JPH0541169A - Linear beam type microwave tube device - Google Patents
Linear beam type microwave tube deviceInfo
- Publication number
- JPH0541169A JPH0541169A JP19779191A JP19779191A JPH0541169A JP H0541169 A JPH0541169 A JP H0541169A JP 19779191 A JP19779191 A JP 19779191A JP 19779191 A JP19779191 A JP 19779191A JP H0541169 A JPH0541169 A JP H0541169A
- Authority
- JP
- Japan
- Prior art keywords
- collector
- electromagnetic coil
- collector electrode
- tube device
- 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.)
- Granted
Links
Landscapes
- Microwave Tubes (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】この発明は、ジャイロトロン、ク
ライストロン、あるいは進行波管のようなマイクロ波電
力を発振あるいは増幅するビーム直進形マイクロ波管装
置に係わり、とくにコレクタ部の改良に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a beam rectilinear microwave tube device for oscillating or amplifying microwave power, such as a gyrotron, a klystron, or a traveling wave tube, and more particularly to improvement of a collector section.
【0002】[0002]
【従来の技術】上記のようなビーム直進形マイクロ波管
装置は、周知の通り、電子ビームを発生する電子銃部、
そのビーム下流に配置された共振空胴部又は遅波回路の
ような高周波作用部、さらにそのビーム下流に配置され
たコレクタ部、電子ビーム集束用磁界装置、および各部
に動作電圧を与える電源装置とを有して構成される。2. Description of the Related Art As is well known, a beam rectilinear microwave tube device as described above has an electron gun section for generating an electron beam,
A high-frequency acting part such as a resonant cavity part or a slow wave circuit arranged downstream of the beam, a collector part arranged further downstream of the beam, a magnetic field device for electron beam focusing, and a power supply device for applying an operating voltage to each part. It is configured with.
【0003】ところで近来は、高周波出力電力の増大が
顕著であり、高周波作用部を経て用済みになった電子ビ
ームを、コレクタ電極壁になるべく均等に分散させて捕
捉することが必要になっている。そのために、コレクタ
電極の外周に電磁コイルを配置し、この電磁コイルに交
流電流を流し、その掃引磁界により電子ビームを分散さ
せる技術が、例えば特開昭62−278732号公報で
知られている。By the way, recently, the increase in the high frequency output power is remarkable, and it is necessary to disperse the electron beam, which has been used through the high frequency acting section, as evenly as possible on the collector electrode wall. . To this end, a technique in which an electromagnetic coil is arranged around the collector electrode, an alternating current is caused to flow through the electromagnetic coil, and the electron beam is dispersed by the sweeping magnetic field is known, for example, in Japanese Patent Laid-Open No. 62-278732.
【0004】[0004]
【発明が解決しようとする課題】このような、電子ビー
ム掃引用電磁コイルに流す電流は、通常、50Hz又は
60Hzの商用電源を周波数はそのままで適当な電圧に
変換して供給している。なお、上記公報には10〜10
0Hzの正弦波を供給する例が示されている。しかしな
がら、コレクタ電極、あるいはそれを冷却するための冷
却ジャケットは、銅あるいはステンレス鋼のような金属
の円筒であり、電磁コイルで発生される交流磁界によっ
てこれらコレクタ電極やジャケットに誘導電流が発生す
る。The current supplied to the electron beam sweeping electromagnetic coil is usually supplied from a commercial power source of 50 Hz or 60 Hz after converting it into an appropriate voltage with the frequency unchanged. In addition, in the above publication, 10 to 10
An example of supplying a 0 Hz sine wave is shown. However, the collector electrode or the cooling jacket for cooling the collector electrode is a metal cylinder such as copper or stainless steel, and an induction current is generated in the collector electrode and the jacket by the alternating magnetic field generated by the electromagnetic coil.
【0005】この誘導電流は、電子ビームを掃引、拡散
させるコレクタ電極内側の磁界を打ち消して磁界強度を
弱めるとともに、コレクタ電極やジャケット自身にジュ
ール熱を発生させる。このジュール熱の発生は、電磁コ
イルに流す電流の周波数が大きいほど大きくなり、無視
できないものとなる。This induced current cancels the magnetic field inside the collector electrode that sweeps and diffuses the electron beam to weaken the magnetic field strength, and also generates Joule heat in the collector electrode and the jacket itself. The generation of this Joule heat increases as the frequency of the current flowing through the electromagnetic coil increases, and cannot be ignored.
【0006】この発明は、以上のような不都合を解消
し、コレクタ電極の内壁に捕捉される電子ビームを良好
に分散させるとともにコレクタ電極や冷却ジャケットへ
の誘導電流の発生、それによるジュール熱の発生を抑制
することができるビーム直進形マイクロ波管装置を提供
することを目的とする。The present invention eliminates the above-mentioned inconveniences, satisfactorily disperses the electron beam trapped on the inner wall of the collector electrode, generates an induced current to the collector electrode and the cooling jacket, and thereby generates Joule heat. An object of the present invention is to provide a beam straight-moving type microwave tube device capable of suppressing the above.
【0007】[0007]
【課題を解決するための手段】この発明は、コレクタ部
のまわりに配置してコレクタ部に入射する電子を交番磁
界により掃引する電磁コイルに流す電流の掃引周波数
を、10Hz未満(0を含まない)に設定したビーム直
進形マイクロ波管装置である。According to the present invention, the sweep frequency of the current flowing in the electromagnetic coil which is arranged around the collector portion and sweeps the electrons incident on the collector portion by the alternating magnetic field is less than 10 Hz (not including 0). ) Is a straight beam type microwave tube device.
【0008】[0008]
【作用】この発明によれば、電磁コイルに流す電流の掃
引周波数が10Hz未満というように低いため、コレク
タ電極や冷却ジャケットへの誘導電流の発生がきわめて
小さく、したがってそれらに発生するジュール熱も無視
できる程度に抑制され、より一層小さい電磁コイル電流
でコレクタ電極内壁に捕捉される電子ビームを良好に分
散させることができる。According to the present invention, since the sweep frequency of the current flowing through the electromagnetic coil is as low as less than 10 Hz, the generation of the induced current in the collector electrode and the cooling jacket is extremely small, so that the Joule heat generated in them is also ignored. The electron beam is suppressed as much as possible, and the electron beam trapped on the inner wall of the collector electrode can be well dispersed with a smaller electromagnetic coil current.
【0009】[0009]
【実施例】以下、図面を参照してこの発明をジャイロト
ロンに実施した例を説明する。図1に示すように、ジャ
イロトロン本体11は、中空電子ビームを発生する電子銃
部12、そのビーム下流に配置された図示しない共振空胴
を有する高周波作用部、さらにそのビーム下流の横方向
に配置された高周波出力部13、および最下流に配置され
た釣鐘状の銅製コレクタ電極14及びステンレス鋼製蒸発
冷却用ジャケット15を有するコレクタ部16を備えてい
る。電子銃部の外周には電子ビーム集束用電磁コイル1
7、高周波作用部には共振空胴のミリ波電界と相互作用
する電子をサイクロトロン周波数で回転させる磁場を発
生する超伝導コイル18がそれぞれ配置されている。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An example in which the present invention is applied to a gyrotron will be described below with reference to the drawings. As shown in FIG. 1, the gyrotron body 11 includes an electron gun section 12 for generating a hollow electron beam, a high-frequency working section having a resonance cavity (not shown) arranged downstream of the beam, and a lateral direction downstream of the beam. It is provided with a high frequency output section 13 arranged, and a collector section 16 having a bell-shaped copper collector electrode 14 and a stainless steel evaporative cooling jacket 15 arranged at the most downstream side. Electron beam focusing electromagnetic coil 1 around the electron gun
7. Superconducting coils 18 for generating a magnetic field for rotating the electrons interacting with the millimeter-wave electric field of the resonance cavity at the cyclotron frequency are arranged in the high-frequency action section.
【0010】そこで、コレクタ部16の外周には、4個の
リング状電磁コイル19,20,21,22 がコレクタ軸の方向に
所定間隔で縦列配置されている。これらの電磁コイル
は、コレクタ部のまわりに設置された複数本の支柱23,2
4 に、複数対のナット25,25 …によって軸方向の位置が
変えられるように取り付けられている。それによって、
各電磁コイルは最適な位置に調整、設定できる。そし
て、ビーム最上流の電磁コイル19と、ビーム最下流の電
磁コイル22には直流電源26,27 から直流電流が供給され
る。それによって、コレクタ電極の内側の直流磁界の分
布を入射電子ビームがほどよく集束あるいは拡散するよ
うに調節設定される。これら2個の電磁コイルの間に配
置した残り2個の電磁コイル20,21 は、適当な軸方向間
隔で配置され、これら両コイルには交流電源28から交番
電流が供給される。この供給交番電流の掃引周波数は、
10Hz未満、より好ましくは例えば5Hz以下に設定
されている。各2個の電磁コイル20,21 から発生する磁
界は、コレクタ電極14の内側空間に前記周波数で変化
し、入射電子ビームのコレクタ電極内壁への衝突位置を
掃引、分散させる。Therefore, four ring-shaped electromagnetic coils 19, 20, 21, 22 are vertically arranged in the outer periphery of the collector portion 16 at predetermined intervals in the direction of the collector axis. These electromagnetic coils consist of a number of columns 23,2 installed around the collector.
It is attached to 4 so that its axial position can be changed by a plurality of pairs of nuts 25, 25 .... Thereby,
Each electromagnetic coil can be adjusted and set to the optimum position. Then, DC currents are supplied from the DC power supplies 26 and 27 to the electromagnetic coil 19 on the most upstream side of the beam and the electromagnetic coil 22 on the most downstream side of the beam. Thereby, the distribution of the DC magnetic field inside the collector electrode is adjusted and set so that the incident electron beam is moderately focused or diffused. The remaining two electromagnetic coils 20 and 21 arranged between these two electromagnetic coils are arranged at appropriate axial intervals, and an alternating current is supplied from an AC power supply 28 to these coils. The sweep frequency of this supply alternating current is
The frequency is set to less than 10 Hz, more preferably 5 Hz or less. The magnetic field generated from each of the two electromagnetic coils 20 and 21 changes in the space inside the collector electrode 14 at the frequency, and sweeps and disperses the collision position of the incident electron beam on the inner wall of the collector electrode.
【0011】なお、2個の電磁コイル20,21 は、好まし
くは、図2及び図3に示すように金属製の半断面コ字状
に整形したボビン31の円周方向の少なくとも1カ所を切
断してここに薄い樹脂絶縁物32を挟み、導線33をコイル
状に例えば500ターン巻いたものである。このよう
に、ボビン31を円周方向に少なくとも1カ所電気的に切
断してあるため、ボビンに発生する誘導電流をさらに低
減することができる。The two electromagnetic coils 20 and 21 are preferably formed by cutting at least one position in the circumferential direction of a bobbin 31 which is made of metal and has a U-shaped cross section as shown in FIGS. Then, a thin resin insulator 32 is sandwiched here, and the conducting wire 33 is wound in a coil shape, for example, 500 turns. As described above, since the bobbin 31 is electrically cut at at least one position in the circumferential direction, the induced current generated in the bobbin can be further reduced.
【0012】図4及び図5に示す実施例の電磁コイル20
(21)は、そのボビン31の外周部を少し残して少なくとも
1カ所にスリット33を形成したものである。このスリッ
ト33によって、ボビンに発生する誘導電流をさらに低減
することができる。The electromagnetic coil 20 of the embodiment shown in FIGS. 4 and 5.
In (21), a slit 33 is formed in at least one place while leaving the outer peripheral portion of the bobbin 31 a little. The slit 33 can further reduce the induced current generated in the bobbin.
【0013】[0013]
【発明の効果】以上説明したように、この発明によれば
コレクタ部のまわりに配置した電磁コイルに流す電流の
掃引周波数を10Hz未満に設定しているため、コレク
タ電極や冷却ジャケットへの誘導電流の発生を小さくで
き、それらに発生するジュール熱を無視できる程度に抑
制することができる。したがって、より一層小さい電磁
コイル電流でコレクタ電極内壁に捕捉される電子ビーム
を良好に掃引、分散させることができる。As described above, according to the present invention, since the sweep frequency of the current flowing through the electromagnetic coil arranged around the collector is set to less than 10 Hz, the induced current to the collector electrode and the cooling jacket is reduced. Can be reduced, and the Joule heat generated in them can be suppressed to a negligible level. Therefore, the electron beam trapped on the inner wall of the collector electrode can be satisfactorily swept and dispersed with a smaller electromagnetic coil current.
【図1】この発明の実施例を示す概略縦断面図である。FIG. 1 is a schematic vertical sectional view showing an embodiment of the present invention.
【図2】この発明の実施例の一部を示す半断面図であ
る。FIG. 2 is a half sectional view showing a part of an embodiment of the present invention.
【図3】図2の要部を示す横断面図である。FIG. 3 is a cross-sectional view showing a main part of FIG.
【図4】この発明の他の実施例の一部を示す半断面図で
ある。FIG. 4 is a half sectional view showing a part of another embodiment of the present invention.
【図5】図4の要部を示す横断面図である。5 is a cross-sectional view showing the main parts of FIG.
【符号の説明】11 …ジャイロトロン本体、12…電子銃部、13…高周波作
用部、16…コレクタ部、19,20,21,22 …電磁コイル、28
…電源。[Explanation of symbols] 11 ... Gyrotron body, 12 ... Electron gun section, 13 ... High frequency acting section, 16 ... Collector section, 19, 20, 21, 22 ... Electromagnetic coil, 28
…Power supply.
───────────────────────────────────────────────────── フロントページの続き (72)発明者 恒岡 まさき 茨城県那珂郡那珂町大字向山801番地の1 日本原子力研究所那珂研究所内 (72)発明者 假家 強 栃木県大田原市下石上1385番の1 株式会 社東芝那須電子管工場内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Masaki Tsuneoka, No. 1 at 801 Mukaiyama, Naka-cho, Naka-cho, Naka-gun, Ibaraki Prefecture, Japan Naka Research Institute, Japan Atomic Energy Research Institute 1 Stock company Toshiba Nasu electron tube factory
Claims (1)
高周波作用部、そのビーム下流に配置されたコレクタ
部、および前記コレクタ部のまわりに配置されてコレク
タ部に入射する電子を交番磁界により掃引する電磁コイ
ル、および該電磁コイルに電流を供給するコイル付勢電
源とを具備するビーム直進形マイクロ波管装置におい
て、 上記電磁コイルに流す電流の掃引周波数が、10Hz未
満に設定されていることを特徴とするビーム直進形マイ
クロ波管装置。1. An electron gun section, a high-frequency acting section arranged downstream of the beam, a collector section arranged downstream of the beam, and an electron arranged around the collector section and incident on the collector section by an alternating magnetic field. In a beam rectilinear microwave tube device including an electromagnetic coil for sweeping and a coil energizing power source for supplying a current to the electromagnetic coil, the sweep frequency of the current flowing through the electromagnetic coil is set to less than 10 Hz. Straight beam type microwave tube device characterized by.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19779191A JP3164606B2 (en) | 1991-08-07 | 1991-08-07 | Beam straight type microwave tube device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19779191A JP3164606B2 (en) | 1991-08-07 | 1991-08-07 | Beam straight type microwave tube device |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH0541169A true JPH0541169A (en) | 1993-02-19 |
JP3164606B2 JP3164606B2 (en) | 2001-05-08 |
Family
ID=16380414
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP19779191A Expired - Lifetime JP3164606B2 (en) | 1991-08-07 | 1991-08-07 | Beam straight type microwave tube device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP3164606B2 (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5780970A (en) * | 1996-10-28 | 1998-07-14 | University Of Maryland | Multi-stage depressed collector for small orbit gyrotrons |
US8687377B2 (en) | 2011-03-31 | 2014-04-01 | Kabushiki Kaisha Toshiba | Storage device, electronic device, and circuit board assembly |
WO2023090365A1 (en) * | 2021-11-19 | 2023-05-25 | 国立研究開発法人量子科学技術研究開発機構 | Large electron tube, magnetic body, and method for using large electron tube |
-
1991
- 1991-08-07 JP JP19779191A patent/JP3164606B2/en not_active Expired - Lifetime
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5780970A (en) * | 1996-10-28 | 1998-07-14 | University Of Maryland | Multi-stage depressed collector for small orbit gyrotrons |
US8687377B2 (en) | 2011-03-31 | 2014-04-01 | Kabushiki Kaisha Toshiba | Storage device, electronic device, and circuit board assembly |
WO2023090365A1 (en) * | 2021-11-19 | 2023-05-25 | 国立研究開発法人量子科学技術研究開発機構 | Large electron tube, magnetic body, and method for using large electron tube |
Also Published As
Publication number | Publication date |
---|---|
JP3164606B2 (en) | 2001-05-08 |
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