JPS59114729A - Permanent magnet device - Google Patents

Permanent magnet device

Info

Publication number
JPS59114729A
JPS59114729A JP22516282A JP22516282A JPS59114729A JP S59114729 A JPS59114729 A JP S59114729A JP 22516282 A JP22516282 A JP 22516282A JP 22516282 A JP22516282 A JP 22516282A JP S59114729 A JPS59114729 A JP S59114729A
Authority
JP
Japan
Prior art keywords
pole piece
magnet
magnets
permanent magnet
magnetic field
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
JP22516282A
Other languages
Japanese (ja)
Inventor
Hisaaki Sato
佐藤 久明
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
NEC Corp
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 NEC Corp, Nippon Electric Co Ltd filed Critical NEC Corp
Priority to JP22516282A priority Critical patent/JPS59114729A/en
Publication of JPS59114729A publication Critical patent/JPS59114729A/en
Pending 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
    • H01J23/10Magnet systems for directing or deflecting the discharge along a desired path, e.g. a spiral path

Abstract

PURPOSE:To reduce unwanted leakage magnetic field and realize reduction in size of magnet by cutting the upper and lower pole piece magnets like a through groove from the surface in the opposite side of the center gap to the magnetizing direction of said magnets. CONSTITUTION:A large groove is provided in the direction at a right angle to the center axis of magnetizing direction of magnet so that the surface not bonded to magnets in the upper pole piece 1 and lower pole piece 2 is almost removed. With such a structure, various kinds of leakage magnetic fields can be fantastically reduced and a magnet can be reduced in size.

Description

【発明の詳細な説明】 本発明は、一様磁界集束形の大電力クライストロンに使
用される永久磁石装置の構造に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to the structure of a permanent magnet device used in a uniform magnetic field focusing type high power klystron.

周知のように大電力クライストロンは電子ビームを発生
させる電子銃部、電子ビームに速度変調及び密度変調を
与え高周波増幅を行なう高周波回路部(キャビティ部)
、電子ビームを捕集するコレクタ部、及び電子ビームを
所定の形状に集束させるビーム集束装置等から構成され
る。このうち、ビーム集束装置としては電磁石を用いた
ものと永久磁石を用いたものがあるが、最近はクライス
トロンの綜合効率の向上、あるいは保守の簡便化の点か
ら、後者の方が主に用いられる傾向にある。
As is well known, a high-power klystron consists of an electron gun section that generates an electron beam, and a high-frequency circuit section (cavity section) that applies velocity modulation and density modulation to the electron beam and performs high-frequency amplification.
, a collector section that collects the electron beam, and a beam focusing device that focuses the electron beam into a predetermined shape. Among these beam focusing devices, there are those that use electromagnets and those that use permanent magnets, but recently the latter has been mainly used in order to improve the overall efficiency of klystrons and simplify maintenance. There is a tendency.

大電力り2イストロンに使用される永久磁石装置の従来
構造の一例を第1図に示す。第1図面の簡単な説明する
と、1及び2が上部ポールピース、下部ポールピースで
ある。上部ポールピース1にはその上面側から穴がおけ
られておシそこにコレクタの一部(図示せず)かはまシ
込む。同様に、下部ポールピース2にはその下面側から
穴があけられておシそこに電子銃部の一部あるいは全部
(図示せず)かはまシ込む。上部ポールピース1、ノ下
側と下部ポールピース2の上側には通常日銃形の凸部が
設けられ、両者の間に発生する磁界の集中化、均一化の
役割を果す。クライストロンの高周波回路部(図示せず
)は前記両ポールピース間の空隙部に配置され、高周波
回路部の中央を貫通する電子ビームに前記磁界(軸方向
)を作用させ電子ビームの発散を抑制させる。前記両ポ
ールピース1,2はいずれも最外径部は四角形であシ、
図に示す如く両対向部に一対の矩形状磁石が取付けられ
る。すなわち、上部ポールピース1には磁石3,4が、
また下部ポールピース2には磁石5,6が取付けられる
。各磁石の極性は例えば図に示す如くN極及びS極が設
定される。磁石の反対側の面にはヨーク7.8が設置さ
れ、以上の組合せでクライストロン用磁気回路が出来上
る。
An example of the conventional structure of a permanent magnet device used in a high-power Istron is shown in FIG. To briefly explain the first drawing, 1 and 2 are an upper pole piece and a lower pole piece. A hole is made in the upper pole piece 1 from the upper surface side, into which a part of the collector (not shown) is inserted. Similarly, a hole is made in the lower pole piece 2 from its lower surface, into which a part or all of the electron gun section (not shown) is inserted. The lower side of the upper pole piece 1 and the upper side of the lower pole piece 2 are usually provided with protrusions in the shape of a sungun, which serve to centralize and homogenize the magnetic field generated between the two. A high-frequency circuit section (not shown) of the klystron is placed in the gap between the two pole pieces, and applies the magnetic field (in the axial direction) to the electron beam passing through the center of the high-frequency circuit section to suppress divergence of the electron beam. . Both of the pole pieces 1 and 2 have a rectangular outermost diameter,
As shown in the figure, a pair of rectangular magnets are attached to both opposing parts. That is, the magnets 3 and 4 are attached to the upper pole piece 1.
Further, magnets 5 and 6 are attached to the lower pole piece 2. The polarity of each magnet is set to, for example, an N pole and an S pole as shown in the figure. A yoke 7.8 is installed on the opposite side of the magnet, and the above combination completes a klystron magnetic circuit.

さてくこのような構造の永久磁石構造において、最大の
関心事は中央空隙部に必要な強さの磁界を発生させるの
に如何に磁石を小形化するかという事である。磁石自身
の材質を一定とすれば、この事はすなわち、中央空隙部
に発生する磁石を確保する際如何にして他の部分に漏洩
する磁界の発生を防ぐかという問題に帰着する。発明者
が第1図に示す構造について漏洩イ1a界の存在を詳イ
、Iffに検討した結果、下記のような漏洩磁界が存在
することが判明した。すなわち、上部ポールピース1及
び下部ポールピース2の4角面で磁石の奴付けられない
面をそれぞれA面、B面とし、両サイドのヨークの磁石
附近の側面を図示する’JO< Ct l 021 D
I lD2面とすれば、A面とB面間に存在する翻洩磁
界、及びA面と01それにD1面間に存在する漏洩磁界
、B面と02それにD3面間に存在する漏洩磁界等が存
在している。こうした漏洩磁界が存在し°Cいたため、
磁石3,4,5.6の形状を必要以上に大きくしなけれ
ばならなかったわけである。
In a permanent magnet structure like this, the biggest concern is how to downsize the magnet in order to generate a magnetic field of the necessary strength in the central gap. Assuming that the material of the magnet itself is constant, this results in the problem of how to prevent the generation of a magnetic field leaking to other parts when securing the magnet generated in the central gap. As a result of the inventor's detailed examination of the existence of the leakage A1a field Iff in the structure shown in FIG. 1, it was found that the following leakage magnetic field exists. In other words, the four sides of the upper pole piece 1 and the lower pole piece 2 where the magnet cannot be attached are the A side and the B side, respectively, and the sides near the magnets of the yokes on both sides are shown in the figure. D
I If it is the 1D2 plane, the leakage magnetic field that exists between the A plane and the B plane, the leakage magnetic field that exists between the A plane, 01 and D1 planes, the leakage magnetic field that exists between the B plane, 02 plane and D3 plane, etc. Existing. Due to the presence of such leakage magnetic fields,
This meant that the shapes of the magnets 3, 4, 5, and 6 had to be made larger than necessary.

以上の如き従来構造の欠点に細み、本発明は不要の漏洩
磁界を比較的少なくでき仮って磁石の小形化を計υ得る
新しい磁石構造を提供するものである。
In view of the above-mentioned drawbacks of the conventional structure, the present invention provides a new magnet structure in which unnecessary leakage magnetic fields can be relatively reduced and the size of the magnet can be reduced.

不発明を採用した磁石構造を第2図に示す。本発明にお
いては、上部ポールピース及び下部ポールピースにおい
て、磁石と接合されない面の大部分を無くするよりに磁
石の磁化方向の中心軸と直角方向に大きな溝を設けてい
る。このような構造にすることによシ、前述したようガ
各種の漏洩磁界は著しく減少でき、磁石の小形化に対し
て非常に有効であることがわかった。磁界は著しく臓少
でき、磁石の小形化に対して非常に有効であることがわ
かった。
Fig. 2 shows a magnet structure employing the invention. In the present invention, in the upper pole piece and the lower pole piece, a large groove is provided in the direction perpendicular to the central axis of the magnetization direction, rather than eliminating most of the surface that is not joined to the magnet. It has been found that by adopting such a structure, the leakage magnetic fields of the various types mentioned above can be significantly reduced, and it is very effective in reducing the size of the magnet. It was found that the magnetic field was significantly reduced, making it very effective for miniaturizing magnets.

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

第1図は従来の永久磁石構造を示す。第2図は本発明に
よる永久磁石構造を示す。 l・・・・・・上部ポールピース、2・・・・・・下部
ポールピース、3〜6・・・・・・i石、7.8・旧・
・ヨーク。
FIG. 1 shows a conventional permanent magnet structure. FIG. 2 shows a permanent magnet structure according to the invention. l... Upper pole piece, 2... Lower pole piece, 3-6... i stone, 7.8 old.
·yoke.

Claims (1)

【特許請求の範囲】[Claims] 上部ポールピース、下部ポールピースと、これらポール
ピースのそれぞれの対向する外周面に径方向に向けて各
2つずつの径方向に磁化された永久磁石が配置され、各
永久磁石の他端がヨークで連結゛された構造の永久磁石
構造において、前記上部ポールピース及び下部ポールピ
ースの少なくとも一方が磁石の磁化の方向に向けて、中
央間隙部と反対働の面より貫通溝状に大きくカットされ
ていることを特徴とする永久磁石装置。
Two radially magnetized permanent magnets are arranged radially on the upper pole piece, the lower pole piece, and the opposing outer peripheral surfaces of each of these pole pieces, and the other end of each permanent magnet is connected to a yoke. In the permanent magnet structure, at least one of the upper pole piece and the lower pole piece is cut in the shape of a penetrating groove in the direction of magnetization of the magnet from a surface opposite to the central gap. A permanent magnet device characterized by:
JP22516282A 1982-12-22 1982-12-22 Permanent magnet device Pending JPS59114729A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22516282A JPS59114729A (en) 1982-12-22 1982-12-22 Permanent magnet device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22516282A JPS59114729A (en) 1982-12-22 1982-12-22 Permanent magnet device

Publications (1)

Publication Number Publication Date
JPS59114729A true JPS59114729A (en) 1984-07-02

Family

ID=16824911

Family Applications (1)

Application Number Title Priority Date Filing Date
JP22516282A Pending JPS59114729A (en) 1982-12-22 1982-12-22 Permanent magnet device

Country Status (1)

Country Link
JP (1) JPS59114729A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4816796A (en) * 1986-10-03 1989-03-28 Hitachi, Ltd. Permanent magnet device
US5115340A (en) * 1988-09-30 1992-05-19 Amoco Corporation High average power Faraday isolator

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4816796A (en) * 1986-10-03 1989-03-28 Hitachi, Ltd. Permanent magnet device
US5115340A (en) * 1988-09-30 1992-05-19 Amoco Corporation High average power Faraday isolator

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