JPH02168537A - Cyclic magnetic field generating device - Google Patents

Cyclic magnetic field generating device

Info

Publication number
JPH02168537A
JPH02168537A JP32422288A JP32422288A JPH02168537A JP H02168537 A JPH02168537 A JP H02168537A JP 32422288 A JP32422288 A JP 32422288A JP 32422288 A JP32422288 A JP 32422288A JP H02168537 A JPH02168537 A JP H02168537A
Authority
JP
Japan
Prior art keywords
magnetic field
shims
shim
magnet
axial direction
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
Application number
JP32422288A
Other languages
Japanese (ja)
Inventor
Toshiji Tanaka
田中 利二
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP32422288A priority Critical patent/JPH02168537A/en
Publication of JPH02168537A publication Critical patent/JPH02168537A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To easily provide a uniform on-axis mag. field distribution by arranging a plurality of shims having a body in specific shape at a certain spacing in the axial direction, and using permanent magnets in the same shape which allows tight fit in the space between adjoining shims. CONSTITUTION:A plurality of shims 12 are arranged at a certain spacing on one axis with spacers 13 interposed. The body 12A of each shim 12 reduces its thickness in axial direction from the internal end toward the external so as to assume a taper. A plurality of ring-shaped permanent magnets 11 in an identical form are fitted between adjoining shims. The permanent magnets 11 are in close contact with respective shims. Thereby the magnetic resistance to the flux leaking to the outside can be increased compared with the case in which the thickness in the axial direction is uniform, and accordingly the leak mag. field is reduced. This lessens the influence of the leak mag. field upon the on-axis mag. field distribution, which will thus be more uniform.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は主として進行波管の電子ビーム収束に用いら
れる周期磁界発生装置の改良に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] This invention relates primarily to improvements in periodic magnetic field generators used for converging electron beams in traveling wave tubes.

〔従来の技術〕[Conventional technology]

第3図は、例えば実公昭51−49874号公報に記載
された進行波管の周期磁界発生装置の概略断面図である
。同図において、lは環状の永久磁石(第4図に正面図
を示す)、2はシム、3はスペ、−サ、4はシム2とス
ペーサ3からなるエンベロープである。
FIG. 3 is a schematic cross-sectional view of a periodic magnetic field generating device for a traveling wave tube described in, for example, Japanese Utility Model Publication No. 51-49874. In the figure, l is an annular permanent magnet (the front view is shown in FIG. 4), 2 is a shim, 3 is a spacer, and 4 is an envelope consisting of the shim 2 and spacer 3.

この周期磁界発生装置は、軸方向に磁化した永久磁石1
をシム2ではさんで、同極性が互いに相対するように多
数配列し、軸上に周期磁界(第6図に示すような磁界分
布を有する磁界)を発生させるものである。
This periodic magnetic field generator consists of a permanent magnet 1 magnetized in the axial direction.
are arranged between shims 2 so that the same polarity faces each other, and a periodic magnetic field (a magnetic field having a magnetic field distribution as shown in FIG. 6) is generated on the axis.

この周期磁界は、各永久磁石1の大きさ、特性を等しく
しても、その尖頭値は第5図に示すように不揃いになり
、均等な分布を持たせることは難しい、これは、第6図
に示すように、第に番目の永久磁石1kを1個にした場
合に軸上に発生する磁界分布が漏洩磁界5のために、シ
ム2a、2b間にも発生することに起因している。永久
磁石lを多数組合わせた場合、この漏洩磁界が相互に影
響し合って、その総合されたものが軸上磁界分布となる
が、装置の端の方になると、近隣の永久磁石1の数が限
らてくるために、漏洩磁界を総合した大きさが、場所に
よって異なり、不揃いが生じるためである。この磁界分
布の不揃いがあると、電子ビームの一部が、エンベロー
プ4内に同軸に収納して絶縁支持される遅波回路構体(
ヘリックス、図示しない)中を進行する際に、咳へワッ
クスに衝突する。この衝突があると、ヘリックスが温度
上昇し、ガスが発生し、進行波管装置の電気的特性に悪
影響を与える。
Even if the size and characteristics of each permanent magnet 1 are equal, the periodic magnetic field will have uneven peak values as shown in Figure 5, and it is difficult to have an even distribution. As shown in Fig. 6, the magnetic field distribution generated on the axis when only one permanent magnet 1k is used is also generated between the shims 2a and 2b due to the leakage magnetic field 5. There is. When a large number of permanent magnets 1 are combined, the leakage magnetic fields influence each other, and the total becomes the axial magnetic field distribution, but towards the end of the device, the number of neighboring permanent magnets 1 This is because the total magnitude of the leakage magnetic field varies from place to place, causing inconsistency. When this magnetic field distribution is uneven, a part of the electron beam is housed coaxially within the envelope 4 and is insulated and supported by the slow wave circuit structure (
As it progresses through the helix (not shown), it collides with the wax. This collision increases the temperature of the helix and generates gas, which adversely affects the electrical properties of the traveling wave tube device.

〔発明が解決しようする課題〕[Problem to be solved by the invention]

上記電子ビームの衝突を防止するため、従来は、進行波
管装置のエンベロープ上の永久磁石1やシムの外周に鉄
片を取り付ける等して、電子ビームの上記衝突が発生し
ないように、磁界分布を調節するようにしているが、こ
の鉄片の取り付は等による調整は進行波管毎に異なるた
め、面倒で手間・時間がかかるという問題があった。
In order to prevent the above-mentioned collision of the electron beam, conventionally, iron pieces were attached to the outer periphery of the permanent magnet 1 and shims on the envelope of the traveling wave tube device, and the magnetic field distribution was adjusted to prevent the above-mentioned collision of the electron beam from occurring. However, since the installation of this iron piece is different for each traveling wave tube, it is troublesome and takes time and effort.

この発明は上記問題を解消するためになされたもので、
従来に比し、均一な軸上磁界分布を容易に得ることがで
きる周期磁界装置を提供することを目的とする。
This invention was made to solve the above problem.
It is an object of the present invention to provide a periodic magnetic field device that can easily obtain a uniform axial magnetic field distribution compared to the prior art.

〔課題を解決するための手段〕[Means to solve the problem]

この発明は上記目的を達成するため、請求項1の発明で
は、エンベロープのシムに、その外周部で軸方向厚さが
狭くなるテーパ形状を持たせ、上記磁石のシム側面を上
記テーパ形状に沿う形状とし、請求項2の発明では、磁
石を、複数個の同一形状の磁石片の組合せ体としたもの
である。
In order to achieve the above-mentioned object, in the invention of claim 1, the shim of the envelope has a tapered shape in which the thickness in the axial direction becomes narrower at the outer peripheral part, and the side surface of the shim of the magnet is aligned with the tapered shape. According to the second aspect of the invention, the magnet is a combination of a plurality of magnet pieces having the same shape.

〔作用〕[Effect]

請求項1の発明では、シムの外周部の軸方向厚さを小さ
くしたので、外部へ漏洩する磁束に対する磁気抵抗が大
きくなり、漏洩磁界の影響が従来に比して大幅に低減さ
れる。また、請求項2の発明では、進行波管装置に取り
つける前に、軸上均一[界分布が得られるように、選択
した磁石片で環状磁石を組んでおけるてので、上記取り
つけ後の調整は不要となり、調整作業は簡単となる。
In the first aspect of the invention, since the axial thickness of the outer circumferential portion of the shim is reduced, the magnetic resistance to the magnetic flux leaking to the outside is increased, and the influence of the leaked magnetic field is significantly reduced compared to the prior art. Furthermore, in the invention of claim 2, the annular magnet can be assembled with selected magnet pieces to obtain a uniform field distribution on the axis before being attached to the traveling wave tube device, so that the adjustment after the above-mentioned attachment is possible. This becomes unnecessary and the adjustment work becomes easy.

〔実施例〕〔Example〕

以下、この発明の一実施例を図面を参照して説明する。 An embodiment of the present invention will be described below with reference to the drawings.

第1図において、1)は軸方向に磁化された環状の永久
磁石、12はシム、12Aはシム本体部12Bはシムの
基部、13はスペーサ、14はエンベロープである。こ
のエンベロープ14!:[数個のシム12を、スペーサ
13で挟んで順次同軸に接続してなり、外周から軸方向
所定間隔を隔ててシム本体部12が突出して並ぶ形状と
なっている。このシム本体部12Aは基部側から外周端
部へ向かう伴い軸方向の板厚が小さくなるテーパ形状を
有し、相隣るシム本体部12Aは、内周側の軸方向長さ
が外周側の軸方向長さより小さい台形状の環状空間Gを
区画している。環状の永久磁石1)はこの環状空間Gに
密に嵌合する形状を有し、同極性側が互いに対向するよ
うに配列されている。
In FIG. 1, 1) is an annular permanent magnet magnetized in the axial direction, 12 is a shim, 12A is a shim main body 12B is a base of the shim, 13 is a spacer, and 14 is an envelope. This envelope 14! : [Several shims 12 are sandwiched between spacers 13 and sequentially connected coaxially, and the shim body portions 12 are arranged in a protruding manner at a predetermined distance in the axial direction from the outer periphery. The shim main body 12A has a tapered shape in which the thickness in the axial direction decreases as it goes from the base side to the outer peripheral end. A trapezoidal annular space G smaller than the axial length is defined. The annular permanent magnets 1) have a shape that tightly fits into this annular space G, and are arranged so that the same polarity sides face each other.

この構成においては、シム本体部12Aの外端部の厚が
基部側に対して小さくなっているので、外部へ漏洩する
磁束に対する磁気抵抗は、軸方向厚が均一である従来の
場合に比して高めることができ、その分、漏洩磁界を低
減することができる。
In this configuration, since the thickness of the outer end of the shim main body 12A is smaller than that of the base, the magnetic resistance against the magnetic flux leaking to the outside is lower than in the conventional case where the thickness in the axial direction is uniform. The leakage magnetic field can be reduced accordingly.

従って、軸上磁界分布に与える漏洩磁界の影響が少なく
なり、従来に比し、軸上磁界分布を均一にすることがで
きる。
Therefore, the influence of the leakage magnetic field on the axial magnetic field distribution is reduced, and the axial magnetic field distribution can be made more uniform than in the past.

なお、上記実施例では、シム本体部12Aにテパ形状を
持たせているが、シム本体部12Aは、その基部側の軸
方向厚に対して外端部の厚さが小く、軸方向厚さ中心に
対して対称な形状を有していればよい。
In the above embodiment, the shim main body 12A has a tapered shape, but the shim main body 12A has a smaller thickness at the outer end than the axial thickness on the base side. It is sufficient if the shape is symmetrical with respect to the center.

第2図はこの発明の他の実施例を示したもので、環状の
永久磁石1として、複数個の形状の等しい磁石片IAを
組合せたもの使用する。磁石片IAとしては、磁力の異
なるものを多種類用意しておく。
FIG. 2 shows another embodiment of the present invention, in which a combination of a plurality of magnet pieces IA of the same shape is used as the annular permanent magnet 1. Many types of magnet pieces IA with different magnetic forces are prepared.

この発明を実施する場合、永久磁石l相互間にシムを介
在して、エンベロープに装着し、軸上磁界を磁界測定器
で測定しつつ、軸上磁界分布が所望の均一度になるよう
に、個々の磁石片IAを取り替え調整し、調整終了後に
、進行波管装置の工ンベロープに装着しなおすようにす
る。
When carrying out this invention, permanent magnets are installed in an envelope with shims interposed between them, and the axial magnetic field is measured with a magnetic field measuring device, so that the axial magnetic field distribution has a desired degree of uniformity. Each magnet piece IA is replaced and adjusted, and after the adjustment is completed, it is reattached to the envelope of the traveling wave tube device.

このようにすれば、進行波管装置に装着したのちは、調
整不要もしくは微調整で済むので、調整の手間と時間を
軽減することかできる。
In this way, after it is attached to the traveling wave tube device, there is no need for adjustment or only fine adjustment is required, so that the effort and time required for adjustment can be reduced.

〔発明の効果〕〔Effect of the invention〕

この発明は以上説明した通り、磁石を磁石片で形成する
ものは、進行波管装置へ装着後は実質上調整が要らなく
なるので、従来に比し、軸上磁界分布を均一にするため
の調整の手間と時間を減らすことができ、シムの外端部
の厚さを小さしたものでは、漏洩磁界の影響を低減する
ことができるので、均一な軸上磁界分布を得やすく、調
整を必要としても微調整で済む。
As explained above, in this invention, since the magnet formed by the magnet piece does not require substantially any adjustment after being attached to the traveling wave tube device, it is possible to make the adjustment to make the axial magnetic field distribution uniform compared to the conventional one. By reducing the thickness of the outer end of the shim, it is possible to reduce the influence of leakage magnetic field, making it easier to obtain a uniform axial magnetic field distribution and eliminating the need for adjustment. All it takes is a little adjustment.

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

第1図はこの発明の実施例を示す断面図、第2図は他の
発明の実施例の要部を示す正面図、第3図は従来の装置
を示す断面図、第4図は上記従来装置における環状磁石
の正面図、第5図は上記従来装置における軸上磁界分布
を示す図、第6図は上記従来装置における漏洩磁束を示
す図である。 図において、1ll−環状の磁石、12−・シム、12
A〜・−シム本体部、13−・−スペーサ、14・・−
エンベロープ。 なお、図中、同一符号は同一または相当部分を示す。
Fig. 1 is a sectional view showing an embodiment of the present invention, Fig. 2 is a front view showing the main parts of an embodiment of another invention, Fig. 3 is a sectional view showing a conventional device, and Fig. 4 is a sectional view showing the above-mentioned conventional device. FIG. 5 is a front view of the annular magnet in the device, FIG. 5 is a diagram showing the axial magnetic field distribution in the conventional device, and FIG. 6 is a diagram showing the leakage magnetic flux in the conventional device. In the figure, 1ll-ring magnet, 12- shim, 12
A~・-Shim body, 13-・-Spacer, 14・・-
envelope. In addition, in the figures, the same reference numerals indicate the same or corresponding parts.

Claims (2)

【特許請求の範囲】[Claims] (1)エンベロープの外周から軸方向所定間隔を隔てて
半径方向に突出形成されたシム相互間の各々に環状の磁
石を装着してなる周期磁界発生装置において、上記シム
が、その外端部の軸方向厚さが基部軸方向厚さに比し小
さく形成された形状を有し、上記磁石のシム側面が上記
形状に沿う形状を有していることを特徴とする周期磁界
発生装置。
(1) In a periodic magnetic field generating device in which an annular magnet is attached to each of the shims protruding in the radial direction at a predetermined axial distance from the outer circumference of the envelope, the shims are located at the outer end of the shim. A periodic magnetic field generator characterized in that the magnet has a shape in which the axial thickness is smaller than the axial thickness of the base, and a shim side surface of the magnet has a shape that follows the shape.
(2)エンベロープの外周から軸方向所定間隔を隔てて
突出形成されたシム相互間の各々に環状の磁石を装着し
てなる周期磁界発生装置において、上記磁石は同一形状
の複数個の磁石片の組合せ体からなることを特徴とする
周期磁界発生装置。
(2) In a periodic magnetic field generator in which annular magnets are attached to each of the shims protruding from the outer periphery of the envelope at a predetermined distance in the axial direction, the magnets are made of a plurality of magnet pieces of the same shape. A periodic magnetic field generator characterized by comprising a combination body.
JP32422288A 1988-12-21 1988-12-21 Cyclic magnetic field generating device Pending JPH02168537A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP32422288A JPH02168537A (en) 1988-12-21 1988-12-21 Cyclic magnetic field generating device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP32422288A JPH02168537A (en) 1988-12-21 1988-12-21 Cyclic magnetic field generating device

Publications (1)

Publication Number Publication Date
JPH02168537A true JPH02168537A (en) 1990-06-28

Family

ID=18163405

Family Applications (1)

Application Number Title Priority Date Filing Date
JP32422288A Pending JPH02168537A (en) 1988-12-21 1988-12-21 Cyclic magnetic field generating device

Country Status (1)

Country Link
JP (1) JPH02168537A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5534750A (en) * 1992-05-13 1996-07-09 Litton Systems, Inc. Integral polepiece magnetic focusing system having enhanced gain and transmission

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5534750A (en) * 1992-05-13 1996-07-09 Litton Systems, Inc. Integral polepiece magnetic focusing system having enhanced gain and transmission

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