JP2000150259A - High frequency coil and transformer - Google Patents

High frequency coil and transformer

Info

Publication number
JP2000150259A
JP2000150259A JP10323499A JP32349998A JP2000150259A JP 2000150259 A JP2000150259 A JP 2000150259A JP 10323499 A JP10323499 A JP 10323499A JP 32349998 A JP32349998 A JP 32349998A JP 2000150259 A JP2000150259 A JP 2000150259A
Authority
JP
Japan
Prior art keywords
frequency coil
conductors
frequency
flat
conductor
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
Application number
JP10323499A
Other languages
Japanese (ja)
Inventor
Toshihiro Nomura
年弘 野村
Toshio Kurosaki
稔雄 黒崎
Yutaka Ito
伊藤  豊
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.)
Fuji Electric Co Ltd
Original Assignee
Fuji 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 Fuji Electric Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP10323499A priority Critical patent/JP2000150259A/en
Publication of JP2000150259A publication Critical patent/JP2000150259A/en
Pending legal-status Critical Current

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  • General Induction Heating (AREA)
  • Coils Of Transformers For General Uses (AREA)
  • Transformer Cooling (AREA)

Abstract

PROBLEM TO BE SOLVED: To provide a high frequency coil, in which heat radiation can be made satisfactory, the number of winding increased, and tap can be easily extracted. SOLUTION: Plural U-shaped plate conductors 2 are accumulated while the terminal parts are connected successively and spirally, and the plate conductors 2 are insulated by removing the connected terminal part so that a high frequency coil 1 is constituted. The heat radiation of the high frequency coil 1 constituted of the laminated body of the plate conductors 2 can be made superior by increasing the surface area, and the number of winding can be readily increased by increasing the number of laminated layers. Also, the number of winding can be sharply increased or decreased, by increasing or decreasing the number of laminated layers. Moreover, an intermediate tap can be interposed in the middle of the laminated plate conductors 2 and can be extracted freely.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】この発明は、誘導加熱装置や
リアクトルなどに有用な高周波コイル及びこれを用いた
高周波トランスに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a high-frequency coil useful for an induction heating device or a reactor, and a high-frequency transformer using the same.

【0002】[0002]

【従来の技術】従来の高周波コイルとして、エナメル
線を数十本から数百本束ねたリッツ線を巻いたもの、
数kW以上の大電力用として水冷金属パイプを巻いたも
の、幅広の帯状導体を巻いたものなどが知られてい
る。
2. Description of the Related Art As a conventional high-frequency coil, a coil wound around a litz wire in which dozens to hundreds of enamel wires are bundled,
Known are those for winding a water-cooled metal pipe and those for winding a wide band-shaped conductor for high power of several kW or more.

【0003】[0003]

【発明が解決しようとする課題】ところが、上記した従
来の高周波コイルは、以下のような問題がある。 (1)下層中心部の放熱が悪く、大電力が扱えない
(,)。 (2)巻数を増やすのが困難である()。 (3)中間タップが出しにくい(,,)。 (4)設計変更や現場修正がしにくい。 (5)コイル内形状(磁路断面形状)が限定される。 そこで、この発明は、これらの問題に容易に対処するこ
とのできる高周波コイル及びこれを用いた高周波トラン
スを得ることを課題とするものである。
However, the above-mentioned conventional high-frequency coil has the following problems. (1) The heat radiation at the center of the lower layer is poor, and large power cannot be handled. (2) It is difficult to increase the number of turns (). (3) It is difficult to output an intermediate tap (,,). (4) It is difficult to make design changes and site modifications. (5) The internal shape of the coil (magnetic path cross-sectional shape) is limited. Therefore, an object of the present invention is to provide a high-frequency coil and a high-frequency transformer using the same, which can easily deal with these problems.

【0004】[0004]

【課題を解決するための手段】この発明は、磁路空間を
部分的に囲むように半閉状に形成した複数枚の同形の平
板導体をそれらの端部同士を順次らせん状に接続しなが
ら積み重ね、前記平板導体間を前記接続端部を除いて互
いに絶縁することにより高周波コイルを構成し、上記課
題を解決するものである(請求項1)。前記半閉状の平
板導体の形状としては、後述するように、U字状、S字
状、C字状、L字状、V字状、W字状、M字状など種々
のものが使用可能である。平板導体間の接続は、圧接又
ははんだ付けやろう付けなどの接合により行う。このよ
うな平板導体の積層体からなる高周波コイルは、表面積
が大きいために優れた放熱性が得られるとともに、積層
枚数の増減により巻数を容易に加減することができる。
また、中間タップは積層された平板導体の途中から自由
に引き出すことができる。その場合、中間タップの口出
し端子は、前記平板導体の接続端部において、導体間に
短冊形の平板導体を挟み込んで形成するのがよい(請求
項2)。
SUMMARY OF THE INVENTION According to the present invention, a plurality of same-shaped plate conductors formed in a semi-closed shape so as to partially surround a magnetic path space are stacked while their ends are sequentially connected in a spiral manner. A high-frequency coil is constituted by insulating the flat conductors from each other except for the connection end, thereby solving the above-mentioned problem (claim 1). Various shapes such as U-shape, S-shape, C-shape, L-shape, V-shape, W-shape, and M-shape can be used as the shape of the semi-closed plate conductor as described later. It is. The connection between the plate conductors is performed by pressure welding or joining such as soldering or brazing. The high-frequency coil formed of such a laminated body of flat conductors has a large surface area and thus has excellent heat radiation properties, and can easily adjust the number of windings by increasing or decreasing the number of laminated layers.
Further, the intermediate tap can be freely pulled out from the middle of the laminated plate conductor. In this case, it is preferable that the lead terminal of the intermediate tap is formed by sandwiching a strip-shaped flat conductor between the conductors at the connection end of the flat conductor.

【0005】前記平板導体は非対称に形成し、この平板
導体を複数枚積み重ねたときに外周面に不揃いが生じる
ようにすれば、この不揃い部分が冷却フィンの役割をし
て冷却作用を高めることができる(請求項3)。一方、
前記平板導体を複数枚の薄板を積層して形成すれば、可
撓性が生じて取扱いが容易になるとともに、高周波電流
の表皮効果の抑制に有効である(請求項4)。その場
合、前記薄板間を部分的に絶縁すれば、表皮効果の抑制
作用が一層高まる(請求項5)。また、複数枚の薄板を
積層して前記平板導体を形成する場合には、その接続端
部において、互いに接続される前記平板導体の前記薄板
を互い違いに重ね合わせるのがよく、これにより接続部
の接触抵抗を大幅に減らすことができる(請求項6)。
If the flat conductors are formed asymmetrically and irregularities occur on the outer peripheral surface when a plurality of the flat conductors are stacked, the irregular portions can serve as cooling fins to enhance the cooling effect. (Claim 3). on the other hand,
When the flat conductor is formed by laminating a plurality of thin plates, flexibility is generated and handling becomes easy, and it is effective for suppressing the skin effect of high-frequency current (claim 4). In this case, if the thin plates are partially insulated, the effect of suppressing the skin effect is further enhanced (claim 5). Further, when the flat conductor is formed by laminating a plurality of thin plates, the thin plates of the flat conductor to be connected to each other are preferably staggered at the connection end thereof, thereby forming the connecting portion. The contact resistance can be greatly reduced (claim 6).

【0006】前記平板導体の外周面には冷却水パイプを
接合して、冷却性能を高めることができ、これにより大
電流の通流が可能になる(請求項7)。また、前記平板
導体間に絶縁物のスペーサを挿入して空隙を形成し、こ
の空隙に空気を通流させることによっても、冷却性能を
高めることができる(請求項8)。その場合、前記空隙
により前記平板導体間の絶縁を兼ねることができる(請
求項9)。
A cooling water pipe can be joined to the outer peripheral surface of the flat conductor to enhance the cooling performance, thereby allowing a large current to flow. The cooling performance can also be enhanced by inserting a spacer made of an insulator between the plate conductors to form a gap and allowing air to flow through the gap. In this case, the gap can also serve as insulation between the flat conductors.

【0007】前記平板導体の端部同士を接離自在に突き
合わせ接続すれば、この接続端部でコイルを分割するこ
とが可能になり、例えば誘導加熱装置におけるワークの
出し入れが容易になる(請求項10)。その場合、前記
接続端部の突き合わせ面をくさび状に形成すれば、接続
部の噛み合いを円滑にし、かつ接触圧力を高めることが
できる(請求項11)。
[0007] If the ends of the flat conductors are butt-connected to each other so as to be able to freely contact and separate from each other, it is possible to divide the coil at the connection ends, and for example, it is easy to take in and out the work in the induction heating device. 10). In this case, if the abutting surfaces of the connection ends are formed in a wedge shape, the engagement of the connection portions can be made smooth and the contact pressure can be increased (claim 11).

【0008】請求項1記載の高周波コイルからなる1次
コイル及び2次コイルを組み合わせれば、高周波トラン
スを構成することができる(請求項12)。また、請求
項1記載の高周波コイルからなる1次コイルの内側に平
板導体を筒状に巻いた2次コイルを設ければ、2次コイ
ルに巨大電流を流すことができる(請求項13)。その
場合、2次コイルの内側に冷却水パイプを設ければ、巨
大電流が流れる2次コイルを効果的に冷却することがで
きる(請求項14)。
A high frequency transformer can be constructed by combining a primary coil and a secondary coil comprising the high frequency coil described in claim 1 (claim 12). Further, if a secondary coil in which a flat conductor is wound in a cylindrical shape is provided inside the primary coil comprising the high-frequency coil described in claim 1, a huge current can flow through the secondary coil (claim 13). In this case, if a cooling water pipe is provided inside the secondary coil, the secondary coil through which a huge current flows can be effectively cooled (claim 14).

【0009】[0009]

【発明の実施の形態】以下、図1〜14図に基づいて、
この発明の実施の形態を説明する。まず図1〜図3は高
周波コイルの基本的な実施の形態を示すもので、図1の
(A)は高周波コイルの平面図、(B)は(A)の側面
図、(C)は(A)の正面図、(D)は回路図、図2の
(A)は図1における平板導体の平面図、(B)はその
正面図、図3は図1の高周波コイルの組立順序を説明す
る平面図である。図1において、高周波コイル1は、平
板導体2が絶縁層3を介して後述する方法で積み重ねら
れて構成され、その上下面にコイル両端の端子U,Vを
形成する短冊形の端子板4がそれぞれ重ねられた上で、
上下各2枚の絶縁物の押え板5を介して、4個所のボル
ト6及びナット7により締め付けられている。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS Referring to FIGS.
An embodiment of the present invention will be described. 1 to 3 show a basic embodiment of a high-frequency coil. FIG. 1A is a plan view of the high-frequency coil, FIG. 1B is a side view of FIG. 1A, and FIG. 1A is a front view, FIG. 2D is a circuit diagram, FIG. 2A is a plan view of the flat conductor in FIG. 1, FIG. 2B is a front view thereof, and FIG. FIG. In FIG. 1, a high-frequency coil 1 is configured by stacking flat conductors 2 via an insulating layer 3 by a method described later, and has a strip-shaped terminal plate 4 on both upper and lower surfaces of which terminals U and V at both ends of the coil are formed. After being stacked on each other,
It is fastened by four bolts 6 and nuts 7 via two upper and lower insulating holding plates 5.

【0010】図2において、平板導体2は板材からの打
抜により、外形が方形のU字状(ないしはコ字状)に形
成されている。絶縁層3は絶縁シートからなり、平板導
体1の片方の脚部2aを除く残余部分を覆うL字状に形
成されている。絶縁層3はシート材の代わりに、塗膜と
することもできる。
In FIG. 2, a flat conductor 2 is formed in a U-shape (or U-shape) having a rectangular outer shape by punching from a plate material. The insulating layer 3 is formed of an insulating sheet, and is formed in an L-shape to cover the remaining portion of the flat conductor 1 excluding one leg 2a. The insulating layer 3 can be a coating film instead of the sheet material.

【0011】図2の平板導体2を用いて図1の高周波コ
イル1を組み立てるには、図3において、(A)に示す
ように下側の2本の押え板5を平行に並べ、その上に
(B)に示すように端子Uの端子板4を直交させて重ね
た後、その上に(C)〜(E)に示すように平板導体2
を必要枚数積み重ね、その上に(F)に示すように端子
Vの端子板4を重ね、最後に(G)に示すように上側の
2本の押え板5を平行に並べて載せ、上下の押え板5,
5間をすでに述べたようにボルト・ナット6,7で締め
付ける。押え板5の両端の穴8はボルト6(図1)を通
すためのものである。
In order to assemble the high-frequency coil 1 shown in FIG. 1 using the flat conductor 2 shown in FIG. 2, in FIG. 3, two lower holding plates 5 are arranged in parallel as shown in FIG. As shown in (B), after the terminal plates 4 of the terminals U are overlapped at right angles, the flat conductors 2 are placed thereon as shown in (C) to (E).
Are stacked in the required number, and the terminal plate 4 of the terminal V is stacked thereon as shown in (F). Finally, the two upper holding plates 5 are placed in parallel as shown in (G), and Plate 5,
The five spaces are tightened with the bolts and nuts 6 and 7 as described above. Holes 8 at both ends of the holding plate 5 are for passing bolts 6 (FIG. 1).

【0012】ここで、図3(C)〜(E)の平板導体2
の積み重ね作業では、平板導体2の上面に絶縁層2を重
ねたもの(図2)を単位として、これを180°ずつ向
きを反転させながら順次積み重ねている。これにより、
図3において、(C)の平板導体2の左側脚部2aの裸
の上面に、(D)の平板導体2の左側脚部の裸の下面が
接触し、次いで(D)の平板導体2の右側脚部の裸の上
面に、(E)の平板導体2の右側脚部の裸の下面が接触
して、結果として上記裸の端部同士が順次らせん状に接
続され、また絶縁層2の存在する平板導体2間は互いに
絶縁されて、(C)〜(E)の3枚の平板導体2で1.5
ターン( 1枚の平板導体2で0.5 ターン)のコイルが構
成されている。以後はこの繰り返しにより、任意の巻数
が得られる。
Here, the flat conductor 2 shown in FIGS.
In the stacking operation of (1), a unit in which the insulating layer 2 is stacked on the upper surface of the flat conductor 2 (FIG. 2) is sequentially stacked while inverting the direction by 180 °. This allows
In FIG. 3, the bare lower surface of the left leg of the flat conductor 2 of FIG. 3D contacts the bare upper surface of the left leg 2a of the flat conductor 2 of FIG. The bare lower surface of the right leg of the flat conductor 2 in (E) comes into contact with the bare upper surface of the right leg, and as a result, the bare ends are sequentially spirally connected to each other. The existing flat conductors 2 are insulated from each other, and the three flat conductors 2 of FIGS.
A coil of turns (0.5 turns with one flat conductor 2) is formed. Thereafter, by repeating this, an arbitrary number of turns can be obtained.

【0013】図3において、端子Uの端子板4は一番下
の平板導体2の右側脚部の裸の下面に接触し、また端子
Vの端子板4は一番上の平板導体2の左側脚部の裸の上
面に接触してそれぞれ高周波コイル1の両端に接続され
ている。そして、平板導体2及び端子板4の接触面は、
ボルト6による締付けにより相手接触面に互いに圧接さ
れる。なお、圧接の代わりに、はんだ付けやろう付けな
どにより接合してもよい。図1(D)はこのような高周
波コイル1の回路構成を示している。また、図1(D)
に示す中間タップV’を任意の位置に引き出すには、図
1(D)に示すように、所要の場所に端子板4’を挟み
込めばよい。中間タップV’は、端子板4’を任意の位
置に挟み込むことにより任意の巻数が得られる。
In FIG. 3, the terminal plate 4 of the terminal U is in contact with the bare lower surface of the right leg of the lowermost flat conductor 2, and the terminal plate 4 of the terminal V is on the left side of the uppermost flat conductor 2. They are connected to both ends of the high-frequency coil 1 in contact with the bare upper surfaces of the legs. The contact surface between the flat conductor 2 and the terminal plate 4 is
Due to the tightening by the bolts 6, the contact surfaces are pressed against each other. It should be noted that joining may be performed by soldering, brazing, or the like instead of pressing. FIG. 1D shows a circuit configuration of such a high-frequency coil 1. FIG. 1 (D)
In order to pull out the intermediate tap V ′ shown in FIG. 1 to an arbitrary position, as shown in FIG. 1 (D), the terminal plate 4 ′ may be inserted at a required place. The intermediate tap V 'can have an arbitrary number of turns by sandwiching the terminal plate 4' at an arbitrary position.

【0014】一方、図2において、平板導体2は磁路の
左右の中心Cに対して、図示寸法がa>b、つまり左右
が非対称になっている。このような平板導体2は180
°ずつ向きを反転させながら積み重ねた場合、図1
(C)に示すように、左右の外周面に不揃いが生じる。
この不揃いは冷却フィンの役割をし、通電時に発熱する
高周波コイル1の冷却に有効である。なお、この非対称
は左右のみならず、前後に設けることが可能であり、ま
た後述するように平板導体2の形状は図示門形に限られ
る訳ではないので、その形状に応じて種々の非対称が設
定可能である。
On the other hand, in FIG. 2, the plate conductor 2 has a dimension a> b, that is, the right and left sides are asymmetric with respect to the center C on the left and right sides of the magnetic path. Such a flat conductor 2 is 180
Fig. 1
As shown in (C), irregularities occur on the left and right outer peripheral surfaces.
The irregularities serve as cooling fins and are effective for cooling the high-frequency coil 1 that generates heat when energized. Note that this asymmetry can be provided not only on the left and right but also on the front and back, and the shape of the plate conductor 2 is not limited to the illustrated gate shape as described later. Can be set.

【0015】図4は、異なる実施の形態を示すものであ
る。図4において、平板導体2は図3におけるものと同
様にU字状であるが、この実施の形態では平板導体2を
90°ずつ向きを変えて、それらの端部同士を順次らせ
ん状に接続しながら積み重ねるものである。その場合、
絶縁層3は平板導体2の接続部となる一方の脚部の先端
部分2aを除く部分を覆うように設けられ、この接続端
部2aの裸の上面と、次の平板導体2の他方の脚部の先
端部分2bの裸の下面とが接触して、らせん状の接続が
行われる。この接続では1枚の平板導体2で0.75ターン
のコイルが得られる。この実施の形態は、図3の実施の
形態に比べて平板導体2間の接触面積は小さいが、少な
い枚数の平板導体2で多くの巻数が得られる。また、図
4に示すように、締付けボルトを通す穴8を平板導体2
に設けておくことにより、押え板5(図1)を省略して
締め付け、小形化を図ることができる。
FIG. 4 shows a different embodiment. In FIG. 4, the flat conductor 2 is U-shaped, as in FIG. 3, but in this embodiment, the flat conductor 2 is turned 90 degrees at a time and their ends are connected in a spiral fashion. It stacks while doing. In that case,
The insulating layer 3 is provided so as to cover a portion of the one leg portion serving as a connecting portion of the flat plate conductor 2 except for the tip portion 2a, and the bare upper surface of the connecting end portion 2a and the other leg of the next flat plate conductor 2 A helical connection is made by contact with the bare lower surface of the tip portion 2b of the portion. In this connection, a coil of 0.75 turns can be obtained with one flat conductor 2. In this embodiment, the contact area between the plate conductors 2 is smaller than in the embodiment of FIG. 3, but a larger number of turns can be obtained with a smaller number of plate conductors 2. Also, as shown in FIG.
In this case, the holding plate 5 (FIG. 1) can be omitted and tightened, and the size can be reduced.

【0016】平板導体2の外形は上に示したように方形
にすれば導体材料を無駄なく使用することができるが、
この外形は基本的には自由であり、円形や多角形など任
意に選択することができる。また、内側(磁路)の形状
についても、方形以外に円形、まゆ形、更に三角、星形
など自由に形成することが可能である。
If the outer shape of the flat conductor 2 is made rectangular as shown above, the conductor material can be used without waste.
This outer shape is basically free and can be arbitrarily selected such as a circle or a polygon. Also, the shape of the inner side (magnetic path) can be freely formed such as a circle, a cocoon, a triangle, a star, and the like in addition to a square.

【0017】図5は平板導体2を複数枚の薄板2’を積
層して形成した実施の形態を示すものである。これによ
り、平板導体2に可撓性が生じてその取扱が容易になる
とともに、高周波電流の表皮効果が抑制される利点が生
じる。その場合、薄板2’間を絶縁する導体内絶縁層9
を設ければ、表皮効果の抑制作用が一層高まる。また、
この平板導体2を積み重ねてらせん状に接続する際、図
6に示すように、その接続端部において、互いに接続さ
れる平板導体2の薄板2’を互い違いに重ね合わせれ
ば、接続部の接触抵抗を薄板2’の枚数分の一に減らす
ことができる。更に、薄板2’を積層して平板導体2を
形成した場合には、平板導体2の1枚当たりの薄板枚数
を加減することにより、後から通電容量(積層枚数に比
例する)やコイル巻数(積層枚数を減らせば増やせる)
を修正することができ、実用試験後の設計変更などに柔
軟に対応することできる。以上示した実施の形態では、
U字状の形状の平板導体2の例を示したが、同様の原理
により、C字状、L字状、V字状などの半開状の任意形
状の平板導体についても高周波コイルを構成することが
できる。
FIG. 5 shows an embodiment in which the flat conductor 2 is formed by laminating a plurality of thin plates 2 '. As a result, there is an advantage that the flat plate conductor 2 becomes flexible and its handling becomes easy, and the skin effect of the high-frequency current is suppressed. In that case, the in-conductor insulating layer 9 for insulating between the thin plates 2 ′
The effect of suppressing the skin effect is further enhanced by providing. Also,
When the flat conductors 2 are stacked and spirally connected, as shown in FIG. 6, if the thin plates 2 'of the flat conductors 2 to be connected to each other are alternately overlapped at their connection ends, the contact resistance of the connection portion is reduced. Can be reduced to 1 / the number of thin plates 2 ′. Further, when the flat conductors 2 are formed by laminating the thin plates 2 ′, the number of thin plates per flat conductor 2 is adjusted so that the current carrying capacity (proportional to the number of laminations) and the number of coil turns ( It can be increased by reducing the number of layers)
Can be corrected, and it is possible to flexibly cope with a design change or the like after a practical test. In the embodiment described above,
Although the example of the U-shaped flat conductor 2 has been described, a high-frequency coil can be formed with a half-open arbitrary flat conductor such as a C-shape, an L-shape, or a V-shape according to the same principle. Can be.

【0018】図7は平板導体2の外周面(図示の場合は
U曲げ部端面)に冷却水パイプ10をろう付けあるいは
はんだ付けにより接合した実施の形態を示すものであ
る。冷却水パイプ10は平板導体2を積み重ねたときに
当たらないように、ホース11が接続される両端を除い
て円管が扁平に潰し加工され、また両端は平板導体相互
間で交互に逆方向に振られている。冷却水パイプ10に
冷却水を通す水冷は、風冷に比べて格段に冷却能力が優
れており、高周波コイルの通電容量を大幅に増大するこ
とができる。平板導体2の内奥部の発熱を冷却水パイプ
10に伝えるためには平板導体2は厚いほど有利であ
り、複数枚の導体板を積層して平板導体2を形成する場
合には、冷却水パイプ10を接合する導体板は厚板と
し、その両側に薄板を重ねるようにするとよい。
FIG. 7 shows an embodiment in which a cooling water pipe 10 is joined to the outer peripheral surface (the end surface of a U-bent portion in the case of the drawing) of the flat conductor 2 by brazing or soldering. The cooling water pipe 10 is formed by flattening a circular pipe except for both ends to which the hose 11 is connected so that the cooling water pipe 10 does not hit when the flat conductors 2 are stacked. It has been shaken. Water cooling, in which cooling water is passed through the cooling water pipe 10, has much better cooling capacity than air cooling, and can greatly increase the current-carrying capacity of the high-frequency coil. In order to transfer the heat generated in the inner part of the plate conductor 2 to the cooling water pipe 10, the thickness of the plate conductor 2 is more advantageous, and when the plate conductor 2 is formed by laminating a plurality of conductor plates, the cooling water The conductor plate for joining the pipe 10 is preferably a thick plate, and thin plates may be stacked on both sides thereof.

【0019】図8は、平板導体2間に絶縁物のスペーサ
を挿入した実施の形態を示すもので、図8の(A)は平
面図、(B)はその側面図である。図8において、2枚
の平板導体2からなるコイル1巻きごとに、絶縁パイプ
から切り出されたスペーサ12が四隅に挿入され、この
部分を貫通するボルト6とナット7とにより、絶縁ワッ
シャ13を介して一体に締め付けられている。スペーサ
12の挿入により平板導体間に空隙14が作られ、この
空隙14に空気が通流するので冷却性能が向上する。図
示の通り、冷却ファン15で送風すれば、冷却性能は更
に高まる。また、空隙14ができたことにより、この部
分に挿入されるべき絶縁層3(図1)を省略することも
可能である。
FIGS. 8A and 8B show an embodiment in which an insulating spacer is inserted between the flat conductors 2. FIG. 8A is a plan view and FIG. 8B is a side view thereof. In FIG. 8, a spacer 12 cut out from an insulating pipe is inserted into each of the four corners for each turn of a coil made up of two flat conductors 2, and a bolt 6 and a nut 7 penetrating this portion via an insulating washer 13. And are tightened together. A gap 14 is created between the flat conductors by the insertion of the spacer 12, and air flows through the gap 14, thereby improving the cooling performance. As shown in the figure, if the air is blown by the cooling fan 15, the cooling performance is further enhanced. In addition, due to the formation of the gap 14, the insulating layer 3 (FIG. 1) to be inserted into this portion can be omitted.

【0020】図9は平板導体の端部同士を接離自在に突
き合わせ接続して構成した高周波コイルの実施の形態を
示すもので、図9の(A)は側面図、(B)はそのB−
B線に沿う断面図、また図10は平板導体を形成するセ
グメントを示し、(A)は側面図、(B)はその右正面
図である。セグメント16は板導体から打ち抜き形成さ
れ、図10に示すように、磁路17(図9)となる部分
が半円形に切り抜かれた形状のU字状で、両脚部先端の
片面が斜めに削除されて斜面16aが設けられ、またそ
の反対側に絶縁ボルト18(図9)を通す半円状の切欠
19が設けられている。なお、セグメント16はすでに
述べた冷却フィンとしての不揃いを生じさせるために、
左右で非対称に形成されている。
FIGS. 9A and 9B show an embodiment of a high-frequency coil constructed by butt-connecting the ends of flat conductors so as to be able to come and go. FIG. 9A is a side view, and FIG. −
FIG. 10 is a cross-sectional view taken along the line B, and FIG. 10 shows a segment forming a flat conductor, (A) is a side view, and (B) is a right front view thereof. The segment 16 is stamped and formed from a plate conductor, and as shown in FIG. 10, a U-shaped portion in which a portion to be a magnetic path 17 (FIG. 9) is cut out in a semicircle, and one end of both leg portions is obliquely deleted. Thus, a slope 16a is provided, and a semicircular notch 19 through which an insulating bolt 18 (FIG. 9) is passed is provided on the opposite side. In order to cause the irregularities as the cooling fins already described,
It is formed asymmetrically on the left and right.

【0021】図9に示すように、セグメント16は斜面
16aが内側になるように2枚重ねられて、両脚部先端
にV字状の溝を有する上側の平板導体20が形成され、
また斜面16aが外側になるように2枚重ねられて、両
脚部先端にA字状の突部を有する下側の平板導体21が
形成される。これら平板導体20と平板導体21とは、
端部の溝と突部とが順次らせん状に突き合わされて高周
波コイルを構成する。ここで、平板導体20は、左右一
対の絶縁物の側板22の間で、図11に示す絶縁シート
23を介して重ねられ、一方の側板22の穴及び平板導
体20の切欠19(図10)を通して他方の側板22の
ねじ穴にねじ込まれた絶縁ボルト18により一体に締め
付けられている。同様に、下側の平板導体21は、左右
一対の絶縁物の側板24の間で絶縁シート23を介して
重ねられ、絶縁ボルト18により一体に締め付けられて
いる。絶縁ボルト18は芯部は金属であるが、表面は絶
縁材18aで被覆されている。
As shown in FIG. 9, two segments 16 are overlapped so that the slope 16a is on the inside, and an upper flat conductor 20 having V-shaped grooves at the ends of both legs is formed.
Also, two sheets are stacked so that the slope 16a is on the outside, and a lower flat conductor 21 having A-shaped protrusions at the ends of both legs is formed. These flat conductor 20 and flat conductor 21 are:
The groove at the end and the protrusion are sequentially butted in a spiral shape to form a high-frequency coil. Here, the flat conductor 20 is overlapped between a pair of left and right insulating side plates 22 via an insulating sheet 23 shown in FIG. 11, and a hole in one of the side plates 22 and a notch 19 of the flat conductor 20 (FIG. 10). And is integrally fastened by an insulating bolt 18 screwed into a screw hole of the other side plate 22. Similarly, the lower flat conductor 21 is overlapped between a pair of left and right insulating side plates 24 via an insulating sheet 23 and integrally fastened by insulating bolts 18. The core of the insulating bolt 18 is metal, but the surface is covered with an insulating material 18a.

【0022】そして、側板22は図9(A)の左端で側
板24にピン25を介してヒンジ結合され、また右端で
蝶ナット26により押さえられるようになっている。蝶
ナット26は押え棒27の上端部のねじ部に螺合され、
押え棒27の下端部は側板24間に渡されたロッド28
の中央に回動自在に保持されている。また、ロッド28
の直上には、側板22間に渡るように横板29が一体形
成され、その中央には押え棒27が嵌入するU字状の溝
29aが切り欠き形成されている。そこで、図9に示す
ように、押え棒27を溝29aに嵌入させ、蝶ナット2
6を締めると、平板導体20と平板導体21の突き合わ
せ端部同士は互いに押し付けられくさび作用により強固
に接続される。また、蝶ナット26を緩め、押え棒27
を倒すことにより、上側の平板導体20を持ち上げ、磁
路17を開放することができる。
The side plate 22 is hinged to the side plate 24 via a pin 25 at the left end in FIG. 9A, and pressed by a wing nut 26 at the right end. The wing nut 26 is screwed into the thread at the upper end of the holding rod 27,
The lower end of the holding rod 27 is a rod 28 passed between the side plates 24.
Is rotatably held in the center of the. The rod 28
A horizontal plate 29 is integrally formed so as to extend between the side plates 22, and a U-shaped groove 29 a into which the presser bar 27 is fitted is cut out at the center thereof. Therefore, as shown in FIG. 9, the presser bar 27 is fitted into the groove 29a, and the wing nut 2 is inserted.
When 6 is tightened, the butted ends of the flat conductor 20 and the flat conductor 21 are pressed against each other and are firmly connected by a wedge action. Also, loosen the wing nut 26 and presser bar 27
, The upper plate conductor 20 can be lifted, and the magnetic path 17 can be opened.

【0023】このような高周波コイルは、例えば長尺の
被加熱物やひょうたん形の被加熱物のくびれた部分など
を加熱する場合に、被加熱物をワンタッチで高周波コイ
ル内にセットすることができる。その場合、斜面16a
を有するセグメント16を2枚重ねることにより、一種
類のセグメント16で上下の平板導体20,21を形成
することができる。また、V字状の溝とA字状の突部と
の突き合わせにより、噛み合いが円滑になるとともに、
くさび作用で大きな接触圧力が得られる。なお、図には
示していないが、2枚のセグメント16の合わせ面、特
に電流が集中する磁路17の中心に近い部分に絶縁皮膜
を設ければ、表皮効果を低減するのに有効である。
Such a high-frequency coil can be set in the high-frequency coil with one touch, for example, when heating a long object to be heated or a constricted portion of a gourd-shaped object to be heated. . In that case, the slope 16a
By stacking two segments 16 each having the same shape, the upper and lower plate conductors 20 and 21 can be formed by one type of segment 16. In addition, the engagement between the V-shaped groove and the A-shaped protrusion makes the engagement smooth,
A large contact pressure is obtained by the wedge action. Although not shown in the drawing, providing an insulating film on the mating surface of the two segments 16, particularly on a portion near the center of the magnetic path 17 where the current is concentrated, is effective in reducing the skin effect. .

【0024】図12はS字状の平板導体を積み重ねて2
つの磁路を持つ高周波コイルを構成した実施の形態を示
すもので、図12の(A)は平板導体の平面図、(B)
は高周波コイルの平面図、(C)はその側面図、(D)
は回路図である。図12において、平板導体30は
(A)に示すようにS字状に形成され、この平板導体3
0が図示の範囲を覆う絶縁シート31を介して交互に裏
返しの関係で積み重ねられることにより、(B)に示す
ように2つの磁路32及び33を有する高周波コイル1
が構成され、端子U,Vはコイル両端に挟み込まれた端
子板34により形成されている。電流iは矢印で示すよ
うに流れ、(D)に示す磁束Φを発生する。
FIG. 12 shows two stacked S-shaped conductors.
FIG. 12A shows an embodiment in which a high-frequency coil having two magnetic paths is configured. FIG. 12A is a plan view of a flat conductor, and FIG.
Is a plan view of the high-frequency coil, (C) is a side view thereof, (D)
Is a circuit diagram. In FIG. 12, the flat conductor 30 is formed in an S shape as shown in FIG.
0 are alternately stacked in an upside-down relationship via an insulating sheet 31 covering the illustrated range, so that the high-frequency coil 1 having two magnetic paths 32 and 33 as shown in FIG.
Are formed, and the terminals U and V are formed by a terminal plate 34 sandwiched between both ends of the coil. The current i flows as shown by the arrow, and generates a magnetic flux Φ shown in (D).

【0025】磁路32及び33を通る磁束Φの向きは、
図12(D)に示すように互いに反対なので、漏れ磁束
は互いに打ち消され、その周囲に対する影響は小さい。
この高周波コイルは、近接した2本の被加熱物を効率よ
く加熱するのに適している。(B)及び(C)に鎖線で
示すように、リアクトル用の透磁率の低いコアを挿入す
れば、損失係数Qの高いリアクトルを作ることができ
る。この実施の形態では磁路が2つの例を示したが、例
えばW字状やM字状の平板導体を使えば磁路が3つの高
周波コイルを作ることができ、更にその延長上で4つ以
上の磁路のものも自由に作ることができる。
The direction of the magnetic flux Φ passing through the magnetic paths 32 and 33 is
Since they are opposite to each other as shown in FIG. 12 (D), the leakage magnetic fluxes cancel each other out and their influence on the surroundings is small.
This high-frequency coil is suitable for efficiently heating two adjacent objects to be heated. As shown by a chain line in (B) and (C), a reactor having a high loss coefficient Q can be manufactured by inserting a core having a low magnetic permeability for the reactor. In this embodiment, an example in which there are two magnetic paths is shown. For example, if a W-shaped or M-shaped flat conductor is used, a high-frequency coil having three magnetic paths can be formed. The above magnetic path can be made freely.

【0026】図13は図1に示したような平板導体から
なる高周波コイルを1次コイル及び2次コイルとして組
み合わせて、高周波トランスを構成した実施の形態を示
すもので、図9の(A)は平面図、(B)はその右側面
図、(C)は回路図である。例えば、誘導加熱用マッチ
ングトランスはトランジスタインバータなどの高周波電
源の電圧を降圧して電流を増倍させる場合が多く、ここ
ではその場合の例として、1次コイル35は薄い平板導
体2を沢山重ねて構成し、また2次コイル36は厚い平
板導体37を1〜2巻き分重ねて構成し、2次コイル3
6を3並列にして1次コイル35の平板導体2間に挟み
込んだものを示している。
FIG. 13 shows an embodiment in which a high-frequency transformer is formed by combining a high-frequency coil made of a flat conductor as shown in FIG. 1 as a primary coil and a secondary coil, and FIG. Is a plan view, (B) is a right side view thereof, and (C) is a circuit diagram. For example, a matching transformer for induction heating often reduces the voltage of a high-frequency power supply such as a transistor inverter to multiply the current. In this case, as an example of such a case, the primary coil 35 is formed by stacking many thin flat conductors 2. The secondary coil 36 is formed by stacking one to two turns of a thick flat conductor 37,
6 is shown in three parallel arrangements and sandwiched between the plate conductors 2 of the primary coil 35.

【0027】2次コイル36の両端の端子u,vは、絶
縁シート38を挟んで垂直に配置された一対のL形断面
の端子板39により形成され、端子板39にねじ40に
より締め付けられた2次導体41が2次コイル36を構
成する平板導体37の両端に重ねられている。1次コイ
ル35の両端の端子U,Vを形成する端子板4、平板導
体2,37、絶縁層3、2次導体41等は四隅を貫通す
るボルト6及びナット7とにより、絶縁ワッシャ13を
介して一体に締め付けられている。磁路42には鉄心が
入るべきであるが、ここでは省略している。図示高周波
トランスは、1次コイル35の間に2次コイル36が密
着して入り込めるので、漏れ磁束や漏れリアクタンスが
少なく高性能となる。
The terminals u and v at both ends of the secondary coil 36 are formed by a pair of L-shaped terminal plates 39 which are vertically arranged with an insulating sheet 38 interposed therebetween, and are fastened to the terminal plate 39 by screws 40. Secondary conductors 41 are overlapped on both ends of the flat plate conductor 37 constituting the secondary coil 36. The terminal washer 4 forming the terminals U and V at both ends of the primary coil 35, the flat conductors 2 and 37, the insulating layer 3, the secondary conductor 41, and the like are formed by the bolts 6 and the nuts 7 penetrating the four corners to form the insulating washer 13. Are fastened together. An iron core should enter the magnetic path 42, but is omitted here. In the illustrated high-frequency transformer, since the secondary coil 36 can be closely inserted between the primary coils 35, leakage magnetic flux and leakage reactance are small and high performance is achieved.

【0028】図14は、1次コイルの内側に、筒状の2
次コイルを配置した高周波トランスの実施の形態を示す
もので、図14の(A)は平面図、(B)はその正面
図、(C)は回路図である。図14において、図13と
同様の1次コイル43の内側に、環状鉄心44を囲んで
1巻きの長い筒状の2次コイル45が配置され、その内
側に1巻きの扁平加工された冷却水パイプ46が2本接
合されている。2次コイル45のu,v端子45a,4
5bは、絶縁シート47を挟んで重ねられた巻き終わり
部分の一端に一体形成されている。1次コイル43の外
側に2次コイル45を巻くと、1次コイル43の放熱が
妨げられるので、図示の通り内側に巻くのがよい。1巻
きの筒状の2次コイル45は大きな電流増倍ができ、巨
大電流が2次コイル45に流れることによる発熱は冷却
水パイプ46により冷却される。冷却水パイプ46は鉄
心44の冷却にも有効であり、これにより鉄心44の過
熱による特性低下が防止される。長い筒状の2次コイル
45は漏れリアクタンスが小さく、高性能の高周波トラ
ンスが得られる。
FIG. 14 shows that a cylindrical 2
FIG. 14A is a plan view, FIG. 14B is a front view thereof, and FIG. 14C is a circuit diagram, showing an embodiment of a high-frequency transformer in which a secondary coil is arranged. In FIG. 14, a long cylindrical secondary coil 45 having one turn surrounding the annular core 44 is disposed inside the primary coil 43 similar to FIG. 13, and one turn of flattened cooling water is disposed inside the secondary coil 45. Two pipes 46 are joined. U, v terminals 45a, 4 of the secondary coil 45
5b is integrally formed at one end of the winding end portion that is stacked with the insulating sheet 47 interposed therebetween. If the secondary coil 45 is wound around the outside of the primary coil 43, the heat radiation of the primary coil 43 is hindered. The one-turn cylindrical secondary coil 45 can multiply a large current, and the heat generated by the huge current flowing through the secondary coil 45 is cooled by the cooling water pipe 46. The cooling water pipe 46 is also effective for cooling the iron core 44, thereby preventing the core 44 from being deteriorated in characteristics due to overheating. The long cylindrical secondary coil 45 has a small leakage reactance, and a high-performance high-frequency transformer can be obtained.

【0029】[0029]

【発明の効果】以上の通り、この発明によれば、平板導
体を積み重ねることにより、従来の巻線形の高周波コイ
ルに比べて以下のような利点が得られる。 (1)導体表面積が大きいので放熱性が高く、更に平板
導体間に空隙を設けたり、平板導体に冷却水パイプを接
合したりすることにより、容易に大電力を扱うことがで
きる。 (2)平板導体の枚数を増やして巻数を増やすことが容
易であり、また平板導体の枚数の増減により巻数の修正
が簡単に行える。 (3)端子板の挟み込みによりタップを形成できるの
で、タップが出しやすく、またタップ位置の変更が容易
である。 (4)薄板を積層した平板導体を用いることにより、高
周波損失の低減が可能である。 (5)複数の磁路を有する高周波コイルが簡単に構成で
きる。 (6)1次巻線と2次巻線とを密着させることができる
ので、漏れリアクタンスの小さい高周波トランスを構成
できる。 (7)ワンタッチで2分割できる高周波コイルを容易に
構成できるので、長尺やくびれのある被加熱物にも適切
に対応することができる。 (8)一種類の平板導体を用い、その枚数の調整だけで
電流容量や巻数の異なる高周波コイルが得られ、また平
板導体を単に積み重ねるだけでよく、曲げ加工や接合な
どの作業が不要なので、少品種の部品在庫で多種の仕様
に短納期で応じることが可能になる。
As described above, according to the present invention, the following advantages can be obtained by stacking flat conductors, as compared with the conventional wound high-frequency coil. (1) Since the conductor has a large surface area, the heat dissipation is high, and a large power can be easily handled by providing a gap between the flat conductors or joining a cooling water pipe to the flat conductor. (2) It is easy to increase the number of turns by increasing the number of flat conductors, and the number of turns can be easily corrected by increasing or decreasing the number of flat conductors. (3) Since the tap can be formed by sandwiching the terminal plate, the tap can be easily formed and the tap position can be easily changed. (4) High-frequency loss can be reduced by using a flat conductor in which thin plates are stacked. (5) A high-frequency coil having a plurality of magnetic paths can be easily configured. (6) Since the primary winding and the secondary winding can be brought into close contact, a high-frequency transformer having a small leakage reactance can be configured. (7) Since a high-frequency coil that can be divided into two by one touch can be easily configured, it is possible to appropriately cope with a long or constricted object to be heated. (8) High-frequency coils with different current capacities and different numbers of windings can be obtained only by adjusting the number of sheets using a single type of flat conductor, and work such as bending or joining is not required because the flat conductors only need to be stacked. It is possible to meet various specifications in a short delivery time with a small variety of parts inventory.

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

【図1】この発明の実施の形態の高周波コイルを示すも
ので、(A)は平面図、(B)は側面図、(C)は正面
図、(D)は回路図である。
FIG. 1 shows a high-frequency coil according to an embodiment of the present invention, wherein (A) is a plan view, (B) is a side view, (C) is a front view, and (D) is a circuit diagram.

【図2】図1における平板導体を示し、(A)は平面
図、(B)は正面図である。
2A and 2B show a flat conductor in FIG. 1, wherein FIG. 2A is a plan view and FIG. 2B is a front view.

【図3】図1の高周波コイルを組み立てる手順を示す平
面図で、(A)は下部押え板、(B)は一方の端子板、
(C)は一番下の平板導体、(D)はその上に積み重ね
られる平板導体、(E)は更にその上に積み重ねられる
平板導体、(F)は他方の端子板、(G)は上部押え板
である。
3A and 3B are plan views showing a procedure for assembling the high-frequency coil of FIG. 1, wherein FIG. 3A is a lower holding plate, FIG.
(C) is the bottom plate conductor, (D) is the plate conductor stacked thereon, (E) is the plate conductor further stacked thereon, (F) is the other terminal plate, and (G) is the upper portion. It is a holding plate.

【図4】この発明の異なる実施の形態の高周波コイルを
組み立てる手順を示す平面図で、(A)は一方の端子
板、(B)は一番下の平板導体、(C)はその上に積み
重ねられる平板導体、(D)は他方の端子板である。
FIG. 4 is a plan view showing a procedure for assembling a high-frequency coil according to a different embodiment of the present invention, wherein (A) is one terminal plate, (B) is the lowermost plate conductor, and (C) is on it. The flat conductors to be stacked, (D) is the other terminal board.

【図5】薄板を積層した平板導体を示し、(A)は平面
図、(B)は側面図、(C)は正面図である。
5A and 5B show a plate conductor in which thin plates are stacked, wherein FIG. 5A is a plan view, FIG. 5B is a side view, and FIG. 5C is a front view.

【図6】図5の平板導体同士を薄板を交互に重ねて接続
した状態を示す正面図である。
6 is a front view showing a state in which the plate conductors of FIG. 5 are connected by alternately stacking thin plates.

【図7】冷却水パイプを接合した平板導体を示し、
(A)は平面図、(B)は側面図、(C)は正面図であ
る。
FIG. 7 shows a plate conductor joined to a cooling water pipe,
(A) is a plan view, (B) is a side view, and (C) is a front view.

【図8】この発明の更に異なる実施の形態の高周波コイ
ルを示し、(A)は平面図、(B)は側面図である。
8A and 8B show a high-frequency coil according to still another embodiment of the present invention, wherein FIG. 8A is a plan view and FIG. 8B is a side view.

【図9】この発明の更に異なる実施の形態の高周波コイ
ルを示し、(A)は平面図、(B)は側面図である。
9A and 9B show a high-frequency coil according to still another embodiment of the present invention, wherein FIG. 9A is a plan view and FIG. 9B is a side view.

【図10】図9における平板導体のエレメントを示し、
(A)は平面図、(B)は側面図である。
10 shows an element of a flat conductor in FIG. 9,
(A) is a plan view and (B) is a side view.

【図11】図9における絶縁シートを示す平面図である。FIG. 11 is a plan view showing the insulating sheet in FIG. 9;

【図12】この発明の更に異なる実施の形態の高周波コイ
ルを示し、(A)は平板導体の平面図、(B)は高周波
コイルの平面図、(C)は側面図、(D)は回路図であ
る。
12 shows a high-frequency coil according to still another embodiment of the present invention, wherein (A) is a plan view of a flat conductor, (B) is a plan view of a high-frequency coil, (C) is a side view, and (D) is a circuit. FIG.

【図13】この発明の実施の形態の高周波トランスを示
し、(A)は平面図、(B)は側面図、(C)は回路図
である。
FIG. 13 shows a high-frequency transformer according to an embodiment of the present invention, where (A) is a plan view, (B) is a side view, and (C) is a circuit diagram.

【図14】この発明の異なる実施の形態の高周波トランス
を示し、(A)は平面図、(B)は正面図、(C)は回
路図である。
14A and 14B show high-frequency transformers according to different embodiments of the present invention, wherein FIG. 14A is a plan view, FIG. 14B is a front view, and FIG. 14C is a circuit diagram.

【符号の説明】[Explanation of symbols]

1 高周波コイル 2 平板導体 3 絶縁層 4 端子板 5 押え板 9 絶縁層 10 冷却水パイプ 12 スペーサ 14 空隙 20 平板導体 21 平板導体 22 側板 23 絶縁シート 24 側板 30 平板導体 31 絶縁シート 34 端子板 35 1次コイル 36 2次コイル 37 平板導体 38 絶縁シート 39 端子板 41 2次導体 43 1次コイル 44 鉄心 45 2次コイル 46 冷却水パイプ 47 絶縁シート DESCRIPTION OF SYMBOLS 1 High frequency coil 2 Flat conductor 3 Insulating layer 4 Terminal plate 5 Holding plate 9 Insulating layer 10 Cooling water pipe 12 Spacer 14 Air gap 20 Flat conductor 21 Flat conductor 22 Side plate 23 Insulating sheet 24 Side plate 30 Flat conductor 31 Insulating sheet 34 Terminal plate 35 1 Primary coil 36 Secondary coil 37 Flat conductor 38 Insulating sheet 39 Terminal plate 41 Secondary conductor 43 Primary coil 44 Iron core 45 Secondary coil 46 Cooling water pipe 47 Insulating sheet

───────────────────────────────────────────────────── フロントページの続き (51)Int.Cl.7 識別記号 FI テーマコート゛(参考) // H05B 6/36 H01F 31/00 C S (72)発明者 伊藤 豊 神奈川県川崎市川崎区田辺新田1番1号 富士電機株式会社内 Fターム(参考) 3K059 AA08 AA16 AD03 AD25 AD36 AD40 CD62 5E043 AA02 AB04 AB09 BA03 DA06 DB09 EA04 EA06 FA02 5E050 AA10 BA05 ──────────────────────────────────────────────────続 き Continued on the front page (51) Int.Cl. 7 Identification symbol FI Theme coat ゛ (Reference) // H05B 6/36 H01F 31/00 CS (72) Inventor Yutaka Ito Arata Tanabe, Kawasaki-ku, Kawasaki-shi, Kawasaki-ku, Kanagawa Field No. 1 Fuji Electric Co., Ltd. F term (reference) 3K059 AA08 AA16 AD03 AD25 AD36 AD40 CD62 5E043 AA02 AB04 AB09 BA03 DA06 DB09 EA04 EA06 FA02 5E050 AA10 BA05

Claims (14)

【特許請求の範囲】[Claims] 【請求項1】磁路空間を部分的に囲むように半閉状に形
成した複数枚の同形の平板導体をそれらの端部同士を順
次らせん状に接続しながら積み重ね、前記平板導体間を
前記接続端部を除いて互いに絶縁して構成したことを特
徴とする高周波コイル。
1. A plurality of semi-closed flat conductors formed in a semi-closed shape so as to partially surround a magnetic path space while their ends are sequentially spirally connected to each other, and the flat conductors are connected to each other. A high-frequency coil characterized by being insulated from each other except for ends.
【請求項2】前記接続端部の導体間に短冊形の平板導体
を挟み込んで口出し端子を形成したことを特徴とする請
求項1記載の高周波コイル。
2. The high-frequency coil according to claim 1, wherein a lead terminal is formed by sandwiching a strip-shaped flat conductor between the conductors at the connection end.
【請求項3】前記平板導体を非対称に形成し、この平板
導体を複数枚積み重ねたときに外周面に不揃いが生じる
ようにしたことを特徴とする請求項1記載の高周波コイ
ル。
3. The high-frequency coil according to claim 1, wherein said plate conductor is formed asymmetrically, and irregularities are generated on an outer peripheral surface when a plurality of said plate conductors are stacked.
【請求項4】前記平板導体を複数枚の薄板を積層して形
成したことを特徴とする請求項1記載の高周波コイル。
4. The high frequency coil according to claim 1, wherein said flat conductor is formed by laminating a plurality of thin plates.
【請求項5】前記薄板間を絶縁したことを特徴とする請
求項4記載の高周波コイル。
5. The high frequency coil according to claim 4, wherein said thin plates are insulated.
【請求項6】前記接続端部において、互いに接続される
前記平板導体の前記薄板を互い違いに重ね合わせたこと
を特徴とする請求項4記載の高周波コイル。
6. The high-frequency coil according to claim 4, wherein the thin plates of the flat conductors connected to each other are alternately overlapped at the connection end.
【請求項7】前記平板導体の外周面に冷却水パイプを接
合したことを特徴とする請求項1記載の高周波コイル。
7. A high-frequency coil according to claim 1, wherein a cooling water pipe is joined to an outer peripheral surface of said flat conductor.
【請求項8】前記平板導体間に絶縁物のスペーサを挿入
して空隙を形成したことを特徴とする請求項1記載の高
周波コイル。
8. The high-frequency coil according to claim 1, wherein a gap is formed by inserting an insulating spacer between said plate conductors.
【請求項9】前記空隙により前記平板導体間の絶縁を兼
ねるようにしたことを特徴とする請求項8記載の高周波
コイル。
9. The high-frequency coil according to claim 8, wherein said gap serves also as insulation between said plate conductors.
【請求項10】前記平板導体の端部同士を接離自在に突き
合わせ接続したことを特徴とする請求項1記載の高周波
コイル。
10. The high-frequency coil according to claim 1, wherein ends of the flat conductors are butt-connected so as to be able to come and go freely.
【請求項11】前記接続端部の突き合わせ面をくさび状に
形成したことを特徴とする請求項10記載の高周波コイ
ル。
11. The high-frequency coil according to claim 10, wherein the abutting surfaces of the connection ends are formed in a wedge shape.
【請求項12】請求項1記載の高周波コイルからなる1次
コイル及び2次コイルを組み合わせて構成したことを特
徴とする高周波トランス。
12. A high-frequency transformer comprising a combination of a primary coil and a secondary coil comprising the high-frequency coil according to claim 1.
【請求項13】請求項1記載の高周波コイルからなる1次
コイルの内側に平板導体を筒状に巻いた2次コイルを設
けたことを特徴とする高周波トランス。
13. A high-frequency transformer comprising a primary coil comprising the high-frequency coil according to claim 1 and a secondary coil formed by winding a flat conductor in a cylindrical shape inside the primary coil.
【請求項14】2次コイルの内側に冷却水パイプを設けた
ことを特徴とする請求項13記載の高周波トランス。コ
イル。
14. The high-frequency transformer according to claim 13, wherein a cooling water pipe is provided inside the secondary coil. coil.
JP10323499A 1998-11-13 1998-11-13 High frequency coil and transformer Pending JP2000150259A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10323499A JP2000150259A (en) 1998-11-13 1998-11-13 High frequency coil and transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10323499A JP2000150259A (en) 1998-11-13 1998-11-13 High frequency coil and transformer

Publications (1)

Publication Number Publication Date
JP2000150259A true JP2000150259A (en) 2000-05-30

Family

ID=18155380

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10323499A Pending JP2000150259A (en) 1998-11-13 1998-11-13 High frequency coil and transformer

Country Status (1)

Country Link
JP (1) JP2000150259A (en)

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