JPH0315324B2 - - Google Patents

Info

Publication number
JPH0315324B2
JPH0315324B2 JP3900684A JP3900684A JPH0315324B2 JP H0315324 B2 JPH0315324 B2 JP H0315324B2 JP 3900684 A JP3900684 A JP 3900684A JP 3900684 A JP3900684 A JP 3900684A JP H0315324 B2 JPH0315324 B2 JP H0315324B2
Authority
JP
Japan
Prior art keywords
conductor
cross
rectangular
diameter side
height
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
Application number
JP3900684A
Other languages
Japanese (ja)
Other versions
JPS60182704A (en
Inventor
Noboru Kimura
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP3900684A priority Critical patent/JPS60182704A/en
Publication of JPS60182704A publication Critical patent/JPS60182704A/en
Publication of JPH0315324B2 publication Critical patent/JPH0315324B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F5/00Coils

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明は電磁石用コイルに関するものである。[Detailed description of the invention] [Field of application of the invention] The present invention relates to an electromagnetic coil.

〔発明の背景〕[Background of the invention]

近年電子加速器の規模増大に伴い電子集束、偏
向用電磁石用コイルへの通電電流が大きくなり、
コイル導体の断面積も大きくなつているが、電磁
石用コイル間には各種観測用ポート等が設置され
るので、コイルの長手方向寸法が制限される。こ
のためコイル端部は導体すなわち平角導体を、こ
の導体の断面積に比べて小さな曲げ半径で巻回し
なければならないが、この巻回時に導体断面が台
形に変形し、曲げ半径内側は導体厚み(高さ)が
増大する。
In recent years, as the scale of electron accelerators has increased, the current flowing through the electromagnetic coils for electron focusing and deflection has increased.
Although the cross-sectional area of the coil conductor is also increasing, the longitudinal dimension of the coil is limited because various observation ports and the like are installed between the electromagnetic coils. Therefore, at the end of the coil, a conductor, that is, a rectangular conductor, must be wound with a bending radius that is smaller than the cross-sectional area of the conductor, but during this winding, the cross-section of the conductor deforms into a trapezoid, and the inner side of the bending radius is the thickness of the conductor ( height) increases.

すなわち電磁石用コイルは第1図に示されてい
るように平角導体1が連続して巻き回し、すなわ
ち巻回され、積層されるが、この巻回時に通常4
隅に曲げ加工部を持つて形成される。ところで平
角導体1は通常第2図にも示されているような断
面、すなわち幅方向に一様な高さを有するものが
使用されるが、これを曲げ加工すると平角導体1
は第3図に示されているように導体幅のほぼ中心
Sを中立軸として曲げ加工内径側1aは圧縮応力
を受けて高さが大きくなり曲げ加工外径側1bは
引張応力を受けて高さが小さくなつて、全体とし
て曲げ加工内径側1aの高さが最も大きく、曲げ
加工外径側1bになるにつれて高さが小さくなる
台形を示すようになる。
That is, in the electromagnet coil, as shown in FIG.
It is formed with a bent part at the corner. By the way, the rectangular conductor 1 is normally used with a cross section as shown in Fig. 2, that is, one having a uniform height in the width direction.
As shown in Fig. 3, the bending inner diameter side 1a increases in height due to compressive stress, and the bending outer diameter side 1b increases in height due to tensile stress, with the neutral axis approximately at the center S of the conductor width. becomes smaller, and as a whole, the height on the bending inner diameter side 1a is the largest, and the height becomes smaller toward the bending outer diameter side 1b, forming a trapezoid.

例えば20mm角程度の断面を持つ平角導体を曲げ
半径約50mmで90゜曲げると高さ方向変形量は片側
で約0.5mmとなり、これを上述の第1図のように
巻回・積層するとコイル4隅部すなわち曲げ加工
部のみコイル高さが高くなるのみならず、巻回・
積層した平角導体間の絶縁である層間絶縁にこの
高くなつた平角導体が局部的に当り層間短絡を起
こすようになる。
For example, if a rectangular conductor with a cross section of about 20 mm square is bent 90 degrees with a bending radius of about 50 mm, the heightwise deformation will be about 0.5 mm on one side.If this is wound and laminated as shown in Figure 1 above, the coil 4 Not only does the height of the coil become higher only at the corners, that is, the bending part, but also the winding and
This raised rectangular conductor locally hits the interlayer insulation that is the insulation between the laminated rectangular conductors, causing an interlayer short circuit.

これを防ぐにはこの曲げ加工部導体高さを曲げ
加工前に機械加工により削り取る必要があり、従
来は巻回・積層作業中に機械加工によつて削り取
つていたので、機械加工および機械加工によつて
生じた切粉の処理等で連続した巻回作業ができ
ず、加工工数が増加し、量産化が著しく阻害され
ていた。
To prevent this, it is necessary to reduce the height of the conductor at the bending part by machining before bending. Continuous winding work was not possible due to the processing of chips generated during processing, which increased the number of processing steps and significantly hindered mass production.

このように機械加工などしないで曲げ加工部の
みコイル高さが高くなるのを防ぐには、回転電機
の電機子コイルのコイル頭部等で実施しているよ
うに、曲げ作業により生じた平角導体の台形断面
部を加圧して直線部の厚さすなわち高さとほぼ同
じにする方法があるが、電磁石用コイル等の連続
して巻回する導体に適用することは実用的でな
い。
In order to prevent the height of the coil from increasing only in the bent part without machining, as is done in the coil head of the armature coil of rotating electric machines, the rectangular conductor created by the bending work can be There is a method of pressurizing the trapezoidal cross-section of the trapezoid so that the thickness, that is, the height, is almost the same as that of the straight section, but it is not practical to apply it to a conductor that is continuously wound, such as an electromagnetic coil.

これとは別に第4図に示されているようにその
断面が台形状の平角導体2を使用してリング状に
巻回・積層することが回転電機の回転子端路環に
実施されている。すなわち曲げ加工内径側2aの
高さを小さく曲げ加工外径側2bの高さを大きく
してその断面を台形状とした平角導体2を使用し
て巻回・積層するのであるが、リング状で曲げ半
径の大きな回転子端絡環の場合には有効である
が、電磁石コイル等のように曲げ半径が小さい場
合には曲げ加工が施されない直線部は、第5図に
示されているようにその積層部の平角導体2の断
面形状が台形のままで、かつその高さが曲げ加工
部の高さより大きくなるため導体2間の絶縁層に
曲げ加工外径側2b、すなわち台形角部がくい込
み、層間短絡をおこしてしまう。
Separately, as shown in Fig. 4, rectangular conductors 2 having a trapezoidal cross section are wound and laminated in a ring shape for the rotor terminal ring of a rotating electric machine. . In other words, the rectangular conductor 2 with a trapezoidal cross section is used to wind and laminate the rectangular conductor 2 with a lower height on the bent inner diameter side 2a and a larger height on the bent outer diameter side 2b. This is effective in the case of a rotor terminal ring with a large bending radius, but when the bending radius is small, such as in an electromagnetic coil, the straight part that is not bent is as shown in Figure 5. The cross-sectional shape of the rectangular conductor 2 in the laminated portion remains trapezoidal, and its height is greater than the height of the bent portion, so the bent outer diameter side 2b, that is, the corner of the trapezoid, bites into the insulating layer between the conductors 2. , causing an interlayer short circuit.

〔発明の目的〕[Purpose of the invention]

本発明は以上の点に鑑みなされたものであり、
製作工数の低減を可能とした電磁石用コイルを提
供することを目的とするものである。
The present invention has been made in view of the above points,
The object of the present invention is to provide an electromagnetic coil that can reduce manufacturing man-hours.

〔発明の概要〕[Summary of the invention]

すなわち本発明は平角導体が巻回され、積層さ
れる電磁石用コイルにおいて、前記巻回される平
角導体が、その断面が導体幅のほぼ中心から巻回
時の曲げ加工内径側が先細となるように形成され
たものであることを特徴とするものであり、これ
によつて巻回される平角導体は、その断面が導体
幅のほぼ中心から曲げ加工内径側が先細に形成さ
れるようになる。
That is, the present invention provides an electromagnetic coil in which rectangular conductors are wound and stacked such that the cross section of the rectangular conductor to be wound is tapered from approximately the center of the width of the conductor to the inner diameter side of the bending process during winding. As a result, the rectangular conductor wound thereon has a cross section tapered from approximately the center of the width of the conductor on the inner diameter side of the bending process.

〔発明の実施例〕[Embodiments of the invention]

以下、図示した実施例に基づいて本発明を説明
する。第6図から第8図には本発明の一実施例が
示されている。なお従来と同じ部品には同じ符号
を付したので説明を省略する。本実施例では巻回
する平角導体3を、その断面を導体幅のほぼ中心
Sから巻回時の曲げ加工内径側3aが先細となる
ように形成した。このようにすることにより巻回
される平角導体3はその断面が導体幅のほぼ中心
Sの中立軸から曲げ加工内径側3aが先細に形成
されるようになつて、製作工数の低減を可能とし
た電磁石用コイルを得ることができる。
The present invention will be explained below based on the illustrated embodiments. An embodiment of the present invention is shown in FIGS. 6-8. Note that parts that are the same as those in the conventional system are given the same reference numerals, and therefore their explanations will be omitted. In this embodiment, the rectangular conductor 3 to be wound is formed so that its cross section is tapered from approximately the center S of the conductor width to the inner diameter side 3a of the conductor when it is wound. By doing so, the rectangular conductor 3 to be wound has a cross section tapered from the neutral axis at approximately the center S of the conductor width on the bending inner diameter side 3a, which makes it possible to reduce the number of manufacturing steps. A coil for an electromagnet can be obtained.

すなわち巻回する平角導体3を、その断面が導
体幅のほぼ中心から曲げ加工内径側のみ曲げ変形
量に見合つた寸法だけ導体高さを小さく、先細に
形成した(第6図参照)。このように形成した平
角導体3を巻回することにより曲げ加工部では第
7図に示されているように、曲げ加工内径側3a
は圧縮応力を受けてその高さが大きく、曲げ加工
外径側3bは引張応力を受けてその高さが小さく
なるが、導体幅のほぼ中心Sから曲げ加工内径側
3aを先細にしたので、圧縮応力を受けてその高
さが大きくなつても導体幅のほぼ中心Sの中立軸
から曲げ加工内径側3aまではその高さが同じよ
うになる。従つて導体幅のほぼ半分がほぼ同じ高
さの平面部を有する平角導体が積層されるように
なつて、局部的な導体3間の当りがなく積層が安
定で、かつ層間短絡の発生が防止できる。そして
曲げ加工部以外の直線部でも第8図に示されてい
るように上述の第6図記載の平角導体3が巻回さ
れるので、その導体幅の半分すなわち曲げ加工外
径側3bの高さが同じな平面部で積層されるよう
になつて、曲げ加工部と同様に積層が安定してお
り、かつ層間短絡をおこす懸念がない。このよう
にその断面を導体幅のほぼ中心から曲げ加工内径
側3aが先細となるように形成した平角導体3で
巻回・積層すれば、巻回・積層作業中に機械加工
をしないでも連続して巻回作業ができるようにな
つて、製作工数が短縮でき、量産化が可能であ
る。
That is, the rectangular conductor 3 to be wound is formed so that its cross section is tapered so that the height of the conductor is reduced by a dimension commensurate with the amount of bending deformation only on the inner diameter side of the bending process from approximately the center of the conductor width (see FIG. 6). By winding the rectangular conductor 3 formed in this way, the bending part is formed on the inner diameter side 3a as shown in FIG.
receives compressive stress and its height becomes large, and the bent outer diameter side 3b receives tensile stress and its height decreases, but since the bent inner diameter side 3a is tapered from approximately the center S of the conductor width, Even if the height increases due to compressive stress, the height remains the same from the neutral axis approximately at the center S of the conductor width to the bending inner diameter side 3a. Therefore, rectangular conductors each having a flat surface with approximately half the conductor width at approximately the same height are stacked, and there is no local contact between the conductors 3, making the stacking stable and preventing the occurrence of interlayer short circuits. can. As shown in FIG. 8, the flat conductor 3 shown in FIG. Since the layers are stacked on the same plane, the stack is stable like the bent portion, and there is no risk of short circuit between the layers. If the rectangular conductor 3 is bent so that its cross section is tapered from the center of the width of the conductor so that the inner diameter side 3a is tapered, the conductor will be continuous even without machining during the winding and laminating work. The winding work can now be done by hand, reducing manufacturing man-hours and making mass production possible.

なお本実施例では平角導体3が中実導体の場合
について説明したが、これのみに限るものではな
く冷却媒体を通す孔を有する中空導体についても
同様に実施することができる。
Although this embodiment has been described with reference to the case where the rectangular conductor 3 is a solid conductor, the present invention is not limited to this, and a hollow conductor having holes through which a cooling medium passes can be similarly implemented.

なおまた平角導体3はその断面が横方向矩形断
面のものを使用したが、正四角断面、縦方向矩形
断面のものでも使用できる。
Although the rectangular conductor 3 has a rectangular cross section in the horizontal direction, it may also have a square cross section or a rectangular cross section in the vertical direction.

〔発明の効果〕〔Effect of the invention〕

上述のように本発明は平角導体を機械加工をせ
ずに連続して巻回できるようになつて、製作工数
の低減を可能とした電磁石用コイルを得ることが
できる。
As described above, according to the present invention, a rectangular conductor can be continuously wound without machining, thereby making it possible to obtain an electromagnetic coil that can reduce manufacturing man-hours.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は従来の電磁石用コイルの曲げ加工部近
傍の斜視図、第2図は従来の電磁石用コイルの平
角導体の断面図、第3図は従来の電磁石用コイル
の曲げ加工部の平角導体の曲げ加工後の状態を示
す断面図、第4図は従来の電磁石用コイルの他の
例の平角導体の断面図、第5図は従来の電磁石用
コイルの他の例の第4図の平角導体を巻回・積層
した場合の曲げ加工をしない直線部の状態を示す
積層導体の断面図、第6図は本発明の電磁石用コ
イルの一実施例の平角導体の断面図、第7図は同
じく一実施例の第6図の平角導体を巻回・積層し
た場合の曲げ加工部の状態を示す積層導体の断面
図、第8図は同じく一実施例の第6図の平角導体
を巻回・積層した場合の曲げ加工をしない直線部
の状態を示す積層導体の断面図である。 3……平角導体、3a……曲げ加工内径側、3
b……曲げ加工外径側。
Figure 1 is a perspective view of the vicinity of the bent portion of a conventional electromagnet coil, Figure 2 is a sectional view of a rectangular conductor of a conventional electromagnet coil, and Figure 3 is a rectangular conductor of a conventional electromagnet coil's bent portion. Figure 4 is a cross-sectional view of a rectangular conductor of another example of a conventional electromagnet coil, and Figure 5 is a cross-sectional view of another example of a conventional electromagnet coil. FIG. 6 is a sectional view of a rectangular conductor of an embodiment of the electromagnet coil of the present invention, and FIG. FIG. 8 is a cross-sectional view of a laminated conductor showing the state of the bent portion when the rectangular conductor shown in FIG. 6 of one embodiment is wound and laminated, and FIG. 8 is a cross-sectional view of the rectangular conductor of FIG. - It is a sectional view of a laminated conductor showing the state of a straight part without bending when laminated. 3...Flat conductor, 3a...Bending inner diameter side, 3
b...bending outer diameter side.

Claims (1)

【特許請求の範囲】[Claims] 1 平角導体が巻回され、積層される電磁石用コ
イルにおいて、前記巻回される平角導体が、その
断面が導体幅のほぼ中心から前記巻回時の曲げ加
工内径側が先細となるように形成されたものであ
ることを特徴とする電磁石用コイル。
1. In an electromagnetic coil in which rectangular conductors are wound and laminated, the rectangular conductor to be wound is formed such that its cross section tapers from approximately the center of the conductor width to the inner diameter side of the bending process during the winding. An electromagnetic coil characterized by:
JP3900684A 1984-02-29 1984-02-29 Coil for electromagnet Granted JPS60182704A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3900684A JPS60182704A (en) 1984-02-29 1984-02-29 Coil for electromagnet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3900684A JPS60182704A (en) 1984-02-29 1984-02-29 Coil for electromagnet

Publications (2)

Publication Number Publication Date
JPS60182704A JPS60182704A (en) 1985-09-18
JPH0315324B2 true JPH0315324B2 (en) 1991-02-28

Family

ID=12541022

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3900684A Granted JPS60182704A (en) 1984-02-29 1984-02-29 Coil for electromagnet

Country Status (1)

Country Link
JP (1) JPS60182704A (en)

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63305503A (en) * 1987-06-05 1988-12-13 Mitsubishi Electric Corp Coil device
JP2736961B2 (en) * 1994-07-29 1998-04-08 和哉 高山 Drive brush device
AT406921B (en) * 1998-08-20 2000-10-25 Asta Elektrodraht Gmbh ELECTRICAL CONDUCTOR
JP4623983B2 (en) * 2004-03-24 2011-02-02 株式会社ケーヒン Linear solenoid valve
JP4623984B2 (en) * 2004-03-24 2011-02-02 株式会社ケーヒン Linear solenoid valve

Also Published As

Publication number Publication date
JPS60182704A (en) 1985-09-18

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