JPH0552015B2 - - Google Patents

Info

Publication number
JPH0552015B2
JPH0552015B2 JP58165938A JP16593883A JPH0552015B2 JP H0552015 B2 JPH0552015 B2 JP H0552015B2 JP 58165938 A JP58165938 A JP 58165938A JP 16593883 A JP16593883 A JP 16593883A JP H0552015 B2 JPH0552015 B2 JP H0552015B2
Authority
JP
Japan
Prior art keywords
collector
core
section
heat
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 - Lifetime
Application number
JP58165938A
Other languages
Japanese (ja)
Other versions
JPS6059633A (en
Inventor
Hisaaki Sato
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.)
NEC Corp
Original Assignee
Nippon Electric Co Ltd
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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP16593883A priority Critical patent/JPS6059633A/en
Publication of JPS6059633A publication Critical patent/JPS6059633A/en
Publication of JPH0552015B2 publication Critical patent/JPH0552015B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J23/00Details of transit-time tubes of the types covered by group H01J25/00
    • H01J23/02Electrodes; Magnetic control means; Screens
    • H01J23/027Collectors
    • H01J23/033Collector cooling devices

Landscapes

  • Microwave Tubes (AREA)

Description

【発明の詳細な説明】 本発明は、直進ビーム形の超大電力マイクロ波
管のコレクタの構造に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to the structure of a collector for a straight beam type ultra-high power microwave tube.

大電力マイクロ波管は、電子ビームを発生させ
る電子銃部、電子ビームのもつエネルギーを高周
波エネルギーに変換する高周波回路部、電子ビー
ムを捕捉するコレクタ部、電子ビームを集束させ
るビーム集束装置等がその主な構成要素である。
超大電力マイクロ波管とは通常の大電力マイクロ
波管より一層大きな電力を扱い、その値は数
100kwから数10Mw(メガ・ワツトアに及ぶ。こ
のような超大電力マイクロ波管においては、連続
波動作のものの他にパルス動作のものもある。パ
ルス動作の場合にも、パルス幅が数μsecから数10
msecの短パルスの場合と、パルス幅が数secから
数10secの長パルスの場合があり、勿論その中間
のパルス幅の場合もある。本発明は、特に長パル
ス動作の直進ビーム形超大電力マイクロ波管のコ
レクタに関するものである。
A high-power microwave tube consists of an electron gun section that generates an electron beam, a high-frequency circuit section that converts the energy of the electron beam into high-frequency energy, a collector section that captures the electron beam, and a beam focusing device that focuses the electron beam. It is the main component.
Ultra-high power microwave tubes handle much more power than ordinary high-power microwave tubes, and the amount of power is several
Ranging from 100kW to several 10Mw (mega watts). In addition to continuous wave operation, such ultra-high power microwave tubes also include pulse operation. Even in the case of pulse operation, the pulse width ranges from several microseconds to several microseconds. Ten
There are cases of short pulses of msec, cases of long pulses whose pulse width is from several seconds to several tens of seconds, and of course cases of pulse widths in between. The present invention relates in particular to collectors for long-pulse operation, straight-beam ultra-high power microwave tubes.

この種のマイクロ波管の従来のコレクタ構造を
第1図に示す。
A conventional collector structure of this type of microwave tube is shown in FIG.

コレクタで発生する膨大な熱量(例えば数メガ
ワツト×数秒)を効率よく外部へ放出するため、
冷却方式としては蒸発冷却方式を採用するのが普
通である。第1図にて、1が電子ビーム入射孔で
あり、2が電子ビームを示す。3はコレクタ・コ
アを示し、これは電子ビームの捕捉を行なうと同
時に真空容器の一部を形成する。コレクタ・コア
3の外側には放射状に形成された放熱体4が多数
設置される。コレクタにおける電力損が数メガ・
ワツトと非常に大きく、かつ長パルス動作の場合
のコレクタの形状は非常に大きくなり(例えば、
直径500mm、高さ1500mm)一体加工が困難となる
ため、コレクタは通常いくつかに分割されて個別
に製作され、あとでそれらを接合(例えばロー
付)して使用される。第1図ではコレクタを軸方
向に4分割した例を示している。更に5はコレク
タの外側に設置されるジヤケツトを示し、コレク
タ・コア3とジヤケツト5の間の空間は蒸留水6
で満たされる。電子ビーム2が入つてくると電子
ビームのもつている運動エネルギがコレクタ・コ
ア3で熱エネルギに変換され、これが放熱体4を
通して水を水蒸気に変え、気化熱として熱を外部
へ放出させるわけである。第1図のコレクタ最外
形部における横断面図を第2図に示す。
In order to efficiently release the huge amount of heat generated in the collector (for example, several megawatts x several seconds) to the outside,
As a cooling method, an evaporative cooling method is normally used. In FIG. 1, 1 is an electron beam entrance hole, and 2 is an electron beam. 3 indicates a collector core, which performs electron beam trapping and forms part of the vacuum vessel. A large number of radially formed heat sinks 4 are installed outside the collector core 3. Power loss in the collector is several megabytes
It is very large, and the shape of the collector becomes very large in the case of long pulse operation (for example,
(diameter: 500 mm, height: 1,500 mm) Since it is difficult to process the collector as a single piece, the collector is usually divided into several pieces, manufactured individually, and then used by joining them together (for example, by brazing). FIG. 1 shows an example in which the collector is divided into four parts in the axial direction. Further, 5 indicates a jacket installed outside the collector, and the space between the collector core 3 and the jacket 5 is filled with distilled water 6.
filled with When the electron beam 2 enters, the kinetic energy of the electron beam is converted into thermal energy by the collector core 3, which converts water into steam through the heat sink 4, and releases the heat to the outside as heat of vaporization. be. A cross-sectional view of the outermost portion of the collector shown in FIG. 1 is shown in FIG.

さて、この種の長パルス動作超大電力マイクロ
波管の従来の構造において、次のような欠点が見
出された。すなわち、比較的少ないビーム印加回
数がくりかえされた後、コレクタ・コア3の接合
部(第1図のaあるいはb部)から真空破れ(リ
ーク)が発生し、マイクロ波管を一瞬のうちに動
作不能にしてしまうのである。
The following drawbacks have been found in the conventional structure of this type of long-pulse operation ultra-high power microwave tube. In other words, after a relatively small number of beam applications are repeated, vacuum breakage (leakage) occurs from the joint between the collector and core 3 (section a or b in Figure 1), causing the microwave tube to operate instantly. It makes it impossible.

発明者らは、こうした事故の原因を調査した結
果、次のことが分つた。すなわち、ビーム印加後
数秒のうちにコレクタ・コア3の内側の温度が
500℃程度にまで達する。一方、コレクタ・コア
3の外側は直接水に接しているからその温度は約
100〜130℃である。この内外の温度差により、コ
レクタ・コア3はコアの内側がそり返るように熱
変形しようとする。この熱変形は、もし放熱体4
の機械的剛性が無視できれば、ほゞビーム入力分
布に応じた形で変形するが、実際には放熱体4の
機械的剛性が大きかつたためこの放熱体4がコレ
クタコアの熱変形に対してリブ(補強体)として
働らき、熱変形の起り得る場所を放熱体4のない
部分に、いいかえればコレクタ・コアの接合部に
集中させてしまう。従来のコレクタにおける熱変
形前後のコレクタ形状の変化を第3図に示す。実
線が熱変形前、点線が熱変形後の形状を示してい
る。熱変形時、接合部(放熱体のない部分)にお
いてコレクタ・コアの外側に引張力、コレクタ・
コアの内側に圧縮力が作用することがわかる。長
パルス動作のマイクロ波管の場合、例えばビーム
印加時間10秒、ビームOFF時間150秒のパルス動
作を行なつているとすると、前記の熱変形が160
秒毎にくり返されることになり、金属が疲労を起
し、ついにはクラツクが発生しそれが進展して最
後には真空破れにつながるわけである。
The inventors investigated the causes of these accidents and found the following. In other words, the temperature inside the collector core 3 increases within a few seconds after the beam is applied.
The temperature reaches around 500℃. On the other hand, since the outside of collector core 3 is in direct contact with water, its temperature is approximately
The temperature is 100-130℃. Due to this temperature difference between the inside and outside, the collector core 3 tends to be thermally deformed so that the inside of the core is warped. This thermal deformation occurs if the heat sink 4
If the mechanical rigidity of the collector core can be ignored, the beam will deform in a manner that roughly corresponds to the beam input distribution, but in reality, the mechanical rigidity of the heat sink 4 is so large that the heat sink 4 has a rib against the thermal deformation of the collector core. It acts as a reinforcement (reinforcing body), and places where thermal deformation can occur are concentrated in areas where there is no heat dissipation body 4, in other words, in the joint between the collector and the core. FIG. 3 shows changes in the collector shape before and after thermal deformation in a conventional collector. The solid line shows the shape before thermal deformation, and the dotted line shows the shape after thermal deformation. During thermal deformation, a tensile force is applied to the outside of the collector core at the joint (the part without a heat sink), and the collector core is
It can be seen that compressive force acts on the inside of the core. In the case of a microwave tube with long pulse operation, for example, if the pulse operation is performed with a beam application time of 10 seconds and a beam OFF time of 150 seconds, the thermal deformation described above will be 160 seconds.
This process is repeated every second, causing fatigue in the metal and eventually causing a crack, which progresses and eventually leads to vacuum failure.

本発明の目的は、前記調査結完に基づき、長パ
ルス動作超大電力マイクロ波管のコレクタとし
て、従来にくらべ格段に耐久性のある構造を有す
るマイクロ波管用コレクタを提供することであ
る。
An object of the present invention is to provide a collector for a microwave tube having a structure that is much more durable than the conventional collector, for use as a collector for a long-pulse operation ultra-high power microwave tube.

それは、放熱体の周方向断面を見た場合、管軸
方向及びそれと直角方向に放熱体を従来以上に細
分化し、以つて放熱体の機械的剛性をコレクタ・
コアのそれに比して著しく弱める方法である。コ
レクタ・コアの表面に放熱体のたち並ぶ様子を従
来の第5図に比して本発明の一実施例を第6図に
示す。第6図においては各放熱体の周方向寸法
(図のa)はコレクタ・コアの厚さ(図のt)に
対して略1/2以下に、またたて寸法(図のb)は
tに対して略2倍以下に設定されるところに特徴
がある。
When looking at the circumferential section of the heat radiator, the heat radiator is divided into smaller parts in the tube axis direction and the direction perpendicular thereto than before, thereby increasing the mechanical rigidity of the heat radiator to the collector.
This method weakens the core significantly compared to that of the core. An embodiment of the present invention is shown in FIG. 6, in comparison with FIG. 5 of the prior art, showing how the heat sinks are lined up on the surface of the collector core. In Figure 6, the circumferential dimension (a in the diagram) of each heat sink is approximately 1/2 or less of the thickness of the collector core (t in the diagram), and the vertical dimension (b in the diagram) is t. The feature is that it is set to approximately twice or less than the actual value.

次に本発明と従来技術との差異について説明す
る。まず、従来の放熱体の設計方針としては主に
放熱特性の確保という点に力点をおいて放熱体の
設計を行なつていたため放熱体の剛性が大きかつ
たが、本発明においては熱応力の緩和という点に
主眼をおいて設計されている点が根本的に異なる
ものである。このため、従来技術では前記t、
a、bの間に何ら規制がない。また、従来技術の
マイクロ波管は出力レベルが数10kw級のものが
殆んどであり、このためコレクタも小形ですみ、
コレクタ・コアは一体加工が可能であつた。この
ためコレクタ・コアの分割化、あるいはそれに伴
なうロー付部のリークといつた問題はほとんど起
つていなかつた。更に長パルス動作の場合には前
述した熱疲労の問題が新らたに発生してくるが、
従来技術ではこうした問題に対し何ら考慮されて
いなかつた。本発明によれば、こうした問題に対
し大きな効果があるコレクタ構造を得ることがで
きる。
Next, differences between the present invention and the prior art will be explained. First, the conventional design policy for heat radiators was to mainly focus on ensuring heat dissipation characteristics, resulting in large rigidity of the heat radiator; however, in the present invention, thermal stress They are fundamentally different in that they are designed with a focus on mitigation. For this reason, in the prior art, the above t,
There are no restrictions between a and b. In addition, most conventional microwave tubes have an output level of several tens of kilowatts, so the collector can also be small.
The collector core could be fabricated as one piece. For this reason, problems such as splitting the collector core or leakage from the brazed portions associated with this have rarely occurred. Furthermore, in the case of long pulse operation, the aforementioned thermal fatigue problem arises.
In the prior art, no consideration was given to these problems. According to the present invention, it is possible to obtain a collector structure that is highly effective in solving these problems.

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

第1図、第2図は従来のコレクタ構造を示す断
面図、第3図は従来コレクタの熱変形の様子を示
す断面図、第4図は本発明によるコレクタ構造を
示す断面図、第5図は従来コレクタの放熱体の外
観図、第6図は本発明による放熱体の外観図を示
す。 1……電子ビーム入射孔、2……電子ビーム、
3……コレクタ・コア、4……放熱体、5……ジ
ヤケツト、6……蒸留水。
1 and 2 are cross-sectional views showing a conventional collector structure, FIG. 3 is a cross-sectional view showing thermal deformation of a conventional collector, FIG. 4 is a cross-sectional view showing a collector structure according to the present invention, and FIG. 5 6 shows an external view of a heat radiating body of a conventional collector, and FIG. 6 shows an external view of a heat radiating body according to the present invention. 1...Electron beam entrance hole, 2...Electron beam,
3... Collector core, 4... Heat sink, 5... Jacket, 6... Distilled water.

Claims (1)

【特許請求の範囲】 1 電子銃部、高周波回路部、コレクタ部、ビー
ム集束装置等で構成された直進ビームマイクロ波
管において、コレクタは蒸発冷却形であり、コレ
クタを構成する部材は複数個に分割されて個別に
製作された後気密接合される構造であり、各コレ
クタ部材の構成は円環状あるいは円錐環状のコレ
クタコアと、その外側に放射状に配置された複数
個の放熱体からなり、前記各放熱体の周方向断面
の管軸方向寸法をb、管軸と直角方向寸法をa、
コレクタコアの厚さをtとした場合、 a1/2t、かつ b2t なる寸法比を有することを特徴とするマイクロ波
管。
[Claims] 1. In a straight beam microwave tube composed of an electron gun section, a high frequency circuit section, a collector section, a beam focusing device, etc., the collector is of an evaporative cooling type, and the collector is composed of a plurality of members. It has a structure that is divided and manufactured individually and then hermetically sealed together, and each collector member consists of an annular or conical annular collector core and a plurality of heat sinks arranged radially outside the collector core. The dimension in the tube axis direction of the circumferential cross section of each heat radiator is b, the dimension in the direction perpendicular to the tube axis is a,
A microwave tube characterized in that it has a dimensional ratio of a1/2t and b2t, where t is the thickness of the collector core.
JP16593883A 1983-09-09 1983-09-09 Microwave tube Granted JPS6059633A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16593883A JPS6059633A (en) 1983-09-09 1983-09-09 Microwave tube

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16593883A JPS6059633A (en) 1983-09-09 1983-09-09 Microwave tube

Publications (2)

Publication Number Publication Date
JPS6059633A JPS6059633A (en) 1985-04-06
JPH0552015B2 true JPH0552015B2 (en) 1993-08-04

Family

ID=15821864

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16593883A Granted JPS6059633A (en) 1983-09-09 1983-09-09 Microwave tube

Country Status (1)

Country Link
JP (1) JPS6059633A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2312323B (en) * 1996-04-20 2000-06-14 Eev Ltd Collector for an electron beam tube

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2458140A1 (en) * 1979-05-31 1980-12-26 Thomson Csf INSULATED COLLECTOR ASSEMBLY FOR POWER TUBES AND TUBE COMPRISING SUCH A COLLECTOR

Also Published As

Publication number Publication date
JPS6059633A (en) 1985-04-06

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