JPS603545Y2 - superconducting winding - Google Patents

superconducting winding

Info

Publication number
JPS603545Y2
JPS603545Y2 JP5529378U JP5529378U JPS603545Y2 JP S603545 Y2 JPS603545 Y2 JP S603545Y2 JP 5529378 U JP5529378 U JP 5529378U JP 5529378 U JP5529378 U JP 5529378U JP S603545 Y2 JPS603545 Y2 JP S603545Y2
Authority
JP
Japan
Prior art keywords
superconducting
superconducting conductor
winding
interlayer insulation
conductor
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
Application number
JP5529378U
Other languages
Japanese (ja)
Other versions
JPS54158582U (en
Inventor
克時 佐々木
Original Assignee
株式会社東芝
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 株式会社東芝 filed Critical 株式会社東芝
Priority to JP5529378U priority Critical patent/JPS603545Y2/en
Publication of JPS54158582U publication Critical patent/JPS54158582U/ja
Application granted granted Critical
Publication of JPS603545Y2 publication Critical patent/JPS603545Y2/en
Expired legal-status Critical Current

Links

Landscapes

  • Superconductors And Manufacturing Methods Therefor (AREA)

Description

【考案の詳細な説明】 本考案は超電導巻線における超電導導体の冷却構造の改
良に関する。
[Detailed Description of the Invention] The present invention relates to an improvement in the cooling structure of a superconducting conductor in a superconducting winding.

液体ヘリウム中で冷却される超電導巻線ま常電導巻線に
比較し、同一寸法のものでは大電流を流すことができ強
磁界を得ることができる。
Compared to superconducting windings cooled in liquid helium or normal conducting windings, those with the same dimensions can carry a large current and generate a strong magnetic field.

このため超電導導体には大きな電磁力が作用し、超電導
巻線の寸法が大きくなるに従って電磁力が増大する。
Therefore, a large electromagnetic force acts on the superconducting conductor, and the electromagnetic force increases as the dimensions of the superconducting winding become larger.

この電磁力を支えるためには従来種々の構造があり、特
に半径方向の力で生ずる超電導導体の円周方向の応力を
低減するために、超電導導体と並列に補強帯を巻回する
構造が用いられている。
Conventionally, various structures have been used to support this electromagnetic force. In particular, in order to reduce stress in the circumferential direction of the superconducting conductor caused by radial force, a structure in which reinforcing bands are wound in parallel with the superconducting conductor has been used. It is being

この補強帯は超電導導体より機械的強度の高い材料例え
ばステンレス鋼が使用されている。
This reinforcing band is made of a material having higher mechanical strength than the superconducting conductor, such as stainless steel.

第1図は超電導巻線の1部であって、1はNbTi合金
線などの超電導線と無酸素鋼などの安定化材とから形成
された超電導導体、2はステンレス鋼などの機械的強度
の高い材料からなる補強帯、3は超電導導体1と補強帯
2との間を絶縁する層間絶縁であって例えばガラスエポ
キシ樹脂などの絶縁物である。
Figure 1 shows a part of a superconducting winding, in which 1 is a superconducting conductor made of superconducting wire such as NbTi alloy wire and a stabilizing material such as oxygen-free steel, and 2 is a superconducting conductor made of mechanically strong material such as stainless steel. The reinforcing band 3 made of a high quality material is an interlayer insulation for insulating between the superconducting conductor 1 and the reinforcing band 2, and is an insulating material such as glass epoxy resin.

一般に超電導導体1、補強帯2と眉間絶縁3とを並列に
重ね合わせて1タ一ン分を形成し、数百ターンから数千
ターンを巻回して超電導巻線を形成している。
Generally, a superconducting conductor 1, a reinforcing band 2, and a glabellar insulation 3 are stacked in parallel to form one turn, and several hundred turns to several thousand turns are wound to form a superconducting winding.

従って超電導導体1の円周方向応力は補強帯2に分配さ
れて低減し増大な電磁力に耐えることができる。
Therefore, the stress in the circumferential direction of the superconducting conductor 1 is distributed to the reinforcing band 2 and reduced, making it possible to withstand increased electromagnetic force.

しかしながら、超電導導体1の冷却面積は両側面のみで
あるので、超電導マグネットの安定化すなわち超電導巻
線の1部が常電導になった場合すぐに超電導に復帰する
ためには充分冷却できる冷却面積が必要であり、大形化
するには冷却面積が小さい欠点があった。
However, since the cooling area of the superconducting conductor 1 is only on both sides, there is not enough cooling area to stabilize the superconducting magnet, that is, to quickly return to superconducting when a part of the superconducting winding becomes normal conductive. However, there was a drawback that the cooling area was small to increase the size.

本考案は上記欠点に鑑みなされたもので、超電導導体の
冷却面積を大巾に拡大した超電導巻線を提供することを
目的とする。
The present invention was devised in view of the above-mentioned drawbacks, and an object of the present invention is to provide a superconducting winding in which the cooling area of the superconducting conductor is greatly expanded.

以下本考案を図面に示す1実施例について説明する。An embodiment of the present invention shown in the drawings will be described below.

第2図において第1図と同じ作用をする部品は同一符号
としたので説明は省略する。
In FIG. 2, parts having the same functions as those in FIG. 1 are designated by the same reference numerals, and their explanations will be omitted.

4は層間絶縁であって冷却媒体である液体ヘリウムの臨
界温度においても圧縮強度を有するテープ状の絶縁物、
例えばガラスエポキシ樹脂からなり、補強帯2にテープ
巾より大きいピッチで間隔2aを設けて巻装している。
4 is a tape-shaped insulator that is interlayer insulation and has compressive strength even at the critical temperature of liquid helium, which is a cooling medium;
For example, it is made of glass epoxy resin and is wound around the reinforcing band 2 at intervals 2a with a pitch larger than the tape width.

この層間絶縁3を巻装した補強帯2と超電導導体1とを
重ねて1タ一ン分を形成した状態で巻線に巻回し超電導
巻線を形成している。
The reinforcing band 2 wrapped with this interlayer insulation 3 and the superconducting conductor 1 are stacked to form one tan, and are wound around a winding wire to form a superconducting winding wire.

次に作用を説明する。Next, the effect will be explained.

補強帯2は超電導導体1に作用する強大な電磁力の1部
を受けもち、機械的強度の弱い超電導導体の円周応力を
低減するのは従来と同じである。
The reinforcing band 2 receives a portion of the strong electromagnetic force acting on the superconducting conductor 1, and reduces the circumferential stress of the superconducting conductor, which has weak mechanical strength, as in the conventional case.

層間絶縁4の間隔2aは超電導導体1が重なっても明い
ているので、層間絶縁4のピッチア1巾をBとすれば超
電導導体1の冷却面積は上下面において概略(1−B/
P)の割合だけ増加することになり、冷却面積の増大は
超電導導体1の安定化に対し非常に大きな効果がある。
The interval 2a of the interlayer insulation 4 remains clear even when the superconducting conductors 1 overlap, so if the width of one pitcher of the interlayer insulation 4 is B, the cooling area of the superconducting conductor 1 on the upper and lower surfaces is approximately (1-B/
The increase in the cooling area has a very large effect on stabilizing the superconducting conductor 1.

すなわち、超電導導体が何らかの原因で超電導状態がや
ぶれ常電導状態になった場合には、電流は銅の部分に流
れるのでジュール熱を発生する。
That is, when a superconducting conductor breaks down from its superconducting state for some reason and becomes a normal conducting state, current flows through the copper portion, generating Joule heat.

常電導状態にもどすには発生したジュール熱を充分冷却
することが必要で、超電導導体1を臨界温度以下にしな
ければならない。
In order to return to the normal conductive state, it is necessary to sufficiently cool the generated Joule heat, and the superconducting conductor 1 must be brought below a critical temperature.

従って超電導導体1の冷却面積が増大し冷却能力が上昇
すれば容易に超電導状態にもどることができる。
Therefore, if the cooling area of the superconducting conductor 1 increases and the cooling capacity increases, the superconducting state can be easily returned.

また超電導導体1は傾斜し、層間絶縁3は斜めに接触し
ているので、発生した液体ヘリウムの泡は層間絶縁4の
側面にそって斜めに上昇するので泡の停滞がなく冷却が
良い。
Further, since the superconducting conductor 1 is inclined and the interlayer insulation 3 is in contact with the superconductor 1 at an angle, the generated liquid helium bubbles rise obliquely along the side surface of the interlayer insulation 4, so that there is no stagnation of the bubbles and cooling is good.

また超電導導体1に強大な電磁力を生じ各層間には圧縮
力が作用しても超電導導体1の上下面の層間絶縁4との
接触は互に交叉するようになるので圧縮力に対する曲げ
応力は大きくなく機械的強度に対しても充分な強度があ
る。
Furthermore, even if a strong electromagnetic force is generated in the superconducting conductor 1 and a compressive force acts between each layer, the contact with the interlayer insulation 4 on the upper and lower surfaces of the superconducting conductor 1 crosses each other, so the bending stress against the compressive force is It is not large and has sufficient mechanical strength.

第3図は他の実施例で層間絶縁4を2重巻きにしたもの
で、層間絶縁4の傾斜が大きくなるので液体ヘリウムの
泡が抜は易くなり冷却性能が向上する。
FIG. 3 shows another embodiment in which the interlayer insulation 4 is double-wound, and since the slope of the interlayer insulation 4 is increased, bubbles of liquid helium can be easily removed and the cooling performance is improved.

特に起電導導体1の巾が大きい場合には効果がある。This is particularly effective when the width of the electromotive conductor 1 is large.

なお、複数巻にしてもよいことは勿論である。Note that it is of course possible to use a plurality of volumes.

以上のように本考案によれば超電導巻線において超電導
導体と並列にテープ状の絶縁物を間隔を設けて層間絶縁
を巻装した補強帯とを重ねて巻回するようにしたので、
超電導導体の側面の外に上下面の層間絶縁の間隔も冷却
面積となり冷却能力が向上し、液体ヘリウムの泡の抜は
出しもよく起電導の安定化が早くなり、製作が容易であ
り大形に適するなどのすぐれた効果がある。
As described above, according to the present invention, in the superconducting winding, tape-shaped insulators are wound in parallel with the superconducting conductor at intervals and reinforcing bands wrapped with interlayer insulation are overlapped.
In addition to the side surfaces of the superconducting conductor, the gap between the interlayer insulation on the top and bottom surfaces also becomes a cooling area, improving the cooling capacity, making it easier to remove bubbles from liquid helium, stabilizing electromotive conduction faster, and making it easier to manufacture and larger. It has excellent effects such as being suitable for

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

第1図は従来の超電導巻線の部分断面斜視図、第2図は
本考案の超電導巻線の1実施例を示す部分断面斜視図、
第3図は他の実施例を示す部分断面斜視図である。 1・・・・・・超電導導体、2・・・・・・補強帯、4
・・・・・・層間絶縁。
FIG. 1 is a partial cross-sectional perspective view of a conventional superconducting winding, and FIG. 2 is a partial cross-sectional perspective view showing an embodiment of the superconducting winding of the present invention.
FIG. 3 is a partially sectional perspective view showing another embodiment. 1...Superconducting conductor, 2...Reinforcement band, 4
・・・・・・Interlayer insulation.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 超電導導体と、層間絶縁と、補強帯とを重ね合せて巻回
して成る超電導巻線において、前記層間絶縁は前記補強
帯にテープ状の絶縁物をテープ巾より大きいピッチで、
間隔を設けて巻装して形成したことを特徴とする超電導
巻線。
In a superconducting winding formed by overlapping and winding a superconducting conductor, interlayer insulation, and reinforcing band, the interlayer insulation includes tape-shaped insulators arranged on the reinforcing band at a pitch larger than the tape width;
A superconducting winding characterized by being formed by winding at intervals.
JP5529378U 1978-04-27 1978-04-27 superconducting winding Expired JPS603545Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5529378U JPS603545Y2 (en) 1978-04-27 1978-04-27 superconducting winding

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5529378U JPS603545Y2 (en) 1978-04-27 1978-04-27 superconducting winding

Publications (2)

Publication Number Publication Date
JPS54158582U JPS54158582U (en) 1979-11-05
JPS603545Y2 true JPS603545Y2 (en) 1985-01-31

Family

ID=28950952

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5529378U Expired JPS603545Y2 (en) 1978-04-27 1978-04-27 superconducting winding

Country Status (1)

Country Link
JP (1) JPS603545Y2 (en)

Also Published As

Publication number Publication date
JPS54158582U (en) 1979-11-05

Similar Documents

Publication Publication Date Title
US3559126A (en) Means to provide electrical and mechanical separation between turns in windings of a superconducting device
US4079187A (en) Superconductor
US3754095A (en) Superconductive cable for carrying either alternating or direct current
US3619479A (en) Electrical conductor of electrically normal conducting metal and superconducting material
US3332047A (en) Composite superconductor
JP2923988B2 (en) Superconducting conductor
US3470508A (en) Superconducting winding
US3550050A (en) Superconducting coil with cooling means
JPS603545Y2 (en) superconducting winding
JPS61113218A (en) Superconductive magnet
US4339681A (en) Superconducting field winding for the rotor of an electric machine
JPH0586053B2 (en)
US3391362A (en) Superconducting magnet coil
US4234861A (en) Electrical windings
JPS6328328B2 (en)
JPS5948488B2 (en) Composite superconducting wire
JPS62214680A (en) Superconductor for thermal permanent current switch
JP3120626B2 (en) Oxide superconducting conductor
JP2549695B2 (en) Superconducting stranded wire and manufacturing method thereof
JP3286036B2 (en) Forced cooling type superconducting conductor
JPS6215803A (en) Superconductive coil
JP2000340420A (en) Superconducting current-limiting device
JPS6266505A (en) Compound strand for power cable conductor
JPH0636625A (en) Superconductor
GB1137459A (en) Superconductor magnetic coils