JPS5857884B2 - Manufacturing method of superconducting electromagnet - Google Patents
Manufacturing method of superconducting electromagnetInfo
- Publication number
- JPS5857884B2 JPS5857884B2 JP52023787A JP2378777A JPS5857884B2 JP S5857884 B2 JPS5857884 B2 JP S5857884B2 JP 52023787 A JP52023787 A JP 52023787A JP 2378777 A JP2378777 A JP 2378777A JP S5857884 B2 JPS5857884 B2 JP S5857884B2
- Authority
- JP
- Japan
- Prior art keywords
- electromagnet
- superconducting
- winding
- manufacturing
- coil bobbin
- 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
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- Coil Winding Methods And Apparatuses (AREA)
Description
【発明の詳細な説明】
本発明は超電導電磁石の製造方法に係り、特に電磁石巻
線の締付は工程に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for manufacturing a superconducting electromagnet, and in particular to a process for tightening electromagnet windings.
良く知られているように、超電導線材は線材温度、印加
磁界および線材通電電流の値がある値(臨界値と呼ばれ
ている)を超えると、超電導状態から常電導状態へ転移
してしまう。As is well known, a superconducting wire transitions from a superconducting state to a normal conducting state when the wire temperature, applied magnetic field, and wire current flow exceed certain values (referred to as critical values).
そこで、超電導線材を有効に活用するためには、超電導
線材の短尺における磁界H−臨界電流Ic特性、いわゆ
る短尺H−Ic特性で示される値まで通電できることが
必要である。Therefore, in order to effectively utilize the superconducting wire, it is necessary to be able to conduct current up to a value shown by the magnetic field H-critical current Ic characteristic in a short length of the superconducting wire, the so-called short length H-Ic characteristic.
しかし、種々の原因によってその値は低下してしまう。However, the value decreases due to various causes.
例えば、第1図に示したような円筒部1aをフランジ部
1bとが一体に形成されたコイルボビン1に、超電導電
磁石巻線2を張力を加えながら巻回して製作された電磁
石では、通電電流は短尺特性の60〜70%位であり、
その主な原因は巻回した超電導線材の励磁中の動きに起
因していることが知られている。For example, in an electromagnet manufactured by winding a superconducting electromagnet winding 2 under tension around a coil bobbin 1 in which a cylindrical part 1a and a flange part 1b are integrally formed as shown in FIG. It is about 60-70% of the short length characteristic,
It is known that the main cause of this is the movement of the wound superconducting wire during excitation.
すなわち、上記のように製作された電磁石を冷媒ヘリウ
ム中で励磁した場合、第2図の矢印に示すような強大な
電磁力が加わるため、電磁石巻線2は破線で示すように
、軸方向へは縮まり、半径方向へは膨張するように変形
される。That is, when the electromagnet manufactured as described above is excited in refrigerant helium, a strong electromagnetic force as shown by the arrow in Fig. 2 is applied, so that the electromagnet winding 2 is moved in the axial direction as shown by the broken line. is deformed so that it contracts and expands in the radial direction.
これらの力のうちで半径方向への膨張力については、導
層時に線材に張力を加えて巻き締めることにより、変形
および線材の動きを防げる。Among these forces, the expansion force in the radial direction can be prevented from deformation and movement of the wire by applying tension to the wire and tightening the wire during conduction.
しかし、軸方向の圧縮力に対しては、巻線に線材を完全
に密接して巻くことが技術的に困難であるために、動き
を生じやすく、励磁運転後観察すると、コイルボビン1
のフランジ部1bとの間に隙間を生じているのが見られ
ることがある。However, in response to compressive force in the axial direction, it is technically difficult to wind the wire in close contact with the winding, so movement tends to occur, and when observed after excitation operation, the coil bobbin 1
A gap may be seen between the flange portion 1b and the flange portion 1b.
つまり、超電導線材の動きが生じているわけで、これが
超電導特性の劣化につながっている。In other words, the superconducting wire moves, which leads to deterioration of superconducting properties.
この欠点を解消するため、近年エポキシ樹脂等を超電導
電磁石巻線部に含浸し、線材の動きを止めて通電電流値
を短尺特性の値に近づける方法が行なわれてきた。In order to overcome this drawback, in recent years a method has been used in which the winding portion of a superconducting electromagnet is impregnated with epoxy resin or the like to stop the movement of the wire and bring the current value closer to the value of the short length characteristic.
この方法によると、短尺特性の85〜100%に対する
ことができるが、その反面下記の如き問題が生じる。According to this method, it is possible to achieve 85 to 100% of the short length characteristics, but on the other hand, the following problems arise.
(1)電磁石全体をエポキシ樹脂等で包んでしまうため
、冷媒との接触が断たれ冷却に時間がかかるようになり
、また例らかの原因で超電導巻線中に熱が発生したよう
なときに電磁石の動作が不安定になる。(1) Since the entire electromagnet is wrapped in epoxy resin, etc., contact with the refrigerant is cut off and cooling takes time.Also, when heat is generated in the superconducting winding for some reason. The operation of the electromagnet becomes unstable.
(2)事故等で超電導線材の一部が焼損したり、断線し
たりした場合や、また電磁石の形状を変更したい場合な
どに、含浸したエポキシ樹脂等を取り去ることができな
いため、高価な超電導線材やコイルボビン等の再使用が
できなくなり、不経済である。(2) If a part of the superconducting wire burns out or breaks due to an accident, or if you want to change the shape of the electromagnet, the epoxy resin impregnated with it cannot be removed, making the superconducting wire expensive. This makes it impossible to reuse the coil bobbin, etc., which is uneconomical.
本発明の目的は、上記した従来技術の欠点を除き、安定
で、しかも経済的な超電導電磁石が得られる製造方法を
提供するにある。An object of the present invention is to provide a manufacturing method that eliminates the above-mentioned drawbacks of the prior art and allows a stable and economical superconducting electromagnet to be obtained.
この目的を達成するため、本発明は、コイルボビンの少
なくとも一方のフランジを軸方向に移動可能にし、極低
温中にて電磁石巻線を励磁して、この時の電磁力で電磁
石巻線をその軸方向に圧縮し、前記フランジを移動して
電磁石巻線を締付は固定したことを特徴とする。In order to achieve this object, the present invention makes at least one flange of a coil bobbin movable in the axial direction, excites the electromagnet winding in a cryogenic temperature, and uses the electromagnetic force generated at this time to move the electromagnet winding along its axis. The flange is moved to tighten and fix the electromagnet winding.
以下、本発明の一実施例を第3図について説明する。An embodiment of the present invention will be described below with reference to FIG.
本実施例で使用するコイルボビンは、円筒部1aと、そ
の両端に軸方向移行可能に嵌合されたフランジ部1bと
からなり、これらのフランジ部1bは円筒部1aの両端
に螺合されたフランジ締付はナツト3により固定されて
いる。The coil bobbin used in this example consists of a cylindrical part 1a and a flange part 1b fitted to both ends of the cylindrical part 1a so as to be able to move in the axial direction. Tightening is done by a nut 3.
このような構造のコイルボビンに超電導電磁石巻線2を
巻回して超電導電磁石を作り、これをクライオスタット
4に充填されている冷媒の液体へjラム5中に浸漬する
と共に、締付はシャフト6の右ねじ部(又は左ねじ部)
6aおよび左ねじ部(又は右ねじ部)6bに螺合された
締付はプレート7により、アダプター8を介して、保持
する。A superconducting electromagnet winding 2 is wound around a coil bobbin having such a structure to create a superconducting electromagnet, and this is immersed in the refrigerant liquid filled in the cryostat 4 into the ram 5. Threaded part (or left-handed threaded part)
6a and the left-hand threaded portion (or right-handed threaded portion) 6b are held by a plate 7 via an adapter 8.
なお第E図中、9はクライオスタットのフランジ、10
は締付はプレート8の回転を防ぐための固定ロフトであ
る。In Figure E, 9 is the flange of the cryostat, 10
The tightening is a fixed loft to prevent rotation of the plate 8.
ついで、このような極低温中に保持された超電導電磁石
の電磁石巻線2に通電して、これを励磁し、その軸方向
に圧縮させた状態で、締付はシャフト6を外部より回転
し、両締付はプレート7を互に近付く方向に移動して、
コイルボビンの両フランジ部1bを移動し、これらのフ
ランジ部1bにより電磁石巻線2を軸方向の両側から締
付ける。Next, the electromagnet winding 2 of the superconducting electromagnet held in such a cryogenic temperature is energized to excite it and compressed in the axial direction, and tightening is carried out by rotating the shaft 6 from the outside. Both tightening moves the plates 7 toward each other,
Both flange portions 1b of the coil bobbin are moved, and the electromagnet winding 2 is tightened from both sides in the axial direction by these flange portions 1b.
このように電磁石巻線を締付けると、フランジ部1bと
締付はナツト3との間には間隙ができるので、これらを
室温部に取出し、締付はナツト3を締付けてフランジ部
1bが電磁石巻線2に対してゆるまないようにする。When the electromagnet winding is tightened in this way, a gap is created between the flange part 1b and the nut 3, so take them out to room temperature and tighten the nut 3 so that the flange part 1b is connected to the electromagnet winding. Make sure that it does not loosen relative to line 2.
この場合、冷媒液体ヘリウム5中より室温部に取出すと
、いったん締ったものが各部品の熱膨張率の違いによっ
てゆるむ場合が考えられる。In this case, when the refrigerant liquid helium 5 is taken out to room temperature, it is conceivable that the once tightened material may loosen due to the difference in the coefficient of thermal expansion of each component.
これを避けるためには、アダプター8を締付はシャフト
6の材料より熱膨張率の大きな、例えば締付はシャフト
6がステンレススチールの場合にはアダプター8をステ
ンレスに対し数倍の熱膨張率のあるエポキシ樹脂材のよ
うなもので作るのがよい。To avoid this, tighten the adapter 8 using a material with a coefficient of thermal expansion larger than that of the shaft 6. For example, if the shaft 6 is made of stainless steel, tighten the adapter 8 with a material that has a coefficient of thermal expansion several times that of stainless steel. It is best to make it from a certain kind of epoxy resin material.
このようにすれば、極低温の冷媒中より室温部に取出す
ときにより強く超電導電磁石巻線部を締付けることがで
きる。In this way, the superconducting electromagnet winding portion can be more strongly tightened when the refrigerant is taken out from the extremely low temperature refrigerant to the room temperature.
このように製作された超電導電磁石における超電導線材
の通電容量は、短尺特性の95〜io。The superconducting wire in the superconducting electromagnet manufactured in this manner has a current carrying capacity of 95 to io, which is a short characteristic.
係に達することが実験により確認された。It has been confirmed through experiments that this can be achieved.
なお、前記のように製作した超電導電磁石に、さらにエ
ポキシ樹脂等を含浸することは、その使用目的によって
は、より有効である。Note that it may be more effective to further impregnate the superconducting electromagnet produced as described above with an epoxy resin or the like, depending on the purpose of its use.
また、前記実験例では、冷媒ヘリウム浸漬方式について
述べたが、ホローコンダクタ−等の強制冷却電機石にも
適用できることは勿論である。Further, in the above-mentioned experimental example, the refrigerant helium immersion method was described, but it goes without saying that it can also be applied to forcibly cooled electrical equipment such as hollow conductors.
さらにまた、本発明は、前記実験例で述べたソレノイド
形電磁石に限らず、特殊な形状の電磁石に対しても広く
適用できることはいうまでもない。Furthermore, it goes without saying that the present invention is widely applicable not only to the solenoid type electromagnet described in the experimental example but also to electromagnets of special shapes.
以上説明したように、本発明によれば、超電導線材の動
きのない超電導特性の安定した超電導電磁石が得られる
と共に、超電導線材、コイルボビン等の分解が容易であ
るため、何度でも設計変更して組替えができ、また故障
時の修理も可能で、きわめて経済的になる。As explained above, according to the present invention, a superconducting electromagnet with stable superconducting properties without any movement of the superconducting wire can be obtained, and since the superconducting wire, coil bobbin, etc. can be easily disassembled, the design can be changed as many times as necessary. It can be reassembled and repaired in the event of a breakdown, making it extremely economical.
第1図は従来における円筒部とフランジ部が一体のコイ
ルボビンを使用した超電導電磁石の断面図、第2図は超
電導電磁石を励磁した場合にその巻線部分に加わる電磁
力の方向を示す説明図、第3図は本発明の製造方法を実
施するために使用される製作装置の断面図である。
1a・・・・・・コイルボビンの円筒部、1b・・・・
・・コイルボビンのフランジ部、2・・・・・・超電導
電磁石巻線、3・・・・・・フランジ締付はナツト、5
・・・・・・液体ヘリウム、6・・・・・・締付はシャ
フト、7・・・・・・締付はプレート。Fig. 1 is a cross-sectional view of a conventional superconducting electromagnet using a coil bobbin with an integral cylindrical part and a flange part, and Fig. 2 is an explanatory diagram showing the direction of electromagnetic force applied to the winding part when the superconducting electromagnet is excited. FIG. 3 is a sectional view of a manufacturing apparatus used to carry out the manufacturing method of the present invention. 1a... Cylindrical part of the coil bobbin, 1b...
... Flange part of coil bobbin, 2 ... Superconducting electromagnet winding, 3 ... Flange tightening with nut, 5
...Liquid helium, 6...Tighten with shaft, 7...Tighten with plate.
Claims (1)
からなる電磁石巻線を巻装した超電導電磁石の製造方法
において、前記フランジの少なくとも一方をコイルボビ
ンの軸方向に移動可能にし、極低温中にて前記電磁石巻
線を励磁して、この時の電磁力で電磁石巻線をその軸方
向に圧縮し、前記フランジを移動して電磁石巻線を締付
は固定したことを特徴とする超電導電磁石の製造方法。1. A method for manufacturing a superconducting electromagnet in which an electromagnet winding made of superconducting wire is wound around a coil bobbin having flanges at both ends, in which at least one of the flanges is made movable in the axial direction of the coil bobbin, and the electromagnet winding is wound in an extremely low temperature. A method for manufacturing a superconducting electromagnet, characterized in that the electromagnet winding is compressed in its axial direction by the electromagnetic force at this time, and the flange is moved to tighten and fix the electromagnet winding.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP52023787A JPS5857884B2 (en) | 1977-03-07 | 1977-03-07 | Manufacturing method of superconducting electromagnet |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP52023787A JPS5857884B2 (en) | 1977-03-07 | 1977-03-07 | Manufacturing method of superconducting electromagnet |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS53109496A JPS53109496A (en) | 1978-09-25 |
| JPS5857884B2 true JPS5857884B2 (en) | 1983-12-22 |
Family
ID=12120023
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP52023787A Expired JPS5857884B2 (en) | 1977-03-07 | 1977-03-07 | Manufacturing method of superconducting electromagnet |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5857884B2 (en) |
-
1977
- 1977-03-07 JP JP52023787A patent/JPS5857884B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS53109496A (en) | 1978-09-25 |
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