JPH0656902B2 - Superconducting device - Google Patents
Superconducting deviceInfo
- Publication number
- JPH0656902B2 JPH0656902B2 JP58112841A JP11284183A JPH0656902B2 JP H0656902 B2 JPH0656902 B2 JP H0656902B2 JP 58112841 A JP58112841 A JP 58112841A JP 11284183 A JP11284183 A JP 11284183A JP H0656902 B2 JPH0656902 B2 JP H0656902B2
- Authority
- JP
- Japan
- Prior art keywords
- cooling pipe
- cryostat
- cooling
- power leads
- power
- 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
Links
Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N60/00—Superconducting devices
- H10N60/80—Constructional details
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- Containers, Films, And Cooling For Superconductive Devices (AREA)
Description
【発明の詳細な説明】 〔発明の属する技術分野〕 本発明は、超電導磁石等を用いた超電導装置に関する。Description: TECHNICAL FIELD The present invention relates to a superconducting device using a superconducting magnet or the like.
一般にクライオスタットに収納された超電導コイルの励
減磁に使用されるパワーリードは大気側からクライオス
タット内に導入されているので、このパワーリードを伝
導してクライオスタット内に熱が侵入する。この熱侵入
を極力減らすためにパワーリードの線径を細くし、かつ
パワーリードから発生するジュール熱でパワーリードが
焼き切れないようにパワーリードをクライオスタット内
のヘリウムガスで冷却している。第1図にパワーリード
を使用したクライオスタットを示す。クライオスタット
(1)内に液体ヘリウム(2)を貯液し、この液体ヘリウム
(2)に超電導コイル(3)を浸漬し、この超電導コイル(3)
の励減磁に使用されるパワーリード(4),(5)がそれぞれ
冷却管(6),(7)内を貫通して大気側に導びかれている。
この冷却管(6),(7)内にクライオスタット(1)内の液体
ヘリウム(2)の蒸発ガスが流れてパワーリード(4),(5)
を冷却して、冷却管(6),(7)の大気側に設けられたガス
回収口(8),(9)から回収される。尚、パワーリード
(4),(5)はそれぞれ絶縁材(10),(11)で冷却管(6),(7)
に固定されている。Generally, the power lead used for excitation / demagnetization of the superconducting coil housed in the cryostat is introduced into the cryostat from the atmosphere side, so that heat is conducted into the cryostat by conducting this power lead. In order to reduce this heat intrusion as much as possible, the wire diameter of the power lead is made thin, and the power lead is cooled by helium gas in the cryostat so that the power lead is not burned out by the Joule heat generated from the power lead. Figure 1 shows a cryostat using power leads. Cryostat
Liquid helium (2) is stored in (1), and this liquid helium is stored.
Immerse the superconducting coil (3) in (2),
The power leads (4) and (5) used for excitation and demagnetization pass through the cooling tubes (6) and (7), respectively, and are guided to the atmosphere side.
Evaporated gas of liquid helium (2) in the cryostat (1) flows into these cooling pipes (6) and (7), and power leads (4) and (5)
Is cooled and is recovered from the gas recovery ports (8) and (9) provided on the atmosphere side of the cooling pipes (6) and (7). In addition, power lead
(4) and (5) are insulation materials (10) and (11), respectively, and cooling pipes (6) and (7).
It is fixed to.
このようなクライオスタット(1)から大気側に導かれる
冷却管(6),(7)が複数本存在する構成であってはバラン
スがとれた状態でヘリウムガスが冷却管(6),(7)内を流
れることはむずかしく、通常、バランスがくずれ、ヘリ
ウムガスは流れ易い冷却管に多量に流れるようになり、
これによりこの流量の多い冷却管はますます冷却されて
より一層ヘリウムガスが流れ易すくなり、他の冷却管の
ヘリウムガスの流量は減り、この中に収容されたパワー
リードの冷却が不足し、パワーリードが焼損に至ること
があった。In a configuration in which there are multiple cooling pipes (6), (7) led from the cryostat (1) to the atmosphere side, the helium gas is in a balanced state and the cooling pipes (6), (7) It is difficult to flow through the inside, and usually the balance is lost, and a large amount of helium gas flows into the cooling pipe that easily flows,
As a result, the cooling pipe with a large flow rate is further cooled and helium gas flows more easily, the flow rate of the helium gas in other cooling pipes decreases, and the power lead accommodated in this cooling pipe is insufficiently cooled. The power lead could be burned.
本発明の目的は、上記の欠点を除去し、熱侵入量が少な
く、パワーリードの焼損の恐れの少ない超電導装置を提
供することにある。An object of the present invention is to eliminate the above-mentioned drawbacks, to provide a superconducting device which has a small amount of heat intrusion and is less likely to burn a power lead.
[発明の概要] 本発明は、クライオスタットと、このクライオスタット
内に貯液される冷媒に浸漬される超電導コイルと、前記
クライオスタットの大気側からこのクライオスタット内
の前記冷媒の液面近傍まで貫通して設けられる冷却管
と、この冷却管内に収納され、前記超電導コイルの励減
磁を行うための複数本のパワーリードとを備えた超電導
装置において、 前記冷却管を電気絶縁材料から構成するとともに、前記
複数本のパワーリードおよび前記冷却管の長軸方向に直
交する方向のそれぞれの断面形状を、前記パワーリード
の外周面と前記冷却管の内壁面とが接触するように形成
し、前記複数本のパワーリード同士を前記冷却管の内壁
面に互いが非接触でかつ前記冷却管内に前記冷媒の蒸発
ガスが通流する連続した実質的に1本の流路を確保する
ように密着固定したことを特徴としている。[Summary of the Invention] The present invention provides a cryostat, a superconducting coil immersed in a refrigerant stored in the cryostat, and a penetrating from the atmosphere side of the cryostat to the vicinity of the liquid surface of the refrigerant in the cryostat. In a superconducting device comprising a cooling pipe to be used and a plurality of power leads for energizing and demagnetizing the superconducting coil, the cooling pipe is made of an electrically insulating material, and The power leads and the cooling tubes are formed so that their respective cross-sectional shapes in a direction orthogonal to the long axis direction are in contact with the outer peripheral surface of the power leads and the inner wall surface of the cooling tube. A continuous substantially single flow in which the leads are not in contact with the inner wall surface of the cooling pipe and the evaporative gas of the refrigerant flows in the cooling pipe. Is characterized in adhesion fixed possible to ensure.
[発明の効果] 本発明に係る超電導装置を用いれば、複数本のパワーリ
ードが均等に冷却されるのでパワーリードの線径を最小
にしてもパワーリードが焼損したりすることがない。ま
た複数本のパワーリードおよび冷却管の長軸方向に直交
する方向のそれぞれの断面形状を、パワーリードの外周
面と冷却管の内壁面とが接触するように形成しているの
で、冷却管に固定する際の接触固定有効面積を大きく取
ることが可能となり、絶縁性能の向上と冷却効率の向上
とを両立して満足することができる。EFFECTS OF THE INVENTION By using the superconducting device according to the present invention, a plurality of power leads are cooled uniformly, so that the power leads are not burned even if the wire diameter of the power leads is minimized. Moreover, since the cross-sectional shape of each of the plurality of power leads and the cooling pipe in the direction orthogonal to the long axis direction is formed so that the outer peripheral surface of the power lead and the inner wall surface of the cooling pipe are in contact with each other, It is possible to take a large contact fixing effective area when fixing, and it is possible to satisfy both improvement of insulation performance and improvement of cooling efficiency.
さらに、冷却管を電気絶縁材料から構成し、複数本のパ
ワーリード同士を冷却管の内壁に互いに非接触となるよ
うに電気絶縁して収納しているので、簡単な構成で冷却
効率の向上を維持したままパワーリード同士を完全に絶
縁することができる。またさらに、パワーリードの線径
を最小にすることができると同時に冷却管も1本なの
で、クライオスタット内への熱侵入量も最小とすること
ができる等の優れた効果を奏する。Further, the cooling pipe is made of an electrically insulating material, and the plurality of power leads are electrically insulated and housed in the inner wall of the cooling pipe so as not to be in contact with each other, so that the cooling efficiency is improved with a simple structure. The power leads can be completely insulated from each other while maintaining. Furthermore, the wire diameter of the power lead can be minimized, and at the same time, since only one cooling pipe is provided, the amount of heat invading into the cryostat can be minimized.
[発明の実施例] 以下、本発明の代表的実施例を第5図乃至第8図を参照
して説明するが、本発明の理解を容易にするために本発
明の超電導装置の前提となる参考例を第2図乃至第4図
に示す。なお、これらはいずれも第1図と同一のものは
同一の符号を付して説明を簡略化している。第2図にお
いて、超電導コイル(3)の励減磁を行い、一部が液体ヘ
リウム(2)内に浸漬されるパワーリード(4),(5)は、ク
ライオスタット(1)の大気側から液体ヘリウム(2)の液面
の近傍まで貫通して設けられた1本の冷却管(12)内を仕
切ることなくかつ蒸発ガスの流れを分断することがない
ように冷却管(12)内に収納されている。クライオスタッ
ト(1)内の液体ヘリウム(2)の蒸発ガスは冷却管(12)の液
体ヘリウム(2)の液面側に設けられたガス流入口(13)を
流入し、そして冷却管(12)内を流通するヘリウムガスは
冷却管(12)の大気側に設けた回収口(14)によって回収さ
れる。又、パワーリード(4),(5)のクライオスタット
(1)内における液体ヘリウム(2)側は第4図に示すような
例えば繊維強化プラスチック(FRP)で形成され、パワー
リード(4),(5)を貫通する孔(15a),(15b)及びガス流通
孔(15c)を具備した板状の絶縁部材(15)、又パワーリー
ド(4),(5)の大気側は第3図に示すような例えばFRPで
形成され、パワーリード(4),(5)が貫通する孔(16a),(1
6b)を具備する板状の絶縁部材(16)によって冷却管(12)
内に絶縁して固定されている。[Embodiment of the Invention] Hereinafter, a representative embodiment of the present invention will be described with reference to Figs. 5 to 8, which is a prerequisite for the superconducting device of the present invention in order to facilitate understanding of the present invention. Reference examples are shown in FIGS. 2 to 4. It should be noted that the same parts as those in FIG. 1 are allotted with the same reference numerals to simplify the description. In Fig. 2, the power leads (4) and (5) that are excited and demagnetized in the superconducting coil (3) and partially immersed in the liquid helium (2) are liquid from the atmosphere side of the cryostat (1). Stored in the cooling pipe (12) so as not to partition the inside of the single cooling pipe (12) provided penetrating to the vicinity of the liquid level of helium (2) and not to interrupt the flow of evaporative gas Has been done. The vaporized gas of liquid helium (2) in the cryostat (1) flows into the gas inlet (13) provided on the liquid level side of the liquid helium (2) of the cooling pipe (12), and then the cooling pipe (12) The helium gas flowing inside is recovered by a recovery port (14) provided on the atmosphere side of the cooling pipe (12). Also, the cryostat of the power leads (4), (5)
The liquid helium (2) side in (1) is made of, for example, fiber reinforced plastic (FRP) as shown in FIG. 4, and holes (15a), (15b) penetrating the power leads (4), (5). And the atmosphere side of the power leads (4) and (5), which are plate-like insulating members (15) provided with gas flow holes (15c), are formed by, for example, FRP as shown in FIG. ), (5) through holes (16a), (1
Cooling pipe (12) by a plate-shaped insulating member (16) equipped with 6b)
It is insulated and fixed inside.
次に動作について説明する。液体ヘリウム(2)の蒸発ガ
スは冷却管(12)のガス流入口(13)及び絶縁部材(15)のガ
ス流通孔(15c)から冷却管(12)内に流入し冷却管(12)内
における流れが分断されることなく、実質的に1本の流
路内を流通するのでパワーリード(4),(5)を均等に冷却
することができる。そしてこの蒸発ガスはパワーリード
(4),(5)を冷却しながら回収口(14)から回収される。Next, the operation will be described. The vaporized gas of liquid helium (2) flows into the cooling pipe (12) through the gas inlet (13) of the cooling pipe (12) and the gas flow hole (15c) of the insulating member (15) and enters the cooling pipe (12). Since the flow in 1 is substantially divided into one flow path without being divided, the power leads (4) and (5) can be cooled uniformly. And this evaporated gas is the power lead
It is recovered from the recovery port (14) while cooling (4) and (5).
尚、ヘリウムの絶縁耐圧は室温でも1KV/cmあり(沿面
放電の場合)、低温ではさらに高くなるのでこの構成で
絶縁耐圧が問題になることがない。It should be noted that the withstand voltage of helium is 1 KV / cm even at room temperature (in the case of creeping discharge), and it becomes higher at low temperatures, so the withstand voltage does not pose a problem in this configuration.
次に、上記参考例に示した構成に比較して、さらにパワ
ーリードの冷却効率の向上と絶縁性能の向上を図った本
発明の超電導装置について第5図乃至第8図を参照して
説明する。なお、第5図乃至第8図は、参考例で示した
第2図乃至第4の改良された要部を拡大して示し、同一
のものは同一の符号を付して説明を省略する。Next, a superconducting device of the present invention, which is further improved in cooling efficiency and insulation performance of the power leads as compared with the configuration shown in the above reference example, will be described with reference to FIGS. 5 to 8. . Note that FIGS. 5 to 8 are enlarged views showing the improved essential parts of FIGS. 2 to 4 shown in the reference example, and the same parts are denoted by the same reference numerals and the description thereof will be omitted.
パワーリード(4),(5)は、第5図に示すように半円筒状
に形成され、断面において第8図に示すように円弧の中
心に放射状に延びたフイン(17)を有し、大気側の端部に
は外部機器との接続に使用される端子(18),(19)を有す
る。円筒状の冷却管はFRP等の絶縁材で形成され、内
壁にはパワーリード(4),(5)間を絶縁できるように軸方
向に突起条部(12a),(12b)を有する。そしてこの冷却管
(12)は第5図に示すようにパワーリード(4),(5)を突起
条部(12a),(12b)を挾んで内壁に沿つて接着剤等によっ
て固定してシールし、収納している。更にこの冷却管(1
2)は、大気側の端部に第7図に示すようにパワーリード
(4),(5)の端子(18),(19)間に絶縁するための突起板(2
1a),(21b)を備え、図示しないクライオスタツトにフラ
ンジ(20)によつて固定される。又、パワーリード(4),
(5)の端子(18),(19)の中心部には第6図に示すように
FRP等の絶縁材で形成された円筒状の回収口(14)が挿
入できるように貫通孔(22)が設けられ、この貫通孔(22)
に回収口(14)が接着剤等で設置されている。The power leads (4), (5) are formed in a semi-cylindrical shape as shown in FIG. 5 and have fins (17) extending radially in the center of the arc as shown in FIG. At the end on the atmosphere side, there are terminals (18), (19) used for connection with external equipment. The cylindrical cooling pipe is formed of an insulating material such as FRP, and has inner wall provided with protrusions (12a) and (12b) in the axial direction so as to insulate between the power leads (4) and (5). And this cooling pipe
As shown in Fig. 5, (12) is a power lead (4), (5) that is sandwiched between the protrusions (12a), (12b) and fixed along the inner wall with an adhesive or the like to seal and store it. ing. Furthermore, this cooling pipe (1
2) is a power lead at the end on the atmosphere side as shown in Fig. 7.
Projection plate (2) for insulation between terminals (18) and (19) of (4) and (5)
1a) and (21b), which are fixed to a cryostat (not shown) by a flange (20). Also, the power lead (4),
As shown in FIG. 6, a through hole (22) is formed in the center of the terminals (18) and (19) of (5) so that a cylindrical recovery port (14) made of an insulating material such as FRP can be inserted. ) Is provided and this through hole (22)
The recovery port (14) is installed with adhesive or the like.
次に動作について説明する。Next, the operation will be described.
液体ヘリウムの蒸発ガスは冷却管(12)の下端部から流入
し、フイン(17)間を流通することによりパワーリード
(4),(5)を冷却しながら冷却管(12)の軸方向に沿つて上
昇し、回収口(14)から大気側に回収される。Liquid helium evaporative gas flows in from the lower end of the cooling pipe (12) and flows between the fins (17), so that power lead is generated.
While cooling (4) and (5), the temperature rises along the axial direction of the cooling pipe (12) and is recovered from the recovery port (14) to the atmosphere side.
このように、パワーリード(4),(5)の断面形状を冷却管
(12)の内壁面と接触するように構成することで、従来の
一般の円形断面のパワーリードに比較して冷却管(12)の
内壁面に接触固定する際の接触固定有効表面積と、冷却
に供せられる冷却有効表面積をともに大きく構成でき、
絶縁性能と冷却性能の双方を同時に満足することができ
る。さらにフィン(17)を形成する場合には、冷却面積を
格段に大きくすることができるので、より効果的にパワ
ーリード(4),(5)は冷却されるととも、前述した参考例
に比較して冷却管(12)を電気絶縁材料で構成し、パワー
リード(4)(5)および冷却管(12)の長軸方向に直交する方
向のそれぞれの断面形状を、パワーリード(4)(5)を外周
面と冷却管(12)の内壁面とが接触するように形成し、パ
ワーリード(4)(5)同士を冷却管(12)の内壁面に互いが非
接触に密着固定しているので、絶縁性能の大幅な向上が
図れる。In this way, change the cross-sectional shape of the power leads (4) and (5) to the cooling pipe.
By configuring so as to contact the inner wall surface of (12), the contact fixing effective surface area when contact fixing to the inner wall surface of the cooling pipe (12) and cooling compared to the conventional power lead having a general circular cross section. The cooling effective surface area provided for
Both the insulation performance and the cooling performance can be satisfied at the same time. Further, when the fins (17) are formed, the cooling area can be remarkably increased, so that the power leads (4) and (5) are cooled more effectively. Then, the cooling pipe (12) is made of an electrically insulating material, and the power lead (4) (5) and the cooling pipe (12) have respective cross-sectional shapes in a direction orthogonal to the longitudinal direction of the power lead (4) ( 5) is formed so that the outer peripheral surface and the inner wall surface of the cooling pipe (12) are in contact with each other, and the power leads (4) and (5) are closely fixed to the inner wall surface of the cooling pipe (12) in a non-contact manner. Therefore, the insulation performance can be significantly improved.
尚、第5図に示した実施例では1本の冷却管(12)の中に
2本のパワーリード(4),(5)を収納した例を示したが、
複数の超電導コイルを独立に励磁する場合はさらに多く
のパワーリードを1本の冷却管の中に入れてもよい。Although the embodiment shown in FIG. 5 shows an example in which two power leads (4) and (5) are housed in one cooling pipe (12),
In the case of independently exciting a plurality of superconducting coils, more power leads may be put in one cooling tube.
又、パワーリードの断面構造は第8図に限定されない。
冷却面積が大きくしかも乱流効果が促進され、過去に圧
力損失が大きくならないものであればよい。Further, the sectional structure of the power lead is not limited to that shown in FIG.
It is sufficient if the cooling area is large, the turbulent flow effect is promoted, and the pressure loss does not increase in the past.
第1図は従来の超電導装置を示す概略断面図、第2図
は、参考例の超電導装置を示す概略断面図、第3図およ
び第4図は、参考例に用いられる絶縁部材を示す正面
図、第5図は、本発明の超電導装置に係る要部を拡大し
て示す斜視図、第6図は、本発明の超電導装置の要部を
示す斜視断面図、第7図は、本発明の超電導装置の要部
を示す斜視図、第8図は、本発明の超電導装置に用いら
れるパワーリードおよび冷却管の形状の一例を示す断面
図である。 (1)……クライオスタツト、(2)……液体ヘリウム(冷
媒)、(3)……超電導コイル、 (4),(5)……パワーリード、(12)……冷却管。FIG. 1 is a schematic sectional view showing a conventional superconducting device, FIG. 2 is a schematic sectional view showing a superconducting device of a reference example, and FIGS. 3 and 4 are front views showing insulating members used in the reference example. FIG. 5 is an enlarged perspective view showing an essential part of the superconducting device of the present invention, FIG. 6 is a perspective sectional view showing an essential part of the superconducting device of the present invention, and FIG. FIG. 8 is a perspective view showing a main part of the superconducting device, and FIG. 8 is a cross-sectional view showing an example of the shapes of the power lead and the cooling pipe used in the superconducting device of the present invention. (1) …… Cryostat, (2) …… Liquid helium (refrigerant), (3) …… Superconducting coil, (4), (5) …… Power lead, (12) …… Cooling tube.
Claims (2)
ト内に貯液される冷媒に浸漬される超電導コイルと、前
記クライオスタットの大気側からこのクライオスタット
内の前記冷媒の液面近傍まで貫通して設けられる冷却管
と、この冷却管内に収納され、前記超電導コイルの励減
磁を行うための複数本のパワーリードとを備えた超電導
装置において、 前記冷却管を電気絶縁材料から構成するとともに、前記
複数本のパワーリードおよび前記冷却管の長軸方向に直
交する方向のそれぞれの断面形状を、前記パワーリード
の外周面と前記冷却管の内壁面とが接触するように形成
し、前記複数本のパワーリード同士を前記冷却管の内壁
面に互いが非接触でかつ前記冷却管内に前記冷媒の蒸発
ガスが通流する連続した実質的に1本の流路を確保する
ように密着固定したことを特徴とする超電導装置。1. A cryostat, a superconducting coil immersed in a refrigerant stored in the cryostat, and a cooling pipe penetrating from the atmosphere side of the cryostat to near the liquid surface of the refrigerant in the cryostat. A superconducting device that is housed in the cooling pipe and has a plurality of power leads for performing demagnetization of the superconducting coil, wherein the cooling pipe is made of an electrically insulating material, and the plurality of power leads are provided. And each cross-sectional shape of the direction orthogonal to the long axis direction of the cooling pipe is formed so that the outer peripheral surface of the power lead and the inner wall surface of the cooling pipe are in contact, and the plurality of power leads are connected to each other. A continuous, substantially single flow path is provided so as to be in non-contact with the inner wall surface of the cooling pipe and to allow the evaporative gas of the refrigerant to flow in the cooling pipe. A superconducting device characterized in that it is closely fixed.
って突出するフィンを形成したことを特徴とする特許請
求の範囲第1項記載の超電導装置。2. The superconducting device according to claim 1, wherein the power lead is formed with a fin protruding toward the inside of the cooling pipe.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58112841A JPH0656902B2 (en) | 1983-06-24 | 1983-06-24 | Superconducting device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58112841A JPH0656902B2 (en) | 1983-06-24 | 1983-06-24 | Superconducting device |
Related Child Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4341056A Division JPH05243623A (en) | 1992-11-30 | 1992-11-30 | Superconducting device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS605576A JPS605576A (en) | 1985-01-12 |
| JPH0656902B2 true JPH0656902B2 (en) | 1994-07-27 |
Family
ID=14596866
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58112841A Expired - Lifetime JPH0656902B2 (en) | 1983-06-24 | 1983-06-24 | Superconducting device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0656902B2 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH05243623A (en) * | 1992-11-30 | 1993-09-21 | Toshiba Corp | Superconducting device |
| JP5628620B2 (en) * | 2010-10-05 | 2014-11-19 | 公益財団法人鉄道総合技術研究所 | Power lead and power transmission system including the power lead |
| CN107424800B (en) * | 2017-09-12 | 2020-08-07 | 中国电力科学研究院 | Heat-dissipating pressure ring |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5742181A (en) * | 1980-08-26 | 1982-03-09 | Toshiba Corp | Low temperature container for superfluidic helium |
-
1983
- 1983-06-24 JP JP58112841A patent/JPH0656902B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS605576A (en) | 1985-01-12 |
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