JPS6120305A - Power lead for ultra low temperature - Google Patents
Power lead for ultra low temperatureInfo
- Publication number
- JPS6120305A JPS6120305A JP59140998A JP14099884A JPS6120305A JP S6120305 A JPS6120305 A JP S6120305A JP 59140998 A JP59140998 A JP 59140998A JP 14099884 A JP14099884 A JP 14099884A JP S6120305 A JPS6120305 A JP S6120305A
- Authority
- JP
- Japan
- Prior art keywords
- conductor
- outer cylinder
- heat
- power lead
- low temperature
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F36/00—Transformers with superconductive windings or with windings operating at cryogenic temperature
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F6/00—Superconducting magnets; Superconducting coils
- H01F6/06—Coils, e.g. winding, insulating, terminating or casing arrangements therefor
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F6/00—Superconducting magnets; Superconducting coils
- H01F6/06—Coils, e.g. winding, insulating, terminating or casing arrangements therefor
- H01F6/065—Feed-through bushings, terminals and joints
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E40/00—Technologies for an efficient electrical power generation, transmission or distribution
- Y02E40/60—Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Superconductors And Manufacturing Methods Therefor (AREA)
- Cooling Or The Like Of Electrical Apparatus (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、極低温下におかれだ超電導マグネット等の電
気機器に常温部より電流を供給するのに使用するパワー
リード(電流リード)に関する。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a power lead (current lead) used to supply current from a normal temperature part to an electrical device such as a superconducting magnet placed at an extremely low temperature. .
従来知られた極低温用パワーリードとしては、第2図乃
至第4図に示すものがある。第2図のパワーリードは、
フィン付チューブ導体1に外筒2を被せてあり、第3図
のそれはメツシュ導体1の集合体に外筒2を被せである
。また、第4図のリードは渦状に巻いた薄肉プレート導
体1に外筒2を被せてあり、このように、いずれのリー
ドも導体を外筒で覆い、この外筒内に低温下におかれた
機器への接続端側から機器冷却用液体ヘリウム等の冷媒
液の蒸発したガスを流して導体を冷却する方式を採って
いる。As conventionally known cryogenic power leads, there are those shown in FIGS. 2 to 4. The power lead in Figure 2 is
A finned tube conductor 1 is covered with an outer cylinder 2, and in the case shown in FIG. 3, an aggregate of mesh conductors 1 is covered with an outer cylinder 2. In addition, the lead shown in Fig. 4 has an outer cylinder 2 covering a spirally wound thin plate conductor 1. In this way, each lead covers the conductor with an outer cylinder and is placed inside this outer cylinder at a low temperature. The conductor is cooled by flowing evaporated gas from a refrigerant such as liquid helium for equipment cooling from the connection end to the equipment.
首記した如きパワーリードは、導体の冷却に関しては充
分な配慮がなされているが、一般にステンレス鋼によっ
て形成される外筒2の冷却性とこれを通じての常温部か
らの熱侵入対策は充分でないO
即ち、外筒2には表面の平滑な有り触れたストレートパ
イプが使用されているが、このパイプは一端部から他端
部に至る伝熱路が短かく、また表面積が小さいので冷却
ガスとの熱交換性も悪く、従って、この外筒を介して外
部熱が極低温機器側に侵入し1機器冷却冷媒液の蒸発を
早め、なおかつ1機器に対しても悪影響を及ぼしている
。Although sufficient consideration has been given to the cooling of the conductor in the power lead as mentioned above, the cooling performance of the outer cylinder 2, which is generally made of stainless steel, and the measures against heat intrusion from the normal temperature part through this are not sufficient. That is, a straight pipe with a smooth surface is used for the outer cylinder 2, but this pipe has a short heat transfer path from one end to the other and has a small surface area, so heat exchange with the cooling gas is difficult. The exchangeability is also poor, and therefore, external heat enters the cryogenic equipment side through this outer cylinder, accelerating the evaporation of the refrigerant liquid for cooling one equipment, and also having an adverse effect on the equipment.
本発明は上述の問題点を無くすため、第1図に示すよう
に、導体11に被せる外筒12を、半径方向の断面視に
おいて交互に凹部13と凸部14の存在する形状として
その長さ方向寸法を大きくせずに一端から他端にかけて
の伝熱路を延長し。In order to eliminate the above-mentioned problems, the present invention, as shown in FIG. Extends the heat transfer path from one end to the other without increasing the directional dimension.
かつ、外筒の表面積を増加させている。これによれば外
部熱の侵入量を減少させることができるのは勿論、導体
の発熱による温度上昇も抑制される。Moreover, the surface area of the outer cylinder is increased. According to this, it is possible to reduce the amount of intrusion of external heat, and also suppress the temperature rise due to heat generation of the conductor.
即ち、外筒12の一端部から他端部に流れる熱量Qは。That is, the amount of heat Q flowing from one end of the outer cylinder 12 to the other end is.
Q”” ” (TI T2 ) / L但し K−外
筒の熱伝導率
A−trの断面積
T 1.T2 =ttの両端温度
L = //の長さ
の式で表わされ、その式のLの値が凹凸のために従来に
比して格段に長くなること及び外筒の表面積が大巾に増
加するので内外面に沿って流れる蒸発冷媒ガスによる冷
却効果が高まることにより外部熱の侵入量が小さくなる
。Q”” ” (TI T2 ) / L However, K - Thermal conductivity of the outer cylinder A - Cross-sectional area of tr T 1.T2 = Temperature at both ends of tt L = Expressed by the length formula of The value of L is much longer than before due to the unevenness, and the surface area of the outer cylinder is greatly increased, which increases the cooling effect of the evaporative refrigerant gas flowing along the inner and outer surfaces, thereby reducing external heat. The amount of penetration becomes smaller.
また、外筒の冷却効果が高まれば、それに囲まれた導体
11の冷却効果も当然良くなり、導体の電気抵抗が下が
るので、 12Rで表ゎさる発熱量が減少して導体の
温度上昇も小さくなる。In addition, if the cooling effect of the outer cylinder increases, the cooling effect of the conductor 11 surrounded by it will also improve, and the electrical resistance of the conductor will decrease, so the amount of heat expressed by 12R will decrease and the temperature rise of the conductor will also be small. Become.
上記外筒12は、凹部13と凸部14が長さ方向に独立
したベローズ管にょ°って形成されているが、上記凹凸
が共に螺旋状に連続するコルゲート管を材料としてもよ
い。また、その素材には、熱伝導率の低いもの1例えば
ステンレス鋼や真鍮等を使用する。中でも前者のベロー
ズ管やコルゲート管は安価な市販品があるので経済的に
有利である。The outer cylinder 12 is formed of a bellows tube in which the concave portion 13 and the convex portion 14 are independent in the length direction, but it may also be made of a corrugated tube in which both the concave and convex portions are continuous in a spiral shape. Further, as the material, a material with low thermal conductivity, such as stainless steel or brass, is used. Among them, the former, bellows pipes and corrugated pipes, are economically advantageous because they are available on the market at low prices.
導体11は、メツシュワイヤの単体又は集合体が望まし
いが、第4図に示しだ渦巻き薄肉プレート導体もプレー
ト層間の隙間を通って外筒の内部に冷却ガスが流れるの
で実用上問題を生じることはない。The conductor 11 is preferably a single mesh wire or a set of mesh wires, but a spiral thin plate conductor as shown in FIG. 4 does not pose any practical problems because the cooling gas flows into the outer cylinder through the gaps between the plate layers. .
まだ、チューブ導体も、途中に多数の貫通孔を設ければ
、その孔から外筒内にガスが流れるので使用可能である
。However, a tube conductor can also be used if a large number of through holes are provided in the middle, since gas will flow into the outer cylinder through the holes.
なお、外筒12の両端には導体支持部15.15を設け
ておくのが望ましい。図の符号1bは常温側端子、17
は低温側端子部、18は外筒を極低温冷媒容器(クライ
オスタット)のトップフランジに固定するため、外筒に
接着する等して一体化した絶縁性フランジである。Note that it is desirable to provide conductor support portions 15.15 at both ends of the outer cylinder 12. The symbol 1b in the figure is the normal temperature side terminal, 17
18 is a low-temperature side terminal portion, and 18 is an insulating flange that is integrated with the outer cylinder by bonding or otherwise, in order to fix the outer cylinder to the top flange of a cryogenic refrigerant container (cryostat).
以上説明した通り1本発明のパワーリードは。 As explained above, the power lead of the present invention is as follows.
外筒に凹凸を付けてその一端部から他端部に至る伝熱路
を長くシ、同時にその外筒の表面積を増加させて冷却効
果も高めたので、外筒を伝って低温部に流れる外部熱の
侵入量が大巾に減少する。The outer cylinder has been made uneven to lengthen the heat transfer path from one end to the other, and at the same time, the surface area of the outer cylinder has been increased to enhance the cooling effect. The amount of heat intrusion is greatly reduced.
また、外筒の冷却効果の向上により導体もより低温に冷
却されるので、導体の発熱による温度上昇も抑制される
。Furthermore, since the conductor is also cooled to a lower temperature due to the improved cooling effect of the outer cylinder, the temperature rise due to heat generation in the conductor is also suppressed.
第1図は1本発明のパワーリードの一実施例を示す部分
破断正面図、第2図乃至第4図はいずれも従来のパワー
リードを示す図である。
11・・・導体、12・・・外筒、13・・・凹部、1
4・・・凸部、15.15・・・導体支持部、16・・
・常温側端子、17・・・低温側端子部、18・・・絶
縁性7ランジ特許出顆人 住友電気工業株式会
社同 代理人 鎌 1) 文 二第1
図
1b
第2図
第3図
第4図
1″FIG. 1 is a partially cutaway front view showing one embodiment of the power lead of the present invention, and FIGS. 2 to 4 are views showing conventional power leads. DESCRIPTION OF SYMBOLS 11... Conductor, 12... Outer cylinder, 13... Recessed part, 1
4...Convex part, 15.15...Conductor support part, 16...
・Normal temperature side terminal, 17... Low temperature side terminal part, 18... Insulating 7 lunge Patent author: Sumitomo Electric Industries, Ltd. Agent: Kama 1) Bun 2 No. 1
Figure 1b Figure 2 Figure 3 Figure 4 Figure 1''
Claims (1)
筒で覆い、その外筒内に冷却ガスを流して導体を冷却す
るパワーリードにおいて、上記外筒を、半径方向の線に
沿った断面視において長さ方向に交互に凹凸の存在する
形状としたことを特徴とする極低温用パワーリード。In a power lead, a conductor that supplies current to electrical equipment placed at extremely low temperatures is covered with an outer cylinder, and a cooling gas is allowed to flow inside the outer cylinder to cool the conductor. A cryogenic power lead characterized by having a shape in which unevenness is alternately present in the length direction when viewed in cross section.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59140998A JPS6120305A (en) | 1984-07-06 | 1984-07-06 | Power lead for ultra low temperature |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59140998A JPS6120305A (en) | 1984-07-06 | 1984-07-06 | Power lead for ultra low temperature |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6120305A true JPS6120305A (en) | 1986-01-29 |
Family
ID=15281779
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP59140998A Pending JPS6120305A (en) | 1984-07-06 | 1984-07-06 | Power lead for ultra low temperature |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6120305A (en) |
-
1984
- 1984-07-06 JP JP59140998A patent/JPS6120305A/en active Pending
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