JPH0620011B2 - Superconducting magnetic field generator - Google Patents

Superconducting magnetic field generator

Info

Publication number
JPH0620011B2
JPH0620011B2 JP58245868A JP24586883A JPH0620011B2 JP H0620011 B2 JPH0620011 B2 JP H0620011B2 JP 58245868 A JP58245868 A JP 58245868A JP 24586883 A JP24586883 A JP 24586883A JP H0620011 B2 JPH0620011 B2 JP H0620011B2
Authority
JP
Japan
Prior art keywords
superconducting
magnetic field
solenoid coil
field generator
superconductor
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.)
Expired - Lifetime
Application number
JP58245868A
Other languages
Japanese (ja)
Other versions
JPS60142506A (en
Inventor
孝司 小林
邦茂 黒田
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 JP58245868A priority Critical patent/JPH0620011B2/en
Publication of JPS60142506A publication Critical patent/JPS60142506A/en
Publication of JPH0620011B2 publication Critical patent/JPH0620011B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F6/00Superconducting magnets; Superconducting coils
    • H01F6/02Quenching; Protection arrangements during quenching

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Magnetic Resonance Imaging Apparatus (AREA)
  • Superconductor Devices And Manufacturing Methods Thereof (AREA)
  • Containers, Films, And Cooling For Superconductive Devices (AREA)

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、特に超電導ソレノ
イドコイル、この超電導ソレノイドコイルと直列に接続
された補正用超電導コイル、これら両者のコイルを収納
している液体ヘリウム容器および超電導体等を有してい
る超電導磁界発生装置に関するものである。
The present invention relates to a superconducting magnetic field generator, and more particularly to a superconducting solenoid coil, a correction superconducting coil connected in series with the superconducting solenoid coil, and both coils. The present invention relates to a superconducting magnetic field generator having a liquid helium container, a superconductor, and the like.

〔発明の背景〕[Background of the Invention]

第1図は核磁気共鳴診断装置に用いられている超電導磁
界発生装置の従来例が示されている。同図に示されてい
るように超電導磁界発生装置は超電導ソレノイドコイル
1、補正用超電導コイル2a,2b、これらおよび寒剤
である液体ヘリウム3を収納している液体ヘリウム容器
4、この液体ヘリウム容器4を真空断熱槽5を介して包
囲している液体窒素容器6、この液体窒素容器6を真空
断熱槽7を介して包囲している外壁8等より構成されて
いる。そして超電導ソレノイドコイル1は核磁気共鳴に
必要な磁界を発生させ、補正用超電導コイル2a,2b
はこの磁界を中心空間9で高均一度にしており、この中
心空間である高均一度空間9の高均一度磁界を利用して
核磁気共鳴診断が行なわれている。
FIG. 1 shows a conventional example of a superconducting magnetic field generator used in a nuclear magnetic resonance diagnostic apparatus. As shown in the figure, the superconducting magnetic field generator comprises a superconducting solenoid coil 1, correction superconducting coils 2a and 2b, a liquid helium container 4 containing these and liquid helium 3 as a cryogen, and this liquid helium container 4 Is constituted by a liquid nitrogen container 6 which surrounds the liquid nitrogen container 5 through a vacuum heat insulating tank 5, an outer wall 8 which surrounds the liquid nitrogen container 6 through a vacuum heat insulating tank 7, and the like. The superconducting solenoid coil 1 generates a magnetic field necessary for nuclear magnetic resonance, and the correction superconducting coils 2a and 2b
This magnetic field has a high homogeneity in the central space 9, and a nuclear magnetic resonance diagnosis is performed using the high homogeneity magnetic field of the high homogeneity space 9 which is the central space.

このように構成された超電導磁界発生装置で外部で磁界
妨害が生じた場合には直接高均一度空間9に影響を与
え、磁界の均一度が低下して診断に支障をきたしてい
た。
In the superconducting magnetic field generator configured as described above, when magnetic field disturbance occurs outside, it directly affects the high homogeneity space 9, and the homogeneity of the magnetic field deteriorates, which hinders diagnosis.

第2図にはこれに代る超電導磁界発生装置の従来例が示
されている。これは超電導ソレノイドコイル1および補
正用超電導コイル2a,2bの外周側に、超電導ソレノ
イドコイル1と同芯でかつ中心が一致している肉厚の薄
い中空円筒状の超電導体10を設け、この超電導体10
で外乱磁界の影響を除去するようにしたものである。こ
の貫通する穴を有した超電導体10はその穴を通る磁束
を一定に保つ性質があるので、この性質を利用して外乱
磁界の影響を軽減する。すなわち超電導体10には開口
部を通る磁束を一定にする作用があるが、これは外乱磁
界が生じた際にはこの外乱磁界と反対向きで、同じ大き
さの磁界を発生させるような電流、すなわち反磁性電流
が超電導体10に流れ、外乱磁界を打ち消し、磁束を一
定に保持する。しかしこの超電導磁界発生装置では反磁
性電流が超電導ソレノイドコイル1に蔽つている超電導
体10全体にわたつて流れ、高均一度空間9の磁界の淫
れを大きくしてしまう欠点を有していた。
FIG. 2 shows a conventional example of a superconducting magnetic field generator which replaces this. The superconducting solenoid coil 1 and the correction superconducting coils 2a and 2b are provided with thin walled hollow cylindrical superconductors 10 which are concentric with the superconducting solenoid coil 1 and whose centers coincide with each other. Body 10
The effect of the disturbance magnetic field is removed by. Since the superconductor 10 having the through hole has a property of keeping the magnetic flux passing through the hole constant, the effect of the disturbance magnetic field is reduced by utilizing this property. That is, the superconductor 10 has a function of making the magnetic flux passing through the opening constant, but when a disturbance magnetic field is generated, this is a current that is in the opposite direction to the disturbance magnetic field and generates a magnetic field of the same magnitude, That is, a diamagnetic current flows through the superconductor 10 to cancel the disturbance magnetic field and keep the magnetic flux constant. However, in this superconducting magnetic field generator, the diamagnetic current flows over the entire superconducting conductor 10 covering the superconducting solenoid coil 1 and has a drawback that the magnetic field in the high homogeneity space 9 becomes unpleasant.

〔発明の目的〕[Object of the Invention]

本発明は以上の点に鑑みなされたものであり、外乱磁界
の影響を軽減し、かつ高均一磁界の保持を可能とした超
電導磁界発生装置を提供することを目的とするものであ
る。
The present invention has been made in view of the above points, and an object of the present invention is to provide a superconducting magnetic field generator capable of reducing the influence of a disturbance magnetic field and maintaining a highly uniform magnetic field.

〔発明の概要〕[Outline of Invention]

すなわち本発明は超電導ソレノイドコイルと、この超電
導ソレノイドコイルと直列に接続された補正用超電導コ
イルと、これら両者のコイルを収納している液体ヘリウ
ム容器とを備え、前記超電導ソレノイドコイルの周囲に
外乱磁界の影響を除去する超電導体が設けられている超
電導磁界発生装置において、前記超電導体の断面積を前
記超電導ソレノイドコイルの断面積に比べ小さく形成す
ると共に、この超電導体を前記超電導ソレノイドコイル
と同軸で超電導ソレノイドコイルの少なくとも軸方向両
側に設け、かつこの夫々の超電導体に超電導状態から常
電導状態に転移する永久電流スイッチを具備させたこと
を特徴とするものであり、これによって反磁性電流は超
電導ソレノイドコイルの断面積より小さな断面積の超電
導体を流れるようになる。
That is, the present invention comprises a superconducting solenoid coil, a correction superconducting coil connected in series with the superconducting solenoid coil, and a liquid helium container accommodating both coils, and a disturbance magnetic field around the superconducting solenoid coil. In a superconducting magnetic field generator provided with a superconductor for removing the effect of, the cross-sectional area of the superconductor is formed smaller than the cross-sectional area of the superconducting solenoid coil, and the superconductor is coaxial with the superconducting solenoid coil. The superconducting solenoid coil is provided at least on both sides in the axial direction, and each of these superconductors is provided with a persistent current switch for transitioning from a superconducting state to a normal conducting state. So that it flows through a superconductor with a cross-sectional area smaller than that of the solenoid coil. It made.

〔発明の実施例〕Example of Invention

以下、図示した実施例に基づいて本発明を説明する。第
3図から第5図には本発明の一実施例が示されている。
なお従来と同じ部品には同じ符号を付したので説明を省
略する。本実施例では超電導体10a,10bの断面積
(断面11)を超電導レノイドコイル1の断面積に比べ
小さく形成すると共に、この超電導体10a,10bを
超電導ソレノイドコイル1と同軸で超電導ソレノイドコ
イル1の軸方向両側に設け、かつこの夫々の超電導体1
0a、10bに超電導状態から常電導状態に転移する永
久電流スイッチ12a、12bを具備させた。このよう
にすることにより反磁性電流は断面の小さな超電導体1
0a,10bを流れるようになつて、高均一磁界9(高
均一度空間)に影響を及ぼさないようになり、外乱磁界
の影響を軽減し、かつ高均一度磁界9の保持を可能とし
た超電導磁界発生装置を得ることができる。
Hereinafter, the present invention will be described based on the illustrated embodiments. One embodiment of the present invention is shown in FIGS.
Since the same parts as those of the prior art are designated by the same reference numerals, the description thereof will be omitted. In the present embodiment, the cross-sectional area (cross-section 11) of the superconductors 10a and 10b is made smaller than the cross-sectional area of the superconducting rhenoid coil 1, and the superconductors 10a and 10b are coaxial with the superconducting solenoid coil 1 and the axis of the superconducting solenoid coil 1 is the same. Provided on both sides in the direction, and each of these superconductors 1
0a and 10b were equipped with persistent current switches 12a and 12b that transition from a superconducting state to a normal conducting state. By doing so, the diamagnetic current is reduced to the superconductor 1 having a small cross section.
0a, 10b, the high-conductivity magnetic field 9 (high-uniformity space) is not affected, the influence of the disturbance magnetic field is reduced, and the high-uniformity magnetic field 9 can be maintained. A magnetic field generator can be obtained.

すなわち超電導ソレノイドコイル1の軸端に閉回路を形
成する超電導体10a,10bを、超電導ソレノイドコ
イル1と共軸で、かつ中心対称に一対設けた。そしてこ
の超電導体10a,10bにはこれを超電導状態から常
電導状態に転移させる永久電流スイツチ12a,12b
を設けると共に、その断面11を従来に比べて小さくし
た。断面11を小さくするには一重巻線または多重巻線
を使用し一重巻線で形成した断面11a,多重巻線で形
成した断面11bのいずれであつてもよい。このように
することにより外乱磁界が発生した場合に超電導体10
a,10bには反磁性電流が流れて外乱磁界を打ち消す
と共に、その断面を小さくしたので従来のように超電導
ソレノイドコイル1全体を蔽つて流れず、流れる部分が
小さくなつて、高均一度空間9に影響を及ぼさないよう
になる。
That is, a pair of superconductors 10a and 10b forming a closed circuit are provided at the shaft end of the superconducting solenoid coil 1 coaxially with the superconducting solenoid coil 1 and symmetrically about the center. The superconductors 10a and 10b are provided with permanent current switches 12a and 12b for transferring the superconductors from the superconducting state to the normal conducting state.
And the cross-section 11 thereof is made smaller than the conventional one. To reduce the cross section 11, a single winding or a multiple winding may be used to form a single winding 11a or a multiple winding 11b. By doing so, when a disturbance magnetic field is generated, the superconductor 10
A diamagnetic current flows through a and 10b to cancel the disturbance magnetic field, and because its cross section is made smaller, it does not flow over the entire superconducting solenoid coil 1 as in the conventional case. Will not affect.

すなわち超電導ソレノイドコイル1および補正用超電導
コイル2a,2bを超電導コイル用電源13で励起する
際に、ヒータ用電源14でヒータ線15,15a,15
bを加熱し、永久電流スイツチ12,12a,12bを
超電導状態から常電導状態に転移させる。そして超電導
ソレノイドコイル1および補正用超電導コイル2a,2
bを励磁し、これらのコイル1,2a,2bの合成磁界
が所定の値に達した時にヒータ線15,15a,15b
に流れる電流を切り、永久電流スイツチ12,12a,
12bを常電導状態から超電導状態に転移させる。この
ようにすると超電導ソレノイドコイル1と補正用超電導
コイル2a,2bとからなる閉回路および超電導体10
a,10bの閉回路は永久電流状態になり、高均一度磁
界9を安定に保持する。そして外乱磁界が生じた際は上
述のように超電導体10a,10bに反磁性電流が流れ
て外乱磁界を打ち消すが、この反磁性電流は超電導体1
0a,10bの断面11の小さな閉回路を流れるので、
高均一度磁界9への影響が軽減でき、高均一磁界9が安
定に保持できる。
That is, when the superconducting solenoid coil 1 and the correction superconducting coils 2a and 2b are excited by the superconducting coil power source 13, the heater power source 14 heats the heater wires 15, 15a, 15b.
b is heated to cause the permanent current switches 12, 12a, 12b to transition from the superconducting state to the normal conducting state. The superconducting solenoid coil 1 and the correction superconducting coils 2a, 2
b is excited, and when the combined magnetic field of these coils 1, 2a, 2b reaches a predetermined value, the heater wires 15, 15a, 15b
The current flowing through the switch to turn off the permanent current switch 12, 12a,
12b is changed from the normal conducting state to the superconducting state. In this way, the closed circuit including the superconducting solenoid coil 1 and the correction superconducting coils 2a and 2b and the superconductor 10 are formed.
The closed circuit of a and 10b becomes a permanent current state, and stably holds the high-uniformity magnetic field 9. When a disturbance magnetic field is generated, a diamagnetic current flows through the superconductors 10a and 10b to cancel the disturbance magnetic field as described above.
Since it flows through a small closed circuit of cross section 11 of 0a and 10b,
The influence on the highly uniform magnetic field 9 can be reduced, and the highly uniform magnetic field 9 can be stably maintained.

第6図には本発明の他の実施例が示されている。本実施
例では超電導ソレノイドコイル1の軸端に断面が小さく
閉回路を形成する超電導体10c,10dおよび10
e,10fを超電導ソレノイドコイルと共軸で、かつ中
心対称に二対設けた。そして超電導ソレノイドコイル1
の外周上に超電導ソレノイドコイル1と同芯で、中心対
称な超電導体10g,10hを設けた。この超電導体1
0g,10hも断面の小さな閉回路に形成したことは云
うまでもない。このよに超電導体10c,10d,10
e,10f,10g,10hを多段に設けたので、前述
の場合よりも外乱磁界の影響を多段にわたつて防止する
ことができ、高均一度磁界9を安定に保持することがで
きる。
FIG. 6 shows another embodiment of the present invention. In this embodiment, superconductors 10c, 10d and 10 having a small cross section and a closed circuit are formed at the shaft end of the superconducting solenoid coil 1.
Two pairs of e and 10f were provided coaxially with the superconducting solenoid coil and symmetrically about the center. And superconducting solenoid coil 1
Centrally symmetric superconductors 10g and 10h which are concentric with the superconducting solenoid coil 1 are provided on the outer periphery of the. This superconductor 1
It goes without saying that 0g and 10h are also formed in a closed circuit having a small cross section. Thus, the superconductors 10c, 10d, 10
Since e, 10f, 10g, and 10h are provided in multiple stages, the influence of the disturbance magnetic field can be prevented over multiple stages as compared with the case described above, and the high-uniformity magnetic field 9 can be stably held.

第7図には本発明に更に他の実施例が示されている。本
実施例では超電導体10c,10dを超電導ソレノイド
コイル1の軸方向の液体ヘリウム容器4の内壁に、超電
導体10g,10hを超電導ソレノイドコイル1の径方
向の液体ヘリウム容器4の内壁に夫々固定した。このよ
うにすることにより、超電導体10c,10d,10
g,10hの位置設定および固定を前述の場合よりも精
度よく、かつ容易にすることができる。
FIG. 7 shows still another embodiment of the present invention. In this embodiment, the superconductors 10c and 10d are fixed to the inner wall of the liquid helium container 4 in the axial direction of the superconducting solenoid coil 1, and the superconductors 10g and 10h are fixed to the inner wall of the liquid helium container 4 in the radial direction of the superconducting solenoid coil 1. . By doing so, the superconductors 10c, 10d, 10
Position setting and fixing of g and 10h can be performed more accurately and easily than in the case described above.

第8図には本発明の更に他の実施例が示されている。本
実施例では超電導体10c,10dを超電導ソレノイド
コイル1の軸方向の液体エリウム容器4の外壁に、超電
導体10g,10hを超電導ソレノイドコイル1の径方
向の液体ヘリウム容器4の外壁に夫々固定した。この場
合にも超電導体10c,10d,10g,10hの位置
設定が精度よく、固定を容易にすることができるように
なつて、前述の場合と同様な作用効果を奏することがで
きる。
FIG. 8 shows still another embodiment of the present invention. In this embodiment, the superconductors 10c and 10d are fixed to the outer wall of the liquid helium container 4 in the axial direction of the superconducting solenoid coil 1, and the superconductors 10g and 10h are fixed to the outer wall of the liquid helium container 4 in the radial direction of the superconducting solenoid coil 1. . Also in this case, the superconductors 10c, 10d, 10g, and 10h can be accurately set in position and can be easily fixed, and the same effect as the above case can be obtained.

第9図には本発明の更に他の実施例が示されている。本
実施例では超電導体10i,10jをくら形で形成し
た。この場合にも前述の場合と同様な作用効果を奏する
ことができる。
FIG. 9 shows still another embodiment of the present invention. In this embodiment, the superconductors 10i and 10j are formed in a square shape. In this case as well, it is possible to obtain the same effects as the above-mentioned case.

なお本実施例ではリング状の超電導体10a〜10hお
よびくら形の超電導体10i,10jをわけて使用する
ようにしたがこれに限るものではなく、これら両者を併
用するようにしてもよい。
In this embodiment, the ring-shaped superconductors 10a to 10h and the paddle-shaped superconductors 10i and 10j are used separately, but the present invention is not limited to this, and both may be used together.

〔発明の効果〕〔The invention's effect〕

上述のように本発明は超電導体に流れる反磁性電流が外
乱磁界は打ち消すが、高均一度磁界には影響を及ぼさな
いようになつて、外乱磁界の影響を軽減し、かつ高均一
度磁界の保持を可能とした超電導磁界発生装置を得るこ
とができる。
As described above, in the present invention, the diamagnetic current flowing in the superconductor cancels the disturbance magnetic field, but does not affect the high homogeneity magnetic field, so that the influence of the disturbance magnetic field can be reduced and the high homogeneity magnetic field can be reduced. It is possible to obtain a superconducting magnetic field generator capable of holding.

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

第1図は従来の超電導磁界発生装置の縦断側面図、第2
図は従来の超電導磁界発生装置の他の例の超電算磁界発
生装置要部の縦断面図、第3図は本発明の超電導磁界発
生装置の一実施例の超電導磁界発生装置要部の縦断側面
図、第4図は同じく一実施例の超電導体の一部縦断正面
図、第5図は第3図の等価回路図、第6図は本発明の超
電導磁界発生装置の他の実施例の超電導磁界発生装置要
部の縦断側面図、第7図は本発明の超電導磁界発生装置
の更に他の実施例の超電導磁界発生装置要部の縦断側面
図、第8図は本発明の超電導磁界発生装置の更に他の実
施例の超電導磁界発生装置要部の縦断側面図、第9図は
本発明の超電導磁界発生装置の更に他の実施例の超電導
磁界発生装置要部の正面および側面図である。 1……超電導ソレノイドコイル、2a,2b……補正用
超電導コイル、4……液体ヘリウム容器、9……高均一
度磁界(空間)、10a,10b,10c,10d,1
0e,10f,10g,10h,10i,10j……超
電導体、11……断面、12,12a,12b……永久
電流スイツチ、13……超電導コイル用電源、14……
ヒータ用電源、15,15a,15b……ヒータ線。
FIG. 1 is a vertical sectional side view of a conventional superconducting magnetic field generator, and FIG.
FIG. 3 is a vertical cross-sectional view of a main part of a superconducting magnetic field generator of another example of the conventional superconducting magnetic field generator, and FIG. FIG. 4 is a partially longitudinal front view of a superconductor of the same embodiment, FIG. 5 is an equivalent circuit diagram of FIG. 3, and FIG. 6 is a superconducting device of another embodiment of the superconducting magnetic field generator of the present invention. FIG. 7 is a vertical sectional side view of a main part of a magnetic field generator, FIG. 7 is a vertical sectional side view of a main part of a superconducting magnetic field generator of still another embodiment of the superconducting magnetic field generator of the present invention, and FIG. 8 is a superconducting magnetic field generator of the present invention. FIG. 9 is a vertical sectional side view of a main part of a superconducting magnetic field generator according to still another embodiment of the present invention. FIG. 9 is a front view and a side view of a main part of a superconducting magnetic field generator according to still another embodiment of the superconducting magnetic field generator of the present invention. 1 ... Superconducting solenoid coil, 2a, 2b ... Correction superconducting coil, 4 ... Liquid helium container, 9 ... Highly uniform magnetic field (space), 10a, 10b, 10c, 10d, 1
0e, 10f, 10g, 10h, 10i, 10j ... Superconductor, 11 ... Section, 12, 12a, 12b ... Permanent current switch, 13 ... Superconducting coil power supply, 14 ...
Power supply for heater, 15, 15a, 15b ... Heater wire.

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】超電導ソレノイドコイルと、この超電導ソ
レノイドコイルと直列に接続された補正用超電導コイル
と、これら両者のコイルを収納している液体ヘリウム容
器とを備え、前記超電導ソレノイドコイルの周囲に外乱
磁界の影響を除去する超電導体が設けられている超電導
磁界発生装置において、前記超電導体の断面積を前記超
電導ソレノイドコイルの断面積に比べ小さく形成すると
共に、この超電導体を前記超電導ソレノイドコイルと同
軸で超電導ソレノイドコイルの少なくとも軸方向両側に
設け、かつこの夫々の超電導体に超電導状態から常電導
状態に転移する永久電流スイッチを具備させたことを特
徴とする超電導磁界発生装置。
1. A superconducting solenoid coil, a correction superconducting coil connected in series with the superconducting solenoid coil, and a liquid helium container accommodating both of these coils, and a disturbance around the superconducting solenoid coil. In a superconducting magnetic field generator provided with a superconductor for removing the influence of a magnetic field, a cross-sectional area of the superconductor is formed smaller than that of the superconducting solenoid coil, and the superconductor is coaxial with the superconducting solenoid coil. 2. A superconducting magnetic field generator, characterized in that it is provided on at least both axial sides of a superconducting solenoid coil, and each of these superconductors is provided with a persistent current switch for transitioning from a superconducting state to a normal conducting state.
【請求項2】前記超電導体が、前記液体ヘリウム容器の
内壁面もしくは外壁面に配置されたものである特許請求
の範囲第1項記載の超電導磁界発生装置。
2. The superconducting magnetic field generator according to claim 1, wherein the superconductor is arranged on an inner wall surface or an outer wall surface of the liquid helium container.
【請求項3】前記超電導体の内径を、前記超電導ソレノ
イドコイルの内径より大きくしたことを特徴とする特許
請求の範囲第1項記載の超電導磁界発生装置。
3. The superconducting magnetic field generator according to claim 1, wherein an inner diameter of the superconductor is larger than an inner diameter of the superconducting solenoid coil.
JP58245868A 1983-12-29 1983-12-29 Superconducting magnetic field generator Expired - Lifetime JPH0620011B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58245868A JPH0620011B2 (en) 1983-12-29 1983-12-29 Superconducting magnetic field generator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58245868A JPH0620011B2 (en) 1983-12-29 1983-12-29 Superconducting magnetic field generator

Publications (2)

Publication Number Publication Date
JPS60142506A JPS60142506A (en) 1985-07-27
JPH0620011B2 true JPH0620011B2 (en) 1994-03-16

Family

ID=17140009

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58245868A Expired - Lifetime JPH0620011B2 (en) 1983-12-29 1983-12-29 Superconducting magnetic field generator

Country Status (1)

Country Link
JP (1) JPH0620011B2 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3829207A1 (en) * 1988-08-29 1990-03-08 Licentia Gmbh Current-limiting induction coil
GB9016184D0 (en) * 1990-07-24 1990-09-05 Oxford Magnet Tech Magnet assembly
JP3731231B2 (en) 1995-11-30 2006-01-05 株式会社日立メディコ Superconducting magnet device

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6058562B2 (en) * 1977-02-09 1985-12-20 古河電気工業株式会社 Method for adjusting magnetic field distribution of superconducting magnets
JPS58186915A (en) * 1982-04-26 1983-11-01 Mitsubishi Electric Corp Superconductive magnet

Also Published As

Publication number Publication date
JPS60142506A (en) 1985-07-27

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