JPS61190906A - Coil for electromagnet - Google Patents
Coil for electromagnetInfo
- Publication number
- JPS61190906A JPS61190906A JP3042585A JP3042585A JPS61190906A JP S61190906 A JPS61190906 A JP S61190906A JP 3042585 A JP3042585 A JP 3042585A JP 3042585 A JP3042585 A JP 3042585A JP S61190906 A JPS61190906 A JP S61190906A
- Authority
- JP
- Japan
- Prior art keywords
- conductor
- coil
- metallic
- connection
- metallic adhesive
- 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.)
- Pending
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F5/00—Coils
Abstract
Description
【発明の詳細な説明】
〔発明の利用分野〕
本発明は、ストランド線から成る導体から構成される電
磁石のコイルの接続部に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to a connection part of a coil of an electromagnet made of a conductor made of a strand wire.
近年、加速器の多様化に伴い、非常に速いパルス運転を
行なう電磁石が要求されてきた。通常の加速器用電磁石
では、パルス運転でも数Hz程度の周波数のものが多く
、中実導体が使用されるが、商用周波数程度のものにな
ると、その渦電流損失が無視でき表い。通常、コイルの
損失は、主に、抵抗損失と、渦電流損失から成るが電流
が決まれば、コイルを構成する素線の断面積に対して、
抵抗損失は反比例し、渦電流損失は断面積の二乗に比例
する。両者の合計値を最小化する最適化を行なうと、は
ぼ、同一オーダーとなってしまう。抵抗損失は、ともか
く、渦電流損失は、素線をストランドにすれば十分小さ
くすることができる。従って、速い/<ルス運転を行な
う電磁石のコイルには、ストランド導体を使う必要が出
てくる。代表的は導体の断面例と第1図に示す。In recent years, with the diversification of accelerators, electromagnets capable of extremely fast pulse operation have been required. Normal accelerator electromagnets often have a frequency of several Hz even in pulse operation, and solid conductors are used, but when the frequency is about the commercial frequency, the eddy current loss is negligible. Normally, coil loss mainly consists of resistance loss and eddy current loss, but once the current is determined,
Resistive losses are inversely proportional, and eddy current losses are proportional to the square of the cross-sectional area. If optimization is performed to minimize the total value of both, they will end up being of the same order. Regardless of resistance loss, eddy current loss can be sufficiently reduced by using strands of wire. Therefore, it becomes necessary to use a strand conductor in the coil of an electromagnet that performs fast/<lusus operation. A typical cross-sectional example of a conductor is shown in FIG.
一方、導体の製造長には限界があることから、コイルに
は通常コイル内接続部、或いは外部系(電流導入端子)
との接続部が必要となる。しかしこのような導体では、
そのストランド構造に起因して、十分な接続をすること
ができなかった。On the other hand, since there is a limit to the manufacturing length of the conductor, the coil usually has a connection part inside the coil or an external system (current introduction terminal).
A connection part is required. However, with such a conductor,
Due to its strand structure, sufficient connections could not be made.
すなわち、通常の中実導体では、導体面同士を、適当な
金属性接着物で、或いは、接合片を使って金属性接着物
で接続するが、このようなストランド導体の場合には、
冷却管と導体部とが異なる独立した材料で構成されてい
るため、この通常の接続法をとることができない。In other words, in the case of a normal solid conductor, the conductor surfaces are connected to each other with a suitable metallic adhesive or with a metallic adhesive using a joint piece, but in the case of such a strand conductor,
This normal connection method is not possible because the cooling pipe and the conductor are made of different and independent materials.
従って、コイル内に接続部を形成することは、構造上難
しいこととなる。この場合、その導体の製造可能限界に
、コイルの大きさが依存することになシ、長尺コイルが
製作できなくなるという問題があった。Therefore, forming connections within the coil is structurally difficult. In this case, there is a problem that the size of the coil depends on the manufacturing limit of the conductor, making it impossible to manufacture a long coil.
また、外部との接続部では、導体の片端を金属性接着物
で一体化して、この後、電流導入端子を金属性接着物で
接続する方法が従来、考えられてきたが、この場合、十
分な接続量を確保することができず、接続部の電流容量
に問題が生じる可能性がある。従来法を第2図に示す。In addition, in the connection part with the outside, conventional methods have been considered to integrate one end of the conductor with a metal adhesive and then connect the current introduction terminal with a metal adhesive, but in this case, it is not enough. Therefore, a problem may occur in the current capacity of the connection part. The conventional method is shown in Figure 2.
本発明の目的はストランド導体にスリーブ等の金属性介
在物と配置させ、これらを金属性接着物で一′体化し、
その後、他の導体、若しくは、電流導入端子と、金属性
接着物で接続することで、良好な接続抵抗をもち、電気
的に安全な接続構造のコイルを提供することにある。The object of the present invention is to arrange a strand conductor with a metallic inclusion such as a sleeve, integrate these with a metallic adhesive,
Thereafter, the coil is connected to another conductor or a current introduction terminal using a metallic adhesive, thereby providing a coil having good connection resistance and an electrically safe connection structure.
〔発明の実施例〕 以下、本発明の実施例を図面によって説明する。[Embodiments of the invention] Embodiments of the present invention will be described below with reference to the drawings.
第3図は、コイル内での導体間の接続を示した図で、ス
トランド線1で構成される導体2は、端部で金属性接着
物4で一体化され、その後、スリーブ等の金属性介在物
6とし、金属性接着物4で全体が一体化接続される。こ
のような構造としたのちに、導体同士をあわせ、金属性
接着物7で導体間を十分な接触面積をもって接続するこ
とで、良好な接続抵抗と構造と得ることができる。FIG. 3 is a diagram showing the connection between conductors in the coil, in which the conductor 2 composed of the strand wire 1 is integrated with a metallic adhesive 4 at the end, and then a metallic adhesive such as a sleeve is attached. The entire body is integrally connected with an inclusion 6 and a metallic adhesive 4. After forming such a structure, by aligning the conductors and connecting them with a sufficient contact area with the metallic adhesive 7, a good connection resistance and structure can be obtained.
第4図は、導体と、外部系(電流導入端子)との接続を
示した図である。導体は、第3図(a)に示したような
構造とし、電気導入端子5とを十分な接続量をもって接
続する。FIG. 4 is a diagram showing the connection between the conductor and the external system (current introduction terminal). The conductor has a structure as shown in FIG. 3(a), and is connected to the electricity introduction terminal 5 with a sufficient amount of connection.
第5図は、他の実施例を示したもので、金属性介在物6
をいくつかの構成部品から成るものとしたものである。FIG. 5 shows another embodiment, in which metallic inclusions 6
It consists of several component parts.
この方法は、導体2と、金属性介在物6との間の電気的
な接続面積を更に増やした一つの改良案である。図中3
は冷却管である。This method is an improved method that further increases the electrical connection area between the conductor 2 and the metallic inclusion 6. 3 in the diagram
is a cooling pipe.
本発明よれば
(1) コイル内での接続が、良好な特性をもつ、て
可能となるため、導体の製造可能長にかかわらず、長尺
コイルの製造が可能となる。According to the present invention, (1) connections within the coil can be made with good characteristics, so long coils can be manufactured regardless of the manufacturable length of the conductor.
(2)十分な接触面積をもち、良好な接続抵抗のコイル
の製造を可能とする。(2) It is possible to manufacture a coil with sufficient contact area and good connection resistance.
第1図は本発明の接続を行なう為に施した導体の加工法
および接続方法を示す図、第2図、第3図は、導体と電
流導入端子との接続方法を示す図、第4図は、代表的な
ストランド導体の一例を示す図、第5図は導体と電流導
入端子との従来の接続方法を示す因である。
1・・・ストランド線、2・・・導体、3・・・冷却管
、4・・・金属性接着物(導体間)、5・・・電流導入
端子、6第1 図
第2Z
(0L)
(bン
第4−2FIG. 1 is a diagram showing a method of processing and connecting a conductor to make the connection of the present invention, FIGS. 2 and 3 are diagrams showing a method of connecting a conductor and a current introduction terminal, and FIG. 1 is a diagram showing an example of a typical strand conductor, and FIG. 5 is a diagram showing a conventional connection method between a conductor and a current introduction terminal. DESCRIPTION OF SYMBOLS 1... Strand wire, 2... Conductor, 3... Cooling pipe, 4... Metallic adhesive (between conductors), 5... Current introduction terminal, 6 Figure 1, Figure 2Z (0L) (B No. 4-2
Claims (1)
る電磁石のコイルに於いて、 前記ストランド線を金属性介在物を用いて一体化した後
に接続することを特徴とする電磁石のコイル。1. 1. An electromagnetic coil constructed by winding a conductor made of strand wires, wherein the strand wires are connected after being integrated using a metallic inclusion.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3042585A JPS61190906A (en) | 1985-02-20 | 1985-02-20 | Coil for electromagnet |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3042585A JPS61190906A (en) | 1985-02-20 | 1985-02-20 | Coil for electromagnet |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61190906A true JPS61190906A (en) | 1986-08-25 |
Family
ID=12303594
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP3042585A Pending JPS61190906A (en) | 1985-02-20 | 1985-02-20 | Coil for electromagnet |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61190906A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH02205003A (en) * | 1989-02-03 | 1990-08-14 | Toshiba Corp | Electromagnet |
JP2007317670A (en) * | 2007-06-18 | 2007-12-06 | Toshiba Corp | Ac electromagnet |
-
1985
- 1985-02-20 JP JP3042585A patent/JPS61190906A/en active Pending
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH02205003A (en) * | 1989-02-03 | 1990-08-14 | Toshiba Corp | Electromagnet |
JP2007317670A (en) * | 2007-06-18 | 2007-12-06 | Toshiba Corp | Ac electromagnet |
JP4550866B2 (en) * | 2007-06-18 | 2010-09-22 | 株式会社東芝 | AC electromagnet |
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