JPH06215899A - Multipolar magnet for accelerator - Google Patents

Multipolar magnet for accelerator

Info

Publication number
JPH06215899A
JPH06215899A JP466093A JP466093A JPH06215899A JP H06215899 A JPH06215899 A JP H06215899A JP 466093 A JP466093 A JP 466093A JP 466093 A JP466093 A JP 466093A JP H06215899 A JPH06215899 A JP H06215899A
Authority
JP
Japan
Prior art keywords
magnetic field
pole
magnet
coil
coils
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
JP466093A
Other languages
Japanese (ja)
Inventor
Masahiro Tadokoro
昌宏 田所
Kazuo Hiramoto
和夫 平本
Junichi Hirota
淳一 廣田
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP466093A priority Critical patent/JPH06215899A/en
Publication of JPH06215899A publication Critical patent/JPH06215899A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To provide an inexpensive multipolar magnet easy to manufacture. CONSTITUTION:Of exciting coils 2, 2', 3, 3', current is carried to the coils 2', 3' in the direction of penetrating the paper surface, and to the coils 2, 3 in the reversed direction. In such a constitution, a magnetic field is generated as shown in the drawing. This magnetic field can generate the same magnetic field as a conventional quadrupole magnet having a coil wound on each pole. Since the number of coils used in the conventional multipolar magnet can be reduced to half, the cost can be reduced by the reduction in material cost and the number of process, and the assembling is facilitated.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、荷電粒子ビームを発生
する線形加速器、及び、線形加速器からの荷電粒子ビー
ムを入射し、加速蓄積する円形加速器システムに使用さ
れる多極磁石に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a linear accelerator for generating a charged particle beam, and a multipole magnet used in a circular accelerator system for injecting and accumulating a charged particle beam from the linear accelerator.

【0002】[0002]

【従来の技術】従来、加速器に使用される多極磁石で
は、加速器(核物理講座6 編集者 熊谷寛夫 共立出
版株式会社)のP.98 に記載の4極磁石を例にとるよ
う各極に励磁用コイルが巻かれている。また、一般に磁
場補正用コイルも各極に巻かれる。
2. Description of the Related Art Conventionally, in a multi-pole magnet used for an accelerator, the four-pole magnet described in P.98 of the accelerator (Nuclear Physics Course 6 Editor Hiroo Kumagai Kyoritsu Shuppan Co., Ltd.) is used for each pole. The excitation coil is wound. Further, generally, a magnetic field correction coil is also wound around each pole.

【0003】[0003]

【発明が解決しようとする課題】従来、多極磁石では、
各極に励磁用コイル及び磁場補正用コイルを巻いている
ため、製作に手間がかかる,巻きにくく製作しずらい等
の問題があった。
Conventionally, in a multipole magnet,
Since the excitation coil and the magnetic field correction coil are wound around each pole, there are problems that the manufacturing is troublesome, the winding is difficult, and the manufacturing is difficult.

【0004】本発明の目的は、製作が容易な多極磁石を
提供することにある。
An object of the present invention is to provide a multi-pole magnet which is easy to manufacture.

【0005】[0005]

【課題を解決するための手段】本発明の課題を解決する
には、従来各極に巻いていた励磁用コイル及び、磁場補
正用コイルを一つ飛ばしの極に巻くことにより達成でき
る。また、励磁用コイル及び、磁場補正用コイル数を極
数の半分にすることにより達成できる。
The object of the present invention can be solved by winding the exciting coil and the magnetic field correcting coil, which are conventionally wound around each pole, on the poles skipped one by one. This can also be achieved by reducing the number of excitation coils and magnetic field correction coils to half the number of poles.

【0006】[0006]

【作用】多極磁石の極に一つ飛ばしに設置された励磁用
コイルを励磁することにより、従来の各極に励磁用コイ
ルを巻いた多極磁石と同様の多極磁場を発生できる。ま
た、多極磁石の極に一つ飛ばしに設置された磁場補正用
コイルを励磁することにより、従来の各極に磁場補正用
コイルを巻いた場合と同様に磁場補正を行うことができ
る。また、コイルの数を極数の半分にすることで、この
作用と同様の効果が得られる。
By exciting the exciting coils, which are placed apart from the poles of the multipolar magnet, it is possible to generate a multipolar magnetic field similar to the conventional multipolar magnet having the exciting coil wound around each pole. In addition, by exciting the magnetic field correction coils that are placed one for each pole of the multi-pole magnet, the magnetic field correction can be performed in the same manner as in the case where the magnetic field correction coil is wound around each conventional pole. Also, by making the number of coils half the number of poles, the same effect as this action can be obtained.

【0007】[0007]

【実施例】以下、本発明の実施例を詳細に説明する。EXAMPLES Examples of the present invention will be described in detail below.

【0008】図1は本発明である一つ飛ばしの極に励磁
用コイルを巻いた4極磁石の断面図である。図中1は磁
石鉄心である。2,2′,3,3′は励磁用コイルであ
り、2,2′が一つのコイル、3,3′が一つのコイル
であり2′,3′は紙面に突き抜ける方向に、2,3は
その逆方向に電流が流れている。このように一つ飛ばし
の極に励磁用コイルを設置した場合、磁場は4のように
生成される。この磁場は、従来の各極にコイルを巻いた
4極磁石が作る磁場と同様の磁場を発生することができ
る。従って、巻くコイルは従来の半分で従来同様の磁場
を得ることができる。また、逆方向に電流を流すことに
より反対の特性を持つ4極磁石になる。図2はコイルの
数を極数の半分にした場合の4極磁石の断面図を示す。
図中21は磁石鉄心である。22,22′,23,2
3′は、励磁用コイルであり、22,22′が一つのコ
イル、23,23′が一つのコイルであり22′,23′
は紙面に突き抜ける方向に、22,23はその逆方向に
電流が流れている。このような構成にした場合、磁場は
24のように生成される。この磁場は、従来の各極にコ
イルを巻いた4極磁石と同様の磁場を発生することがで
きる。また、逆方向に電流を流すことにより反対の特性
を持つ4極磁石になる。
FIG. 1 is a sectional view of a quadrupole magnet in which an exciting coil is wound around one pole of the present invention. In the figure, 1 is a magnet iron core. 2, 2 ', 3, 3'are excitation coils, 2, 2'is one coil, 3, 3'is one coil, and 2', 3'are 2, 3 Has a current flowing in the opposite direction. In this way, when the exciting coils are installed at the poles skipped one by one, the magnetic field is generated as shown by 4. This magnetic field can generate a magnetic field similar to the magnetic field created by a conventional quadrupole magnet having a coil wound around each pole. Therefore, the wound coil can obtain a magnetic field similar to the conventional one with half the conventional coil. Also, by passing a current in the opposite direction, a quadrupole magnet having opposite characteristics is obtained. FIG. 2 shows a sectional view of a 4-pole magnet when the number of coils is half the number of poles.
In the figure, 21 is a magnet iron core. 22,22 ', 23,2
3'is an excitation coil, 22 and 22 'are one coil, and 23 and 23' are one coil, 22 'and 23'.
The current flows in the direction of penetrating through the sheet of paper and in the opposite direction of 22 and 23. With such a configuration, the magnetic field is generated as in 24. This magnetic field can generate a magnetic field similar to a conventional quadrupole magnet having a coil wound around each pole. Also, by passing a current in the opposite direction, a quadrupole magnet having opposite characteristics is obtained.

【0009】図3は本発明である一つ飛ばしの極に励磁
用コイルを巻いた6極磁石の断面図である。図中31は
磁石鉄心である。32,32′,33,33′,34,
34′は、励磁用コイルであり、32,32′が一つのコ
イル、33,33′が一つのコイル、34,34′が一
つのコイルであり32′,33′,34′は紙面に突き
抜ける方向に、32,33,34はその逆方向に電流が
流れている。このように一つ飛ばしの極に励磁用コイル
を設置した場合、磁場は35のように生成される。この
磁場は、従来の各極にコイルを巻いた6極磁石と同様の
磁場を発生することができる。また、逆方向に電流を流
すことにより反対の特性を持つ6極磁石になる。
FIG. 3 is a sectional view of a 6-pole magnet in which an exciting coil is wound around one pole of the present invention. Reference numeral 31 in the drawing is a magnet iron core. 32, 32 ', 33, 33', 34,
34 'is an exciting coil, 32, 32' is one coil, 33, 33 'is one coil, 34, 34' is one coil, and 32 ', 33', 34 'penetrates into the paper surface. , 32, 33, 34 have current flowing in the opposite direction. In this way, when the exciting coils are installed at the poles skipped one by one, the magnetic field is generated as in 35. This magnetic field can generate a magnetic field similar to a conventional 6-pole magnet having a coil wound around each pole. In addition, by passing a current in the opposite direction, a 6-pole magnet having opposite characteristics is obtained.

【0010】図4はコイルの数を極数の半分にした場合
の6極磁石の断面図を示す。図中41は磁石鉄心であ
る。42,42′,43,43′,44,44′は、励
磁用コイルであり、42,42′が一つのコイル、4
3,43′が一つのコイル、44,44′が一つのコイ
ルであり42′,43′,44′は紙面に突き抜ける方
向に、42,43,44はその逆方向に電流が流れてい
る。このような構成にした場合、磁場は45のように生
成される。この磁場は、従来の各極にコイルを巻いた6
極磁石と同様の磁場を発生することができる。また、逆
方向に電流を流すことにより反対の特性を持つ6極磁石
になる。
FIG. 4 shows a sectional view of a 6-pole magnet when the number of coils is half the number of poles. In the figure, 41 is a magnet iron core. 42, 42 ', 43, 43', 44, 44 'are excitation coils, and 42, 42' are one coil, 4
3, 43 'is one coil, 44, 44' is one coil, and 42 ', 43', 44 'have a current penetrating in the plane of the paper, and 42, 43, 44 have a current flowing in the opposite direction. With such a configuration, the magnetic field is generated as shown by 45. This magnetic field is 6
A magnetic field similar to that of a polar magnet can be generated. In addition, by passing a current in the opposite direction, a 6-pole magnet having opposite characteristics is obtained.

【0011】4極,6極磁石について述べたがそれ以上
の極数を持つ多極磁石についても同様である。また、磁
場補正用コイルの場合も、励磁用コイルと巻き方は同じ
であるので省略する。
Although the 4-pole and 6-pole magnets have been described, the same applies to multi-pole magnets having more poles. Also, in the case of the magnetic field correction coil, the winding method is the same as that of the excitation coil, and therefore the description thereof is omitted.

【0012】本発明の励磁用コイルと磁場補正用コイル
は組み合わせて使用することもできるし、従来の各極に
コイルを巻き付ける方法と併用して使用することもでき
る。以下、図5を用い従来の4極磁石に本発明の磁場補
正用コイルを巻いた1実施例を示す。図中51は磁石鉄
心52は従来の各極に巻かれた励磁用コイルである。5
3が本発明の一つ飛ばしの極に設置された補正用コイル
である。53の補正用コイルを励磁することにより磁場
を補正できる。
The exciting coil and the magnetic field correcting coil of the present invention can be used in combination, or can be used in combination with the conventional method of winding the coil around each pole. An embodiment in which the magnetic field correction coil of the present invention is wound around a conventional quadrupole magnet will be described below with reference to FIG. In the figure, 51 is a magnet iron core 52, and a conventional magnetizing coil is wound around each pole. 5
Reference numeral 3 is a correction coil installed at one skipping pole of the present invention. The magnetic field can be corrected by exciting the correction coil 53.

【0013】[0013]

【発明の効果】本発明によれば、従来の多極磁石に使用
されたコイルの数を半分にすることができるので、材料
費,工数の低減によるコストダウン、全ての極にコイル
を巻かなくて良いので、容易な組立が可能になる。
According to the present invention, the number of coils used in the conventional multi-pole magnet can be halved, so that the material cost and the cost can be reduced by reducing the man-hours, and the coils can be wound on all the poles. Since it is unnecessary, easy assembly is possible.

【図面の簡単な説明】[Brief description of drawings]

【図1】一つ飛ばしの極に励磁用コイルを巻き付けた4
極磁石の平面図。
[Fig. 1] 4 with an exciting coil wrapped around one pole
The top view of a polar magnet.

【図2】励磁用コイルの数を従来の半分にした4極磁石
の平面図。
FIG. 2 is a plan view of a quadrupole magnet in which the number of exciting coils is halved as compared with the conventional one.

【図3】一つ飛ばしの極に励磁用コイルを巻き付けた6
極磁石の平面図。
[Fig. 3] 6 with an exciting coil wound around one pole
The top view of a polar magnet.

【図4】励磁用コイルの数を従来の半分にした6極磁石
の平面図。
FIG. 4 is a plan view of a 6-pole magnet in which the number of exciting coils is halved as compared with the conventional one.

【図5】従来の4極磁石に本発明の磁場補正用コイルを
巻き付けた4極磁石の平面図。
FIG. 5 is a plan view of a quadrupole magnet in which a magnetic field correction coil of the present invention is wound around a conventional quadrupole magnet.

【符号の説明】[Explanation of symbols]

1,21,31,41,51…磁石鉄心、4,24…4
極磁場、22,23,32,33,34,42,43,
44,52…励磁用コイル、35,45…6極磁場。
1, 21, 31, 41, 51 ... Magnet iron core, 4, 24 ... 4
Polar magnetic field, 22, 23, 32, 33, 34, 42, 43,
44, 52 ... Excitation coil, 35, 45 ... 6-pole magnetic field.

Claims (6)

【特許請求の範囲】[Claims] 【請求項1】加速器に使用される多極磁石において、励
磁用コイルの数を極数より小さくすることを特徴とする
加速器の多極磁石。
1. A multi-pole magnet for use in an accelerator, wherein the number of exciting coils is smaller than the number of poles.
【請求項2】加速器に使用される多極磁石において、励
磁用コイルの数を極数の半分にすることを特徴とする加
速器の多極磁石。
2. A multipole magnet for use in an accelerator, wherein the number of exciting coils is half the number of poles.
【請求項3】加速器に使用される多極磁石において、励
磁用コイルを一つ飛ばしの極に設置することを特徴とす
る加速器の多極磁石。
3. A multi-pole magnet for an accelerator, wherein a multi-pole magnet used in the accelerator is provided with an exciting coil at a pole separated by one.
【請求項4】加速器に使用される多極磁石において、磁
場補正用コイルの数を極数より小さくすることを特徴と
する加速器の多極磁石。
4. A multipole magnet for use in an accelerator, wherein the number of magnetic field correction coils is smaller than the number of poles.
【請求項5】加速器に使用される多極磁石において、磁
場補正用コイルの数を極数の半分にすることを特徴とす
る加速器の多極磁石。
5. A multipole magnet for use in an accelerator, wherein the number of magnetic field correction coils is half the number of poles.
【請求項6】加速器に使用される多極磁石において、磁
場補正用コイルを一つ飛ばしの極に設置することを特徴
とする加速器の多極磁石。
6. A multi-pole magnet for an accelerator, wherein a multi-pole magnet used in the accelerator is provided with a magnetic field correction coil at a skipping pole.
JP466093A 1993-01-14 1993-01-14 Multipolar magnet for accelerator Pending JPH06215899A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP466093A JPH06215899A (en) 1993-01-14 1993-01-14 Multipolar magnet for accelerator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP466093A JPH06215899A (en) 1993-01-14 1993-01-14 Multipolar magnet for accelerator

Publications (1)

Publication Number Publication Date
JPH06215899A true JPH06215899A (en) 1994-08-05

Family

ID=11590092

Family Applications (1)

Application Number Title Priority Date Filing Date
JP466093A Pending JPH06215899A (en) 1993-01-14 1993-01-14 Multipolar magnet for accelerator

Country Status (1)

Country Link
JP (1) JPH06215899A (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1323889A2 (en) * 2001-12-27 2003-07-02 Hideo Hoshi High-speed cylinder apparatus
CN104681230A (en) * 2014-12-16 2015-06-03 中国原子能科学研究院 Beam homogenizing sextupole magnet for accelerator
CN104703378A (en) * 2015-03-17 2015-06-10 中国原子能科学研究院 Homogenized sextupole magnet of permanent magnet beam
CN110191566A (en) * 2019-02-25 2019-08-30 中国科学技术大学 A kind of magnetic field gradient can modulation two four-electrode pattern magnetic field bending magnets
JP6898508B1 (en) * 2020-10-29 2021-07-07 株式会社トーキン Multipolar electromagnet
CN114388219A (en) * 2022-01-21 2022-04-22 北京高能锐新科技有限责任公司 Coreless dipolar magnet for positive and negative electronic collider intensifier

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1323889A2 (en) * 2001-12-27 2003-07-02 Hideo Hoshi High-speed cylinder apparatus
EP1323889A3 (en) * 2001-12-27 2003-10-29 Hideo Hoshi High-speed cylinder apparatus
US6981440B2 (en) 2001-12-27 2006-01-03 Hideo Hoshi High-speed cylinder apparatus
CN104681230A (en) * 2014-12-16 2015-06-03 中国原子能科学研究院 Beam homogenizing sextupole magnet for accelerator
CN104703378A (en) * 2015-03-17 2015-06-10 中国原子能科学研究院 Homogenized sextupole magnet of permanent magnet beam
CN110191566A (en) * 2019-02-25 2019-08-30 中国科学技术大学 A kind of magnetic field gradient can modulation two four-electrode pattern magnetic field bending magnets
JP6898508B1 (en) * 2020-10-29 2021-07-07 株式会社トーキン Multipolar electromagnet
CN114388219A (en) * 2022-01-21 2022-04-22 北京高能锐新科技有限责任公司 Coreless dipolar magnet for positive and negative electronic collider intensifier
CN114388219B (en) * 2022-01-21 2022-09-09 北京高能锐新科技有限责任公司 Coreless dipolar magnet for positive and negative electronic collider intensifier

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