JPS5928042B2 - superconducting coil - Google Patents
superconducting coilInfo
- Publication number
- JPS5928042B2 JPS5928042B2 JP51017338A JP1733876A JPS5928042B2 JP S5928042 B2 JPS5928042 B2 JP S5928042B2 JP 51017338 A JP51017338 A JP 51017338A JP 1733876 A JP1733876 A JP 1733876A JP S5928042 B2 JPS5928042 B2 JP S5928042B2
- Authority
- JP
- Japan
- Prior art keywords
- coil
- groove
- superconducting
- superconducting coil
- cooling medium
- 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
- 239000000463 material Substances 0.000 claims description 16
- 238000001816 cooling Methods 0.000 claims description 6
- 238000007599 discharging Methods 0.000 claims 1
- 239000002826 coolant Substances 0.000 description 22
- 230000000694 effects Effects 0.000 description 5
- 239000002184 metal Substances 0.000 description 4
- 230000000087 stabilizing effect Effects 0.000 description 4
- 230000004927 fusion Effects 0.000 description 3
- 239000012212 insulator Substances 0.000 description 3
- 230000007423 decrease Effects 0.000 description 2
- 229910052734 helium Inorganic materials 0.000 description 2
- 239000001307 helium Substances 0.000 description 2
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 2
- 239000007788 liquid Substances 0.000 description 2
- 230000005347 demagnetization Effects 0.000 description 1
- 230000005284 excitation Effects 0.000 description 1
- 230000020169 heat generation Effects 0.000 description 1
- 239000011810 insulating material Substances 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000000630 rising effect Effects 0.000 description 1
Landscapes
- Superconductors And Manufacturing Methods Therefor (AREA)
- Containers, Films, And Cooling For Superconductive Devices (AREA)
Description
【発明の詳細な説明】
この発明は一般に高磁界を発生する超電導コイル、特に
核融合装置等に使用される大形の超電導コイルの構造に
関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention generally relates to a superconducting coil that generates a high magnetic field, and particularly to the structure of a large superconducting coil used in a nuclear fusion device or the like.
一般に高磁界を発生する装置として超電導コイルが多く
使用されているが、超電導コイルは通常の電磁石と異な
り極低温、主として液体ヘリウム温度にまで冷却される
必要があり、さらにメガ・ジュール以上特に核融合装置
に使用されるとみられているキガ・ジュール以上の磁界
エネルギーを保有する大形の超電導コイルにおいてはそ
のコイルによつて発生される巨大な電磁力に耐える支持
構造をいかに構成するかが重要な問題となり、次に述べ
るようなものが従来開発されている。Generally, superconducting coils are often used as devices that generate high magnetic fields, but unlike ordinary electromagnets, superconducting coils need to be cooled to extremely low temperatures, mainly liquid helium temperatures, and even more than mega joules, especially nuclear fusion. For the large superconducting coils that are expected to be used in devices that have magnetic field energy of more than kilojoules, it is important to construct a support structure that can withstand the huge electromagnetic force generated by the coils. This has become a problem, and the following methods have been developed in the past.
第1図は従来の超電導コイル群体の構成を示す断面図で
ある。図において、1は超電導コイルでボルト2及びナ
ット3で締付けて組立てられ超電導コイル群体100を
構成している。FIG. 1 is a sectional view showing the structure of a conventional superconducting coil group. In the figure, reference numeral 1 denotes a superconducting coil which is assembled by tightening bolts 2 and nuts 3 to form a superconducting coil group 100.
第2図は第1図における超電導コイル1の構成を示す斜
視図である。FIG. 2 is a perspective view showing the structure of the superconducting coil 1 in FIG. 1.
図において4は金属又は絶縁物よりなる板状の保持部材
で両側面には複数個のコイル溝4aが設けられている。In the figure, reference numeral 4 denotes a plate-shaped holding member made of metal or an insulator, and a plurality of coil grooves 4a are provided on both sides.
5は超電導材で上記コイル溝4a内に収納されその周囲
の空間には液体ヘリウム等の冷却媒体6が充満されてい
る。A superconducting material 5 is housed in the coil groove 4a, and the space around it is filled with a cooling medium 6 such as liquid helium.
7は冷却媒体通路Taを有する間隔部材で上記超電導材
5を保持している。Reference numeral 7 denotes a spacing member having a cooling medium passage Ta that holds the superconducting material 5.
なおこの間隔部材7は保持部材4が金属の場合は絶縁物
または表面に絶縁処理を施した金属であり、保持部材4
が絶縁物の場合には絶縁物でも金属でもよい。而してこ
れら4、4a、5、6、7、Taは超電導コイル1を構
成している。以上のように構成された超電導コイル1で
は保持部材4に設けたコイル溝4aにおいて超電導材5
を、その周囲が冷却媒体6に接するように間隔部材7に
よつて保持しているためコイルが巨大な電磁力に耐える
と共に、冷却表面積の増加による安定化電流を増加させ
ることができコイル運転電流の増加をもたらすことがで
きる。Note that when the holding member 4 is made of metal, this spacing member 7 is an insulating material or a metal whose surface has been subjected to insulation treatment.
If it is an insulator, it may be an insulator or a metal. These 4, 4a, 5, 6, 7, and Ta constitute the superconducting coil 1. In the superconducting coil 1 configured as described above, the superconducting material 5 is formed in the coil groove 4a provided in the holding member 4.
is held by the spacing member 7 so that its periphery is in contact with the cooling medium 6, so that the coil can withstand a huge electromagnetic force, and the stabilizing current can be increased by increasing the cooling surface area, which reduces the coil operating current. can bring about an increase in
この場合、超電導材5は冷却媒体6により所定の温度に
冷却されているわけであるが、超電導コイル1の励磁、
減磁の際や外部からの交流磁界が印加される時に超電導
材5に若干の発熱を生じ冷却媒体6が蒸発して気泡を発
生することがあるので、間隔部材7に冷却媒体通路7a
を設けてその気泡を逃がしている。しかるに、図示の第
1区間で発生した気泡は冷却媒体通路7aを通過して第
2区間で発生した気泡と合わさつて大きくなりながらさ
らに次の区間に入り込み、その大きな気泡が超電導材5
に付着して冷却効果を悪くしコイル安定化電流を低下さ
せる。又、安定化電流が低下すれば運転電流も低下しな
ければならないので同一空間に同一磁界を発生する場合
、コイルを大きくしなければならず装置としても大きな
ものとなる等の欠点を有していた。この発明は上記従来
装置の欠点を解消することを目1(Uとして成されたも
のである。In this case, the superconducting material 5 is cooled to a predetermined temperature by the cooling medium 6, but the excitation of the superconducting coil 1,
During demagnetization or when an external alternating magnetic field is applied, the superconducting material 5 may generate some heat and the cooling medium 6 may evaporate and generate bubbles, so a cooling medium passage 7a is provided in the spacing member 7.
is installed to allow the air bubbles to escape. However, the bubbles generated in the first section shown in the figure pass through the cooling medium passage 7a, combine with the bubbles generated in the second section, become larger, and further enter the next section, and the large bubbles enter the superconducting material 5.
It adheres to the coil, impairing the cooling effect and lowering the coil stabilizing current. In addition, if the stabilizing current decreases, the operating current must also decrease, so if the same magnetic field is to be generated in the same space, the coil must be larger, resulting in a larger device. Ta. This invention has been accomplished with the aim of eliminating the drawbacks of the above-mentioned conventional devices.
以下この発明における超電導コイルの一実施例を図に基
づいて詳細に説明する。DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of a superconducting coil according to the present invention will be described in detail below with reference to the drawings.
第3図はこの発明における超電導コイルの一実施例の構
成を示す斜視図である。FIG. 3 is a perspective view showing the structure of an embodiment of a superconducting coil according to the present invention.
図において保持部材4、コイル溝4a1超電導材5、冷
却媒体6は従来のものと同様なので説明を省略する。In the figure, the holding member 4, the coil groove 4a1, the superconducting material 5, and the cooling medium 6 are the same as those of the conventional ones, so their explanation will be omitted.
8はコイル溝4a内に設けられた間隔部材で超電導材5
を保持する。Reference numeral 8 denotes a spacing member provided in the coil groove 4a, and the superconducting material 5
hold.
9は保持部材4に形成された冷却媒体通路で上記間隔部
材8によつて仕切られた各区間に枝路9aを介して各々
連通し冷却媒体6内に発生した気泡を外部に排出する。Reference numeral 9 denotes a cooling medium passage formed in the holding member 4, which communicates with each section partitioned by the spacing member 8 via a branch passage 9a, and discharges bubbles generated in the cooling medium 6 to the outside.
而してこれら4,4a,5,6,8,9,9aは超電導
コイル10を構成している。以上、第3図のように構成
された超電導コイル10においても従来の超電導コイル
1と同様に超電導コイル10の励磁、減磁の際や外部か
ら交流磁界が印加する時に超電導材5に若干の発熱を生
じ冷却媒体6が蒸発して気泡を発生するわけであるが、
間隔部材8によつて仕切られた区間は枝路9aによつて
各々単独に冷却媒体通路9に連通しているので、単一区
間で発生した気泡はその区間で枝路9aにより取り除か
れるために他の区間の超電導材5の冷却効果を悪くする
ようなことがなくなる。These 4, 4a, 5, 6, 8, 9, and 9a constitute a superconducting coil 10. As mentioned above, in the superconducting coil 10 configured as shown in FIG. 3, as in the conventional superconducting coil 1, the superconducting material 5 generates a slight amount of heat when the superconducting coil 10 is excited or demagnetized or when an alternating current magnetic field is applied from the outside. This causes the cooling medium 6 to evaporate and generate bubbles.
Since the sections partitioned by the spacing members 8 are each independently connected to the cooling medium passage 9 by the branch passages 9a, air bubbles generated in a single section are removed by the branch passages 9a in that section. There is no possibility that the cooling effect of the superconducting material 5 in other sections will be deteriorated.
第4図はこの発明における超電導コイルの他の実施例の
構成を示す斜視図である。FIG. 4 is a perspective view showing the structure of another embodiment of the superconducting coil according to the present invention.
図において保持部材4、コイル溝4a1超電導材5、冷
却媒体6、間隔部材8、冷却媒体通路9は第3図におけ
る超電導コイル10のものと同様なので説明を省略する
。In the figure, the holding member 4, the coil groove 4a1, the superconducting material 5, the cooling medium 6, the spacing member 8, and the cooling medium passage 9 are the same as those of the superconducting coil 10 in FIG. 3, so a description thereof will be omitted.
9bは冷却媒体通路9より間隔部材8により仕切られた
区間に連通する枝路で、上記気泡の上昇方向にそつて斜
め、すなわち、冷却媒体通路9及びコイル溝4aと垂直
にならないように形成されている。Reference numeral 9b denotes a branch passage communicating with the section partitioned by the spacing member 8 from the cooling medium passage 9, and is formed obliquely along the rising direction of the bubbles, that is, not perpendicular to the cooling medium passage 9 and the coil groove 4a. ing.
而してこれら4,4a,5,6,8,9,9bは超電導
コイル20を構成している。今、第3図における超電導
コイル10において冷却媒体通路9を通る気泡の量が多
くなるとその気泡の一部が枝路9aを逆流して超電導材
5に達し冷却効果に幣害を与える恐れが考えられるが、
第4図における超電導コイル20におけるように枝路9
bを斜めに形成したことにより、上記幣害のおそれを除
去することができる。These 4, 4a, 5, 6, 8, 9, and 9b constitute a superconducting coil 20. Now, if the amount of bubbles passing through the cooling medium passage 9 in the superconducting coil 10 in FIG. However,
Branch 9 as in superconducting coil 20 in FIG.
By forming b obliquely, it is possible to eliminate the above-mentioned risk of damage.
以上要するに本発明は超電導コイルの超電導材の発熱に
よつて生じる冷却媒体内の気泡を外部に取り出す通路を
形成したことにより、超電導材の冷却媒体による冷却効
果を向上させてコイル安定化電流を増加させることがで
き、コイル運転電流の増加をもたらす。In summary, the present invention improves the cooling effect of the cooling medium of the superconducting material and increases the coil stabilizing current by forming a passage to take out the air bubbles in the cooling medium generated by heat generation of the superconducting material of the superconducting coil to the outside. This results in an increase in coil operating current.
これによつて同一空間に同一磁界を発生させる場合、コ
イルのコンパクト化さらにクライオスタツトや冷却シス
テムのコンパクト化をもたらす効果があり、核融合装置
、超電導回転機などの大形超電導コイルを容易に且つコ
ンパクトに製作できるという点において実用上の効果は
絶大である。When generating the same magnetic field in the same space, this has the effect of making the coil more compact, as well as the cryostat and cooling system, making it easier to create large superconducting coils for nuclear fusion devices, superconducting rotating machines, etc. The practical effect is tremendous in that it can be manufactured compactly.
第1図は従来の超電導コイル群体の構成を示す断面図、
第2図は第1図における超電導コイルの構成を示す斜視
図、第3図はこの発明における超電導コイルの一実施例
の構成を示す斜視図、第4図はこの発明における超電導
コイルの他の実施例の構成を示す斜視図である。
図において1は超電導コイル、2はボルト、3はナツト
、4は保持部材、4aはコイル溝、5は超電導材、6は
冷却媒体、7は間隔部材、7aは冷却媒体通路、8は間
隔部材、9は冷却媒体通路、9a,9bは枝路、10,
20は超電導コイルである。Figure 1 is a cross-sectional view showing the configuration of a conventional superconducting coil group;
FIG. 2 is a perspective view showing the configuration of the superconducting coil in FIG. 1, FIG. 3 is a perspective view showing the configuration of one embodiment of the superconducting coil in this invention, and FIG. 4 is another embodiment of the superconducting coil in this invention. FIG. 2 is a perspective view showing an example configuration. In the figure, 1 is a superconducting coil, 2 is a bolt, 3 is a nut, 4 is a holding member, 4a is a coil groove, 5 is a superconducting material, 6 is a cooling medium, 7 is a spacing member, 7a is a cooling medium passage, 8 is a spacing member , 9 is a cooling medium passage, 9a, 9b are branch passages, 10,
20 is a superconducting coil.
Claims (1)
、該コイル溝に収納された超電導材、及び該超電導部材
を前記保持部材から間隔を置いて保持する間隔部材、を
備え、前記保持部材には、前記コイル溝間において該コ
イル溝と平行に設けられた溝と、隣接する前記間隔部材
により仕切られた区間における前記コイル溝と前記溝と
を連通する少なくとも一つの枝溝と、が設けられており
、前記溝及び前記コイル溝に前記超電導材を冷却する媒
体を充満させると共に前記コイル溝内において前記媒体
内に発生した気泡を前記枝溝及び溝を介して排出させる
ことを特徴とした超電導コイル。 2 前記枝溝が、前記溝と垂直にならないように形成さ
れている特許請求の範囲第1項記載の超電導コイル。[Scope of Claims] 1 A holding member having a coil groove on at least one side surface, a superconducting material housed in the coil groove, and a spacing member that holds the superconducting member at a distance from the holding member, The holding member includes a groove provided parallel to the coil groove between the coil grooves, and at least one branch groove communicating the coil groove and the groove in a section partitioned by the adjacent spacing member. , for filling the groove and the coil groove with a medium for cooling the superconducting material and discharging air bubbles generated in the medium in the coil groove through the branch groove and groove. Characteristic superconducting coil. 2. The superconducting coil according to claim 1, wherein the branch grooves are formed not to be perpendicular to the grooves.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP51017338A JPS5928042B2 (en) | 1976-02-19 | 1976-02-19 | superconducting coil |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP51017338A JPS5928042B2 (en) | 1976-02-19 | 1976-02-19 | superconducting coil |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS52100895A JPS52100895A (en) | 1977-08-24 |
JPS5928042B2 true JPS5928042B2 (en) | 1984-07-10 |
Family
ID=11941253
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP51017338A Expired JPS5928042B2 (en) | 1976-02-19 | 1976-02-19 | superconducting coil |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5928042B2 (en) |
Families Citing this family (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS57113208A (en) * | 1981-01-06 | 1982-07-14 | Toshiba Corp | Superconducing device |
JP6854988B1 (en) * | 2020-04-20 | 2021-04-07 | 三菱電機株式会社 | Superconducting electromagnet device |
-
1976
- 1976-02-19 JP JP51017338A patent/JPS5928042B2/en not_active Expired
Also Published As
Publication number | Publication date |
---|---|
JPS52100895A (en) | 1977-08-24 |
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