JPH03220500A - Coil for charged particle bending electromagnet - Google Patents

Coil for charged particle bending electromagnet

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Publication number
JPH03220500A
JPH03220500A JP1538890A JP1538890A JPH03220500A JP H03220500 A JPH03220500 A JP H03220500A JP 1538890 A JP1538890 A JP 1538890A JP 1538890 A JP1538890 A JP 1538890A JP H03220500 A JPH03220500 A JP H03220500A
Authority
JP
Japan
Prior art keywords
coil
coils
superconducting
bobbin
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
JP1538890A
Other languages
Japanese (ja)
Inventor
Yoshio Imai
良夫 今井
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 JP1538890A priority Critical patent/JPH03220500A/en
Publication of JPH03220500A publication Critical patent/JPH03220500A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To enable elimination of arrangement limit and lessening of an occupation space of a coil by placing a bobbin block between main and adjusting coils made of continuous leads having no connection part, for the purpose of magnetic field generation, and by housing them in a common vessel. CONSTITUTION:A super-conducting coil 1a constituting an electro-magnet, consists of super-conductive main coil and adjusting coil 4 and 5 and, after completion of a winding work of the coil 5, the continuous coil 4 is wound by making the lead to be a crossing part 10, as it was. Then, a bobbin block 12, being shaped to have a predetermined width, is inserted between the both coils 4 and 5 at arbitrarily designated relative positions. This coil 1a is supported and fixed to the inside of a monolithic bobbin 11 of a common vessel. In this way, both coils 4 and 5 are continuously wound and are housed in the common bobbin 11 and therefore there is no connection point, the performance can be much improved and an occupation space is diminished, as well. Moreover, gap length between both coils 4 and 5 can be arbitrarily selected by the block 12 and a magnetic field conformable to specifications can be firmly obtained.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、例えばシンクロトロン放射光発生装置など
に用いられる荷電粒子偏向電磁石用コイトに関するもの
である。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a coil for a charged particle deflection electromagnet used, for example, in a synchrotron radiation light generating device.

〔従来の技術〕[Conventional technology]

超電導材料で作られた導線から成り、粒子軌道に対応し
て湾曲した半円形状の超電導主コイルと超電導補正コイ
ルとが、前記粒子軌道を挾んで対向配置された超電導偏
向電磁石を用いた荷電粒子装置は、例えば特開昭64−
2300号公報及び特開昭61−294800号公報に
示されたものがある。
Charged particles using a superconducting bending electromagnet, in which a semicircular superconducting main coil and a superconducting correction coil, each made of a conductive wire made of a superconducting material and curved in accordance with the particle trajectory, are arranged opposite to each other with the particle trajectory in between. The device is, for example, disclosed in Japanese Patent Application Laid-Open No. 1986-
There are those shown in Japanese Patent Application Laid-open No. 2300 and Japanese Patent Application Laid-Open No. 61-294800.

即ち、第5図は上記特開昭64−2300号公報に示さ
れたものと同種の荷電粒子装置の原理図であり、図示さ
れていない入射部及び加速部を経て入射された荷電粒子
は、対向する2個の超電導偏向電磁石(1)により長円
形の軌道(21上を運動する。
That is, FIG. 5 is a principle diagram of a charged particle device of the same type as that shown in the above-mentioned Japanese Patent Application Laid-Open No. 64-2300. Charged particles incident through an injection section and an acceleration section (not shown) are It moves on an elliptical orbit (21) by two opposing superconducting bending electromagnets (1).

ところで前記超電導偏向電磁石(1)の構成要部である
超電導コイル(la)は、第6図・第7図に示すように
、超電導材料で作られた導線β)を巻回して構成された
超電導主コイル(4)と超電導補正コイル(5)とから
成り、これら両コイル(イ)、(5)が前記粒子軌道(
2)を挾んで上下に対向配置されている。そして前記超
電導主コイル4及び超電導補正コイル(5)は共に粒子
軌道(2)の外径方向へ突出するように所定の曲率で半
円形状に湾曲しており、粒子軌道(2)の内径方向側に
位置する内径部(4a) (5a)と、粒子軌道(2)
の外径方向側に位置する外径部(4bH5b)及び湾曲
両端部(4c) (5c)に区分される。このように構
成された両コイル(41(51は、例えば−268℃の
極低温に冷却されて超電導状態となり、これに電流を流
すことにより数テスラの高い磁束密度の磁界が得られ、
この磁界により、荷電粒子の軌道(2)は図に示すよう
に偏向される。
By the way, the superconducting coil (la), which is the main component of the superconducting bending electromagnet (1), is a superconducting coil made of a superconducting wire (β) made of a superconducting material, as shown in FIGS. 6 and 7. It consists of a main coil (4) and a superconducting correction coil (5), and both of these coils (A) and (5) are connected to the particle trajectory (
2) are placed vertically facing each other. Both the superconducting main coil 4 and the superconducting correction coil (5) are curved in a semicircular shape with a predetermined curvature so as to protrude in the direction of the outer diameter of the particle trajectory (2), and are curved in the inner diameter direction of the particle trajectory (2). The inner diameter part (4a) (5a) located on the side and the particle trajectory (2)
It is divided into an outer diameter part (4bH5b) located on the outer diameter direction side and curved both end parts (4c) (5c). Both coils (41 (51) configured in this way are cooled to an extremely low temperature of -268°C, for example, and become superconducting. By passing current through them, a magnetic field with a high magnetic flux density of several Tesla is obtained.
Due to this magnetic field, the trajectory (2) of the charged particles is deflected as shown in the figure.

第8図は例えは特開昭61−294800号公報に示さ
れた従来の超電導偏向電磁石の超電導コイル(1a)の
製作過程を示す斜視説明図であり、まず超電導線(3)
を図のZ軸方向へ所定回数巻き上けて1層目を形成し、
次にその外周に沿って2層目を巻き上げ、このようにし
て順次所要の層数になるまで巻回するのである。そして
完成されたコイルは、第9図に示すように、主コイル(
4)、補正コイル(5)をそれぞれのコイル容器(6)
に収容支持した後コイル台口に固定される。その後、第
10図及び第11図に示すように、電流リードf81を
設けるが、第10図は接続部(9)において主コイル(
イ)と補正コイル(9とが接続された場合を、また第1
1図は主コイル(2)と補正コイル(51とにそれぞれ
電流リード(8)を設けた場合を示している。
FIG. 8 is a perspective explanatory view showing the manufacturing process of a superconducting coil (1a) of a conventional superconducting bending electromagnet disclosed in, for example, Japanese Patent Application Laid-Open No. 61-294800.
is rolled up a predetermined number of times in the Z-axis direction in the figure to form the first layer,
Next, the second layer is rolled up along its outer periphery, and the winding is continued in this manner until the required number of layers is reached. The completed coil is the main coil (
4), the correction coil (5) into each coil container (6)
After being accommodated and supported, the coil is fixed to the base opening. Thereafter, as shown in FIGS. 10 and 11, a current lead f81 is provided, but in FIG. 10, the main coil (
A) and the correction coil (9) are connected, and the first
FIG. 1 shows a case where the main coil (2) and the correction coil (51) are each provided with a current lead (8).

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

上記のような従来の荷電粒子偏向電磁石用コイルにおい
ては、コイル容器が、コイルに作用する電磁力を支持す
るに足る容積を必要とするため、1コイル当りの占有容
積が大きくなり、主コイルと補正コイルとの間隔も一定
以上の距離が必要になる。
In the conventional charged particle bending electromagnet coils described above, the coil container requires a volume sufficient to support the electromagnetic force acting on the coil, so the volume occupied by each coil is large, and the main coil The distance from the correction coil also needs to be at least a certain distance.

従って、主コイルと補正コイルとの相対的な配置の選択
に制約が生じ、両コイルで発生し得る磁場の形態も一定
の範囲内に制限されることになる。
Therefore, there are restrictions on the selection of the relative arrangement of the main coil and the correction coil, and the form of the magnetic field that can be generated by both coils is also restricted within a certain range.

また、特に超電導コイルの場合には、第10図に示すよ
うにリードを付設する場合、主コイルと補正コイルとの
間に接続部が存在することから、いわゆる接続抵抗の影
響により、特に永久電流モードで運転する場合などにお
いて電流及び発生磁界の減衰が著しく、超電導コイルの
性能悪化を招くことになる。また第11図に示すように
電流リードを多用すると、超電導コイルへの熱侵入量が
増加するという問題点があった。
In addition, especially in the case of superconducting coils, when a lead is attached as shown in Figure 10, there is a connection between the main coil and the correction coil, so due to the influence of so-called connection resistance, the persistent current When operating in this mode, the attenuation of the current and the generated magnetic field is significant, leading to deterioration in the performance of the superconducting coil. Furthermore, as shown in FIG. 11, if many current leads are used, there is a problem in that the amount of heat entering the superconducting coil increases.

本発明は、かかる問題点を解決するためになされたもの
で、偏向電磁石内のコイル配置の制約を減らし、かつコ
イルの占有空間の減少を図り、導体接続部による性能悪
化のない荷電粒子偏向電磁石用コイルを得ることを目的
とする。
The present invention has been made in order to solve these problems, and is designed to reduce restrictions on the arrangement of coils within a deflecting electromagnet, reduce the space occupied by the coil, and provide a charged particle deflecting electromagnet without deterioration of performance due to conductor connections. The purpose is to obtain a coil for use.

〔課題を解決するための手段および作用〕この発明に係
る荷電粒子偏向電磁石用コイルは、主コイルと補正コイ
ルとをそのわたり部を含め、接続部分のない連続した導
線で楕成し、かつ、上記両コイル間に磁場発生に必要な
間隔を確保するための巻型フロックを介在させ上記両コ
イルを共通の容器に収容したものである。
[Means and effects for solving the problem] The coil for a charged particle deflection electromagnet according to the present invention has a main coil and a correction coil formed into an ellipse including a continuous conductive wire without a connecting part, and A winding flock is interposed between the two coils to ensure the spacing necessary for generating a magnetic field, and both the coils are housed in a common container.

導体接続部がなくなりコイルとしての性能が向上し、両
コイルを共通の容器に収容するので、配置上の制約が解
消しコイルの占有空間も縮小する。
The performance of the coil is improved by eliminating the conductor connection part, and since both coils are housed in a common container, restrictions on arrangement are eliminated and the space occupied by the coils is also reduced.

〔実施例〕〔Example〕

第1図・第2図はこの発明の一実施例を示し、第3図及
び第4図は他の実施例を示すもので、これらの図におい
て、上記従来の超電導偏向電磁石と同一符号を付した部
分は同一または相当部分である。
Figures 1 and 2 show one embodiment of the present invention, and Figures 3 and 4 show other embodiments. The parts shown are the same or equivalent parts.

第1図・第2図に示す実施例では、超電導偏向電磁石(
1)を構成する超電導コイル<la)は、主コイル(4
)と補正コイル(5)との2個でしかも両者の導線巻回
方向が同一の場合を示している。そして、補正コイル(
5)の巻線作業が完了すると、導線をそのままわたり部
αO)として更に連続して主コイル(4)の巻線作業へ
移行して所要の巻線を行なう。両コイル(イ)(51の
間には所定幅に成形された巻型ブロック(12)が挿入
され、両コイル(41(51が任意に指定された相対位
置になるよう構成されている。このようにして製作され
た超電導コイル(Ia)は第2図に示すように、共通の
容器である一体型巻枠(11)内に支持固定される。
In the embodiment shown in Figs. 1 and 2, a superconducting bending electromagnet (
The superconducting coil <la) constituting 1) is the main coil (4
) and a correction coil (5), and the winding direction of the conducting wires in both is the same. And the correction coil (
When the winding work 5) is completed, the conductor is left as it is at the crossing portion αO), and then the winding work of the main coil (4) is continued to perform the required winding. A winding block (12) formed to a predetermined width is inserted between both coils (A) (51), and both coils (41 (51) are configured so that they are in an arbitrarily specified relative position. The superconducting coil (Ia) manufactured in this manner is supported and fixed within an integral winding frame (11), which is a common container, as shown in FIG.

また第3図に示すように、わたり部00)で導線を逆方
向にし、主コイル(2)の巻回方向を補正コイル((5
)のそれと反対にすることによって、通電方向の異なる
主コイル(イ)と補正コイル(9とを備えた超電導コイ
ル(la)を製作することができる。
In addition, as shown in Figure 3, the conductor is reversed at the crossing point 00), and the winding direction of the main coil (2) is changed to the correction coil ((5).
), it is possible to manufacture a superconducting coil (la) comprising a main coil (a) and a correction coil (9) with different current direction.

更に第4図に示すように、補正コイル四の内側に第2の
補正コイル(5a)を設けることもでき、この場合製作
に際しては、第2の補正コイル(5a)から補正コイル
(5)、主コイル(イ)へと順次わたり部QO)を介し
て連続的に巻線作業を行うのであるが、巻回方向はそれ
ぞれ異なってもよい。
Furthermore, as shown in FIG. 4, a second correction coil (5a) can be provided inside the correction coil 4. In this case, during manufacturing, the correction coil (5), the second correction coil (5a), Although the winding work is performed successively to the main coil (A) via the crossing section QO), the winding direction may be different from each other.

以上のように、これら実施例においては、両コイル(4
1(5)を連続して巻回し、両者を共通の一体型巻枠(
11)に収容したので、接続点(9)がなくなり超電導
コイルとしての性能が向上するとともに、コイルの占有
空間か低減する。更に、両コイル(イ)(5)の間隔は
巻型ブロック(12)により任意の寸法に設定できるの
で、要求された仕様の磁場が確実に得られることになる
As described above, in these embodiments, both coils (4
1 (5) in succession, and both are wrapped around a common integrated winding frame (
11), the connection point (9) is eliminated, improving the performance of the superconducting coil and reducing the space occupied by the coil. Furthermore, since the spacing between the coils (a) and (5) can be set to any size using the winding block (12), a magnetic field of the required specifications can be reliably obtained.

なおこの発明を実施するに当り、各コイルの巻線方向の
高さ及びコイル断面の大きさが必ずしも同じである必要
はなく、コイル間に段差があり、またコイル断面積が異
なっていてもよい。またコイルの個数にも制限はない、
更にコイル構成線材として超電導線以外の銅線その他の
導体材料を使用したものとしてもよい。
Note that in carrying out this invention, the height in the winding direction and the size of the coil cross section of each coil do not necessarily have to be the same, and there may be a step between the coils or the coil cross section may be different. . There is also no limit to the number of coils.
Furthermore, copper wire or other conductive material other than superconducting wire may be used as the coil constituent wire.

〔発明の効果〕〔Effect of the invention〕

この発明は以上のように構成されているので、主コイル
と補正コイルとの両コイル間に接続点がなくなりコイル
の性能が向上するとともに偏向電磁石内でのコイルの占
有空間が低減する。更に、両コイルの間隔を任意に選定
できるので、要求された磁場が確実に得られる。
Since the present invention is constructed as described above, there is no connection point between the main coil and the correction coil, which improves the performance of the coil and reduces the space occupied by the coil within the deflection electromagnet. Furthermore, since the spacing between both coils can be arbitrarily selected, the required magnetic field can be reliably obtained.

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

第1図はこの発明の一実施例による超電導コイルの部分
斜視図、第2図は第1図に示す超電導コイルの収容例を
示す断面図、第3図は他の実施例による部分斜視図、第
4図は更に他の実施例とその収容状態を示す断面図、第
5図は荷電粒子装置の原理説明図、第6図は従来の超電
導コイルを示す平面図、第7図は第6図における■−■
線の断面図、第8図は従来の超電導コイルの製作過程を
示す説明図、第9図は従来の超電導コイルとその収容構
造を示す断面部分斜視図、第1O図及び第11図は従来
の超電導コイルの電流リード付設手段を示す断面図であ
る。 図において、(1)は超電導偏向電磁石、 (la)は
超電導コイル、 (21は粒子軌道、(イ)は超電導主
コイル。 (9は超電導補正コイル、αO)はわたり部、(II)
は共通の容器としての一体型巻枠、 (12)は巻型ブ
ロックである。 なお、各図中同一符号は同一または相当部分を示す。
FIG. 1 is a partial perspective view of a superconducting coil according to an embodiment of the present invention, FIG. 2 is a sectional view showing an example of housing the superconducting coil shown in FIG. 1, and FIG. 3 is a partial perspective view of another embodiment. FIG. 4 is a sectional view showing still another embodiment and its accommodation state, FIG. 5 is a diagram explaining the principle of the charged particle device, FIG. 6 is a plan view showing a conventional superconducting coil, and FIG. ■-■
8 is an explanatory diagram showing the manufacturing process of a conventional superconducting coil, FIG. 9 is a partial perspective view of a conventional superconducting coil and its housing structure, and FIGS. FIG. 3 is a cross-sectional view showing current lead attachment means for a superconducting coil. In the figure, (1) is a superconducting bending electromagnet, (la) is a superconducting coil, (21 is a particle orbit, (a) is a superconducting main coil, (9 is a superconducting correction coil, αO) is a crossing part, (II)
is an integrated winding frame as a common container, and (12) is a winding form block. Note that the same reference numerals in each figure indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】  それぞれ導線を巻回して構成され荷電粒子偏向に必要
な磁場を発生させるため所定の間隔を設けて配設された
主コイルと補正コイル、およびこれらコイルを収容支持
する容器を備えたものにおいて、 上記両コイルをそのわたり部を含め、接続部分のない連
続した導線で構成し、かつ、上記両コイル間に上記間隔
を確保するための巻型ブロックを介在させ上記両コイル
を共通の容器に収容したことを特徴とする荷電粒子偏向
電磁石用コイル。
[Claims] A main coil and a correction coil each formed by winding a conducting wire and arranged at a predetermined interval in order to generate a magnetic field necessary for deflecting charged particles, and a container that accommodates and supports these coils. The above-mentioned coils are constructed of a continuous conductor without a connecting part, including the crossing part, and a winding block is interposed between the above-mentioned coils to ensure the above-mentioned interval. A coil for a charged particle deflection electromagnet, characterized in that the coil is housed in a common container.
JP1538890A 1990-01-24 1990-01-24 Coil for charged particle bending electromagnet Pending JPH03220500A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1538890A JPH03220500A (en) 1990-01-24 1990-01-24 Coil for charged particle bending electromagnet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1538890A JPH03220500A (en) 1990-01-24 1990-01-24 Coil for charged particle bending electromagnet

Publications (1)

Publication Number Publication Date
JPH03220500A true JPH03220500A (en) 1991-09-27

Family

ID=11887360

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1538890A Pending JPH03220500A (en) 1990-01-24 1990-01-24 Coil for charged particle bending electromagnet

Country Status (1)

Country Link
JP (1) JPH03220500A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2000046999A (en) * 1998-07-31 2000-02-18 Rikagaku Kenkyusho Uniform magnetic field generator
JP2009301992A (en) * 2008-06-17 2009-12-24 Toshiba Corp Superconducting coil device

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61294800A (en) * 1985-06-24 1986-12-25 シ−メンス、アクチエンゲゼルシヤフト Magnetic field device for charged particle acceleration or storage equipment
JPS6427199A (en) * 1987-07-22 1989-01-30 Hitachi Ltd Deflection magnet and exciter thereof
JPH01307197A (en) * 1988-06-06 1989-12-12 Mitsubishi Electric Corp charged particle device

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61294800A (en) * 1985-06-24 1986-12-25 シ−メンス、アクチエンゲゼルシヤフト Magnetic field device for charged particle acceleration or storage equipment
JPS6427199A (en) * 1987-07-22 1989-01-30 Hitachi Ltd Deflection magnet and exciter thereof
JPH01307197A (en) * 1988-06-06 1989-12-12 Mitsubishi Electric Corp charged particle device

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2000046999A (en) * 1998-07-31 2000-02-18 Rikagaku Kenkyusho Uniform magnetic field generator
JP2009301992A (en) * 2008-06-17 2009-12-24 Toshiba Corp Superconducting coil device

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