JPS6119104A - Superconducting magnetic field generator - Google Patents

Superconducting magnetic field generator

Info

Publication number
JPS6119104A
JPS6119104A JP59139299A JP13929984A JPS6119104A JP S6119104 A JPS6119104 A JP S6119104A JP 59139299 A JP59139299 A JP 59139299A JP 13929984 A JP13929984 A JP 13929984A JP S6119104 A JPS6119104 A JP S6119104A
Authority
JP
Japan
Prior art keywords
superconducting
magnetic field
coil
electromagnetic force
field generator
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
JP59139299A
Other languages
Japanese (ja)
Inventor
Takamasa Fujinaga
藤永 高正
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 JP59139299A priority Critical patent/JPS6119104A/en
Publication of JPS6119104A publication Critical patent/JPS6119104A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F6/00Superconducting magnets; Superconducting coils

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Containers, Films, And Cooling For Superconductive Devices (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明は、超電導磁界発生装置に係り、特に紫外光発生
装置−一;マクイグラー参−ウ)に好適な超電導磁界発
生装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to a superconducting magnetic field generator, and particularly to a superconducting magnetic field generator suitable for an ultraviolet light generator (1); MacQuigler (3).

〔発明の背景〕[Background of the invention]

はぼ光速に近い電子を高真空に排気した無端(ドーナツ
状)ダクトの中に導入し、電子軌道をある曲率をもって
曲げるときに、光を放射する5OR(シンクロトロン軌
道放射)装置が実用に供されている。
A 5OR (synchrotron orbital emission) device has been put into practical use, which emits light when electrons at speeds close to the speed of light are introduced into an endless (doughnut-shaped) duct evacuated to a high vacuum and the electron orbit is bent with a certain curvature. has been done.

シンクロトロン放射による放射光の波長λCは、と表わ
される。ただし、kは定数、Boは電子軌道に垂直な磁
束密度、EはGeVで表わした電子のエネルギーである
The wavelength λC of synchrotron radiation is expressed as follows. Here, k is a constant, Bo is the magnetic flux density perpendicular to the electron orbit, and E is the electron energy expressed in GeV.

また、曲率半径ρは、 と表わされる。ただし、βとγとは電子の速度Vと光速
Cにより定まる定数2mは電子の質量、eは電子の電荷
であろう (1)式からは、磁束密度BOおよび電子のエネルギー
Eが大きいほど波長が短い光が得られることがわかす、
(2)式からは、磁束密度Boが大きいほど電子軌道の
曲率半径が小さくなることがわかる。
Further, the radius of curvature ρ is expressed as follows. However, β and γ are constants determined by the electron speed V and the speed of light C. 2m is the mass of the electron, and e is the charge of the electron. From equation (1), it can be seen that the larger the magnetic flux density BO and the energy E of the electron, the longer the wavelength. shows that short light can be obtained.
From equation (2), it can be seen that the larger the magnetic flux density Bo, the smaller the radius of curvature of the electron orbit.

従来のSOR装置においては、銅、鉄を用いたいわゆる
偏向電磁石により、電子軌道を曲げていた。この種の銅
、鉄電磁石においては、磁束密度Boは10〜20キロ
ガウス程度であり、短い波長の光を得るには、美大な電
力を消費する加速器を使用し、電子のエネルギーを高め
ていた。
In conventional SOR devices, electron orbits are bent using so-called bending electromagnets made of copper or iron. In this type of copper or iron electromagnet, the magnetic flux density Bo is about 10 to 20 kilogauss, and in order to obtain short wavelength light, an accelerator that consumes a huge amount of power is used to increase the energy of the electrons. .

エネルギーロスを少なくして磁束密度Boを高めるには
、超電導磁石を使うことが有効な手段である。電子軌道
に曲率を与えるための超電導磁石の従来構造の一例を1
部破断状態で第3図に示す。
Using superconducting magnets is an effective means to reduce energy loss and increase magnetic flux density Bo. An example of the conventional structure of a superconducting magnet for giving curvature to electron orbits is shown below.
It is shown in FIG. 3 in a partially broken state.

超電導コイル1は押え板2およびボルト3で容器4の内
側部分4Aに固定される。超電導コイル1に働く電磁力
は、矢印5A、5Bで示すコイルを押し広げようとする
方向の力と、矢印6A、6Bで示す向い合ったコイル間
の吸引力とになる。超電導コイルに働く電磁力によるコ
イルの変形は、その変形過程において、摩擦熱や歪エネ
ルギーの開放などにより、超電導コイルの温度を上昇さ
せ、超電導状態から常電導状態に転移する主要因となる
The superconducting coil 1 is fixed to the inner part 4A of the container 4 with a holding plate 2 and bolts 3. The electromagnetic force acting on the superconducting coil 1 is a force in the direction shown by arrows 5A and 5B that tries to spread the coils apart, and an attractive force between the opposing coils shown by arrows 6A and 6B. The deformation of the superconducting coil due to the electromagnetic force acting on it causes the temperature of the superconducting coil to rise due to the release of frictional heat and strain energy during the deformation process, which is the main cause of the transition from the superconducting state to the normal conducting state.

そこで、超電導コイルには、電磁力によって変形しない
ように、電磁力に対向する向きに支持部材を設けである
。第3図に示す従来の超電導磁石においては、矢印5B
の方向の電磁力を、次のような経路で容器4の内側部分
4Aに伝達し支持させていた。
Therefore, the superconducting coil is provided with a support member in a direction opposite to the electromagnetic force so as not to be deformed by the electromagnetic force. In the conventional superconducting magnet shown in FIG.
The electromagnetic force in the direction was transmitted to and supported by the inner portion 4A of the container 4 through the following path.

超電導コイル1→当て板7→押しボルト10→支持板8
→固定ボルト9→容器内一部分4Aこの構造においては
、固定ボルト9に曲げモーメントが加わシ、超電導コイ
ル1に発生する電磁力に対向するには、多数のボルトを
必要としていた。それでも変形を完全に押えるのは不可
能で、常電導に転移することがしばしばあった。
Superconducting coil 1 → backing plate 7 → push bolt 10 → support plate 8
→Fixing bolt 9→Part inside the container 4A In this structure, a bending moment is applied to the fixing bolt 9, and a large number of bolts are required to counteract the electromagnetic force generated in the superconducting coil 1. Even so, it was impossible to completely suppress the deformation, and the transition to normal conductivity often occurred.

第3図の矢印11は、電子ビームの方向を示すが、これ
を平面的に模式表現したのが第4図である。第4図にお
いて、左方から入射した電子ビーム11は、第1磁極2
1(−列として紙面に垂直で下向き)により偏向される
。次に第2磁極22(−列として紙面に垂直上向き)に
より逆方向に偏向される。更に第3磁極23(第1磁極
と同極)により元の軌道方向の延長上に戻るような偏向
を受ける。
The arrow 11 in FIG. 3 indicates the direction of the electron beam, and FIG. 4 is a schematic two-dimensional representation of this. In FIG. 4, the electron beam 11 incident from the left is directed to the first magnetic pole 2.
1 (perpendicular to the plane of the paper and downward as a - column). Next, it is deflected in the opposite direction by the second magnetic pole 22 (directed upward perpendicularly to the plane of the paper as the - column). Further, it is deflected by the third magnetic pole 23 (same pole as the first magnetic pole) so as to return to the original extension in the orbital direction.

それぞれの磁極間隔t1が長いと、電子〉−ムの偏向量
tzが大きくなり、容器4の内側部分4Aの幅t3を広
くしておかなければならない。
If the distance t1 between the respective magnetic poles is long, the amount of deflection tz of electrons becomes large, and the width t3 of the inner portion 4A of the container 4 must be widened.

従来の超電導磁石では、当て板7.支持板8.押しボル
ト10を設けるための空間が必要であ勺、磁極間隔t1
が長くなるから、容器全体が大型化せざるを得なかった
In conventional superconducting magnets, the backing plate 7. Support plate 8. A space is required to install the push bolt 10, and the magnetic pole spacing t1 is required.
Because the length of the container was longer, the entire container had to be larger.

〔発明の目的〕[Purpose of the invention]

本発明の目的は、従来の超電導磁石の欠点を解消するこ
とで多少、よシ具体的には、超電導コイルの変形を押え
る容器が小型軽量の超電導磁石を備えた超電導磁界発生
装置を提供することである。
The purpose of the present invention is to overcome some of the drawbacks of conventional superconducting magnets. Specifically, it is an object of the present invention to provide a superconducting magnetic field generator equipped with a superconducting magnet whose container is small and lightweight to suppress deformation of a superconducting coil. It is.

〔発明の概要〕[Summary of the invention]

本発明は、従来の当て板と支持板と押しボルトとによる
超電導コイルの支持構造に代えて、超電導コイルの周囲
を取巻く支持部材とこれに溶接等で取付けられる上下板
かかr手舎とを採用したものである。
In place of the conventional superconducting coil support structure that includes a patch plate, a support plate, and a push bolt, the present invention uses a support member that surrounds the superconducting coil and upper and lower plates or handshafts that are attached to this by welding or the like. This is what was adopted.

〔発明の実施例〕[Embodiments of the invention]

次に、第1図と第2図とを参照して、本発明の一実施例
につき、更に詳細に説明する。
Next, one embodiment of the present invention will be described in more detail with reference to FIGS. 1 and 2.

超電導コイル31に密接してスペーサ32を設ける。ス
ペーサ32は、コイル周方向に沿って飛び飛びに配置し
、冷媒の通路を形成する。本発明の特徴である電磁力支
持部材33は、コイル周方向に沿った形状とし、スペー
サ32を介して、超電導コイル31を押え込むように取
付ける。更に上板34.と下板35とを用いて、超電導
コイル31と電磁力支持部材33とをサンドイッチ状に
はさみ込むようにしである。
A spacer 32 is provided in close contact with the superconducting coil 31. The spacers 32 are arranged at intervals along the circumferential direction of the coil to form coolant passages. The electromagnetic force support member 33, which is a feature of the present invention, has a shape along the circumferential direction of the coil, and is attached so as to press down the superconducting coil 31 via the spacer 32. Furthermore, the upper plate 34. The superconducting coil 31 and the electromagnetic force supporting member 33 are sandwiched between the superconducting coil 31 and the lower plate 35.

支持部材33の取付は方法としては、超電導コイル31
と支持部材33に温度差を与え、熱膨張の差ですきまを
生じた状態において取付ける方法(いわゆる焼ばめ)や
、支持部材33を複数個に分割しておき、外周から圧力
を加えつつ溶接等により接続して取付ける方法が用いら
れる。
The supporting member 33 is attached using the superconducting coil 31.
There is a method of applying a temperature difference to the support member 33 and attaching it with a gap created due to the difference in thermal expansion (so-called shrink fit), or a method of dividing the support member 33 into multiple pieces and welding them while applying pressure from the outer periphery. A method of connecting and attaching is used.

また、上板34と下板35とは、支持部材33との接触
部36と37とにおいて溶接等にょシ固定される。
Further, the upper plate 34 and the lower plate 35 are fixed by welding or the like at contact portions 36 and 37 with the support member 33.

こうして形成した超電導コイルユニツ)30は、矢印3
8.39方向の電磁力を支持部材33が直接支持し、更
に上下板34.35が補強部材として作用するので、変
形がなく強固なユニットとなる。
The thus formed superconducting coil unit) 30 is shown by the arrow 3
Since the supporting member 33 directly supports the electromagnetic force in the 8.39 direction, and the upper and lower plates 34 and 35 act as reinforcing members, the unit becomes strong without deformation.

第2図は、コイル二二ッ)30を容器4に取付けた状態
を示す。容器4への取付けは、第1図示のボルト孔40
17C通したボルト41にょシ容器の内側部分4Aに固
定するだけでよく、極めて簡単である。
FIG. 2 shows the state in which the coil 22) 30 is attached to the container 4. For installation to the container 4, use the bolt hole 40 shown in the first diagram.
It is extremely simple, as it only needs to be fixed to the inner part 4A of the container using the bolt 41 passed through 17C.

本実施例によれば、以下のような効果が得られる。According to this embodiment, the following effects can be obtained.

(1)電磁力支持部材が超電導コイルに密接しているか
ら、従来の構造に比べて、第4図に示す磁極間隔1.が
短くなる。従って、容器全体を小形化できる。
(1) Since the electromagnetic force support member is in close contact with the superconducting coil, the magnetic pole spacing shown in FIG. 4 is 1. becomes shorter. Therefore, the entire container can be made smaller.

(2)磁極間隔1.を短くすると、第4図に示す偏向量
t2 も少なくなるので、容器の内側寸法t3を小さく
できる。
(2) Magnetic pole spacing 1. By shortening, the amount of deflection t2 shown in FIG. 4 also decreases, so the inner dimension t3 of the container can be reduced.

(3)容器の内側寸法t3を小さくすると、第3図に矢
印6A、6]3で示す方向の電磁力が小さくなシ、容器
4の内側部分4Aの厚さを薄くできる。
(3) By reducing the inner dimension t3 of the container, the electromagnetic force in the direction shown by arrows 6A, 6]3 in FIG. 3 is reduced, and the thickness of the inner portion 4A of the container 4 can be reduced.

(4)全体として小型軽量となるため、冷却用極低温冷
媒(液体ヘリウム)の使用量を削減可能である。
(4) Since the overall size is small and lightweight, the amount of cryogenic refrigerant (liquid helium) used for cooling can be reduced.

なお、上記実施例および第4図の模式図では、電子ビー
ムが曲がることにょム 1種数の波長の光だけが放射さ
れる場合を示したが、例えばコイルユニット2組でひと
つの磁極を形成し、コイルユニット6組を用いて、隣接
しある磁束方向が互いに逆方向であるようにした場合が
これに該当する。波長の異なる2種類以上の放射光を得
たいときは、それを直列接続すルばよい。このように多
数のコイルユニットを用いる場合、本発明の小型軽量化
の効果が特に著しい。
In addition, in the above embodiment and the schematic diagram in FIG. 4, the electron beam is bent and only light of one kind of wavelength is emitted. However, for example, two sets of coil units form one magnetic pole. However, this applies to the case where six sets of coil units are used so that adjacent magnetic flux directions are opposite to each other. If you want to obtain two or more types of emitted light with different wavelengths, you can connect them in series. When such a large number of coil units are used, the effect of the present invention in reducing the size and weight is particularly remarkable.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、超電導コイルの周囲を支持部材で取巻
きしかも上下板で更に補強することになるので、磁極間
隔を長くとる必要がなく、超電導コイルの変形を押える
容器が小型軽量の超電導磁石を備えた超電導磁界発生装
置が得られる。
According to the present invention, since the superconducting coil is surrounded by a supporting member and further reinforced by upper and lower plates, there is no need to increase the distance between the magnetic poles, and the container that suppresses deformation of the superconducting coil can be used as a small and lightweight superconducting magnet. A superconducting magnetic field generator equipped with the above is obtained.

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

第1図は本発明による超電導磁石を示す部分断面図、第
2図はその超電導磁石を用いる超電導磁界発生装置を示
す部分断面図、第3図は従来の超電導磁界発生装置を示
す部分断面図、第4図は電子ビームの方向と磁極の配列
を平面的に示す模式1・・・超電導コイル、2・・・押
え板、3・・・ボルト、4・・・容器、4A・・・容器
の内側部分、5A、5B。 6A、6B・・・超電導コイルに働く電磁力の方向、7
・・・当て板、8・・・支持板、9・・・ボルト、10
・・・押しボルト、11・・・電子ビームの方向、21
,22゜23・・・磁極、30・・・コイルユニット、
31・・・超を導コイル、32・・・スペーサ、33・
・・支持部材、34・・・上板、35・・・下板、36
.37・・・支持部材と上下板との接合部、38.39
・・・超電導コイルに働く電磁力の方向、40・・・ボ
ルト孔、41・・・ボルト。
FIG. 1 is a partial sectional view showing a superconducting magnet according to the present invention, FIG. 2 is a partial sectional view showing a superconducting magnetic field generator using the superconducting magnet, and FIG. 3 is a partial sectional view showing a conventional superconducting magnetic field generating device. Figure 4 is a schematic diagram showing the direction of the electron beam and the arrangement of magnetic poles in plan view. 1... superconducting coil, 2... holding plate, 3... bolt, 4... container, 4A... container. Inner part, 5A, 5B. 6A, 6B... Direction of electromagnetic force acting on the superconducting coil, 7
... Backing plate, 8... Support plate, 9... Bolt, 10
... Push bolt, 11 ... Direction of electron beam, 21
, 22° 23... Magnetic pole, 30... Coil unit,
31... Super conducting coil, 32... Spacer, 33...
...Supporting member, 34...Upper plate, 35...Lower plate, 36
.. 37...Joint part between support member and upper and lower plates, 38.39
...Direction of electromagnetic force acting on the superconducting coil, 40...Bolt hole, 41...Volt.

Claims (1)

【特許請求の範囲】 1、電磁力により電子軌道を曲げて光を放射するシンク
ロトロン軌道放射装置等に用いる超電導磁界発生装置に
おいて、超電導コイルの周囲を電磁力支持部材で取巻い
てコイルユニットを形成し、複数のコイルユニットをひ
とつの極低温容器内に収納した超電導磁石を備えたこと
を特徴とする超電導磁界発生装置。 2、特許請求の範囲第1項において、超電導コイルと電
磁力支持部材との間に冷媒を通すスペースを形成したコ
イルユニットを用いることを特徴とする超電導磁界発生
装置。 3、特許請求の範囲第1項または第2項において、電磁
力支持部材が上下板と溶接等により固定され補強されて
いることを特徴とする超電導磁界発生装置。 4、上記特許請求の範囲のいずれか一項において、コイ
ルユニットは6個以上であり、コイルユニット2個1組
でひとつの磁極を形成し、隣接しあう磁極の磁束方向が
互いに逆方向であることを特徴とする超電導磁界発生装
置。
[Claims] 1. In a superconducting magnetic field generator used in a synchrotron orbital radiator, etc. that emits light by bending electron orbits using electromagnetic force, a coil unit is constructed by surrounding a superconducting coil with an electromagnetic force supporting member. 1. A superconducting magnetic field generator characterized by comprising a superconducting magnet in which a plurality of coil units are formed and housed in a single cryogenic container. 2. A superconducting magnetic field generating device according to claim 1, characterized in that a coil unit is used in which a space for passing a coolant is formed between the superconducting coil and the electromagnetic force supporting member. 3. A superconducting magnetic field generating device according to claim 1 or 2, characterized in that the electromagnetic force supporting member is fixed and reinforced to the upper and lower plates by welding or the like. 4. In any one of the above claims, there are six or more coil units, one set of two coil units forms one magnetic pole, and the magnetic flux directions of adjacent magnetic poles are opposite to each other. A superconducting magnetic field generator characterized by:
JP59139299A 1984-07-05 1984-07-05 Superconducting magnetic field generator Pending JPS6119104A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59139299A JPS6119104A (en) 1984-07-05 1984-07-05 Superconducting magnetic field generator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59139299A JPS6119104A (en) 1984-07-05 1984-07-05 Superconducting magnetic field generator

Publications (1)

Publication Number Publication Date
JPS6119104A true JPS6119104A (en) 1986-01-28

Family

ID=15242043

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59139299A Pending JPS6119104A (en) 1984-07-05 1984-07-05 Superconducting magnetic field generator

Country Status (1)

Country Link
JP (1) JPS6119104A (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5588309A (en) * 1978-12-27 1980-07-04 Japan Atom Energy Res Inst Coil supporting device

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5588309A (en) * 1978-12-27 1980-07-04 Japan Atom Energy Res Inst Coil supporting device

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