JPH02132736A - Large power klystron - Google Patents
Large power klystronInfo
- Publication number
- JPH02132736A JPH02132736A JP28697188A JP28697188A JPH02132736A JP H02132736 A JPH02132736 A JP H02132736A JP 28697188 A JP28697188 A JP 28697188A JP 28697188 A JP28697188 A JP 28697188A JP H02132736 A JPH02132736 A JP H02132736A
- Authority
- JP
- Japan
- Prior art keywords
- output
- waveguide
- cavity
- cavities
- klystron
- 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
Links
- 230000008878 coupling Effects 0.000 claims description 16
- 238000010168 coupling process Methods 0.000 claims description 16
- 238000005859 coupling reaction Methods 0.000 claims description 16
- 238000010894 electron beam technology Methods 0.000 claims description 6
- 208000028659 discharge Diseases 0.000 description 8
- 230000005684 electric field Effects 0.000 description 8
- 230000000694 effects Effects 0.000 description 1
- 230000010355 oscillation Effects 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 238000011144 upstream manufacturing Methods 0.000 description 1
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Abstract
Description
【発明の詳細な説明】
[発明の目的]
(産業上の利用分野)
この発明はビーム直進型大電力クライストロンに係り、
特にその出力空胴及び出力導波管の改良に関する。[Detailed description of the invention] [Object of the invention] (Industrial application field) This invention relates to a beam straight-travel type high-power klystron,
In particular, it relates to improvements in its output cavity and output waveguide.
(従来の技術)
一般にビーム直進型大電力クライストロンは、第2図に
示すように、電子銃1と、入力空胴2、複数の中間空胴
3、出力空胴4をドリフト管5で連結した電子作用部6
と、コレクタ7と、入力導波管8と、出力導波管9とで
構成されている。(Prior Art) In general, a beam straight-travel type high-power klystron, as shown in FIG. Electronic action part 6
, a collector 7 , an input waveguide 8 , and an output waveguide 9 .
動作時には、電子銃1で発射した電子ビームを入力導波
管8から入力空胴2に導入された入力信号で速度変調し
、中間空胴3及びドリフト管5で徐々に密度変調に変え
、その密度変調された電子ビームが出力空胴4の間隙を
通過することにより、出力空胴4から増幅されたマイク
ロ波を得、出力導波管9から取出している。この際、用
済みとなった電子ビームはコレクタ7に捕捉される。During operation, the electron beam emitted by the electron gun 1 is velocity-modulated by an input signal introduced into the input cavity 2 from the input waveguide 8, and is gradually changed to density modulation by the intermediate cavity 3 and the drift tube 5. By passing the density-modulated electron beam through the gap in the output cavity 4, amplified microwaves are obtained from the output cavity 4 and extracted from the output waveguide 9. At this time, the used electron beam is captured by the collector 7.
ところで、従来の出力空胴及び出力導波管は、第3図(
a)、(b)に示すように構成され、1つの出力空胴4
にその外部結合用孔10を覆うように出力導波管9が結
合されている。尚、11は出力窓である。By the way, the conventional output cavity and output waveguide are shown in Fig. 3 (
Constructed as shown in a) and (b), one output cavity 4
An output waveguide 9 is coupled to cover the external coupling hole 10 . Note that 11 is an output window.
又、別の従来例では、第4図(a)、(b)に示すよう
に、2つの空胴12A,12Bからなる出力空胴12の
うちの1つに出力導波管9が結合されている。尚、13
は両空胴12A,12Bを結合する結合孔である。In another conventional example, as shown in FIGS. 4(a) and 4(b), an output waveguide 9 is coupled to one of the output cavities 12 consisting of two cavities 12A and 12B. ing. In addition, 13
is a coupling hole that couples both cavities 12A and 12B.
(発明が解決しようとする問題点)
第3図(a)、(b)の従来例では、大出力マイクロ波
を得ようとすると、出力空胴4の間隙に大きな電界が生
ずる。これが放電に至るところから、1つのクライスト
ロンから得られる出力値が制限される。(Problems to be Solved by the Invention) In the conventional example shown in FIGS. 3(a) and 3(b), a large electric field is generated in the gap between the output cavities 4 when attempting to obtain a high output microwave. Since this leads to discharge, the output value that can be obtained from one klystron is limited.
又、第4図(a)、(b)の従来例では、互いに結合さ
れた2つの空胴12A,12Bからなる出力空胴12を
もつクライストロンは、1つの空胴の間隙に発生する電
界は、その空胴に電子ビームから与えられるマイクロ波
電力の平方根に略比例すると考えられる。従って、2つ
の空胴12A112Bを備えれば、各空胴12A,12
Bの間隙に発生する電界は放電の危険のない値に抑えた
まま、大電力マイクロ波を得ることが出来るとの考えに
立っている。In addition, in the conventional example shown in FIGS. 4(a) and 4(b), the klystron has an output cavity 12 consisting of two cavities 12A and 12B coupled to each other, and the electric field generated in the gap between one cavity is , is considered to be approximately proportional to the square root of the microwave power applied to the cavity from the electron beam. Therefore, if two cavities 12A and 112B are provided, each cavity 12A, 12
The idea is that high-power microwaves can be obtained while the electric field generated in the gap B is suppressed to a value that poses no risk of discharge.
しかしながら、発生したマイクロ波は、外部結合用孔1
0を介して1つの出力導波管9に結合されており、出力
導波管9が結合されている空胴12Aでは、大きなマイ
クロ波電力が集中する。However, the generated microwaves are transmitted through the external coupling hole 1.
In the cavity 12A to which the output waveguide 9 is coupled, a large microwave power is concentrated.
このため、この方式のクライストロンでは、必ずしも大
電力で安定な動作は期待出来ない。又、相互に結合して
いるため、或る周波数や電子ビームの速度によっては、
発振などの不安定な状態を生ずる。For this reason, this type of klystron cannot necessarily be expected to operate stably with high power. Also, because they are mutually coupled, depending on a certain frequency or speed of the electron beam,
This causes unstable conditions such as oscillation.
この発明は、上記事情に鑑みなされたもので、複数個の
縦列空胴からなる出力空胴の各々の間隙における電界強
度を放電の危険のない値に抑制しつつ、安定な大電力マ
イクロ波の出力を可能とする大電力クライストロンを提
供することを目的とする。This invention was made in view of the above circumstances, and allows stable high-power microwave generation while suppressing the electric field strength in each gap between output cavities consisting of a plurality of columns of cavities to a value that does not pose the risk of electrical discharge. The purpose is to provide a high-power klystron that enables output.
[発明の構成コ
(問題点を解決するための手段)
この発明は、出力空胴がそれぞれ外部結合用孔をもつ複
数個縦列の空胴で構成され、且つ出力導波管は複数個縦
列の空胴の各結合用孔を一括して覆うように結合された
ビーム流れ方向に長い導波管であって、外方に行くに従
って徐々に短小化されて出力端とされてなる大電力クラ
イストロンである。[Structure of the Invention (Means for Solving the Problems)] This invention is characterized in that the output cavity is composed of a plurality of columns of cavities each having an external coupling hole, and the output waveguide is composed of a plurality of columns of cavities each having an external coupling hole. A high-power klystron is a waveguide that is long in the beam flow direction and is connected so as to collectively cover each coupling hole in the cavity, and is gradually shortened as it goes outward to serve as the output end. be.
(作用)
この発明によれば、出力空胴を構成する各空胴の間隙に
おける電界強度が放電の危険のない値に抑制しながら総
合的に大電力マイクロ波を安定に導出することが出来る
。(Operation) According to the present invention, it is possible to stably derive a high-power microwave as a whole while suppressing the electric field strength in the gaps between the cavities constituting the output cavity to a value that does not pose a risk of discharge.
(実施例)
以下、図面を参照して、この発明の一実施例を詳細に説
明する。(Example) Hereinafter, an example of the present invention will be described in detail with reference to the drawings.
この発明による大電力クライストロンの出力空胴付近は
、第1図(a) 、(b)に示すように構成され、(a
)は縦断面図、(b)は横断面図である。The vicinity of the output cavity of the high-power klystron according to the present invention is configured as shown in FIGS. 1(a) and (b), and (a)
) is a longitudinal cross-sectional view, and (b) is a cross-sectional view.
即ち、従来例(第3図)と同一箇所は同一符号を付すと
、出力空胴14はそれぞれ外部結合用孔10をもつ2個
縦列の空胴14A、14Bからなっており、外部結合用
孔10の周縁部10aは、各空胴14A、14Bに適切
な外部Q値を与える絞りとなっている。又、(a)図の
15は、各空胴14A,14Bで発生するマイクロ波電
力を外部へ導く結合部である。That is, the same parts as in the conventional example (Fig. 3) are given the same reference numerals, and the output cavity 14 consists of two columns of cavities 14A and 14B each having an external coupling hole 10. The peripheral edge portion 10a of 10 serves as an aperture that provides an appropriate external Q value to each cavity 14A, 14B. Further, 15 in the figure (a) is a coupling portion that guides the microwave power generated in each cavity 14A, 14B to the outside.
このような出力空胴14の両外部結合用孔1oを覆うよ
うに、出力導波管16が結合されている。The output waveguide 16 is coupled so as to cover both external coupling holes 1o of the output cavity 14.
この出力導波管16はビーム流れ方向に長い矩形導波管
にして、その長さは出力空胴14のビーム上流側からビ
ーム下流側までの長さに略等しい。The output waveguide 16 is a rectangular waveguide long in the beam flow direction, and its length is approximately equal to the length from the beam upstream side to the beam downstream side of the output cavity 14.
又、この出力導波管16は、(a)図から明らかなよう
に外方に行くに従って徐々に短小化されて出力端とされ
ている。この場合、出力空胴14より遠ざかるにつれて
、少なくともクライストロン動作波長よりも長い距離に
わたって徐々に且つ滑らかな境界(テーバ部16a)に
よって短くなり、標準的な導波管に接続される。即ち、
このテーパ部16aで標準導波管への整合をとっており
、先端近くには出力窓11が設けられている。この出力
窓11の位置は限定されるものではなく、例えば結合部
15に空胴の数だけ設けても良い。Further, as is clear from the figure (a), the output waveguide 16 is gradually shortened toward the outside to form the output end. In this case, away from the output cavity 14, it is gradually shortened by a smooth boundary (Taber section 16a) over a distance at least longer than the klystron operating wavelength and connected to a standard waveguide. That is,
The tapered portion 16a matches the standard waveguide, and an output window 11 is provided near the tip. The position of this output window 11 is not limited, and for example, the number of output windows 11 may be provided in the coupling portion 15 as many as the number of cavities.
更に、この出力導波管16は、標準的な導波管よりも電
界方向の高さが大きくなっている。Additionally, the output waveguide 16 has a greater height in the electric field direction than a standard waveguide.
尚、この発明の大電力クライストロンは、上記以外は第
2図及び第3図と同様構成ゆえ、詳細な説明は省略する
。Note that the high-power klystron of the present invention has the same configuration as that shown in FIGS. 2 and 3 except for the above, and therefore detailed explanation will be omitted.
さて、出力電力をPoとし、出力空胴を構成するN個の
空胴より均一に出力電力が得られるとすれば、各空胴間
隙に発生する高周波電圧はP o / Nとなる。Nを
増すことによって、高周波電圧を下げ、放電を抑制する
ことが出来る。Now, assuming that the output power is Po, and that the output power is uniformly obtained from the N cavities forming the output cavity, the high frequency voltage generated in each cavity gap is P o /N. By increasing N, the high frequency voltage can be lowered and discharge can be suppressed.
又、出力電力は管軸と略直角方向へ各々の空胴より平等
に取出されており、一部の空胴への電力集中による放電
が発生しない。Further, the output power is taken out equally from each cavity in a direction substantially perpendicular to the tube axis, so that no discharge occurs due to concentration of power in some cavities.
更に、出力電力は徐々に且つ滑らかな境界(テーバ部1
6a)によって取出されるため、反射を生じることなく
、従って安定である。Furthermore, the output power gradually and smoothly increases (Taber part 1
6a), it does not cause reflections and is therefore stable.
又、必ずしも標準導波管を用いる必要のない場合は、テ
ーパ部16aを設ける必要がなく、テーバ部16aを用
いず、電界方向の高さが高い導波管により直接導出すれ
ば、導波管内での放電も抑止出来る。In addition, if it is not necessary to use a standard waveguide, there is no need to provide the tapered part 16a, and if the waveguide is directly guided with a high height in the electric field direction without using the tapered part 16a, the inside of the waveguide can be discharge can also be suppressed.
上記実施例では、出力空胴として2個縦列配置されたも
のであるが、これに限らず、3個、4個等、複数個の空
胴で構成し、各空胴の結合用孔を一括して覆うように出
力導波管を設ければ良い。In the above embodiment, two output cavities are arranged in tandem, but the configuration is not limited to this, and a plurality of cavities such as three or four cavities may be arranged, and the coupling holes of each cavity may be connected at once. What is necessary is to provide an output waveguide so as to cover it.
[発明の効果]
この発明によれば、出力空胴はそれぞれ外部結合用孔を
もつ複数個縦列の空胴て構成され、且つ出力導波管はこ
れら空胴の各結合用孔を一括して覆うように結合された
ビーム流れ方向に長い導波管にして、外方に行くに従っ
て徐々に短小化されているので、出力空胴を構成する冬
空胴の間隙における電界強度を放電の危険のない値に抑
制しながら、総合的に大電力マイクロ波を安定に導出す
ることが出来る。[Effects of the Invention] According to the present invention, the output cavity is composed of a plurality of columns of cavities each having an external coupling hole, and the output waveguide collectively connects each coupling hole of these cavities. The waveguide is long in the beam flow direction and is gradually shortened as it goes outward, so that the electric field strength in the gap between the winter cavities that make up the output cavity can be reduced without the risk of discharge. It is possible to stably derive high-power microwaves overall while suppressing the value to a certain value.
第1図(a)、(b)はこの発明の一実施例に係る大電
力クライストロンの要部(出力空胴付近)を示す縦断面
図と横断面図、第2図は一般的な大電力クライストロン
の全体を示す概略断面図、第3図(a)、(b)は従来
の大電力クライストロンの要部(出力空胴付近)を示す
縦断面図と横断面図、第4図(a)、(b)は別の従来
の大電力クライストロンの要部(出力空胴付近)を示す
縦断面図と横断面図である。
1・・・電子銃、2・・・入力空胴、3・・・中間空胴
、5・・・ドリフト管、7・・・コレクタ電極、10・
・・外部外部結合用孔、14・・・出力空胴、14A、
14B・・・空胴、16・・・出力導波管。
第2図FIGS. 1(a) and (b) are longitudinal and cross-sectional views showing the main parts (near the output cavity) of a high-power klystron according to an embodiment of the present invention, and FIG. 2 is a general high-power klystron. A schematic cross-sectional view showing the entire klystron, FIGS. 3(a) and (b) are a vertical cross-sectional view and a cross-sectional view showing the main part (near the output cavity) of a conventional high-power klystron, and FIG. 4(a) , (b) are a vertical cross-sectional view and a cross-sectional view showing the main part (near the output cavity) of another conventional high-power klystron. DESCRIPTION OF SYMBOLS 1... Electron gun, 2... Input cavity, 3... Intermediate cavity, 5... Drift tube, 7... Collector electrode, 10...
... External external coupling hole, 14... Output cavity, 14A,
14B...Cavity, 16...Output waveguide. Figure 2
Claims (1)
空胴、出力空胴及びコレクタ電極が縦列配置され、上記
出力空胴に出力導波管が結合されてなる大電力クライス
トロンにおいて、 上記出力空胴はそれぞれ外部結合用孔をもつ複数個縦列
の空胴で構成され、且つ上記出力導波管は上記複数個縦
列の空胴の各結合用孔を一括して覆うように結合された
ビーム流れ方向に長い導波管であって、外方に行くに従
って徐々に短小化されて出力端とされてなることを特徴
とする大電力クライストロン。[Claims] An input cavity, a plurality of intermediate cavities, an output cavity, and a collector electrode are arranged in series along an electron beam path from an electron gun, and an output waveguide is coupled to the output cavity. In a high power klystron, the output cavity is composed of a plurality of columns of cavities each having an external coupling hole, and the output waveguide collectively connects each coupling hole of the plurality of columns of cavities. A high-power klystron characterized by a waveguide that is long in the direction of beam flow and coupled in a covering manner, and gradually becomes shorter and smaller as it goes outward to form an output end.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP28697188A JPH02132736A (en) | 1988-11-14 | 1988-11-14 | Large power klystron |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP28697188A JPH02132736A (en) | 1988-11-14 | 1988-11-14 | Large power klystron |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH02132736A true JPH02132736A (en) | 1990-05-22 |
Family
ID=17711329
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP28697188A Pending JPH02132736A (en) | 1988-11-14 | 1988-11-14 | Large power klystron |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH02132736A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6180136B1 (en) | 1998-11-10 | 2001-01-30 | Idexx Laboratories, Inc. | Phospholipid-coated microcrystals for the sustained release of pharmacologically active compounds and methods of their manufacture and use |
JP2012526360A (en) * | 2009-05-05 | 2012-10-25 | バリアン・メディカル・システムズ・インコーポレイテッド | Multiple output cavities in sheet beam klystrons. |
CN108648979A (en) * | 2018-05-21 | 2018-10-12 | 中国工程物理研究院应用电子学研究所 | Four cavity high power microwave amplifiers of one kind and its application method |
-
1988
- 1988-11-14 JP JP28697188A patent/JPH02132736A/en active Pending
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6180136B1 (en) | 1998-11-10 | 2001-01-30 | Idexx Laboratories, Inc. | Phospholipid-coated microcrystals for the sustained release of pharmacologically active compounds and methods of their manufacture and use |
US6423338B1 (en) | 1998-11-10 | 2002-07-23 | Idexx Pharmaceuticals, Inc. | Phospholipid-coated microcrystals for the sustained release of pharmacologically active compounds and methods of their manufacture and use |
JP2012526360A (en) * | 2009-05-05 | 2012-10-25 | バリアン・メディカル・システムズ・インコーポレイテッド | Multiple output cavities in sheet beam klystrons. |
CN108648979A (en) * | 2018-05-21 | 2018-10-12 | 中国工程物理研究院应用电子学研究所 | Four cavity high power microwave amplifiers of one kind and its application method |
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