JPS6348402B2 - - Google Patents
Info
- Publication number
- JPS6348402B2 JPS6348402B2 JP12250382A JP12250382A JPS6348402B2 JP S6348402 B2 JPS6348402 B2 JP S6348402B2 JP 12250382 A JP12250382 A JP 12250382A JP 12250382 A JP12250382 A JP 12250382A JP S6348402 B2 JPS6348402 B2 JP S6348402B2
- Authority
- JP
- Japan
- Prior art keywords
- superconducting
- coil
- winding
- wire
- wires
- 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
Classifications
-
- 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
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Containers, Films, And Cooling For Superconductive Devices (AREA)
Description
【発明の詳細な説明】
この発明は超電導コイルの巻線、特に巻線に使
用する超電導線の接続に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to the winding of a superconducting coil, and particularly to the connection of superconducting wire used in the winding.
一般に、従来の巻枠に超電導線を巻回して成る
超電導コイルにおいて、1本の長尺の超電導線を
巻回してつくられる場合には、超電導線の接続の
問題は起らないが、細い超電導線によつて比較的
大きな超電導コイルを巻線する場合には超電導線
の接続の必要性が必ず生じ、例えば、直径1m、
長さ1mのコイルを断面が1mm×1mmの超電導線
で巻いて、必要巻数を10000ターンとすると、必
要超電導線長さは約30Kmにもなる。この様な断面
が1mm×1mm程度の超電導線であれば、現在の技
術によつて連続長さ5〜10Kmのものが作られ、従
つて、この例のようなコイルでは最低3本の超電
導線を2ケ所で接続することが必要である。 In general, when a superconducting coil is made by winding a superconducting wire around a conventional winding frame, the problem of connecting the superconducting wire does not occur when a single long superconducting wire is wound. When winding a relatively large superconducting coil with a wire, it is necessary to connect the superconducting wire, for example, a wire with a diameter of 1 m,
If a 1 m long coil is wound with superconducting wire with a cross section of 1 mm x 1 mm, and the required number of turns is 10,000 turns, the required length of superconducting wire will be approximately 30 km. With current technology, a superconducting wire with a cross section of about 1 mm x 1 mm can be made with a continuous length of 5 to 10 km, so a coil like this example requires at least three superconducting wires. It is necessary to connect them at two places.
この様な超電導コイル1は、従来一般には、例
えば添付図面の第1図に示されるように巻枠2に
超電導線3が巻かれて、接続部4がコイル巻線部
の内部に設けられている。第2図は、第1図に示
されるこの超電導コイル1の巻線および接続部4
の原理図で、第2図に示されるように、一般には
超電導線3の接続は2本の超電導線3を並列にし
てハンダ、圧着等で接続されている。この様な接
続部4が第3図に拡大して示されており、矢印に
よつて電流の流れる方向が示されている。これら
の図から明らかなように、超電導線3の接続部4
においては電気的には1ターン分であつても物理
的には2ターン分のスペースが必要とされる。従
つて、この様な従来の超電導コイルの接続部は上
述のように構成されているので、ターン数を1タ
ーン損をすることになり、このために1ターン分
の死空間が生じ、巻線の均一性が乱され且つ発生
磁界の均一度を悪化させる等の欠点がみられる。
特に、高均一磁界が要求されるコイルでは、この
様なことは致命的欠陥となる。 Conventionally, such a superconducting coil 1 has a superconducting wire 3 wound around a winding frame 2, and a connecting portion 4 provided inside the coil winding portion, as shown in FIG. 1 of the accompanying drawings. There is. FIG. 2 shows the windings and connection portions 4 of this superconducting coil 1 shown in FIG.
As shown in FIG. 2, two superconducting wires 3 are generally connected in parallel by soldering, crimping, or the like. Such a connection 4 is shown enlarged in FIG. 3, and arrows indicate the direction of current flow. As is clear from these figures, the connection portion 4 of the superconducting wire 3
In this case, even if the space is electrically equivalent to one turn, physically the space is required to be equivalent to two turns. Therefore, since the connection part of such a conventional superconducting coil is configured as described above, one turn is lost, which creates a dead space for one turn, and the winding There are disadvantages in that the uniformity of the magnetic field is disturbed and the uniformity of the generated magnetic field is deteriorated.
In particular, this is a fatal defect in coils that require a highly uniform magnetic field.
従つて、この発明の目的はこの様な従来におけ
る欠点を除去するために、超電導コイルの接続部
をコイル巻線部の外部に設け、且つ超電導線の接
続を電流が折り返して流れるようにすることによ
つて、コイル巻線中の1ターンの損失を防ぐと共
に、発生磁界の均一度の低下を防ぐようにした超
電導コイルを提供することにある。 Therefore, an object of the present invention is to provide a connection portion of a superconducting coil outside the coil winding portion and to allow current to flow through the connection of the superconducting wire in a looped manner, in order to eliminate such conventional drawbacks. Therefore, it is an object of the present invention to provide a superconducting coil which prevents loss of one turn in the coil winding and also prevents a decrease in the uniformity of the generated magnetic field.
この発明に依れば、超電導コイルは、複数本の
超電導線を接続して連続して巻回する超電導コイ
ルにおいて、超電導線の接続部を、コイル巻線部
の外部にて且つ互いに接続する2本の超電導線に
流れる電流が折り返してくるように接続して設け
られている。 According to this invention, in a superconducting coil in which a plurality of superconducting wires are connected and wound continuously, the connecting portions of the superconducting wires are connected to each other outside the coil winding portion. The superconducting wires are connected so that the current flowing through them is turned around.
この発明の他の目的や特長および利点は以下の
図面に沿つての詳細な説明から明らかになろう。 Other objects, features and advantages of the present invention will become apparent from the detailed description taken in conjunction with the following drawings.
第4図においてはこの発明に従つた超電導コイ
ルの一実施例が示されており、先に説明した第1
図と同一および相当部分には同一符号が付けられ
ている。図示実施例では、この発明の超電導コイ
ル1は巻枠2に超電導線3が巻かれて成り、接続
部4は1層目のコイルが巻き終つて2層目の巻線
に入る時にコイル巻線部の外部に設けられてい
る。この様に、接続部4がコイル巻線の外部にあ
るために、コイル巻線部内に1ターンの損失を生
じることがない。更に、第5図に拡大して示され
る様に、接続部4における接続は2本の超電導線
3を並列して折り返した形で、ハンダや圧着等に
より実施されているので、接続部4では2方向の
電流が流れるために全体として電流が零となり、
接続部4には磁場を殆んど発生しない。従つて、
超電導コイル1の発生磁界が接続部4によつて乱
されることが全くなく、超電導コイル1の均一度
が良くなる。 FIG. 4 shows an embodiment of the superconducting coil according to the present invention, and shows the first embodiment of the superconducting coil according to the present invention.
Identical or equivalent parts to those in the figures are given the same reference numerals. In the illustrated embodiment, the superconducting coil 1 of the present invention is made up of a superconducting wire 3 wound around a winding frame 2, and the connecting portion 4 connects the coil winding when the first layer coil finishes winding and enters the second layer winding. It is located outside the department. In this manner, since the connecting portion 4 is located outside the coil winding, no loss of one turn occurs within the coil winding. Furthermore, as shown in an enlarged view in FIG. 5, the connection at the connection part 4 is made by folding two superconducting wires 3 in parallel and is made by soldering, crimping, etc. Since current flows in two directions, the overall current becomes zero,
Almost no magnetic field is generated in the connecting portion 4. Therefore,
The magnetic field generated by the superconducting coil 1 is not disturbed by the connecting portion 4 at all, and the uniformity of the superconducting coil 1 is improved.
また、この例では、超電導線の接続を、超電導
コイルにおいて1層目巻線から2層目巻線に移る
ところで実施しているが、超電導線3の連続長さ
との関連で、都合の良い任意の層からその次の層
に移る時に超電導線の接続を好適に行うことがで
きることは勿論である。 In addition, in this example, the superconducting wires are connected at the transition from the first layer winding to the second layer winding in the superconducting coil, but in relation to the continuous length of the superconducting wire 3, it is possible to connect the superconducting wires at any convenient point. Needless to say, the superconducting wires can be suitably connected when moving from one layer to the next layer.
この様に、この発明に依れば、超電導線の接続
をコイル巻線の外部で実施したので、接続部にお
けるコイル巻線内の1ターン分の死空間が無くな
り、また巻線の均一性の乱れもなくなり、その結
果発生磁界の均一度が向上されると共に、超電導
線の接続を電流が折り返して流れるように成した
ので、超電導線の接続部には殆んど磁界を発生せ
ず且つ均一度が良くなる等の効果を達成すること
ができる。 As described above, according to the present invention, since the superconducting wire is connected outside the coil winding, there is no dead space for one turn in the coil winding at the connection part, and the uniformity of the winding is improved. There is no disturbance, and as a result, the uniformity of the generated magnetic field is improved, and since the current flows through the connections of the superconducting wires in a folded manner, almost no magnetic field is generated at the connections of the superconducting wires, and the magnetic field is uniform. You can achieve effects such as getting better once.
第1図は従来の超電導コイルの概略説明図、第
2図は第1図における巻線および超電導線の接続
の原理図、第3図は第2図における接続部の拡大
図、第4図はこの発明に従つた超電導コイルの概
略説明図、第5図は第4図における接続部の拡大
図である。
図中、1……超電導コイル、2……巻枠、3…
…超電導線、4……接続部。なお、図中、同一符
号は同一、または相当部分を示す。
Figure 1 is a schematic explanatory diagram of a conventional superconducting coil, Figure 2 is a diagram of the principle of connection of the winding and superconducting wire in Figure 1, Figure 3 is an enlarged view of the connection part in Figure 2, and Figure 4 is A schematic explanatory diagram of a superconducting coil according to the present invention, FIG. 5 is an enlarged view of the connection portion in FIG. 4. In the figure, 1... superconducting coil, 2... winding frame, 3...
...Superconducting wire, 4... Connection part. In addition, in the figures, the same reference numerals indicate the same or equivalent parts.
Claims (1)
る超電導コイルにおいて、超電導線の接続部を、
コイルの主巻線部の外部にて且つ互いに接続する
2本の超電導線に流れる電流が折り返してくるよ
うに接続して設けることを特徴とする超電導コイ
ル。1 In a superconducting coil in which multiple superconducting wires are connected and wound continuously, the connection part of the superconducting wire is
A superconducting coil, characterized in that the two superconducting wires are connected to each other so that the current flowing through the two superconducting wires is connected to each other outside the main winding portion of the coil.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12250382A JPS5911603A (en) | 1982-07-12 | 1982-07-12 | Superconductive coil |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12250382A JPS5911603A (en) | 1982-07-12 | 1982-07-12 | Superconductive coil |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5911603A JPS5911603A (en) | 1984-01-21 |
| JPS6348402B2 true JPS6348402B2 (en) | 1988-09-29 |
Family
ID=14837452
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP12250382A Granted JPS5911603A (en) | 1982-07-12 | 1982-07-12 | Superconductive coil |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5911603A (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5247271A (en) * | 1984-09-07 | 1993-09-21 | Mitsubishi Denki Kabushiki Kaisha | Superconducting solenoid coil |
| DE4020112A1 (en) * | 1990-06-23 | 1992-01-09 | Bruker Analytische Messtechnik | MAGNETIC DEVELOPMENT WITH COMPENSATION |
| JP4590344B2 (en) | 2005-11-21 | 2010-12-01 | 株式会社リコー | Electrostatic latent image carrier, image forming apparatus using the same, process cartridge, and image forming method |
| JP5548108B2 (en) | 2010-11-22 | 2014-07-16 | 株式会社神戸製鋼所 | Oxide superconducting solenoid coil and method for manufacturing the same |
-
1982
- 1982-07-12 JP JP12250382A patent/JPS5911603A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5911603A (en) | 1984-01-21 |
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