JPS6025845B2 - Manufacturing method of composite superconducting conductor - Google Patents
Manufacturing method of composite superconducting conductorInfo
- Publication number
- JPS6025845B2 JPS6025845B2 JP4113079A JP4113079A JPS6025845B2 JP S6025845 B2 JPS6025845 B2 JP S6025845B2 JP 4113079 A JP4113079 A JP 4113079A JP 4113079 A JP4113079 A JP 4113079A JP S6025845 B2 JPS6025845 B2 JP S6025845B2
- Authority
- JP
- Japan
- Prior art keywords
- superconducting conductor
- grooves
- groove
- large number
- composite superconducting
- 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
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- Superconductors And Manufacturing Methods Therefor (AREA)
Description
【発明の詳細な説明】
本発明は、超電導送電用ケーブルや各種の超電導マグネ
ット等に使用される複合超電導導体の製造方法に関する
。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for manufacturing a composite superconducting conductor used for superconducting power transmission cables, various superconducting magnets, and the like.
複合超電導導体は超電導材と常電導材からなり、例えば
直径5ムm〜250山nの超電導素線を、銅、アルミニ
ウムあるいはその他の金属、またはそられの金属の合金
等の常電導材の中に埋め込んで、丸線、平角線、中空線
に仕上げたものである。A composite superconducting conductor consists of a superconducting material and a normal conducting material. For example, a superconducting wire with a diameter of 5 mm to 250 threads is placed in a normal conducting material such as copper, aluminum, other metals, or alloys of these metals. These wires are embedded into round wires, flat wires, and hollow wires.
第1図は従来の複合超電導導体の一例を示す断面図、多
数の超電導素線1が銅やアルミニウムなどの常電導材2
中に埋め込され、平角線として仕上げられてる。Figure 1 is a cross-sectional view showing an example of a conventional composite superconducting conductor, in which a large number of superconducting strands 1 are made of a normal conducting material 2 such as copper or aluminum.
It is embedded inside and finished as a flat wire.
矩形断面の最辺側には絶縁体3が張られ、最辺側の面で
絶縁体3を介して接するように巻回されてコイルを構成
する。線材は超電導性を示すから、一定磁界一定電流の
もとでは発熱しないが、通電電流の時間的変化に対して
は磁化にともなう損失を発生する。また、万一、何らか
の原因で超電導性が破れたとき、多大のジュール発熱を
生ずる。このため、複合超電導導体の一部例えば矩形断
面の短辺側4を液体ヘリウムと直接接して冷却される冷
却面とするべく、隣接したコイルとの間に液体ヘリウム
の通る隙間10(幅1〜5凧)を設けてある。超導領域
の拡大を防止する条件は、次式で与えられる。An insulator 3 is placed on the edge of the rectangular cross section, and the coil is wound so as to be in contact with the edge of the coil through the insulator 3. Since the wire exhibits superconductivity, it does not generate heat under a constant magnetic field and constant current, but it generates loss due to magnetization when the current changes over time. Furthermore, if the superconductivity is broken for some reason, a large amount of Joule heat will be generated. Therefore, in order to make a part of the composite superconducting conductor, for example, the short side 4 of the rectangular cross section, a cooling surface that is cooled by coming into direct contact with liquid helium, a gap 10 (width 1 to 5 kites) are provided. The conditions for preventing the expansion of the superconducting region are given by the following equation.
鯖<・ ・.・・.・・.・tl’あぶる雛議
孫電鰐鞠の彰鰐q:冷却熱流速、である。Mackerel<・・..・・・.・・・.・tl'Aburu Hinagisonden Wanimari's Showaniq: Cooling heat flow rate.
電流値や冷却条件ぎ与えられた場合、式{1)を満足さ
せるには、冷却周囲長Pおよび帯電導体の断面積Aを大
きくしなければならない。Given the current value and cooling conditions, the cooling perimeter P and the cross-sectional area A of the charged conductor must be increased in order to satisfy equation {1).
すなわち、多量の常電導材を使わねばならず、菱贋の大
形化、重量増加などコスト上昇の大きな要因となってい
る。この一つの対策として、例えば特公昭45一22斑
8号公報に記載のように複合超電導導体の表面に、深さ
1肋、中1帆の矩形溝をピッチ2側で設けたりする方法
が知られている。That is, a large amount of normal conductive material must be used, which is a major factor in increasing costs, such as increasing the size and weight of the diamond counterfeit. As one countermeasure against this problem, a method is known in which a rectangular groove with one rib in depth and one sail in middle is provided on the surface of the composite superconducting conductor on the pitch 2 side, as described in Japanese Patent Publication No. 8 of Japanese Patent Publication No. 45-22. It is being
この方法は、前述の冷却周囲長Pを約2倍ほど高める効
果が期待されるが、なお十分なのとは言いきれない。超
電導マグネットのように、狭に冷却チャンネル中に置か
れたとき、このような冷却面は必ずしも表面積の増加に
比例た冷却量(P×q)が得られるは限らず、むしろ低
くなる。また、Pを増すために特閥昭52−7078y
号公報に記載のように狭いピッチで深い溝を彫ると切削
に伴い切りくず導体に付着してコイル中にまぎれこみ、
絶縁体3を狭む導体2−2間あるいは液体ヘリウム用の
隙間10を介したコイル間で電気的に短落する可能性が
ある。本発明は、上述たような門合点を解決するために
なされたもので、複合超電導導体の冷却面の表皮帯城に
、底部に鋭角部を有する間隔の小さい多数の溝と、これ
らの溝にて隔てられ、先端が鋭角的に先細り状をしてい
る多数の隆起部とを、鋤き起し加工によって切り肩を出
すことなく形成し、冷却量の増大をはかったものである
。Although this method is expected to have the effect of increasing the cooling perimeter P by about twice, it cannot be said that it is still sufficient. When placed in a narrow cooling channel like a superconducting magnet, such a cooling surface does not necessarily provide a cooling amount (P×q) proportional to the increase in surface area, but rather becomes lower. In addition, in order to increase P, we added
When deep grooves are carved with a narrow pitch as described in the publication, chips adhere to the conductor and get mixed into the coil.
There is a possibility of electrical short-circuiting between the conductors 2 and 2 that narrow the insulator 3 or between the coils via the gap 10 for liquid helium. The present invention was made to solve the above-mentioned problems, and includes a large number of closely spaced grooves each having an acute angle at the bottom in the skin band of the cooling surface of a composite superconducting conductor. A large number of ridges are separated from each other and have sharply tapered tips, and are formed by plowing without exposing the cut shoulder, thereby increasing the amount of cooling.
以下、本発明方法の一実施例を第2図により説明する。An embodiment of the method of the present invention will be described below with reference to FIG.
第2図は平角線に仕上げた複合超電導導体の矩諺断面の
短辺側に冷却面が形成され最辺側に絶縁体3が張られて
いる場合である。まず多数の超電導素線1を銅やアルミ
ニウムなどの常電導材2の中に埋め込む。次に冷却面の
表皮帯域に、多数の連続接近する並行な第1の溝5と、
第1の溝5により隔てられた多数の連続する並行な隆起
部6とを形成する。この時の加工法としては、表皮帯城
を切除することなく鋤き起すように塑性変形させる方法
を用い、微細で深い溝を接近させた状態にする。また加
工用のバイトは刃先形状が同じかやや異なるものを教本
用意し、段階的に加工を行う。鋤き起し用のバイトは、
切出し状の刃先すなわち斜めに刃が形成されたものを用
いればよい。これにより、溝5は底部に鋭角部を有し、
また、第1の溝5により隔てられる多数の並行な隆起部
6は先端が鋭角部に先細り状となっている。第1の溝5
の大きさは、例えば中0.2脚、深さ0.8肋、ピッチ
0.4肌である。したがって隆起部6の大きさも中0.
2職、高さ0.8肋となる。このような構成では、表面
積は非加工面の3倍になる。第3図は、本発明の複合超
電導導体の製造方法の他の実施例を説明するための図で
複合超電導導体の冷却面の表皮帯城の拡大図である。FIG. 2 shows a case where a cooling surface is formed on the short side of the rectangular cross section of a composite superconducting conductor finished into a rectangular wire, and an insulator 3 is stretched on the farthest side. First, a large number of superconducting wires 1 are embedded in a normal conductive material 2 such as copper or aluminum. then in the skin zone of the cooling surface a number of successively adjacent parallel first grooves 5;
forming a number of consecutive parallel ridges 6 separated by first grooves 5; The processing method used at this time is to plastically deform the epidermis by plowing it up without cutting it, thereby creating fine, deep grooves that are close to each other. In addition, a textbook is prepared for machining bits with the same or slightly different cutting edge shapes, and machining is performed in stages. The bit for raising the plow is
A cut-out cutting edge, that is, one with an obliquely formed blade may be used. As a result, the groove 5 has an acute angle at the bottom,
Further, a large number of parallel raised portions 6 separated by the first groove 5 have tips tapered to an acute angle portion. First groove 5
The size is, for example, 0.2 legs in the middle, 0.8 ribs in depth, and 0.4 skin in pitch. Therefore, the size of the raised portion 6 is also medium.
2 jobs, 0.8 ribs in height. In such a configuration, the surface area is three times that of the unprocessed surface. FIG. 3 is a diagram for explaining another embodiment of the method for manufacturing a composite superconducting conductor of the present invention, and is an enlarged view of the skin band on the cooling surface of the composite superconducting conductor.
第3図においては、まず、複合超電導導体の常電導材2
表面に、数の刻み用の突状をもったロ−ルを具備するロ
ーレット器を圧接し、複合超電導導体をロール回転方向
に移動する。これにより常電導材2の表皮帯城には間隔
の小なる比較的浅い第2の溝8が一定のピッチで多数形
成される。第2の溝8が形成されたら、第2の溝8と交
叉する方向に第1の溝5の加工を行う。溝加工用のバイ
トは刃先形成が同じかやや異なるもの教本を用意し、段
階的に加工を行う。この時の加工は、常電導材2の表面
を切除することなく、鋤き起こすように変形させる方法
を用い、微細で深い溝を接近させた状態にする。これに
より常電導材2の冷却面の表皮帯域には、底部に鋭角部
を有する間隔の小さい多数の連続する並行な第1の溝5
とこの溝5によって隔離され、先端が鋭角的に先細り状
となっていると共に先端からの深さが第1の溝5の深さ
よりも浅く底部が鋭角状に鏡斜しているV字形の間隔の
小なる谷7をもった隆起部6が形成される。例えば第1
の溝5の中0.2肌、深さ0.8柵、ピッチ0.4肋、
谷7のピッチ0.6柳、深さ0.4肌の場合、表面積は
非加工面の3.5倍ほどに達する。このようにして得ら
れた効果を第4図にて説明する。In Fig. 3, first, the normal conducting material 2 of the composite superconducting conductor is
A knurling machine equipped with a roll having protrusions for incrementing numbers is pressed onto the surface, and the composite superconducting conductor is moved in the direction of rotation of the roll. As a result, a large number of relatively shallow second grooves 8 with small intervals are formed at a constant pitch in the skin band of the normal conductive material 2. After the second groove 8 is formed, the first groove 5 is processed in a direction intersecting with the second groove 8. A textbook for groove machining tools with the same or slightly different cutting edge formation is prepared, and the machining is performed step by step. In this processing, the surface of the normal conductive material 2 is not cut away, but is deformed in a plowing manner, so that fine, deep grooves are formed close to each other. As a result, in the skin zone of the cooling surface of the normal conductive material 2, a large number of successive parallel first grooves 5 with small intervals each having an acute angle at the bottom are formed.
and a V-shaped interval separated by this groove 5, the tip tapering at an acute angle, the depth from the tip being shallower than the depth of the first groove 5, and the bottom being mirror-slanted at an acute angle. A raised portion 6 having a small valley 7 is formed. For example, the first
In the groove 5, 0.2 skin, depth 0.8 fence, pitch 0.4 rib,
In the case of valley 7 with a pitch of 0.6 and a depth of 0.4, the surface area reaches about 3.5 times that of the unprocessed surface. The effects obtained in this way will be explained with reference to FIG.
第4図は、冷却の性能を表わすために、横軸に導体表面
の温度Twと冷却流体である液体ヘリウムの温度Tb(
4.2K)との差をとり、縦軸に導体表面から液体ヘリ
ウムへ伝えられる熱流東q(熱流Qを表面積Aで割った
値)をとったものである。ここで、Aとしては投影面積
(すなわち非加工面の表面積)をとる。冷却チャンネル
の大きさは、すきま約2.3柳、長さ約5仇帆、中1仇
舷であり、Twは長さ方向の平均的な値である。曲線a
は通常の研摩した銅の表面の特性、曲像bは第3図に示
した実施例の表面の特性である。熱流東qを上げてゆく
と、はじめ核沸騰によって伝達が行われ、ある熱流東q
maxで膜沸騰に遷移する。こで、qを下げるとqmj
nで再び該沸騰に戻る。qmaxとqmjnの間は実験
できないので推定で示した。超電導導体が万一何らかの
原因で温度が上昇し際沸騰領域に転移したときその原因
が消失すれば核沸騰領域に戻り超電導特性を回復するた
めにはqmaxとqminができるだけ高いことが望ま
しく、とくにqminの影響は大きい。In Fig. 4, in order to express the cooling performance, the horizontal axis shows the temperature Tw of the conductor surface and the temperature Tb (
4.2 K), and the vertical axis is the heat flow east q (the value obtained by dividing the heat flow Q by the surface area A) transferred from the conductor surface to the liquid helium. Here, the projected area (ie, the surface area of the unprocessed surface) is taken as A. The size of the cooling channel is approximately 2.3 mm in clearance, approximately 5 mm in length, and 1 mm in length, and Tw is the average value in the length direction. curve a
is the characteristic of a normal polished copper surface, and curved image b is a characteristic of the surface of the embodiment shown in FIG. As the heat flow east q is raised, the transfer is first carried out by nucleate boiling, and a certain heat flow east q
At max, it transitions to film boiling. Here, if q is lowered, qmj
Return to the boiling point again at n. Since experiments cannot be performed between qmax and qmjn, the values are estimated. In the unlikely event that a superconducting conductor transitions to the boiling region due to an increase in temperature for some reason, it will return to the nucleate boiling region and recover the superconducting properties if the cause disappears, so it is desirable that qmax and qmin be as high as possible, especially qmin. has a large impact.
曲線bのqmaxは、曲線aのqmaxにくらべてあま
り増えていない。このことは実施例に示すような微細な
表面構造は狭い空間では必ずしも表面積増加に対応した
qmaxの増加が得られないことを示している。一方、
曲線bのqmjnは曲線aのqmlnの4倍以上に達し
、表面積増加に比例する分以上の熱流東増加がある。本
実施例に示すような微細な表面構造が、膜沸騰の安定性
を阻害しているのではないかと思われる。〈に隆起部の
鋭角部が好影響を及どしていると想像される。以上述べ
たように本発明の製法は、複合超電導導体の冷却面の表
皮帯域に、鋤き起し加工により切り層を出すことなく、
鋭角状の底部を有する多数の溝を形成すると同時に、溝
により隔てられ先端が鋭角的に先細り状の多数の隆起部
を形成するようにしたので、従来にくらべて冷却表面の
膜沸騰の限界熱流東qmjnを大幅に増加することがで
きる。qmax of curve b does not increase much compared to qmax of curve a. This shows that with a fine surface structure as shown in the example, an increase in qmax corresponding to an increase in surface area cannot necessarily be obtained in a narrow space. on the other hand,
The qmjn of the curve b is more than four times the qmln of the curve a, and there is an increase in the heat flow east by an amount more than proportional to the increase in the surface area. It is thought that the fine surface structure shown in this example impedes the stability of film boiling. It is thought that the acute angles of the ridges have a positive effect on the 〈. As described above, the manufacturing method of the present invention does not create a cut layer in the skin zone of the cooling surface of the composite superconducting conductor by plowing.
By forming a large number of grooves with acute-angled bottoms and at the same time forming a large number of ridges separated by the grooves and tapered at acute angles, the critical heat flow for film boiling on the cooling surface is reduced compared to conventional methods. East qmjn can be significantly increased.
しかもこの溝の形成寺時には切削の如く切りくずが出な
いので切りくずによる電気的短絡の恐れが生じないとい
う効果がある。Moreover, when forming the groove, no chips are produced as in cutting, so there is no risk of electrical short circuits caused by chips.
第1図は従来の複合超電導導体の一例を示す断面図、第
2図は本発明の方法の一実施例により製造された複合超
電導導体の拡大斜視図、第3図は本発明の方法の実施例
により製造された複合超電導導体の要部拡大斜視図、第
4図は従来の複合超電導導体と本発明の方法により製造
された第3図に示す複合超電導導体とを比較した特性図
である。
1・・・・・・超電導素線、2・・・常電導材、3・・
・・・・絶縁体、5・・・・・・第1の溝、6・・・・
・・隆起部、7・・・谷。
オー図豹2図
第3図
兼4図FIG. 1 is a sectional view showing an example of a conventional composite superconducting conductor, FIG. 2 is an enlarged perspective view of a composite superconducting conductor manufactured by an embodiment of the method of the present invention, and FIG. 3 is an implementation of the method of the present invention. FIG. 4 is an enlarged perspective view of the main part of the composite superconducting conductor manufactured according to the example, and is a characteristic diagram comparing the conventional composite superconducting conductor and the composite superconducting conductor shown in FIG. 3 manufactured by the method of the present invention. 1...Superconducting wire, 2...Normal conductive material, 3...
...Insulator, 5...First groove, 6...
...ridge, 7...valley. O figure leopard figure 2 figure 3 figure and 4 figure
Claims (1)
の1部又は全部にわたつて、鋤き起し加工を行ない、間
隔の小さい多数の連続接近する第1の溝と、該第1の溝
によつて隔てられ先端が鋭角的に先細り状となつている
多数の隆起部とを形成するとを特徴とする複合超電導導
体の製造方法。 2 超電導材と常電導材からなる複合超電導導体の表面
の1部又は全部にわたつて、まず、機械加工により間隔
の小さい多数の連続接近する第2の溝を形成し、次に第
2の溝と交叉する方向に、該第2の溝より深く鋤き起し
加工を行ないこれにより、間隔が小さく、かつ前記第2
の溝より深い多数の連続接近する第1の溝と、先端が鋭
角的に先細り状をなすと共に先端からの深さが前記第1
の溝より浅い多数のV字形の谷を備えた多数の隆起部と
を形成することを特徴とする複合超電導導体の製造方法
。[Claims] 1 A plowing process is performed over part or all of the surface of a composite superconducting conductor made of a superconducting material and a normal conducting material, and a large number of successively approaching first grooves with small intervals are formed. , and a large number of protuberances separated by the first groove and each having an acutely tapered tip. 2. First, a large number of closely spaced second grooves are formed by machining over part or all of the surface of a composite superconducting conductor made of a superconducting material and a normal conducting material, and then the second grooves are The plowing process is performed to be deeper than the second groove in the direction intersecting with the second groove.
a plurality of consecutively approaching first grooves deeper than the grooves of the first groove;
A method for producing a composite superconducting conductor, the method comprising: forming a large number of ridges having a large number of V-shaped valleys that are shallower than the grooves of the composite superconducting conductor.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4113079A JPS6025845B2 (en) | 1979-04-06 | 1979-04-06 | Manufacturing method of composite superconducting conductor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4113079A JPS6025845B2 (en) | 1979-04-06 | 1979-04-06 | Manufacturing method of composite superconducting conductor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5556306A JPS5556306A (en) | 1980-04-25 |
| JPS6025845B2 true JPS6025845B2 (en) | 1985-06-20 |
Family
ID=12599851
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4113079A Expired JPS6025845B2 (en) | 1979-04-06 | 1979-04-06 | Manufacturing method of composite superconducting conductor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6025845B2 (en) |
-
1979
- 1979-04-06 JP JP4113079A patent/JPS6025845B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5556306A (en) | 1980-04-25 |
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