JPH11149876A - Microwave tube - Google Patents

Microwave tube

Info

Publication number
JPH11149876A
JPH11149876A JP31233897A JP31233897A JPH11149876A JP H11149876 A JPH11149876 A JP H11149876A JP 31233897 A JP31233897 A JP 31233897A JP 31233897 A JP31233897 A JP 31233897A JP H11149876 A JPH11149876 A JP H11149876A
Authority
JP
Japan
Prior art keywords
waveguide
output
cooling medium
microwave tube
rectangular waveguide
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
Application number
JP31233897A
Other languages
Japanese (ja)
Other versions
JP3107779B2 (en
Inventor
Setsuo Miyake
節雄 三宅
Katsuhiko Tezuka
勝彦 手塚
Koichiro Hirano
耕一郎 平野
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
Japan Atomic Energy Agency
Original Assignee
Toshiba Corp
Japan Nuclear Cycle Development Institute
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, Japan Nuclear Cycle Development Institute filed Critical Toshiba Corp
Priority to JP09312338A priority Critical patent/JP3107779B2/en
Publication of JPH11149876A publication Critical patent/JPH11149876A/en
Application granted granted Critical
Publication of JP3107779B2 publication Critical patent/JP3107779B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

(57)【要約】 【課題】マイクロ波管における出力矩形導波管の気密窓
の熱損傷および出力導波管の温度上昇を所定の水準に維
持できるマイクロ波管の構造を提供する。 【解決手段】この発明のマイクロ波管は、出力空胴4で
分岐される電子が出力矩形導波管の端部に設けられた気
密窓5の誘電体板5aに直接衝突することを防止するた
めに、ドリフト管から気密窓を直接見通すことができな
いよう、矩形導波管内壁から電界方向と平行または垂直
に延出された障壁部材8a,8bを有する。障壁部材8
a,8bの先端部分に、冷却媒体による冷却を可能とす
る冷媒通路9a,9bが形成され、冷媒通路への冷却媒
体の注入により、温度上昇が抑えられている。
(57) An object of the present invention is to provide a structure of a microwave tube capable of maintaining thermal damage of an airtight window of an output rectangular waveguide and a temperature rise of the output waveguide at a predetermined level. A microwave tube according to the present invention prevents electrons branched by an output cavity from directly colliding with a dielectric plate of a hermetic window provided at an end of an output rectangular waveguide. For this reason, barrier members 8a and 8b extending from the inner wall of the rectangular waveguide in parallel or perpendicular to the direction of the electric field are provided so that the airtight window cannot be directly seen through the drift tube. Barrier member 8
Refrigerant passages 9a and 9b that allow cooling by a cooling medium are formed at the distal end portions of the a and 8b, and the temperature rise is suppressed by injecting the cooling medium into the refrigerant passage.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】この発明は、クライストロ
ン、線形加速器、ジャイロトロンあるいは進行波管等の
マイクロ波管に係り、特に、その出力導波管部の改良に
関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a microwave tube such as a klystron, a linear accelerator, a gyrotron, or a traveling wave tube, and more particularly to an improvement in an output waveguide portion thereof.

【0002】[0002]

【従来の技術】例えば、クライストロン等のマイクロ波
管において、出力電力は、連続出力として数キロワット
以上で、パルス状の尖頭値としては数メガワット以上に
も達するものが開発されている。
2. Description of the Related Art For example, a microwave tube such as a klystron has been developed which has a continuous output of several kilowatts or more and a pulse-like peak value of several megawatts or more.

【0003】ところで、出力電力が上述したように大出
力になると、出力導波管の気密窓がドリフト管側から見
通せる構造である場合、ドリフト管等に衝突して起こる
反射電子あるいは二次電子が出力導波管を通って誘電体
気密窓に衝突する現象が強まる。この衝突した電子が気
密窓近傍に蓄積されると、蓄積された電子から放電が生
じるなどの理由により、気密窓の誘電体に亀裂が生じた
り、気密窓の誘電体の真空側と大気側との間で絶縁破壊
が生じることが知られている。
When the output power becomes large as described above, if the airtight window of the output waveguide has a structure that can be seen from the drift tube side, reflected electrons or secondary electrons generated by colliding with the drift tube or the like are generated. The phenomenon of colliding with the dielectric hermetic window through the output waveguide increases. When the colliding electrons are accumulated near the hermetic window, cracks may occur in the dielectric of the hermetic window or the vacuum side and the atmospheric side of the dielectric of the hermetic window may be discharged because of the discharge from the accumulated electrons. It is known that dielectric breakdown occurs between the two.

【0004】このことから、特開昭51−126031
号公報の第3図ないし第5図にも示されていろように、
出力導波管内に、ドリフト管を通る電子ビームと気密窓
とを光学的に遮蔽する障壁板を配置して、気密窓を保護
する例がある。
[0004] From this, Japanese Patent Laid-Open No. Sho 51-126031
As shown in FIG. 3 to FIG.
There is an example in which a barrier plate that optically shields an electron beam passing through a drift tube and an airtight window is arranged in an output waveguide to protect the airtight window.

【0005】[0005]

【発明が解決しようとする課題】しかしながら、出力導
波管内に、上述した特開昭51−126031号公報に
見られるような障壁板を配置することにより、出力導波
管内を通過する電磁波の出力が増大されることで、導波
管および障壁板における誘導損失や導波管内の浮遊電子
の衝突等により、導波管および障壁板が、不所望に加熱
されることになる。
However, by disposing a barrier plate as disclosed in Japanese Patent Laid-Open No. Sho 51-126031 in the output waveguide, the output of the electromagnetic wave passing through the output waveguide can be reduced. Is increased, the waveguide and the barrier plate are undesirably heated due to induced loss in the waveguide and the barrier plate, collision of stray electrons in the waveguide, and the like.

【0006】ところで、障壁板が配置されていない場合
には、導波管の外壁に接する大気による自然冷却あるい
は導波管を外部から冷却するための冷却装置の付加によ
る強制冷却により、導波管内の温度を所定の水準に冷却
できるが、障壁板が形成されている場合には、障壁板の
先端部および障壁板と導波管とが接続される障壁板の脚
部の近傍の導波管の温度が上昇することにより、導波管
が変形するおそれがある。
When the barrier plate is not provided, the inside of the waveguide is cooled by natural cooling by the air in contact with the outer wall of the waveguide or by forced cooling by adding a cooling device for cooling the waveguide from outside. Can be cooled to a predetermined level, but when a barrier plate is formed, the waveguide near the tip of the barrier plate and the leg of the barrier plate where the barrier plate and the waveguide are connected. When the temperature rises, the waveguide may be deformed.

【0007】上述した理由により、導波管が変形する
と、高周波出力特性が変化し、所望の出力電力が得られ
なくなる問題がある。また、温度上昇の程度が所定の水
準を越えた場合には、気密窓および気密窓の誘電体の損
傷などが生じる問題がある。
For the above-mentioned reason, when the waveguide is deformed, there is a problem that the high-frequency output characteristics change and a desired output power cannot be obtained. Further, when the degree of temperature rise exceeds a predetermined level, there is a problem that the hermetic window and the dielectric of the hermetic window are damaged.

【0008】この発明の目的は、マイクロ波管における
出力導波管の気密窓の熱損傷および出力導波管の温度上
昇を所定の水準に維持できるマイクロ波管の構造を提供
するものである。
SUMMARY OF THE INVENTION An object of the present invention is to provide a structure of a microwave tube capable of maintaining a thermal damage to an airtight window of an output waveguide and a temperature rise of the output waveguide at a predetermined level.

【0009】[0009]

【課題を解決するための手段】この発明は、上記問題点
に基づきなされたもので、誘電体板からなる電磁波通過
用気密窓と出力空胴との間に出力矩形導波管を有し、上
記矩形導波管内に、該導波管の伝送マイクロ波の電界方
向と平行または垂直な該導波管壁面から途中まで突き出
した導電体製障壁部材が互いに所定間隔を置きかつ上記
空胴内の電子ビーム通過路から上記気密窓の誘電体板が
直接見通せないように互いに突設されているマイクロ波
管において、上記障壁部材内に第1の冷却媒体通路を有
していることを特徴とするマイクロ波管である。
SUMMARY OF THE INVENTION The present invention has been made based on the above problems, and has an output rectangular waveguide between an electromagnetic wave passing hermetic window made of a dielectric plate and an output cavity. In the rectangular waveguide, conductive barrier members protruding partway from the waveguide wall parallel or perpendicular to the direction of the electric field of the transmitted microwave of the waveguide are spaced apart from each other by a predetermined distance, and are formed in the cavity. In a microwave tube projecting from each other so that a dielectric plate of the hermetic window cannot be directly seen through an electron beam passage, a first cooling medium passage is provided in the barrier member. Microwave tube.

【0010】また、この発明のマイクロ波管は、前記矩
形導波管の外壁に第2の冷却媒体通路が伝熱的に形成さ
れ、上記第2の冷却媒体通路が前記障壁部材内の上記第
1の冷却媒体通路に連通されていることを特徴とする。
さらに、この発明のマイクロ波管は、前記障壁部材内の
上記第1の冷却媒体通路が前記障壁部材の先端付近に形
成されることを特徴とする。
In the microwave tube according to the present invention, a second cooling medium passage is formed on the outer wall of the rectangular waveguide so as to conduct heat, and the second cooling medium passage is formed in the barrier member. It is characterized by being connected to one cooling medium passage.
Further, the microwave tube according to the present invention is characterized in that the first cooling medium passage in the barrier member is formed near a tip of the barrier member.

【0011】[0011]

【発明の実施の形態】以下、図面を用いてこの発明の実
施の形態を説明する。図1は、マイクロ波管の中でも発
振出力の増幅または中継出力の減衰分を増幅により補償
するクライストロン管を説明する概略図である。
Embodiments of the present invention will be described below with reference to the drawings. FIG. 1 is a schematic diagram for explaining a klystron tube that compensates for amplification of oscillation output or attenuation of relay output by amplification among microwave tubes.

【0012】図1に示されるように、クライストロン管
1は、ドリフト管2、出力空胴4、及び出力矩形導波管
3を有している。矩形導波管3は、出力空胴と対向する
側の端部に、誘電体板5aが所定位置に固定された円形
の気密窓5を有している。
As shown in FIG. 1, the klystron tube 1 has a drift tube 2, an output cavity 4, and an output rectangular waveguide 3. The rectangular waveguide 3 has a circular airtight window 5 in which a dielectric plate 5a is fixed at a predetermined position at an end facing the output cavity.

【0013】出力矩形導波管3は、出力空胴4への接続
部4aと、気密窓5との間に、ドリフト管間隙Gを通る
電子7が気密窓5に到達することを防止するために、導
波管3の内部に、導波管3の長手方向の離れた位置に互
いに反対側の壁面から2枚の衝立状の第1および第2の
障壁部材8a,8bが配置されている。すなわち、第
1、第2の障壁部材8a,8bは、電子ビーム通路から
気密窓5の誘電体板5aを直接見通すことができないよ
うに、導波管3の伝送マイクロ波の電界方向と平行また
は垂直な導波管壁面に、図2に示されるように、出力導
波管3の管内中央部を越える長さに、電子ビーム通路の
途中まで形成されている。
The output rectangular waveguide 3 prevents electrons 7 passing through the drift tube gap G from reaching the hermetic window 5 between the connection portion 4a to the output cavity 4 and the hermetic window 5. In the waveguide 3, two screen-shaped first and second barrier members 8a and 8b are arranged at positions separated from each other in the longitudinal direction of the waveguide 3 from opposite wall surfaces. . That is, the first and second barrier members 8a and 8b are parallel or parallel to the direction of the electric field of the transmitted microwave of the waveguide 3 so that the dielectric plate 5a of the hermetic window 5 cannot be directly seen through the electron beam path. As shown in FIG. 2, the output waveguide 3 is formed on the vertical waveguide wall so as to extend beyond the central portion of the output waveguide 3 in the middle of the electron beam path.

【0014】第1および第2の障壁部材8a,8bの先
端部すなわち図2に示されるように障壁部材8a,8b
において矩形導波管3の内壁からこの導波管3の断面方
向に最も離れた部分には、障壁部材8a,8bおよび導
波管壁を冷却するための冷却媒体たとえば水が案内され
る第1の冷却媒体通路(以下冷媒通路と略称する)9
a、9bが形成されている。
The distal ends of the first and second barrier members 8a, 8b, ie, the barrier members 8a, 8b as shown in FIG.
In the first part, the barrier member 8a, 8b and a cooling medium for cooling the waveguide wall, for example, water, are guided to the portion farthest from the inner wall of the rectangular waveguide 3 in the cross-sectional direction of the waveguide 3. Cooling medium passage (hereinafter abbreviated as refrigerant passage) 9
a, 9b are formed.

【0015】また、矩形導波管3の外周には、この導波
管壁を冷却するための第2の冷媒通路10a、10bが
設けられている。なお、これら冷媒通路9a、9b、1
0aおよび10bのそれぞれは、図示しない接続部によ
り一本の冷媒通路として接続されている。すなわち、第
1の冷媒通路9a、9bには、例えば第2の冷媒通路1
0aを経由して図示しない冷媒供給装置から冷却水が供
給される。また、同様に、他の第1冷媒通路9bを通っ
た冷却水は、第2冷媒通路10bを経由して図示しない
冷媒供給装置に戻される。
On the outer periphery of the rectangular waveguide 3, there are provided second refrigerant passages 10a and 10b for cooling the waveguide wall. The refrigerant passages 9a, 9b, 1
Each of Oa and 10b is connected as one refrigerant passage by a connection part (not shown). That is, for example, the first refrigerant passages 9a and 9b are
Cooling water is supplied from a refrigerant supply device (not shown) via Oa. Similarly, the cooling water that has passed through the other first refrigerant passage 9b is returned to a not-shown refrigerant supply device via the second refrigerant passage 10b.

【0016】上述したように、図1および図2を用いて
説明したクライストロン管においては、断面形状が矩形
に形成された出力矩形導波管内部に、ドリフト管2から
出力空胴4で分岐される電子が出力導波管の端部に設け
られた気密窓5の誘電体板5aに直接衝突することを防
止するために、ドリフト管2から気密窓5を見通すこと
ができないよう、導波管内壁から電界方向と平行または
垂直に延出された障壁部材8a,8bが設けられ、気密
窓5が保護される。障壁部材8a,8bの先端部分に、
冷却媒体による冷却を可能とする冷媒通路9a,9bが
形成され、温度上昇が抑えられている。これにより、誘
電損失あるいは電子の衝突に起因して、障壁部材の温度
が不所望に上昇して出力導波管が変形したり気密窓に損
傷が生じることが防止される。
As described above, in the klystron tube described with reference to FIGS. 1 and 2, the output cavity 4 branches from the drift tube 2 into the output rectangular waveguide having a rectangular cross section. In order to prevent the electrons from directly colliding with the dielectric plate 5a of the hermetic window 5 provided at the end of the output waveguide, the inside of the waveguide is controlled so that the hermetic window 5 cannot be seen through the drift tube 2. Barrier members 8a, 8b extending from the wall in a direction parallel or perpendicular to the direction of the electric field are provided to protect the hermetic window 5. At the tip portions of the barrier members 8a and 8b,
Refrigerant passages 9a and 9b that enable cooling by a cooling medium are formed, and a rise in temperature is suppressed. This prevents the temperature of the barrier member from undesirably increasing due to dielectric loss or electron collision, thereby preventing the output waveguide from being deformed or causing damage to the hermetic window.

【0017】[0017]

【発明の効果】以上説明したように、この発明によれ
ば、出力矩形導波管の不所望な温度上昇を低減できる。
これにより、出力導波管が変形して、高周波出力特性が
劣化することが防止される。また、気密窓に損傷が生じ
る等の構造上の不具合が発生することが防止される。
As described above, according to the present invention, an undesired rise in the temperature of the output rectangular waveguide can be reduced.
This prevents the output waveguide from deforming and deteriorating the high-frequency output characteristics. Further, it is possible to prevent a structural defect such as damage to the airtight window from occurring.

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

【図1】この発明の一実施例のクライストロン管の要部
の縦断面図。
FIG. 1 is a longitudinal sectional view of a main part of a klystron tube according to an embodiment of the present invention.

【図2】図1のa−a′における横断面図。FIG. 2 is a cross-sectional view taken along aa 'of FIG.

【符号の説明】[Explanation of symbols]

1 ・・・クライストロン管、 3 ・・・出力矩形導波管、 4 ・・・出力空胴、 5 ・・・気密窓、 5a・・・誘電体板、 7 ・・・電子流、 8a,8b ・・・障壁部材、 9a,9b ・・・第1の冷媒通路、 10a,10b ・・・第2の冷媒通路。 DESCRIPTION OF SYMBOLS 1 ... Klystron tube, 3 ... Output rectangular waveguide, 4 ... Output cavity, 5 ... Airtight window, 5a ... Dielectric plate, 7 ... Electron flow, 8a, 8b ... barrier member, 9a, 9b ... first refrigerant passage, 10a, 10b ... second refrigerant passage.

フロントページの続き (72)発明者 平野 耕一郎 茨城県東茨城郡大洗町成田町4002 動力 炉・核燃料開発事業団大洗工学センター内Continued on the front page (72) Inventor Koichiro Hirano 4002 Narita-cho, Oarai-machi, Higashiibaraki-gun, Ibaraki Power reactor and nuclear fuel development corporation Oarai engineering center

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】誘電体板からなる電磁波通過用気密窓と出
力空胴との間に出力矩形導波管を有し、上記矩形導波管
内に、該導波管の伝送マイクロ波の電界方向と平行また
は垂直な該導波管壁面から途中まで突き出した導電体製
障壁部材が互いに所定間隔を置きかつ上記空胴内の電子
ビーム通過路から上記気密窓の誘電体板が直接見通せな
いように互いに突設されているマイクロ波管において、 上記障壁部材内に第1の冷却媒体通路を有していること
を特徴とするマイクロ波管。
An output rectangular waveguide is provided between an electromagnetic wave passage hermetic window made of a dielectric plate and an output cavity, and an electric field direction of a microwave transmitted through the waveguide is provided in the rectangular waveguide. Conductor barrier members protruding halfway from the waveguide wall parallel or perpendicular to each other are spaced apart from each other at a predetermined interval, and the dielectric plate of the hermetic window cannot be directly seen through the electron beam passage in the cavity. A microwave tube protruding from each other, wherein the microwave tube has a first cooling medium passage in the barrier member.
【請求項2】前記矩形導波管の外壁に第2の冷却媒体通
路が伝熱的に形成され、上記第2の冷却媒体通路が前記
障壁部材内の上記第1の冷却媒体通路に連通されている
ことを特徴とする請求項1に記載のマイクロ波管。
2. A second cooling medium passage is formed on the outer wall of the rectangular waveguide so as to conduct heat, and the second cooling medium passage communicates with the first cooling medium passage in the barrier member. The microwave tube according to claim 1, wherein:
【請求項3】前記障壁部材内の上記第1の冷却媒体通路
は、前記障壁部材の先端付近に形成されることを特徴と
する請求項1または2のいづれかに記載のマイクロ波
管。
3. The microwave tube according to claim 1, wherein the first cooling medium passage in the barrier member is formed near a tip of the barrier member.
JP09312338A 1997-11-13 1997-11-13 Microwave tube Expired - Fee Related JP3107779B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP09312338A JP3107779B2 (en) 1997-11-13 1997-11-13 Microwave tube

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP09312338A JP3107779B2 (en) 1997-11-13 1997-11-13 Microwave tube

Publications (2)

Publication Number Publication Date
JPH11149876A true JPH11149876A (en) 1999-06-02
JP3107779B2 JP3107779B2 (en) 2000-11-13

Family

ID=18028045

Family Applications (1)

Application Number Title Priority Date Filing Date
JP09312338A Expired - Fee Related JP3107779B2 (en) 1997-11-13 1997-11-13 Microwave tube

Country Status (1)

Country Link
JP (1) JP3107779B2 (en)

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JP2007234344A (en) * 2006-02-28 2007-09-13 Toshiba Corp Microwave tube
EP1826805A3 (en) * 2006-02-28 2009-02-25 Kabushiki Kaisha Toshiba Microwave tube
US7710041B2 (en) 2006-02-28 2010-05-04 Kabushiki Kaisha Toshiba Microwave tube
CN111139099A (en) * 2020-01-19 2020-05-12 北京诺芯环境科技有限公司 Microwave pyrolysis equipment
CN111154508A (en) * 2020-01-19 2020-05-15 北京诺芯环境科技有限公司 A waveguide protection device and microwave pyrolysis equipment
CN111154508B (en) * 2020-01-19 2025-02-14 北京诺芯环境科技有限公司 A waveguide protection device and microwave pyrolysis equipment

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