JPS6351524B2 - - Google Patents
Info
- Publication number
- JPS6351524B2 JPS6351524B2 JP1933082A JP1933082A JPS6351524B2 JP S6351524 B2 JPS6351524 B2 JP S6351524B2 JP 1933082 A JP1933082 A JP 1933082A JP 1933082 A JP1933082 A JP 1933082A JP S6351524 B2 JPS6351524 B2 JP S6351524B2
- Authority
- JP
- Japan
- Prior art keywords
- superconducting
- coil
- superconducting coil
- cryocase
- walls
- 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
Links
- 239000003507 refrigerant Substances 0.000 claims 2
- 239000000853 adhesive Substances 0.000 claims 1
- 230000001070 adhesive effect Effects 0.000 claims 1
- 125000006850 spacer group Chemical group 0.000 claims 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F6/00—Superconducting magnets; Superconducting coils
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Containers, Films, And Cooling For Superconductive Devices (AREA)
- Magnetic Resonance Imaging Apparatus (AREA)
Description
【発明の詳細な説明】
〔発明の技術分野〕
本発明は、超電導マグネツトに係り、特に超電
導コイルの固定手段を改良した超電導マグネツト
に関する。DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a superconducting magnet, and more particularly to a superconducting magnet with improved fixing means for superconducting coils.
一般に、超電導マグネツトにおいて、安定した
動作を行なわせるためには、超電導マグネツトの
主要部である超電導コイルを常に超電導状態にし
ておく必要がある。すなわち、超電導コイルを形
成する超電導線を常電導転移温度以下に冷却する
とともに通電時に生じる電磁力で超電導線に歪が
生じないようにするため、超電導コイルの周囲に
液体ヘリウム等の冷媒を通流させることによつて
冷却するとともに、たとえば超電導コイルを支持
する支持体の剛性を大きくすることによつて超電
導コイルを形成する超電導線に歪が生じないよう
に配慮されている。
Generally, in order to ensure stable operation of a superconducting magnet, it is necessary to keep the superconducting coil, which is the main part of the superconducting magnet, in a superconducting state at all times. In other words, a coolant such as liquid helium is passed around the superconducting coil in order to cool the superconducting wire that forms the superconducting coil to below the normal conduction transition temperature and to prevent distortion of the superconducting wire due to the electromagnetic force generated when electricity is applied. In addition to cooling the superconducting coil by increasing the rigidity of the support that supports the superconducting coil, consideration is given to preventing distortion from occurring in the superconducting wire that forms the superconducting coil.
第1図は上述のような対策を施した超電導マグ
ネツトの一例の要部を示す断面図である。すなわ
ち、内部に冷媒を収容したクライオケース1内に
剛性を向上させるために樹脂等の含浸材に浸して
製作されたモールド型の超電導コイル2を収容
し、この超電導コイル2をこの超電導コイル2と
クライオケース1の内面3との間に介挿されたス
ペーサ4a,4b,4c,4dおよび上記クライ
オケース1の両側壁の内面3に形成された凹部5
に嵌入固定された支持材6およびこの支持材6と
上記超電導コイル2との間に介挿された別のスペ
ーサ7等で固定するようにしている。 FIG. 1 is a cross-sectional view showing a main part of an example of a superconducting magnet in which the above-mentioned measures have been taken. That is, a molded superconducting coil 2 manufactured by soaking it in an impregnating material such as resin to improve rigidity is housed in a cryocase 1 containing a refrigerant, and this superconducting coil 2 is spacers 4a, 4b, 4c, 4d inserted between the inner surface 3 of the cryo case 1 and the recesses 5 formed on the inner surfaces 3 of both side walls of the cryo case 1;
The superconducting coil 2 is fixed by a support member 6 fitted into and fixed to the superconducting coil 2, and another spacer 7 inserted between the support member 6 and the superconducting coil 2.
なお、超電導コイルの剛性を向上させる手段と
して、上述した構成以外にも超電導コイルの外周
面をステンレスワイヤで巻付固定するようにした
ものも考えられている。 As a means for improving the rigidity of the superconducting coil, in addition to the above-described configuration, a method in which the outer circumferential surface of the superconducting coil is wrapped and fixed with stainless steel wire is also being considered.
しかしながら、上記のように構成された超電導
マグネツトにあつては次のような問題があつた。
However, the superconducting magnet constructed as described above has the following problems.
すなわち、モールド型の超電導コイルあるいは
ステンレスワイヤによつて補強された超電導コイ
ルであつても、冷媒によつて上記超電導コイルを
冷却すると、超電導コイルを構成している超電導
線が熱収縮を起こし、超電導コイルとスペーサと
の間等に間隙が生じる。このように間隙が生じる
と超電導コイルはクライオケース内で比較的動き
やすい状態となり、この状態で上記超電導コイル
に電流を流すと、電磁力により超電導線に大きな
歪が発生する。その結果、超電導状態から常電導
状態に移行するクエンチ現象が発生し、安定した
動作を行なわせることができない虞れがあつた。
特に、二つの超電導コイルを対向して配置した超
電導マグネツトにおいては、二つの超電導コイル
相互間に大きな電磁力が作用するので上述した歪
が、より一層大きくなる問題があつた。 In other words, even if it is a molded superconducting coil or a superconducting coil reinforced with stainless steel wire, when the superconducting coil is cooled with a refrigerant, the superconducting wire that makes up the superconducting coil will undergo thermal contraction, and the superconducting coil will become superconducting. A gap is created between the coil and the spacer. When a gap is created in this way, the superconducting coil is in a state where it is relatively easy to move within the cryocase, and when a current is passed through the superconducting coil in this state, a large strain is generated in the superconducting wire due to electromagnetic force. As a result, a quench phenomenon occurs in which the superconducting state shifts to the normal conducting state, and there is a risk that stable operation may not be possible.
In particular, in a superconducting magnet in which two superconducting coils are disposed facing each other, a large electromagnetic force acts between the two superconducting coils, resulting in the problem that the above-mentioned distortion becomes even larger.
そこで、このような不具合を解消するために、
第1図のようにモールド型超電導コイルを使用す
る場合には、上記コイルの剛性を向上させるため
に含浸材の量を増加させて超電導コイルを厚い被
覆層で覆うことが考えられるが、このようにする
と、超電導線と冷媒との間の間隔が大きくなり、
冷却効果が低下するので、冷却用の液体ヘリウム
の使用量を増加させなければならない問題があ
る。 Therefore, in order to eliminate such problems,
When using a molded superconducting coil as shown in Figure 1, it is conceivable to increase the amount of impregnating material and cover the superconducting coil with a thick coating layer in order to improve the rigidity of the coil. , the distance between the superconducting wire and the refrigerant increases,
Since the cooling effect is reduced, there is a problem in that the amount of liquid helium used for cooling must be increased.
本発明は、このような事情に鑑みてなされたも
ので、その目的とするところは、簡単な構成で、
クライオケースと超電導コイルとをより強固に一
体化させることができ、これによつて結果的に超
電導コイルの剛性を上げることができ、もつて、
耐電磁力性に優れるとともに動作が安定であるこ
とから運転効率の向上化を図れる超電導マグネツ
トを提供することにある。
The present invention has been made in view of these circumstances, and its purpose is to have a simple configuration,
The cryocase and the superconducting coil can be more firmly integrated, and as a result, the rigidity of the superconducting coil can be increased.
The object of the present invention is to provide a superconducting magnet that has excellent resistance to electromagnetic force and is stable in operation, thereby improving operating efficiency.
本発明の超電導マグネツトは、クライオケース
の対向する2つの壁面間でモールド型超電導コイ
ルの両端面を支持させるようにするとともに2つ
の壁部と、超電導コイルの両端面との間に上記壁
部の内面およびコイルの両端面に接着剤で固定さ
れた冷媒通路形成用スペーサをそれぞれ介在さ
せ、さらに上記2つの壁部間を締結機構にて締付
固定してなることを特徴としている。
In the superconducting magnet of the present invention, both end faces of a molded superconducting coil are supported between two opposing wall faces of a cryo case, and the above-mentioned wall part is supported between the two wall parts and both end faces of the superconducting coil. It is characterized in that spacers for forming refrigerant passages fixed with adhesive are interposed on the inner surface and both end faces of the coil, and the two walls are further tightened and fixed by a fastening mechanism.
このような構成であると、液体ヘリウム等の冷
媒を超電導コイルの周囲に通流させて上記超電導
コイルを冷却すると、上記超電導コイルを構成す
る超電導線には熱収縮応力が加わり、上記超電導
コイルは収縮しようとする。しかし、超電導コイ
ルの両端面は接着剤、スペーサ、接着剤を介して
クライオケースに一体的に固定されており、また
上記超電導コイルを挾んだクライオケースの2つ
の壁部相互はボルト等の締結機構にて締付固定さ
れているので、上述の熱収縮応力が上記超電導コ
イルに加わつても、上記超電導コイルの端面と上
記壁部との間に間隙が生じるような虞れがない。
従つて、電磁力により上記超電導コイルが大きく
動くことはないので、超電導線に大きな歪が発生
するようなこともない。このためクエンチ現象の
発生を防止できる。
With such a configuration, when a refrigerant such as liquid helium is passed around the superconducting coil to cool the superconducting coil, thermal shrinkage stress is applied to the superconducting wire constituting the superconducting coil, and the superconducting coil trying to shrink. However, both end faces of the superconducting coil are integrally fixed to the cryo case via an adhesive, a spacer, or an adhesive, and the two walls of the cryo case that sandwich the superconducting coil are fastened together using bolts, etc. Since the superconducting coil is tightened and fixed by the mechanism, even if the above-mentioned heat shrinkage stress is applied to the superconducting coil, there is no possibility that a gap will be created between the end face of the superconducting coil and the wall portion.
Therefore, since the superconducting coil does not move significantly due to electromagnetic force, no large strain occurs in the superconducting wire. Therefore, the occurrence of the quench phenomenon can be prevented.
また、超電導コイルとクライオケースとをより
強固に一体化できるので、結果的に、超電導コイ
ルの剛性とクライオケースの剛性を向上させるこ
とができるので、コイルを被覆する樹脂被覆層を
薄くでき、これによつて超電導コイルを冷却する
ために必要な液体ヘリウムの量を低減化できるば
かりかクライオケースの肉厚も薄くでき、これに
よつて発生磁界の有効利用化を図ることができ
る。 In addition, since the superconducting coil and cryo case can be more firmly integrated, the rigidity of the superconducting coil and the cryo case can be improved, which allows the resin coating layer covering the coil to be made thinner. Not only can the amount of liquid helium required to cool the superconducting coil be reduced, but also the thickness of the cryocase can be made thinner, thereby making it possible to effectively utilize the generated magnetic field.
第2図は本発明の一実施例に係る超電導マグネ
ツトの概略構成を示す斜視図であり、第3図は第
2図におけるA−A線に沿つて切断し矢印方向に
見た断面図であり、第4図は同じくB−B線に沿
つて切断し矢印方向に見た切断図である。
FIG. 2 is a perspective view showing a schematic configuration of a superconducting magnet according to an embodiment of the present invention, and FIG. 3 is a cross-sectional view taken along line A-A in FIG. 2 and viewed in the direction of the arrow. , FIG. 4 is a cutaway view taken along the line B-B and viewed in the direction of the arrow.
図中11は、たとえばステンレス鋼板等でほぼ
直方体状に形成されたクライオケースである。こ
のクライオケース11の中央部には断面形状が逆
T字形をした風抜き用の空洞12が設けられてお
り、この空洞12の存在によつてクライオケース
11内に第3図に示すように2つの偏平状のコイ
ル収納部13a,13bが平行に形成されてい
る。そして各コイル収納部13a,13bには、
それぞれモールド型の超電導コイル14a,14
bが上記コイル収納部13a,13bを構成する
側壁15a,16aおよび15b,16bにその
両端面がそれぞれ支持される形にそれぞれ収納さ
れている。 In the figure, reference numeral 11 denotes a cryocase formed of, for example, a stainless steel plate or the like in a substantially rectangular parallelepiped shape. A venting cavity 12 having an inverted T-shaped cross section is provided in the center of the cryocase 11. Due to the existence of this cavity 12, two air vents are formed inside the cryocase 11 as shown in FIG. Two flat coil housing portions 13a and 13b are formed in parallel. And in each coil storage part 13a, 13b,
Molded superconducting coils 14a and 14, respectively.
b are housed in such a manner that both end surfaces thereof are supported by side walls 15a, 16a and 15b, 16b constituting the coil housing portions 13a, 13b, respectively.
上記超電導コイル14aとコイル収納部13a
を構成する側壁15a,16aとの間には第4図
に示すように、片面にスパイラル状の溝17を有
したスペーサ18が上記溝17を超電導コイル1
4aの端面に向け極低温用の接着剤19によつて
上記超電導コイル14aの両端面と上記側壁15
a,16aとに接着された状態に介挿されてい
る。なおもう一方の超電導コイル14bも同様に
コイル収納部13bに収納されている。 The superconducting coil 14a and the coil storage section 13a
As shown in FIG. 4, a spacer 18 having a spiral groove 17 on one side is provided between the side walls 15a and 16a constituting the superconducting coil 1.
Both end faces of the superconducting coil 14a and the side wall 15 are bonded to the end faces of the superconducting coil 14a with a cryogenic adhesive 19 toward the end face of the superconducting coil 14a.
a, 16a and are inserted in a bonded state. Note that the other superconducting coil 14b is similarly stored in the coil storage portion 13b.
しかして、前記コイル収納部13a,13bを
構成する前記側壁15a,16aとの間および1
5b,16bとの間には、これらの側壁を超電導
コイル14a,14bの内側位置において貫通
し、対向する上記側壁間を締付けるボルト20が
複数本ずつそれぞれ装着されており、外側位置に
はスペーサ28を介してボルト29が複数装着さ
れている。また、コイル収納部13a,13bの
図中上方空間には、前述した側壁と側壁とを連結
するための連結棒21が装着されている。さら
に、前記コイル収納部13a,13bの上部開口
端には、これらを共通に蓋する蓋体22が装着さ
れており、この蓋体22の中央部に上記コイル収
納部13a,13bに液体ヘリウム23を注入す
るための注入口24が設けられている。 Therefore, between the side walls 15a and 16a constituting the coil storage parts 13a and 13b, and
A plurality of bolts 20 are installed between the superconducting coils 14a and 16b at positions inside the superconducting coils 14a and 16b, respectively, to tighten the opposing side walls, and a spacer 28 is installed at the outside position. A plurality of bolts 29 are attached through the bolts. Furthermore, a connecting rod 21 for connecting the side walls described above is installed in the space above the coil storage portions 13a and 13b in the drawing. Further, a lid 22 is attached to the upper open end of the coil storage parts 13a, 13b to cover them in common, and a liquid helium 22 is placed in the center of the lid 22 to cover the coil storage parts 13a, 13b. An injection port 24 is provided for injecting.
なお、図中25,26は、上記コイル収納部1
3a,13bの側壁15a,15bを補強するた
めのボルトおよびスペーサである。 In addition, 25 and 26 in the figure are the above-mentioned coil storage part 1.
These are bolts and spacers for reinforcing the side walls 15a, 15b of 3a, 13b.
このように構成された超電導マグネツトにあつ
て、液体ヘリウム23を注入口24からコイル収
納部13a,13b内へ注入すると、上記液体ヘ
リウム23がスペーサ18の溝17を通流し超電
導コイル14a,14bの内側にも流入する。そ
して、上記コイル収納部13a,13b内に液体
ヘリウム23を充満させると、上記超電導コイル
14a,14bの外側面、内側面および両端面が
上記液体ヘリウム23に完全に接触するので、上
記超電導コイル14a,14bは超電導状態まで
冷却される。このような状態で超電導コイル14
a,14bに付勢電流を通流し、これを永久電流
モードに切換えることによつて各超電導コイル1
4a,14bに連続した高磁界を発生させること
ができる。 In the superconducting magnet constructed as described above, when liquid helium 23 is injected into the coil storage parts 13a, 13b from the injection port 24, the liquid helium 23 flows through the grooves 17 of the spacer 18 and flows into the superconducting coils 14a, 14b. It also flows inside. When the coil storage parts 13a and 13b are filled with liquid helium 23, the outer surfaces, inner surfaces and both end surfaces of the superconducting coils 14a and 14b completely contact the liquid helium 23, so that the superconducting coils 14a and 14b are completely in contact with the liquid helium 23. , 14b are cooled to a superconducting state. In this state, the superconducting coil 14
By passing an energizing current through a and 14b and switching it to persistent current mode, each superconducting coil 1
A continuous high magnetic field can be generated at 4a and 14b.
そして、この場合には、前述の如く側壁15
a,16a間および15b,16b間をボルト等
の締結機構で締付けるとともに超電導コイル14
a,14bの両端面を接着剤19〜スペーサ18
〜接着剤19を介して対応する各側壁に固定して
いるので、超電導コイル14a,14bと対応す
る側壁15a,16a,15b,16bとを完全
に機械的に一体化させることができる。したがつ
て、上述のように超電導コイル14a,14bを
絶対温度の零度近くまで冷却しても、上記超電導
コイル14a,14bと側壁15a,16a,1
5b,16bとの間に間隙が生じるようなことは
ない。したがつて、上記超電導コイル14a,1
4b間に第3図の矢印27で示す磁界による力F
が加わつた場合においても、上記超電導コイル1
4a,14bは大きく動くことはないので、超電
動線に大きな歪が発生するようなことはなく、し
たがつて、クエンチ現象の発生を防止でき、安定
した動作を行なわせることができる。 In this case, as described above, the side wall 15
A, 16a and 15b, 16b are tightened using a fastening mechanism such as a bolt, and the superconducting coil 14
Adhesive 19 to spacer 18 on both end surfaces of a and 14b
- Since the superconducting coils 14a and 14b are fixed to the corresponding side walls via the adhesive 19, the superconducting coils 14a and 14b and the corresponding side walls 15a, 16a, 15b and 16b can be completely mechanically integrated. Therefore, even if the superconducting coils 14a, 14b are cooled to near zero absolute temperature as described above, the superconducting coils 14a, 14b and the side walls 15a, 16a, 1
5b and 16b will not form a gap. Therefore, the superconducting coils 14a, 1
Force F due to the magnetic field shown by arrow 27 in FIG. 3 between 4b
Even when the superconducting coil 1
Since 4a and 14b do not move significantly, there is no possibility that a large strain will occur in the superelectric wire, and therefore, the occurrence of the quench phenomenon can be prevented and stable operation can be performed.
また、上記のように超電導コイル14a,14
bと各側壁とを強固に一体化することができるの
で、結果的に超電導コイル14a,14bの剛性
を上げることができる。したがつて、超電導コイ
ル14a,14bの樹脂被覆層の厚さを薄くする
ことができるので、冷却のための液体ヘリウム2
3の使用量の低減化を図ることができる。したが
つて運転費用の低減化を図れ、しかも安定した動
作が可能となる。 In addition, as described above, superconducting coils 14a, 14
b and each side wall can be firmly integrated, and as a result, the rigidity of the superconducting coils 14a, 14b can be increased. Therefore, since the thickness of the resin coating layer of the superconducting coils 14a and 14b can be reduced, liquid helium 2 for cooling can be reduced.
It is possible to reduce the usage amount of 3. Therefore, operating costs can be reduced and stable operation can be achieved.
さらに、クライオケース11のコイル収納部1
3a,13b全体の構造を超電導コイルを側壁で
挾んだサンドイツチ構造としているので、ハニカ
ム構造と同様に側壁等を薄く形成しても従来の装
置に比較して強度が大幅に低下することはない。
したがつて、超電導コイルを他の機器へより接近
させることができるので発生した磁界の効率的な
利用を図ることもでき、結局、前述した効果が得
られる。 Furthermore, the coil storage section 1 of the cryo case 11
Since the overall structure of 3a and 13b is a sandwich structure in which the superconducting coil is sandwiched between side walls, the strength will not be significantly reduced compared to conventional devices even if the side walls etc. are made thin like a honeycomb structure. .
Therefore, since the superconducting coil can be brought closer to other equipment, the generated magnetic field can be used more efficiently, and the above-mentioned effects can be obtained after all.
第1図は従来の超電導マグネツトの要部を取り
出して示す断面図、第2図は本発明の一実施例に
係る超電導マグネツトの一部を切欠して示す概略
構成斜視図、第3図は第2図におけるA−A線に
沿つて切断して矢印方向に見た断面図、第4図は
同じくB−B線に沿つて切断し矢印方向に見た断
面図である。
11……クライオケース、12……空洞、13
a,13b……コイル収納部、14a,14b…
…超電導コイル、15a,15b,16a,16
b……側壁、17……溝、18,26,28……
スペーサ、19……接着剤、20,25,29…
…ボルト、22……蓋体、23……液体ヘリウ
ム、24……注入口。
FIG. 1 is a sectional view showing the main parts of a conventional superconducting magnet, FIG. 2 is a partially cutaway schematic perspective view of a superconducting magnet according to an embodiment of the present invention, and FIG. 2 is a cross-sectional view taken along the line A--A and viewed in the direction of the arrow, and FIG. 4 is a cross-sectional view similarly taken along the line B--B and viewed in the direction of the arrow. 11...Cryocase, 12...Cavity, 13
a, 13b...Coil storage section, 14a, 14b...
...Superconducting coils, 15a, 15b, 16a, 16
b... Side wall, 17... Groove, 18, 26, 28...
Spacer, 19... Adhesive, 20, 25, 29...
...Bolt, 22...Lid, 23...Liquid helium, 24...Inlet.
Claims (1)
このクライオケース内に上記クライオケースの対
向する2つの壁部によつてその両端面が支持され
る関係に収容された樹脂モールド型超電導コイル
と、この超電導コイルの両端面と前記2つの壁部
との間にそれぞれ介在し、かつ上記2つの壁部の
内面および上記超電導コイルの両端面に接着剤で
固定された一対の冷媒通路形成用スペーサと、前
記2つの壁部間に締付力を付与する締結機構とを
具備してなることを特徴とする超電導マグネツ
ト。1 A cryocase in which a refrigerant is stored,
A resin-molded superconducting coil is housed in the cryocase in such a manner that both end faces thereof are supported by the two opposing walls of the cryocase, and both end faces of the superconducting coil and the two walls are supported by the two opposing walls of the cryocase. A pair of refrigerant passage forming spacers interposed between the two walls and fixed with adhesive to the inner surfaces of the two walls and both end surfaces of the superconducting coil, and applying a tightening force between the two walls. A superconducting magnet characterized by comprising a fastening mechanism.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1933082A JPS58137205A (en) | 1982-02-09 | 1982-02-09 | Superconductive magnet |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1933082A JPS58137205A (en) | 1982-02-09 | 1982-02-09 | Superconductive magnet |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58137205A JPS58137205A (en) | 1983-08-15 |
| JPS6351524B2 true JPS6351524B2 (en) | 1988-10-14 |
Family
ID=11996393
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1933082A Granted JPS58137205A (en) | 1982-02-09 | 1982-02-09 | Superconductive magnet |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58137205A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE19711373A1 (en) * | 1997-03-19 | 1998-09-24 | Alsthom Cge Alcatel | Spacers for an elongated substrate |
| GB2444507B (en) * | 2006-12-06 | 2010-09-29 | Siemens Magnet Technology Ltd | Wound in-situ moulded magnet end coil and method for production thereof |
-
1982
- 1982-02-09 JP JP1933082A patent/JPS58137205A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58137205A (en) | 1983-08-15 |
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