JPS60195840A - Gyrotron oscillation tube - Google Patents

Gyrotron oscillation tube

Info

Publication number
JPS60195840A
JPS60195840A JP5110584A JP5110584A JPS60195840A JP S60195840 A JPS60195840 A JP S60195840A JP 5110584 A JP5110584 A JP 5110584A JP 5110584 A JP5110584 A JP 5110584A JP S60195840 A JPS60195840 A JP S60195840A
Authority
JP
Japan
Prior art keywords
reflector
electron beam
magnetic field
electric wave
collector
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
Application number
JP5110584A
Other languages
Japanese (ja)
Inventor
Toru Sugawara
亨 菅原
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Toshiba Corp
Original Assignee
Toshiba Corp
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Toshiba Corp filed Critical Toshiba Corp
Priority to JP5110584A priority Critical patent/JPS60195840A/en
Publication of JPS60195840A publication Critical patent/JPS60195840A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J25/00Transit-time tubes, e.g. klystrons, travelling-wave tubes, magnetrons
    • H01J25/02Tubes with electron stream modulated in velocity or density in a modulator zone and thereafter giving up energy in an inducing zone, the zones being associated with one or more resonators
    • H01J25/025Tubes with electron stream modulated in velocity or density in a modulator zone and thereafter giving up energy in an inducing zone, the zones being associated with one or more resonators with an electron stream following a helical path

Abstract

PURPOSE:To enable a collector to be independent from a waveguide passage by providing an electric wave reflector between an electron beam collector and a resonance cavity in order to transfer the electric wave. CONSTITUTION:Supposing that a figure of an electromagnetic wave generated in a resonance cavity 4 is TEon provided that (n) is a positive integral number, the conversion into the linear poralization as well as the conversion of the electric wave advance direction is performed generally by cutting an opening of a cylindrical waveguide tube part 8 obliquely while joining it together with a reflector 9 having a reflection face tangential to a parabolic column. In the case shown by the figure, the electric wave advances in the direction of the output tubes 10 and 7. An electron beam is guided by a magnetic field generated by means of a magnetic field generation coil 3c so as to be advanced without colliding with the members 8 and 9 for being collected by an electron beam collector with an expanded heat receiving area widened in a horn shape. Further, not only the reflector having the reflection face tangential to the parabolic column but also the reflection face tangential to the ellipsoidal column can be used for the refelctor 9, whereby the focusing effect of the electromagnetic wave beam of the linear polarization can be improved.

Description

【発明の詳細な説明】 〔発明の属する技術分野〕 本発明はEHF帝の電波を発生するジャイロトロン発振
管に関する。
DETAILED DESCRIPTION OF THE INVENTION [Technical field to which the invention pertains] The present invention relates to a gyrotron oscillator tube that generates EHF radio waves.

〔従来技術とその問題点〕[Prior art and its problems]

従来のジャイロトロン発振管の構成を第1図に示す。こ
のジャイロトロン発振管は、陰極1と陽極2から成る電
子銃と、電子を案内する磁場を発生する巻線3と共振空
胴4と電子ビームコレクタ5とから成る。共振空胴で発
生した電波は、絶縁物で構成される窓6を通過し出力導
波管7へ前進する。
The configuration of a conventional gyrotron oscillation tube is shown in FIG. This gyrotron oscillation tube consists of an electron gun consisting of a cathode 1 and an anode 2, a winding 3 that generates a magnetic field for guiding electrons, a resonant cavity 4, and an electron beam collector 5. Radio waves generated in the resonant cavity pass through a window 6 made of an insulator and advance to an output waveguide 7.

この発振管では、電子ビームコレクタとなる管部と電波
の導波用管部が5で示す部分で共用されている。大電力
用発振管では、コレクタ5に集められる電子ビームの残
留エネルギーは極めて大きくコレクタ5の冷却責務は厳
しい。然しなから、コレクタ管部が導波用管部と共用さ
れているため導波機能を妨害することなく高い冷却責務
を果させることL困難である欠点がある。
In this oscillator tube, the portion indicated by 5 is used in common as a tube portion serving as an electron beam collector and a tube portion for guiding radio waves. In a high-power oscillator tube, the residual energy of the electron beam collected in the collector 5 is extremely large, and the responsibility for cooling the collector 5 is severe. However, since the collector tube portion is shared with the waveguide tube portion, it is difficult to perform a high cooling duty without interfering with the waveguide function.

〔発明の目的〕[Purpose of the invention]

この発明は上述した欠点を改良するもので電波の前進方
向を電子ビームの進行方向から分離させたジャイロトロ
ン発振管を提供することを目的とする。
The present invention aims to improve the above-mentioned drawbacks and provides a gyrotron oscillation tube in which the forward direction of radio waves is separated from the forward direction of electron beams.

〔発明の概要〕[Summary of the invention]

本発明は、電子ビームコレクタと共振空胴との間に電波
反射器を設けて電波を転進させ、以って導波路と独立せ
られたコレクタを可能とするジャイロトロン発振管であ
る。
The present invention is a gyrotron oscillator tube in which a radio wave reflector is provided between an electron beam collector and a resonant cavity to propagate radio waves, thereby enabling a collector independent of a waveguide.

〔発明の効果〕〔Effect of the invention〕

本発明によれば大電力用発振管を構成でき、また直線偏
波の出力波を得ることができる。
According to the present invention, a high power oscillation tube can be constructed and a linearly polarized output wave can be obtained.

〔発明の実施例〕[Embodiments of the invention]

以下本発明の実施例を詳細に説明する。第2図は本発明
のジャイロトロン発振管の構成を示す。
Examples of the present invention will be described in detail below. FIG. 2 shows the configuration of the gyrotron oscillation tube of the present invention.

電子銃部は図から省略した。また、従来装置と同一の部
分については同一符号を附は説明を省く。
The electron gun section is omitted from the figure. Further, the same parts as those of the conventional device are given the same reference numerals, and the explanation will be omitted.

共振空胴4で発生する電磁波の姿態がnを正整数として
TEonであるとすると一般に円筒導波管部8の開口を
斜めに切断し放物柱に接する反射面をもつ反射器9と組
み合わせることによって直線偏波への変換ならびに電波
前進方向の転換が行なわれる。第2図に示した実施例の
場合、電波は出力管10および7の方向へ進む。電子ビ
ームは8および9の部材に衝突することなく進行せしめ
るよう磁場発生巻線3CKよる磁場で案内し、IIII
IA状に広げて受熱面積を拡大した電子ビームコレクタ
に集められる。
Assuming that the form of electromagnetic waves generated in the resonant cavity 4 is TEon, where n is a positive integer, the opening of the cylindrical waveguide section 8 is generally cut diagonally and combined with a reflector 9 having a reflecting surface in contact with a parabolic column. Conversion to linearly polarized waves and reversal of the forward direction of radio waves are performed. In the embodiment shown in FIG. 2, the radio waves travel in the direction of the output tubes 10 and 7. The electron beam is guided by the magnetic field generated by the magnetic field generating winding 3CK so that it can travel without colliding with the members 8 and 9.
The electron beams are collected in an electron beam collector that is expanded into an IA shape to increase the heat receiving area.

同5反射器9は放物柱に接する反射面をもつ反射器にと
どまらず楕円柱に接する反射面を用いても良くこの場合
には直線偏波の電磁波ビームの収束効果を向上させるこ
とができる。
The reflector 9 is not limited to a reflector with a reflecting surface that touches a parabolic column, but may also use a reflecting surface that touches an elliptical column, and in this case, the convergence effect of the linearly polarized electromagnetic wave beam can be improved. .

【図面の簡単な説明】[Brief explanation of drawings]

第1図は従来のジャイロトロン発振管を示す断面図、第
2図は本発明によるジャイロトロン発振管を示す断面図
である。 1・・・電子銃陰極、2・・・電子銃陽極、3・・・巻
線、4・・・共振空胴、5・・・電子ビームコνクタ、
6・・・電磁波出力窓、7・・・電磁波出力導波管、8
・・・斜切断円筒導波管、9・・・反射器、10・・・
電磁波出力導波路、11・・・電子ビームコレクタ。 代理人 弁理士 則 近 憲 佑(ほか1名)第1図 ? 第2図
FIG. 1 is a sectional view showing a conventional gyrotron oscillation tube, and FIG. 2 is a sectional view showing a gyrotron oscillation tube according to the present invention. DESCRIPTION OF SYMBOLS 1... Electron gun cathode, 2... Electron gun anode, 3... Winding wire, 4... Resonance cavity, 5... Electron beam controller,
6... Electromagnetic wave output window, 7... Electromagnetic wave output waveguide, 8
...Oblique cut cylindrical waveguide, 9...Reflector, 10...
Electromagnetic wave output waveguide, 11...electron beam collector. Agent Patent Attorney Noriyuki Chika (and 1 other person) Figure 1? Figure 2

Claims (3)

【特許請求の範囲】[Claims] (1)電子銃と磁場発生器と共振空胴とから成るジャイ
ロトロン発振管において共振空胴の電波出力端九電波反
射器を設は出力電波の前進方向を電子銃より発せられ、
磁場発生器によって生成せられた磁場で案内せられた電
子ビームの前進方向と異ならせて構成したことを特徴と
するジャイロトロン発振管。
(1) In a gyrotron oscillation tube consisting of an electron gun, a magnetic field generator, and a resonant cavity, nine radio wave reflectors are installed at the radio wave output end of the resonant cavity to direct the forward direction of the output radio waves emitted from the electron gun.
A gyrotron oscillation tube characterized in that the gyrotron oscillation tube is configured such that the forward direction of an electron beam guided by a magnetic field generated by a magnetic field generator is different.
(2)電波反射器を放物柱にtIは接する反射面をもつ
反射器としたことを特徴とする特許請求の範囲第1項記
載のジャイロトロン発振管。
(2) The gyrotron oscillation tube according to claim 1, wherein the radio wave reflector is a reflector having a reflecting surface that is in contact with a parabolic column.
(3)電波反射器を楕円柱に#′!は接する反射面をも
つ反射器としたことを特徴とする特許請求の範囲第1項
記載のジャイロトロン発振管。
(3) Make the radio wave reflector into an elliptical cylinder #'! 2. The gyrotron oscillation tube according to claim 1, wherein is a reflector having reflective surfaces in contact with each other.
JP5110584A 1984-03-19 1984-03-19 Gyrotron oscillation tube Pending JPS60195840A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5110584A JPS60195840A (en) 1984-03-19 1984-03-19 Gyrotron oscillation tube

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5110584A JPS60195840A (en) 1984-03-19 1984-03-19 Gyrotron oscillation tube

Publications (1)

Publication Number Publication Date
JPS60195840A true JPS60195840A (en) 1985-10-04

Family

ID=12877524

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5110584A Pending JPS60195840A (en) 1984-03-19 1984-03-19 Gyrotron oscillation tube

Country Status (1)

Country Link
JP (1) JPS60195840A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03192633A (en) * 1989-12-21 1991-08-22 Toshiba Corp Gyrotron oscillation tube
US5187409A (en) * 1990-03-26 1993-02-16 Kabushiki Kaisha Toshiba Gyrotron having a quasi-optical mode converter

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03192633A (en) * 1989-12-21 1991-08-22 Toshiba Corp Gyrotron oscillation tube
US5187409A (en) * 1990-03-26 1993-02-16 Kabushiki Kaisha Toshiba Gyrotron having a quasi-optical mode converter

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