Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPH0779048B2 - How to connect saddle type superconducting magnet coil - Google Patents
[go: Go Back, main page]

JPH0779048B2 - How to connect saddle type superconducting magnet coil - Google Patents

How to connect saddle type superconducting magnet coil

Info

Publication number
JPH0779048B2
JPH0779048B2 JP16947286A JP16947286A JPH0779048B2 JP H0779048 B2 JPH0779048 B2 JP H0779048B2 JP 16947286 A JP16947286 A JP 16947286A JP 16947286 A JP16947286 A JP 16947286A JP H0779048 B2 JPH0779048 B2 JP H0779048B2
Authority
JP
Japan
Prior art keywords
layer coil
coil
wire
inner layer
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 - Lifetime
Application number
JP16947286A
Other languages
Japanese (ja)
Other versions
JPS6325905A (en
Inventor
則雄 武井
勝朗 大石
至 井上
▲長▼ 池田
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Furukawa Electric Co Ltd
Original Assignee
Furukawa Electric Co Ltd
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 Furukawa Electric Co Ltd filed Critical Furukawa Electric Co Ltd
Priority to JP16947286A priority Critical patent/JPH0779048B2/en
Publication of JPS6325905A publication Critical patent/JPS6325905A/en
Publication of JPH0779048B2 publication Critical patent/JPH0779048B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Landscapes

  • Particle Accelerators (AREA)
  • Superconductors And Manufacturing Methods Therefor (AREA)

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は鞍形超電導マグネットの接続方法の改良に関す
るものである。
DETAILED DESCRIPTION OF THE INVENTION (Industrial field of application) The present invention relates to an improvement in a method for connecting a saddle type superconducting magnet.

(従来の技術) 鞍形超電導マグネットコイルは高エネルギー物理学分野
において加速器等の荷電粒子偏向用などに使用されてい
る。この鞍形超電導マグネットコイルは第4図(a)に
示すように断面が半円筒状の外層コイル(1)(1′)
と内層コイル(2)(2′)を上下に夫々重ね合せて二
層の円筒状としたものである。この鞍形超電導マグネッ
トコイルは臨界電流値など超電導特性を所望のものとす
るため各々のコイルに使用する超電導線は断面積および
寸法が異なるのが通常である。一般に内層コイルは外層
コイルより高い磁界に曝される。超電導線の臨界電流密
度は磁界が高くなるにしたがって低くなるため、内層コ
イル用超電導層の断面積は外層コイル用超電導線の断面
積より大きくなっている。
(Prior Art) Saddle-shaped superconducting magnet coils are used in the field of high energy physics, such as for deflecting charged particles in accelerators and the like. This saddle-shaped superconducting magnet coil is an outer layer coil (1) (1 ') having a semi-cylindrical cross section as shown in FIG. 4 (a).
And the inner layer coils (2) and (2 ') are vertically stacked to form a two-layer cylindrical shape. In this saddle type superconducting magnet coil, the superconducting wire used for each coil usually has different cross-sectional areas and dimensions in order to obtain desired superconducting characteristics such as a critical current value. Generally, the inner layer coil is exposed to a higher magnetic field than the outer layer coil. Since the critical current density of the superconducting wire decreases as the magnetic field increases, the cross-sectional area of the inner layer superconducting layer is larger than that of the outer coil superconducting wire.

超電導マグネットコイルは上記の内層コイルと外層コイ
ルを直列に接続してマグネットとするものであるが、従
来接続線を別に製作して接続していた。この接続線は、
内層コイル等の同等の高磁界に曝されるため、その断面
積は内層コイル用超電導線と同じで、その巾は外層コイ
ルの半径方向の厚さからはみ出さないよう外層コイル用
超電導線の巾に合わされたものである。すなわち第4図
(b)に示すように外層コイル(1)および(1′)と
内層コイル(2)および(2′)を接続線(3)
(3′)を用いて(4)(4′)および(5)(5′)
においてハンダ付けなどによりろう接して接続してい
た。しかしながらこのような接続方法においては第4図
(c)に示すように断面がキーストン状をなしている内
層コイル(2′)の超電導線(6)に巾(c)に対し接
続線(3)の巾(c′)が小さいため、両者の接触面積
を大きくとることが出来ず、接続抵抗が大きくなり電力
ロスをまねいたり、また接続強度が弱く巾寸法の違いに
よる隙間の部分が電磁力による線材の動きを許容するこ
とになり、超電導コイルとしての特性の安定性を損ねる
などの問題があった。
In the superconducting magnet coil, the above-mentioned inner layer coil and outer layer coil are connected in series to form a magnet, but conventionally, a connecting wire was separately manufactured and connected. This connecting line
Since it is exposed to the same high magnetic field as the inner layer coil, its cross-sectional area is the same as that of the inner layer coil superconducting wire, and its width is the width of the outer layer coil superconducting wire so that it does not protrude from the radial thickness of the outer layer coil. It has been adapted to. That is, as shown in FIG. 4 (b), the outer layer coils (1) and (1 ') are connected to the inner layer coils (2) and (2') by connecting wires (3).
Using (3 '), (4) (4') and (5) (5 ')
At that time, they were connected by brazing, such as by soldering. However, in such a connecting method, as shown in FIG. 4 (c), the superconducting wire (6) of the inner layer coil (2 ') having a keystone cross section is connected to the connecting wire (3) with respect to the width (c). Since the width (c ') is small, the contact area between them cannot be made large, resulting in a large connection resistance, leading to power loss, and weak connection strength and gaps due to differences in width due to electromagnetic force. Since the movement of the wire is allowed, there is a problem that the stability of the characteristics of the superconducting coil is impaired.

(問題点を解決するための手段) 本発明は上記の問題を解決するためになされたもので、
断面寸法の異なう超電導線を巻線した内層コイルと外層
コイルを重ね合せて配置し、直列に接続する鞍形超電導
マグネットコイルの接続方法において、接続線の断面積
を内層コイルの超電導線と等しくし、かつ接続線の巾を
内層コイルおよび外層コイルの超電導線と等しくした接
続線により接続することを特徴とする鞍形超電導マグネ
ットコイルの接続方法である。
(Means for Solving Problems) The present invention has been made to solve the above problems,
In the method of connecting a saddle type superconducting magnet coil in which the inner layer coil and the outer layer coil wound with superconducting wires with different cross-sectional dimensions are stacked and connected in series, the cross-sectional area of the connecting wire is equal to that of the inner layer coil. In addition, the method for connecting a saddle-shaped superconducting magnet coil is characterized in that the connecting wires are connected by making the width of the connecting wires equal to the superconducting wires of the inner layer coil and the outer layer coil.

すなわち本発明はNb3Sn、V3Gaなどの化合物超電導線ま
たはNbTiなどの合金超電導線の断面がキーストン状の超
電導線を用い、これをレーストラック状に巻回してコイ
ルとし、プレスなどにより鞍形に成形した、いわゆる鞍
形超電導マグネットコイルで、内層コイルと外層コイル
に重ね合せ、外層コイルの超電導線と内層コイルの超電
導線とを接続する際に、接続線の断面積を、高磁界側に
配置されるため断面積が大きい内層コイル用超電導線の
断面積と等しくし、かつ接続線の巾を内層コイルおよび
外層コイルの超電導線と等しくなるように接続線の寸法
を変えた接続線により接続するものである。
That is, the present invention uses Nb 3 Sn, compound superconducting wire such as V 3 Ga or alloy superconducting wire such as NbTi having a keystone cross-section, which is wound into a racetrack to form a coil, which is then saddle-bonded by pressing or the like. In the so-called saddle-shaped superconducting magnet coil formed into a shape, when overlapping the inner layer coil and the outer layer coil and connecting the superconducting wire of the outer layer coil and the superconducting wire of the inner layer coil, the cross-sectional area of the connecting wire is set to the high magnetic field side. The connecting wire has the same cross-sectional area as that of the superconducting wire for the inner layer coil, and the width of the connecting wire is changed so that the width of the connecting wire is equal to the superconducting wire of the inner layer coil and the outer layer coil. To connect.

上記の接続線の断面積を内層コイルの超電導線の断面積
と等しくする理由は、内層コイルとの接続部分も内層コ
イルと同等の高磁界に曝されるため、接続線も内層コイ
ル用超電導と同等の臨界電流特性を持つ必要があるから
である。従ってここで等しくとは、同等以上という意味
であり若干大きくても差支えない。また接続線の巾を内
層コイルおよび外層コイルの超電導線の巾と等しくなる
のは、内層および外層と両方の超電導線の巾に合わせな
いと接続抵抗の減少に寄与しないからである。
The reason why the cross-sectional area of the connection wire is equal to the cross-sectional area of the superconducting wire of the inner layer coil is that the connection part with the inner layer coil is also exposed to the same high magnetic field as the inner layer coil. This is because it is necessary to have equivalent critical current characteristics. Therefore, "equal" means "equal to or greater than" and may be slightly larger. Further, the width of the connecting wire is made equal to the width of the superconducting wires of the inner layer coil and the outer layer coil, because the width of the superconducting wire of both the inner layer and the outer layer does not contribute to the reduction of the connection resistance.

しかして上記の接続線は超電導線と同じ材料を用いて別
途スエージングにより製作してもよく、また断面積の大
きい内層コイルの超電導線を予め外層コイルの超電導線
の巾に合せて接続部となる部分をスエージングなどによ
り加工したもので接続してもよい。
However, the above-mentioned connecting wire may be separately manufactured by swaging using the same material as the superconducting wire, and the superconducting wire of the inner layer coil having a large cross-sectional area is previously connected to the connecting portion in accordance with the width of the superconducting wire of the outer layer coil. The parts may be connected by being processed by swaging or the like.

(実施例) 以下に本発明の一実施例について説明する。(Example) An example of the present invention will be described below.

第1図(a),(b)に示すようにNb3Snからなる超電
導線の線材寸法A×B×Cが1.9mm×1.6mm×10mmの超電
導線(6)を内層コイル用とし、また線材寸法A′×
B′×C′が2.1mm×1.9mm×6mmの超電導線(7)を外
層コイル用とした。上記の内層コイル用超電導線を第2
図に示すように内半径66mm、外半径が76mmの鞍形コイル
に成形して内層コイル(2)(2′)とした。また外層
コイル用超電導線を内半径77mm、外半径が83mmの鞍形コ
イルに成形して外層コイル(1)(1′)とした。そし
て上記の内層コイルの端部と外層コイルの端部を接続部
(4)(4′)および(5)(5′)において接続線
(3)(3′)とハンダ付けにより接続した。上記の接
続線(3)は第3図(a)および(b)に示すように線
の断面積は一定であるが一端が厚さDが1.76mm、巾Cが
10mmの寸法となっており別の一端は厚さD′が2.94mm、
巾C′が6mmの一本の線で寸法が異なる線材をスエージ
ングにより加工し、(c)に示すように曲げ成形したも
のである。この接続線は線の巾Cが第1図(b)に示す
ように内層コイルの超電導線(6)の巾Cと等しくなっ
ており、また一方の線の巾C′は第1図(a)のように
外層コイルの超電導線(7)の巾(c′)と等しくなっ
ている。
As shown in FIGS. 1 (a) and 1 (b), the superconducting wire made of Nb 3 Sn has a wire material dimension A × B × C of 1.9 mm × 1.6 mm × 10 mm for the inner layer coil, and Wire size A '×
A superconducting wire (7) having B ′ × C ′ of 2.1 mm × 1.9 mm × 6 mm was used for the outer layer coil. The second superconducting wire for the inner layer coil
As shown in the figure, a saddle-shaped coil having an inner radius of 66 mm and an outer radius of 76 mm was formed into inner layer coils (2) and (2 '). Further, the superconducting wire for the outer layer coil was formed into a saddle type coil having an inner radius of 77 mm and an outer radius of 83 mm to obtain outer layer coils (1) and (1 '). Then, the ends of the inner layer coil and the ends of the outer layer coil were connected to the connecting wires (3) and (3 ') at the connecting portions (4), (4') and (5) (5 ') by soldering. As shown in FIGS. 3 (a) and 3 (b), the connecting wire (3) has a constant cross-sectional area, but one end has a thickness D of 1.76 mm and a width C of
It has a size of 10 mm and the other end has a thickness D'of 2.94 mm,
A wire having a width C'of 6 mm and having different dimensions is processed by swaging and bent as shown in (c). The width C of this connecting wire is equal to the width C of the superconducting wire (6) of the inner coil as shown in FIG. 1 (b), and the width C'of one wire is shown in FIG. 1 (a). ) Is equal to the width (c ') of the superconducting wire (7) of the outer layer coil.

このように1本の接続線で断面積が内層コイルの断面積
と等しく接続部となる両端の寸法の異なる線材を接続線
に使用することにより、内層コイルと外層コイルとで寸
法の異なった超電導線を、接続部での寸法をそれぞれ完
全に一致させて接続できるのである。
In this way, by using a wire rod whose cross-sectional area is equal to the cross-sectional area of the inner layer coil in one connecting wire and has different dimensions at both ends to be the connecting portion, the superconducting wire having different dimensions in the inner layer coil and the outer layer coil The wires can be connected with the dimensions of the connecting portions perfectly matched.

上記の第2図に示す本発明の接続方法によれば従来の線
厚が2.94mm、線巾6mmの断面寸法が一定の接続線を使用
した場合と比較すると内層コイル接続部において接続抵
抗が約3/5に減少し、発熱量を約0.1w低減することが出
来る。なおシンクロトロン加速器の軌道上にはこの種の
超電導マグネットが数百台設置され電力量は数百wとい
われることからかなりの電力量の低減効果がある。
According to the connection method of the present invention shown in FIG. 2 described above, the connection resistance at the inner layer coil connection portion is about as compared with the conventional connection wire having a constant cross-sectional dimension of 2.94 mm and a line width of 6 mm. It can be reduced to 3/5 and the calorific value can be reduced by about 0.1w. Since hundreds of superconducting magnets of this kind are installed on the orbit of the synchrotron accelerator, and the amount of electric power is said to be several hundreds w, there is a considerable reduction in the amount of electric power.

(効果) 以上に説明したように本発明は接続線の断面積を内層コ
イルの超電導線と等しくし、またその巾を内層および外
層コイルの超電導線の巾と等しくしているので、接続強
度が高くなって電磁力による線材の動きがなくなり、そ
の結果接続抵抗が減少し電力ロスが低減するなど多くの
効果を奏するものである。
(Effect) As described above, according to the present invention, the cross-sectional area of the connecting wire is made equal to that of the superconducting wire of the inner layer coil, and the width thereof is made equal to the width of the superconducting wire of the inner layer coil and the outer layer coil. As a result, the movement of the wire rod due to the electromagnetic force is eliminated, and as a result, the connection resistance is reduced and the power loss is reduced.

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

第1図は本発明の接続線と超電導線の接続部の断面図、
第2図は本発明の内層コイルと外層コイルの接続状態を
示す断面図、第3図は本発明の接続線の説明図であり
(a)は正面図、(b)は平面図、(c)は斜視図、第
4図な従来の接続方法を示す図であり、(a)は鞍形超
電導マグネットコイルの斜視図、(b)は鞍形超電導マ
グネットの断面図、(c)は超電導線と接続線の断面図
である。 1、1′……外層コイル、2、2′……内層コイル、
3、3′……接続線、4、4′……接続部、5、5′…
…接続部、6、6′……内層コイル超電導線、7、7′
……外層コイル超電導線
FIG. 1 is a cross-sectional view of a connecting portion of a connecting wire and a superconducting wire according to the present invention,
FIG. 2 is a cross-sectional view showing the connection state of the inner layer coil and the outer layer coil of the present invention, FIG. 3 is an explanatory view of the connection line of the present invention, (a) is a front view, (b) is a plan view, (c) 4A is a perspective view, and FIG. 4 is a view showing a conventional connection method. FIG. 4A is a perspective view of a saddle type superconducting magnet coil, FIG. 4B is a sectional view of a saddle type superconducting magnet, and FIG. It is sectional drawing of and a connection line. 1, 1 '... outer layer coil, 2 2' ... inner layer coil,
3, 3 '... Connection line 4, 4' ... Connection part 5, 5 '...
... Connecting part, 6, 6 '... Inner layer coil superconducting wire, 7, 7'
...... Outer layer coil superconducting wire

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】断面寸法の異なる超電導線を巻線した内層
コイルと外層コイルを重ね合せて配置し、直列に接続す
る鞍形超電導マグネットコイルの接続方法において、接
続線の断面積を内層コイルの超電導線と等しくし、かつ
接続線の巾を内層コイルおよび外層コイルの超電導線と
等しくした接続線により接続することを特徴とする鞍形
超電導マグネットコイルの接続方法。
1. A method for connecting a saddle type superconducting magnet coil, in which an inner layer coil and an outer layer coil wound with superconducting wires having different cross-sectional dimensions are superposed on each other and connected in series. A connecting method for a saddle type superconducting magnet coil, which is characterized in that the connecting wires are made equal to the superconducting wires and the widths of the connecting wires are made equal to the superconducting wires of the inner layer coil and the outer layer coil.
JP16947286A 1986-07-18 1986-07-18 How to connect saddle type superconducting magnet coil Expired - Lifetime JPH0779048B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16947286A JPH0779048B2 (en) 1986-07-18 1986-07-18 How to connect saddle type superconducting magnet coil

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16947286A JPH0779048B2 (en) 1986-07-18 1986-07-18 How to connect saddle type superconducting magnet coil

Publications (2)

Publication Number Publication Date
JPS6325905A JPS6325905A (en) 1988-02-03
JPH0779048B2 true JPH0779048B2 (en) 1995-08-23

Family

ID=15887187

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16947286A Expired - Lifetime JPH0779048B2 (en) 1986-07-18 1986-07-18 How to connect saddle type superconducting magnet coil

Country Status (1)

Country Link
JP (1) JPH0779048B2 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5879749B2 (en) * 2011-05-30 2016-03-08 住友電気工業株式会社 Superconducting coil, superconducting magnet, and manufacturing method of superconducting coil
JP2014165304A (en) * 2013-02-25 2014-09-08 Sumitomo Electric Ind Ltd Superconducting apparatus
WO2014162379A1 (en) * 2013-04-01 2014-10-09 株式会社 日立製作所 Superconducting wire and manufacturing method for same, as well as superconducting coil

Also Published As

Publication number Publication date
JPS6325905A (en) 1988-02-03

Similar Documents

Publication Publication Date Title
US5398398A (en) Method of producing a superconducting joint with niobium-tin
US4392072A (en) Dynamoelectric machine stator having articulated amorphous metal components
US4310821A (en) Spiralled printed inductance
US4704592A (en) Chip inductor electronic component
JPH0855738A (en) Transformer
JPH0779048B2 (en) How to connect saddle type superconducting magnet coil
US4218668A (en) Superconductive magnet device
JPS639903A (en) Pancake magnet
JPH0330299A (en) Manufacture of coil for charged particle deflecting electromanet
JPH0676649A (en) Composite superconductor
JP2940066B2 (en) Lead wire opening structure of sheet winding transformer
JPH02127013U (en)
JPH0464444B2 (en)
JPH0124908Y2 (en)
JPH1041163A (en) Chip type inductor
JP2602414Y2 (en) Air core reactor
EP0370666A1 (en) Electromagnetic actuator
DE102025111736A1 (en) COIL DEVICE
JPS61190906A (en) electromagnet coil
JP2777166B2 (en) electromagnet
JPH0311877Y2 (en)
DE2318507C3 (en) Superconducting magnet coil with a two-pole or multi-pole winding
JPH0224004B2 (en)
JPS5854735B2 (en) Manufacturing method for levitation ground coil for magnetic levitation trains
JPS63193514A (en) High-frequency coil