is modulated, so that the kinetic energy of the electron beam after the interaction causes velocity dispersion.
Therefore, the potential can be lowered to a potential at which the slowest electron beam group can be captured. However, if the potential is further reduced to further improve the efficiency, a part of the primary electron beam group that does not have a sufficient velocity to be trapped by the collector and the secondary electrons generated from the inner surface of the collector are more likely to be emitted. It goes back to the high-potential high-frequency circuit section and acts on the high-frequency circuit, adversely affecting the transmission characteristics such as amplitude distortion and phase distortion, and causing abnormal oscillation, unstable operation, etc. This hinders efficiency improvement. Therefore, in order to prevent retrograde electrons, a deflection magnet is attached to the outside of the collector to apply a magnetic field to the surface inside the collector perpendicular to the tube axis, and the Lorentzker that acts on the electrons bends the electron trajectory to prevent retrograde to the high frequency circuit. Measures are being taken to do so.
しかしながら、強制空冷形マイクロ波管の場合は、コレ
クタコアの外周に熱伝導率の良い銅などを材料とする放
熱翼を放射状にろう付した構造になっているので偏向用
マグネットをコレクタコアの近くに取付けられない。従
って放熱翼の外側に偏向用マグネットを取り付けること
になるが、偏向用マグネットがコレクタコアから離れて
いるので、コレクタコア内部に印加される磁界は距離の
2乗に反比例して弱くなり電子に作用するローレンツカ
が非常に弱くなってしまい逆行電子防止効果が小さくな
ってしまう。その結果、従来の強制空冷形マイクロ波管
ではコレクタ電位を高周波回路電位に対して十分低下す
ることができないので効率改善が制限されるという欠点
があった。However, in the case of a forced air-cooled microwave tube, since the radiator blades made of copper with good thermal conductivity are brazed to the outer circumference of the collector core in a radial fashion, the deflection magnet is placed near the collector core. Cannot be installed on. Therefore, the deflection magnet is attached to the outside of the radiator blade, but since the deflection magnet is separated from the collector core, the magnetic field applied inside the collector core weakens in inverse proportion to the square of the distance and acts on electrons. The Lorentzka becomes extremely weak and the effect of preventing retrograde electrons becomes small. As a result, the conventional forced air cooling type microwave tube has a drawback that the collector potential cannot be sufficiently lowered with respect to the high frequency circuit potential, so that the efficiency improvement is limited.
上述した従来の強制空冷形マイクロ波管のコレクタ構造
に対して本発明はコレクタ入口部に鉄などの強磁性材を
管軸に対し点対称に配設しさらに放熱翼のまわりに鉄な
どの強磁性材を配して、放熱翼の外側に取付けた偏向用
マグネットによってコレクタコア部に磁気帰還回路を構
成して、偏向磁界を弱めることなく、コレクタコア内部
に十分に強い偏向磁界を印加することができるという独
創的内容を有する。In contrast to the conventional forced-air cooling type microwave tube collector structure described above, the present invention is arranged such that a ferromagnetic material such as iron is arranged point-symmetrically with respect to the tube axis at the collector inlet portion, and a strong material such as iron is arranged around the heat dissipation blade. Applying a sufficiently strong deflection magnetic field to the inside of the collector core without weakening the deflection magnetic field by arranging a magnetic material and constructing a magnetic feedback circuit in the collector core section with a deflection magnet attached to the outside of the radiator blade. It has the original content that you can do it.
本発明による強制空冷形マイクロ波管は、電子ビームを
放射形成する電子銃部と、電子ビームとの相互作用によ
り高周波増幅を行なう高周波回路部と、電子ビームを高
周波回路内に集束せしめる集束磁界装置部と、高周波回
路との相互作用で増幅に寄与した電子ビームを捕捉する
ためのコレクタ部とで構成され、コレクタ部は、非磁性
である無酸素銅製のコレクタコア入口部に鉄などの強磁
性材を管軸に対して点対称に配設し、この近傍でコレク
タの外側に偏向用マグネットを取付け、さらに放熱翼の
周囲に鉄などの強磁性材を配した構造を有している。The forced air-cooled microwave tube according to the present invention includes an electron gun portion that radiates and forms an electron beam, a high frequency circuit portion that performs high frequency amplification by interaction with the electron beam, and a focusing magnetic field device that focuses the electron beam in the high frequency circuit. Part and a collector part for trapping the electron beam that contributed to amplification by the interaction with the high-frequency circuit. The collector part is made of non-oxygen-free oxygen-free copper and has a ferromagnetic core such as iron at the inlet part of the collector core. The material is arranged point-symmetrically with respect to the tube axis, a deflection magnet is attached to the outside of the collector in the vicinity of the material, and a ferromagnetic material such as iron is arranged around the heat dissipation blade.
次に、本発明について図面を参照して説明する。 Next, the present invention will be described with reference to the drawings.
第1図は本発明の一実施例の縦断面図、第2図は、第1
図のコレクタ部のA−A断面図を示す。FIG. 1 is a vertical sectional view of an embodiment of the present invention, and FIG.
The sectional view on the AA of the collector part of a figure is shown.
マイクロ波管は、電子銃部1,高周波回路部2,集束用磁界
装置部3,コレクタ部4からなりコレクタ部4は、コレク
タコア5とその外周部にろう付固定された放熱翼6とコ
レクタ外部に取付けた偏向用マグネット7から構成され
ている。The microwave tube is composed of an electron gun section 1, a high frequency circuit section 2, a focusing magnetic field device section 3 and a collector section 4, and the collector section 4 includes a collector core 5 and a radiating blade 6 and a collector fixed to the outer periphery thereof by brazing. It is composed of a deflection magnet 7 attached to the outside.
また、コレクタコア5は熱伝導率の大きい非磁性無酸素
銅を材料とし、その入口部分の材料の一部に鉄などの強
磁性材8を管軸に対して点対称となる位置にろう付など
に配され、さらに放熱翼6の外周部に鉄などの強磁性材
9が固定されている。The collector core 5 is made of non-magnetic oxygen-free copper having a high thermal conductivity, and a ferromagnetic material 8 such as iron is brazed to a part of the material of the inlet portion at a position symmetrical with respect to the tube axis. Etc., and a ferromagnetic material 9 such as iron is fixed to the outer peripheral portion of the radiator blade 6.
偏向用マグネット7はコレクタ外部で強磁性材8の近傍
に取り付けられ、磁界がコレクタコア5の中心に向かう
ように取付けることにより、第2図に示すようにコレク
タコア5の入口部に配された強磁性材8を磁力線が通
り、放熱翼6の外部の強磁性材9をもどる磁気帰還回路
を形成することにより、コレクタコア5の入口部の管軸
に垂直な面に充分強い磁界を発生することができる。The deflection magnet 7 is attached to the vicinity of the ferromagnetic material 8 outside the collector, and is attached so that the magnetic field is directed toward the center of the collector core 5, so that the deflection magnet 7 is arranged at the inlet of the collector core 5 as shown in FIG. By forming a magnetic feedback circuit in which magnetic lines of force pass through the ferromagnetic material 8 and return to the ferromagnetic material 9 outside the heat radiating blade 6, a sufficiently strong magnetic field is generated in a plane perpendicular to the tube axis at the inlet of the collector core 5. be able to.
以上説明したように本発明は、非磁性の無酸素銅製のコ
レクタコアの入口部分の材料の一部に鉄などの強磁性材
を管軸に対し、点対称な位置に配し、この近傍に偏向用
マグネットをコレクタ外部に取付け、放熱翼の外周部を
おおうように鉄などの強磁性材を配することにより、コ
レクタ入口部に磁気帰還回路を形成し、コレクタ入口部
の管軸に垂直な面に充分強い磁界を発生することができ
るので戻り電子や2次電子に作用してその軌道を曲げ高
周波回路への逆流を効果的に防止することができる。As described above, according to the present invention, a ferromagnetic material such as iron is placed in a part of the material of the inlet portion of the non-magnetic oxygen-free copper collector core in a point-symmetrical position with respect to the tube axis, and in the vicinity of this. By attaching a deflection magnet to the outside of the collector and arranging a ferromagnetic material such as iron so as to cover the outer circumference of the radiator blade, a magnetic feedback circuit was formed at the collector inlet, and a magnetic feedback circuit was formed perpendicular to the collector inlet tube axis. Since a sufficiently strong magnetic field can be generated on the surface, it acts on return electrons and secondary electrons to bend their orbits and effectively prevent backflow to the high frequency circuit.
従って、コレクタ電位の大幅な低下が可能となり効率向
上に効果がある。Therefore, the collector potential can be drastically reduced, and the efficiency can be improved.
第1図は本発明の一実施例の縦断面図、第2図は第1図
のコレクタ部のA−A断面図 1……電子銃部、2……高周波回路部、3……集束用磁
界装置部、4……コレクタ部、5……コレクタコア、6
……放熱翼、7……偏向用マグネット、8,9……強磁性
材、10……絶縁石。FIG. 1 is a longitudinal sectional view of an embodiment of the present invention, and FIG. 2 is a sectional view taken along the line AA of the collector section in FIG. 1 ... Electron gun section, 2 ... High frequency circuit section, 3 ... For focusing Magnetic field device section, 4 ... Collector section, 5 ... Collector core, 6
...... Radiating blades, 7 ...... Deflection magnets, 8, 9 ...... Ferromagnetic materials, 10 ...... Insulating stones.
Claims (1)
子ビームとの相互作用により高周波増幅を行なう高周波
回路部と、電子ビームを高周波回路内に集束せしめる集
束磁界装置部と、高周波回路との相互作用で増幅に寄与
した電子ビームを捕捉するコレクタ部とで構成されるマ
イクロ波管において、コレクタ部はその入口部に鉄など
の強磁性材を管軸に対して点対称に配しかつこの強磁性
材の近傍でコレクタ側に偏向用マグネットを取付け、さ
らにコレクタコアの入口部のコレクタ外周部をおおうよ
うに強磁性材を配したことを特徴とするマイクロ波管。1. An electron gun section for radiating and forming an electron beam, a high frequency circuit section for high frequency amplification by interaction with the electron beam, a focusing magnetic field device section for focusing the electron beam in the high frequency circuit, and a high frequency circuit. In a microwave tube composed of a collector section that captures an electron beam that has contributed to amplification by the interaction of, the collector section has a ferromagnetic material such as iron at its entrance and is arranged point-symmetrically with respect to the tube axis. A microwave tube characterized in that a deflection magnet is attached to the collector side in the vicinity of the ferromagnetic material, and further the ferromagnetic material is arranged so as to cover the outer peripheral portion of the collector at the inlet of the collector core.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP29112887A JPH0711938B2 (en) | 1987-11-17 | 1987-11-17 | Microwave tube |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP29112887A JPH0711938B2 (en) | 1987-11-17 | 1987-11-17 | Microwave tube |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01132031A JPH01132031A (en) | 1989-05-24 |
| JPH0711938B2 true JPH0711938B2 (en) | 1995-02-08 |
Family
ID=17764816
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP29112887A Expired - Lifetime JPH0711938B2 (en) | 1987-11-17 | 1987-11-17 | Microwave tube |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0711938B2 (en) |
-
1987
- 1987-11-17 JP JP29112887A patent/JPH0711938B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH01132031A (en) | 1989-05-24 |
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