JPH0612991A - Traveling wave tube - Google Patents
Traveling wave tubeInfo
- Publication number
- JPH0612991A JPH0612991A JP17253592A JP17253592A JPH0612991A JP H0612991 A JPH0612991 A JP H0612991A JP 17253592 A JP17253592 A JP 17253592A JP 17253592 A JP17253592 A JP 17253592A JP H0612991 A JPH0612991 A JP H0612991A
- Authority
- JP
- Japan
- Prior art keywords
- magnet
- magnetic field
- traveling wave
- wave tube
- shaped
- 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
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- Microwave Tubes (AREA)
Abstract
(57)【要約】
【目的】この発明は、中心磁界の軸非対称性を補正して
軸対称な磁界を得、電子ビームの透過性を向上した進行
波管を提供することを目的とする。
【構成】この発明の進行波管は、入力導波部4と出力導
波部とに接続された遅波線路の外周に、板状にして中心
に筒状ハブが設けられたポールピース8とリング状スペ
ーサ2とが交互に積み重ねられ、ポールピース間にリン
グ状磁石5が配置された磁界集束装置が設けられてな
り、更に入力導波部又は出力導波部に対応する磁石にU
字状切欠き6が設けられると共に、この磁石に隣接する
ポールピース7,8の対向する各ハブ端面7b,8bは
テーパ状に形成され、且つ両ハブ端面間隔が磁石の切欠
きのある部分が狭くなっており、上記の目的を達成する
ことが出来る。
(57) [Summary] [Object] An object of the present invention is to provide a traveling wave tube in which the axial asymmetry of the central magnetic field is corrected to obtain an axially symmetric magnetic field and the electron beam transparency is improved. A traveling wave tube according to the present invention comprises a pole piece 8 having a plate-like cylindrical hub provided at the center on the outer periphery of a slow wave line connected to an input waveguide section 4 and an output waveguide section. A magnetic field concentrator in which the ring-shaped spacers 2 are alternately stacked and the ring-shaped magnet 5 is arranged between the pole pieces is provided, and the magnet corresponding to the input waveguide part or the output waveguide part is provided with U.
The letter-shaped notch 6 is provided, and the facing hub end surfaces 7b and 8b of the pole pieces 7 and 8 adjacent to the magnet are formed in a tapered shape, and the distance between the hub end surfaces is such that there is a notch in the magnet. It is narrow, and the above-mentioned purpose can be achieved.
Description
【0001】[0001]
【産業上の利用分野】この発明は進行波管に係り、特に
その磁界集束装置の改良に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a traveling wave tube, and more particularly to improvement of a magnetic field focusing device for the traveling wave tube.
【0002】[0002]
【従来の技術】一般に、進行波管は電子ビームと高周波
との相互作用を利用して高周波を増幅するものであり、
電子ビームを発生する電子銃部と、電子ビームと高周波
を相互作用させる遅波回路(高周波作用部)と、この遅
波回路の外周に設けられ磁界を集束させる磁界集束装置
と、相互作用に関与し終った電子ビームを捕捉するコレ
クタ部とからなっている。2. Description of the Related Art Generally, a traveling wave tube amplifies a high frequency by utilizing an interaction between an electron beam and a high frequency.
Participates in interaction with an electron gun unit that generates an electron beam, a slow-wave circuit (high-frequency acting unit) that interacts the electron beam with a high frequency, and a magnetic field focusing device that is provided on the outer periphery of the slow-wave circuit to focus a magnetic field It consists of a collector that captures the finished electron beam.
【0003】このような進行波管では、軸対称の棒状電
子ビームが用いられるので、この電子ビームを集束する
ための磁界も軸対称であることが要求される。従って、
磁界を作る磁界集束装置の磁石およびポールピース(磁
極片)の形状も軸対称とするのが基本である。しかし、
遅波回路の両端付近にはそれぞれ入力導波部と出力導波
部とが突設されているため、軸非対称な部分を有してい
る。その影響を受ける磁石はしばしば切欠きが設けら
れ、軸非対称部分を回避することにより装着されてい
る。この時、従来の進行波管では、軸非対称部分の影響
のない非対称磁石に隣接するポールピースは軸対称構造
のままであった。Since such a traveling wave tube uses an axially symmetric rod-shaped electron beam, the magnetic field for focusing the electron beam is also required to be axially symmetric. Therefore,
Basically, the shapes of the magnet and the pole piece (pole piece) of the magnetic field concentrating device that creates the magnetic field are also axially symmetric. But,
Since the input waveguide portion and the output waveguide portion are provided in the vicinity of both ends of the slow wave circuit, respectively, they have axially asymmetric portions. The affected magnets are often notched and mounted by avoiding axial asymmetry. At this time, in the conventional traveling wave tube, the pole piece adjacent to the asymmetric magnet, which is not affected by the axially asymmetric portion, has the axisymmetric structure.
【0004】[0004]
【発明が解決しようとする課題】ところが、切欠きを設
けることによって磁石は軸非対称となるにも拘らず、そ
の磁石に隣接するポールピースが軸対称のままであるこ
とにより、切欠きを有する磁石の中心磁界が軸非対称と
なり、その結果、軸対称な電子ビームを乱し電子ビーム
透過性の悪化の原因となった。However, although the magnet is axially asymmetric by providing the notch, the pole piece adjacent to the magnet remains axially symmetric, so that the magnet having the notch is provided. The central magnetic field was axially asymmetric, and as a result, the axially symmetric electron beam was disturbed and the electron beam transparency was deteriorated.
【0005】この発明は、上記事情に鑑みなされたもの
で、中心磁界の軸非対称性を補正して軸対称な磁界を
得、電子ビームの透過性を向上した進行波管を提供する
ことを目的とする。The present invention has been made in view of the above circumstances, and an object of the present invention is to provide a traveling wave tube in which the axial asymmetry of the central magnetic field is corrected to obtain an axially symmetric magnetic field and the electron beam transparency is improved. And
【0006】[0006]
【課題を解決するための手段】この発明は、入力導波部
と出力導波部とに接続された遅波線路の外周に、板状に
して中心に筒状ハブが設けられたポールピースとリング
状スペーサとが交互に積み重ねられ、ポールピース間に
リング状磁石が配置された磁界集束装置が設けられてな
り、更に入力導波部又は出力導波部に対応する磁石にU
字状切欠きが設けられると共に、この磁石に隣接するポ
ールピースの対向する各ハブ端面はテーパ状に形成さ
れ、且つ両ハブ端面間隔が磁石の切欠きのある部分が狭
くなっている進行波管である。According to the present invention, there is provided a pole piece in which a cylindrical hub is provided in the center of a plate on the outer circumference of a slow wave line connected to an input waveguide section and an output waveguide section. A magnetic field concentrator in which ring-shaped spacers are alternately stacked and a ring-shaped magnet is arranged between pole pieces is provided, and a U corresponding to the magnet corresponding to the input waveguide section or the output waveguide section.
A traveling wave tube provided with a V-shaped notch, the facing hub end faces of the pole pieces adjacent to the magnet are formed in a tapered shape, and the distance between the hub end faces is narrow in the notched portion of the magnet. Is.
【0007】[0007]
【作用】この発明によれば、磁石の軸非対称形状に起因
する中心磁界の軸非対称性が補正され、ほぼ軸対称的な
磁界分布が提供出来る。その結果、電子ビームの透過性
が向上する。According to the present invention, the axial asymmetry of the central magnetic field due to the axially asymmetrical shape of the magnet is corrected, and a substantially axially symmetrical magnetic field distribution can be provided. As a result, the electron beam transparency is improved.
【0008】[0008]
【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。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described in detail below with reference to the drawings.
【0009】この発明における進行波管の遅波回路およ
び磁界集束装置は図1に示すように構成され、遅波回路
におけるパイプ状真空容器には、金属パイプの代わりに
真直度・伝熱性が優れたIPP(インテグラル・ポール
ピース)構造が用いられている。即ち、板状にして中心
に筒状ハブ1aが貫通したポールピース1とリング状ス
ペーサ2を交互に積み重ねて配置されて真空容器が形成
され、各ポールピース1の間には磁石3が配設され、こ
れらにより磁界集束装置が構成されている。The slow wave circuit of the traveling wave tube and the magnetic field concentrating device according to the present invention are constructed as shown in FIG. 1, and the pipe-shaped vacuum container in the slow wave circuit has excellent straightness and heat transfer property instead of the metal pipe. An IPP (Integral Pole Piece) structure is used. That is, a vacuum container is formed by alternately arranging pole pieces 1 and ring-shaped spacers 2 which are plate-shaped and through which a cylindrical hub 1a penetrates at the center, and a magnet 3 is arranged between the pole pieces 1. The magnetic field focusing device is constituted by these components.
【0010】更に、この実施例では、遅波回路の入力側
に入力導波部として同軸導波管(図示せず)が、又、出
力側に出力導波部として同軸導波管4が突設されてい
る。そして、同軸導波管4に対応する磁石5は図2に示
すように構成され、リング状にして中心孔を含むように
U字状切欠き6が設けられている。この磁石5に隣接す
るポールピース7,8は他のポールピース1と異なり、
板状にして中心に筒状ハブ7a,8aが設けられている
が、図3からも明らかなように、対面する各ハブ端面7
b,8bはテーパ状に形成され、且つ対向する両ハブ端
面間隔が磁石5の切欠き6側が狭くなるように、各ポー
ルピース7,8が配設されている。つまり、狭くなって
いる部分のハブは、それだけ通常のものより突出してい
ることになる。図1から明らかなように、隣り合う通常
のハブ間の寸法をaとすれば、狭くなっている部分のハ
ブ間の寸法bは、a>bの関係にある。ハブ端面7b,
8b間には、長さの短いリング状スペーサ9が配設され
ている。Further, in this embodiment, a coaxial waveguide (not shown) is provided as an input waveguide section on the input side of the slow wave circuit, and a coaxial waveguide 4 is provided as an output waveguide section on the output side. It is set up. The magnet 5 corresponding to the coaxial waveguide 4 is configured as shown in FIG. 2, and is formed into a ring shape and a U-shaped notch 6 is provided so as to include the central hole. The pole pieces 7, 8 adjacent to the magnet 5 are different from the other pole pieces 1,
The hubs 7a and 8a are formed in a plate shape and are provided in the center, but as is apparent from FIG. 3, the hub end surfaces 7 facing each other are formed.
b and 8b are formed in a tapered shape, and the pole pieces 7 and 8 are arranged so that the distance between the opposing end faces of the hubs becomes narrower on the notch 6 side of the magnet 5. In other words, the hub of the narrowed portion is projected more than usual. As is apparent from FIG. 1, when the dimension between adjacent normal hubs is a, the dimension b between the hubs in the narrowed portion has a relationship of a> b. Hub end surface 7b,
A ring-shaped spacer 9 having a short length is arranged between 8b.
【0011】尚、両ポールピース7,8は全く同じ形状
をしているが、使用時にはテーパ状のハブ端面7b,8
bが対向するように配置される。又、出力導波管3に対
応する箇所について述べたが、入力導波部に対応する箇
所についても全く同じ構造になっている。そして、ポー
ルピース1とスペーサ2とからなる真空容器内には、ヘ
リックスからなる遅波線路10が挿入され、図示しない
誘電体支持棒により支持固定されている。 (他の実施例)Although both pole pieces 7 and 8 have exactly the same shape, when they are used, the tapered hub end surfaces 7b and 8 are formed.
b are arranged so as to face each other. Further, although the portion corresponding to the output waveguide 3 has been described, the portion corresponding to the input waveguide portion has the completely same structure. Then, a slow wave line 10 made of a helix is inserted in a vacuum container formed of the pole piece 1 and the spacer 2, and is supported and fixed by a dielectric support rod (not shown). (Other embodiments)
【0012】図4に示す実施例は、空胴結合型進行波管
にこの発明を適用したものである。遅波線路は、多数の
空胴11を構成する多数の空胴隔壁12で構成されてい
る。そして、出力導波部となる矩形導波管4が、磁石5
の切欠き6ところに配置されている。これを両側から挾
むポールピース7,8のハブは、磁石5の切欠き6のと
ころでテーパ状に突出して間隔が狭くなった筒状ハブ7
a,8aを有している。尚、図中の符号13は、コレク
タ(図示せず)に電子ビームを案内する円筒導体を表わ
している。又、この発明は、磁界集束装置がIPP構造
の進行波管ばかりではなく、独立したパイプ状真空容器
を有する進行波管にも適用可能である。The embodiment shown in FIG. 4 is an application of the present invention to a cavity-coupled traveling wave tube. The slow wave line is composed of a large number of cavity partition walls 12 that form a large number of cavities 11. Then, the rectangular waveguide 4 serving as the output waveguide section is replaced by the magnet 5
It is arranged at six notches. The hubs of the pole pieces 7 and 8 sandwiching this from both sides are cylindrical hubs 7 that taperly project at the notches 6 of the magnet 5 and have a narrow gap.
a and 8a. Reference numeral 13 in the drawing represents a cylindrical conductor for guiding the electron beam to a collector (not shown). Further, the present invention can be applied not only to a traveling wave tube having a magnetic field focusing device of an IPP structure, but also to a traveling wave tube having an independent pipe-shaped vacuum container.
【0013】[0013]
【発明の効果】この発明によれば、入力導波部又は出力
導波部とに対応する磁石にU字状切欠きが設けられると
共に、この磁石に隣接するポールピースの対向する各ハ
ブ端面はテーパ状に形成され、且つ両ハブ端面間隔が磁
石の切欠きのある方で狭くなるように配設されているの
で、磁石の軸非対称形状に起因する中心磁界の軸非対称
性が補正され、ほぼ軸対称な磁界分布が提供出来る。そ
の結果、電子ビームの透過性が向上する。According to the present invention, the magnet corresponding to the input waveguide portion or the output waveguide portion is provided with a U-shaped notch, and the facing hub end faces of the pole pieces adjacent to the magnet are provided. Since it is formed in a taper shape and the distance between both hub end surfaces is narrowed in the notch of the magnet, the axial asymmetry of the central magnetic field due to the axial asymmetric shape of the magnet is corrected, and Axisymmetric magnetic field distribution can be provided. As a result, the electron beam transparency is improved.
【図1】この発明の一実施例に係る進行波管の要部を示
す縦断面図。FIG. 1 is a vertical cross-sectional view showing a main part of a traveling wave tube according to an embodiment of the present invention.
【図2】図1のA−A′線に沿って切断した磁石を示す
断面図。FIG. 2 is a cross-sectional view showing a magnet taken along the line AA ′ in FIG.
【図3】この発明の進行波管で用いるポールピースを示
す斜視図。FIG. 3 is a perspective view showing a pole piece used in the traveling wave tube of the present invention.
【図4】この発明の他の実施例の要部を示す縦断面図。FIG. 4 is a vertical cross-sectional view showing the main parts of another embodiment of the present invention.
1…ポールピース、2…スペーサ、3…磁石、4…同軸
導波管,5…磁石,6…切欠き、7,8…ポールピー
ス、7a,8a…ハブ、7b,8b…ハブ端面、9…ス
ペーサ。DESCRIPTION OF SYMBOLS 1 ... Pole piece, 2 ... Spacer, 3 ... Magnet, 4 ... Coaxial waveguide, 5 ... Magnet, 6 ... Notch, 7,8 ... Pole piece, 7a, 8a ... Hub, 7b, 8b ... Hub end surface, 9 …Spacer.
Claims (1)
遅波線路の外周に、板状にして中心に筒状ハブが設けら
れたポールピースとリング状スペーサとが交互に積み重
ねられ、上記ポールピース間にリング状磁石が配置され
た磁界集束装置が設けられてなる進行波管において、 上記入力導波部又は出力導波部に対応する上記磁石にU
字状切欠きが設けられると共に、該磁石に隣接する上記
ポールピースの対向する各ハブ端面はテーパ状に形成さ
れ、且つ両ハブ端面間隔が上記磁石の切欠きのある部分
が狭くなっていることを特徴とする進行波管。1. A pole piece having a plate-shaped cylindrical hub at the center and ring-shaped spacers are alternately stacked on the outer periphery of a slow-wave line connected to an input waveguide and an output waveguide. In the traveling wave tube provided with a magnetic field concentrator in which a ring-shaped magnet is arranged between the pole pieces, a U is added to the magnet corresponding to the input waveguide section or the output waveguide section.
In addition to providing a notch, the facing hub end faces of the pole pieces adjacent to the magnet are formed in a tapered shape, and the distance between the hub end faces is narrow at the notched portion of the magnet. Traveling wave tube characterized by.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17253592A JPH0612991A (en) | 1992-06-30 | 1992-06-30 | Traveling wave tube |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17253592A JPH0612991A (en) | 1992-06-30 | 1992-06-30 | Traveling wave tube |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0612991A true JPH0612991A (en) | 1994-01-21 |
Family
ID=15943706
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP17253592A Pending JPH0612991A (en) | 1992-06-30 | 1992-06-30 | Traveling wave tube |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0612991A (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN112233954A (en) * | 2020-09-01 | 2021-01-15 | 中国电子科技集团公司第十二研究所 | Magnetic steel sheet, magnetic focusing system and traveling wave tube comprising same |
| CN113871277A (en) * | 2021-09-09 | 2021-12-31 | 中国电子科技集团公司第十二研究所 | High-frequency structure |
| CN115692137A (en) * | 2022-09-15 | 2023-02-03 | 中国电子科技集团公司第十二研究所 | Pole shoe and magnetic structure |
-
1992
- 1992-06-30 JP JP17253592A patent/JPH0612991A/en active Pending
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN112233954A (en) * | 2020-09-01 | 2021-01-15 | 中国电子科技集团公司第十二研究所 | Magnetic steel sheet, magnetic focusing system and traveling wave tube comprising same |
| CN113871277A (en) * | 2021-09-09 | 2021-12-31 | 中国电子科技集团公司第十二研究所 | High-frequency structure |
| CN113871277B (en) * | 2021-09-09 | 2024-09-24 | 中国电子科技集团公司第十二研究所 | High-frequency structure |
| CN115692137A (en) * | 2022-09-15 | 2023-02-03 | 中国电子科技集团公司第十二研究所 | Pole shoe and magnetic structure |
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