JPS62219605A - High-frequency transformer - Google Patents

High-frequency transformer

Info

Publication number
JPS62219605A
JPS62219605A JP6227586A JP6227586A JPS62219605A JP S62219605 A JPS62219605 A JP S62219605A JP 6227586 A JP6227586 A JP 6227586A JP 6227586 A JP6227586 A JP 6227586A JP S62219605 A JPS62219605 A JP S62219605A
Authority
JP
Japan
Prior art keywords
winding
secondary winding
windings
transformer
parallel
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
JP6227586A
Other languages
Japanese (ja)
Inventor
Takahiro Matsumoto
松本 孝広
Naoyoshi Maehara
前原 直芳
Shigeru Kusuki
楠木 慈
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP6227586A priority Critical patent/JPS62219605A/en
Publication of JPS62219605A publication Critical patent/JPS62219605A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To restrain heat generation of windings by decreasing a loss resistance of a secondary winding by connecting at least two secondary windings in parallel. CONSTITUTION:As two secondary windings 13a and 13b are connected in parallel, a cross-sectional area of a secondary winding is a sum of the cross-sectional areas of said two windings. To equalize a current density of the secondary winding which is composed at least two windings connected in parallel to that of the secondary winding composed one winding, a thin wire should be used, so that an influence of skin effect can be exceedingly reduced. Accordingly, even if a diameter of the winding is reduced, a virtual current density of the secondary winding of a high-frequency transformer does not increase so much as a cross-sectional area of the winding is reduced and heat generation decreases. Also, an occupation volume of the winding becomes small.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、高周波トランスに関し、さらに詳しく言えば
、大電力、大電流を扱う電源トランスの改良に関するも
のである。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a high frequency transformer, and more specifically, to an improvement in a power transformer that handles large amounts of power and current.

従来の技術 一般に、大電力を扱うトランスは銅損による巻線の発熱
およびヒステリシス損によるコアの発熱のため、大きい
ものとなる。従って、その小型化、2 ベー゛ 軽量化、あるいは低コスト化のために様々な構成のもの
が提案されている。
BACKGROUND OF THE INVENTION Generally, transformers that handle large amounts of power are large because of heat generation in the windings due to copper loss and heat generation in the core due to hysteresis loss. Therefore, various configurations have been proposed to reduce the size, weight, or cost of the device.

第5図は、従来の高周波トランスの断面図を示す。図に
おいて、1はフェライトコアa、2はフェライトコアb
であり、留め具3で押さえられている。4はトランスの
1次巻線で、5は2次巻線である。
FIG. 5 shows a cross-sectional view of a conventional high frequency transformer. In the figure, 1 is ferrite core a, 2 is ferrite core b
and is held down by the fastener 3. 4 is the primary winding of the transformer, and 5 is the secondary winding.

第6図には、銅損の周波数特性を示す。446図が示す
とうり、周波数が高くなると表皮効果の影響で抵抗がふ
えて損失が増加するので、巻線が異状に過熱してしまい
、線の絶縁皮膜が焼けて線間絶縁が保てなくなったりす
る。そこで、1次巻線4は細い銅線を束ねたいわゆるリ
ッツ線をもちいることにより、表皮効果の影響を少なく
している。
FIG. 6 shows the frequency characteristics of copper loss. As shown in Figure 446, as the frequency increases, resistance increases due to the effect of the skin effect and losses increase, causing the winding to overheat abnormally, causing the insulation film of the wire to burn and making it impossible to maintain insulation between the wires. or Therefore, the influence of the skin effect is reduced by using a so-called Litz wire, which is a bundle of thin copper wires, for the primary winding 4.

一方、2次巻線5は線間耐圧をもたし、スペースが少な
くてすむように整列、多層巻きとなっている。各巻線間
の耐圧を高くし放熱を良くするためにフェス処理を行な
いより小型のトランスが実現されていた。
On the other hand, the secondary winding 5 has line-to-line withstand voltage and is arranged and wound in multiple layers so as to require less space. A smaller transformer was realized by applying face treatment to increase the withstand voltage between each winding and improve heat dissipation.

発明が解決しようとする問題点 3 ・、 しかしながら、このような従来の高周波トランスは次の
ような欠点があった。
Problem 3 to be solved by the invention: However, such conventional high frequency transformers have the following drawbacks.

大電流を扱う電源トランスでは高圧巻線5の銅損による
発熱が問題であり、これを押さえるために放熱をよくす
る等の工夫をする必要があった。
Power transformers that handle large currents have a problem with heat generation due to copper loss in the high-voltage winding 5, and in order to suppress this problem, it is necessary to take measures such as improving heat dissipation.

例えば、コアと高圧巻線の間に熱伝導の良い絶縁材料6
を使用して巻線の熱をコアに逃がしたり、巻線の断面積
を増やしたすせざるをえなかった。
For example, an insulating material 6 with good thermal conductivity is used between the core and the high-voltage winding.
It was necessary to use a wire to release heat from the winding to the core, or to increase the cross-sectional area of the winding.

そのためにトランスの小型化が妨げられコストも大きく
なるという問題を有していた。さらに扱う周波数が高く
なると、表皮効果の影響により巻線の損失抵抗は線径を
増やすことにより断面積を増やしても減少せず発熱によ
る巻線皮膜の炭化等によりトランスの寿命が短くなり信
頼性を著しく低下させるという欠点があった。
This has resulted in problems in that miniaturization of the transformer has been hindered and costs have also increased. Furthermore, as the handling frequency increases, due to the skin effect, the loss resistance of the winding does not decrease even if the cross-sectional area is increased by increasing the wire diameter, and the life of the transformer is shortened due to carbonization of the winding film due to heat generation, reducing reliability. It had the disadvantage of significantly lowering the

問題点を解決するための手段 本発明はこのような従来の高周波トランスの欠点を解決
するためになされたものであり、以下に述べる手段によ
り構成された高周波トランスである。
Means for Solving the Problems The present invention has been made to solve the drawbacks of such conventional high frequency transformers, and is a high frequency transformer constructed by the means described below.

即ち、コアと、1次巻線と、各々独立して構成された2
つまたはそt″LL以上次巻線とを備え、前記2次巻線
は、並列かつ同一極性に接続するように構成したもので
ある。
That is, the core, the primary winding, and the two
The secondary winding has one or more secondary windings, and the secondary windings are connected in parallel and with the same polarity.

作  用 本発明は上記構成により以下に述べる作用を有する。即
ち、本発明の高周波トランスは、2次巻線を2つ以上並
列に接続することで、2次巻線の損失抵抗を低下させて
巻線の発熱を抑えることができる。また並列に2つ以上
接続した場合2次巻線の電流密度を1つの2次巻線から
構成された場合と同等とするためには細い線を使用すれ
ばよいので表皮効果の影響を大幅に少ないものとするこ
とができる。従って高周波トランスの2次巻線の″実質
的電流密度は線径を細くしても線の断面積が小さくなっ
た割合程はだかくならないので発熱が少なくなり、巻線
の占有体積も少なくてすむ。
Effects The present invention has the following effects due to the above configuration. That is, in the high frequency transformer of the present invention, by connecting two or more secondary windings in parallel, the loss resistance of the secondary windings can be reduced and heat generation in the windings can be suppressed. Furthermore, when two or more are connected in parallel, thin wires can be used to make the current density of the secondary winding equal to that of a single secondary winding, which greatly reduces the influence of the skin effect. It can be made smaller. Therefore, even if the wire diameter is made thinner, the actual current density in the secondary winding of a high-frequency transformer does not increase as much as the wire's cross-sectional area becomes smaller, resulting in less heat generation and the volume occupied by the winding. Finish.

発熱が少なくなるので巻線の皮膜は耐熱性の低いもので
よく、冷却も容易になり寿命及び信頼性が向上した低コ
ストのトランスが実現できるよう6 ・\−1゛ になるのである。
Since less heat is generated, the winding film only needs to have a low heat resistance, and it can be easily cooled, making it possible to realize a low-cost transformer with improved lifespan and reliability.

実施例 以下、本発明の実施例を添付図面にもとづいて説明する
Embodiments Hereinafter, embodiments of the present invention will be described based on the accompanying drawings.

、、第1図は本発明の一夾廊例のトランスの断面図であ
る。
,, FIG. 1 is a sectional view of a transformer according to an example of the present invention.

図において、8,9はコアでイエライトからなりギャッ
プ10を持り磁路を形成している。コア8.9は止め具
11で固定されている。12は1、盗巻線でり、ツツ線
!世いている。13a、13b、憾2次巻線で並列に接
稗されている。、1次、!=1i2と2次巻線13bの
間には絶縁材14がもうけられている。また2次巻線の
周囲には絶シテープ15が巻かれており、巻線の沿面は
絶縁材16が施されている。
In the figure, cores 8 and 9 are made of yellowite and have a gap 10 to form a magnetic path. The core 8.9 is fixed with a stop 11. 12 is 1, stolen winding wire, Tsutsu wire! The world is alive. 13a and 13b are connected in parallel with secondary windings. , 1st order,! An insulating material 14 is provided between =1i2 and the secondary winding 13b. Further, an insulation tape 15 is wrapped around the secondary winding, and an insulating material 16 is applied to the creeping surface of the winding.

上記構成において、2次巻線13a、13bは2本の線
が並列につながっているので2次巻線の断面積は2本の
線の断面積の和となる。たとえば、2次巻線に0.5φ
の銅線を使用した場倉断兜積の和は 6 ヘーノ 2×πX0.252= 0−39 (mm2)となる。
In the above configuration, since the two wires of the secondary windings 13a and 13b are connected in parallel, the cross-sectional area of the secondary winding is the sum of the cross-sectional areas of the two wires. For example, 0.5φ for the secondary winding.
The sum of the Bakura cut-off products using the copper wire is 6 Heno2 x πX0.252 = 0-39 (mm2).

同等の断面積を1本の線で得るためにはとなるので0.
7φの銅線が必要になる。ここで第5図に示しだように
高周波電流番導線に流す場合表皮効果のた′め抵抗が大
きくなるので、50)1zの交流の場合には本発−の構
成によれば直流抵抗あように一本の線で2次巻線を構成
すると約1゜17倍の2次巻線抵抗となる。損失4m線
の抵抗に比例するので次式で示すとおり約1.1倍の発
熱量となる。
In order to obtain the same cross-sectional area with one line, it is 0.
A 7φ copper wire is required. As shown in Figure 5, when a high frequency current is passed through a conductor, the resistance increases due to the skin effect, so in the case of an alternating current of 50) 1z, according to the configuration of the present invention, the direct current resistance will increase. If the secondary winding is constructed from one wire, the secondary winding resistance will be approximately 1°17 times as large. Since the loss is proportional to the resistance of the 4m wire, the amount of heat generated is about 1.1 times as shown by the following equation.

1、17/1.07 = 1.09 従って本発明により2次巻線の損美すなわち発熱は10
チ減少することができる。第2図には銅線の損失抵抗の
周波数特性を実測した結果を示す。
1, 17/1.07 = 1.09 Therefore, according to the present invention, the damage or heat generation of the secondary winding is reduced to 10
can be reduced. Figure 2 shows the results of actually measuring the frequency characteristics of the loss resistance of copper wire.

実験に使用したコイルは空心で巻巾10mm’で400
ターン銅線を巻いたものである。第2図に示す通り、周
波数が高い所(10k Hz以上)では銅線の径が0.
3 φよりも0.6φの方(すなわ7へ ち断面積が大きい方)がかえって損失抵抗が大きい。し
たがって、2次巻線の線径を細くすることはそれだけで
損失抵抗を下げるのに効果があるが本実施例のように2
次巻線を2分割することで線径を細くすれば電流密度が
大きくならないので一層損失を下げるのに効果がある。
The coil used in the experiment was air-core with a winding width of 10 mm and a coil width of 400 mm.
It is made of turned copper wire. As shown in Figure 2, at high frequencies (10kHz or higher) the diameter of the copper wire is 0.
The loss resistance of 0.6φ (that is, the one with a larger cross-sectional area of 7 heel) is actually larger than that of 3φ. Therefore, reducing the wire diameter of the secondary winding alone is effective in lowering the loss resistance, but as in this example,
If the wire diameter is made thinner by dividing the next winding into two, the current density will not increase, which is effective in further reducing loss.

損失が少なくなれば発熱量が少なくなるので冷却が容易
になると共にコアや巻線皮膜さらにトランスの絶縁材料
の耐熱性が低いものでも使用ができるようになるため低
コスト化が可能となると共に信頼性が著しく向上し、ト
ランスの効率も良くなる。
Less loss means less heat generation, which makes cooling easier, and allows the use of cores, winding coatings, and transformer insulation materials with low heat resistance, making it possible to lower costs and increase reliability. The performance of the transformer is significantly improved, and the efficiency of the transformer is also improved.

線径を細くするためにはりッツ線を使用する方法も考え
られるが高圧トランスの2次側は巻き数が多いため細い
線を寄り合わせたリッツ線では巻き上げが容易ではない
。しかし、本実施例のように一本づつ別々にコイルを作
る構成にすると一般的な巻線機や既存の生産工程による
方法で作成することが可能である。
One possibility is to use a litz wire to reduce the wire diameter, but since the secondary side of a high-voltage transformer has a large number of turns, it is not easy to wind up a litz wire made of thin wires tied together. However, if the coils are made separately one by one as in this embodiment, it is possible to make them using a general winding machine or a method using an existing production process.

次に本発明の他の実施例を第3図、第4図に示す。第3
図、第4図ともにトランスの断面図であり、第1図と同
じ構成要素は同符号を付しである。
Next, other embodiments of the present invention are shown in FIGS. 3 and 4. Third
Both FIG. 4 and FIG. 4 are cross-sectional views of the transformer, and the same components as in FIG. 1 are given the same reference numerals.

第3図において、2次巻線j3a 、13bは互いに並
列かつ同一極性に接続されており、2次巻線13&の外
側に13hを巻きつける構成となっている。このような
構成であれば、1つの巻線機で、内側の次巻線13aを
巻いた後に続けて外側の2次巻線13bを巻くというこ
とも可能で製造が容易になる。
In FIG. 3, the secondary windings j3a and 13b are connected to each other in parallel and with the same polarity, and 13h is wound around the outside of the secondary winding 13&. With such a configuration, it is possible to wind the inner secondary winding 13a and then the outer secondary winding 13b using one winding machine, which facilitates manufacturing.

第4図において、2次巻線13a、13bの沿面に空間
17を設けた構成となっており、トランスの強制冷却を
行なう場合に風の通りがよく冷却効果が高くなる。周波
数が高くなれば発熱も多くなるので冷却効果の高いトラ
ンスは信頼性の向上のために非常に有効となる。
In FIG. 4, a space 17 is provided along the side surfaces of the secondary windings 13a and 13b, so that when forced cooling of the transformer is performed, the airflow is good and the cooling effect is enhanced. As the frequency increases, the amount of heat generated also increases, so a transformer with a high cooling effect is extremely effective in improving reliability.

以上のように2次巻線の線径を細くするためにリッツ線
を使用するのではなく2つ以上に分割して並列接続する
事で製造と冷却が容易でコンパクトな高周波トランスが
実現できる。
As described above, instead of using a Litz wire to reduce the wire diameter of the secondary winding, a compact high-frequency transformer that is easy to manufacture and cool can be realized by dividing the wire into two or more and connecting them in parallel.

発明の効果 9 ・\−2 以上のように本発明の高周波トランスによれば、次の効
果が得られる。
Effects of the Invention 9 -\-2 As described above, according to the high frequency transformer of the present invention, the following effects can be obtained.

(1)2次巻線の発熱が少なくなるので耐熱グレードの
低い巻線が使用でき低コスト化が可能となる。
(1) Since the secondary winding generates less heat, windings with lower heat resistance grades can be used, making it possible to reduce costs.

(21発熱が少なくなるので巻線の電流密度を従来より
高くでき、小型、低コストのトランスが実現できる。
(21) Since less heat is generated, the current density in the winding can be made higher than before, and a small, low-cost transformer can be realized.

(j 強制冷却を行なうトランスの場合、発熱量が少な
いので簡単な冷却構成とすることができる。
(j) In the case of a transformer that performs forced cooling, the amount of heat generated is small, so a simple cooling configuration can be used.

(4発熱損失を低減できるので、変換効率の高いトラン
スを実現することができる。
(4) Since heat loss can be reduced, a transformer with high conversion efficiency can be realized.

(6発熱が少なくなるのでトランスの絶縁材料の耐熱性
が低いものでよいので低コスト化がはかれる。
(6) Since less heat is generated, the insulating material of the transformer can be made of a material with low heat resistance, resulting in cost reduction.

(6)銅線を一本づつ巻いたコイルを並列に接続する構
成なので製造が容易である。
(6) Manufacture is easy because coils each made of copper wire are connected in parallel.

(7)2次巻線が2つ以上に分割されているので巻線の
表面積が大きくなり冷却効果かたかくなる。
(7) Since the secondary winding is divided into two or more, the surface area of the winding becomes large and the cooling effect becomes stronger.

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

第1図は本発明の第1実施例における高周波ト10=−
。 ランスの断面図、第2図は銅線コイル損失抵抗の周波数
特性図、第3図は本発明の第2実施例における高周波ト
ランスの断面図、第4図は本発明の第3実施例における
高周波トランスの断面図、第5図は従来例における高周
波トランスの断面図、4i46図は銅線の表皮効果によ
る抵抗増加分の周波数特性図である。 8.9・・・・・・コア、12・・・・・・1次巻線、
13&。 13b・・・・・・2次巻線。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名δ、
?−−−コア /2−/炙巷臘 /J(2,/Jb−−−2人巷珠− □ 第1図 第2図 Pl 液炊
FIG. 1 shows the high frequency t10=- in the first embodiment of the present invention.
. 2 is a frequency characteristic diagram of a copper wire coil loss resistance, FIG. 3 is a sectional view of a high frequency transformer in a second embodiment of the present invention, and FIG. 4 is a diagram of a high frequency transformer in a third embodiment of the present invention. FIG. 5 is a cross-sectional view of a high-frequency transformer in a conventional example, and FIG. 4i46 is a frequency characteristic diagram of increased resistance due to the skin effect of copper wire. 8.9...Core, 12...Primary winding,
13&. 13b...Secondary winding. Name of agent: Patent attorney Toshio Nakao and one other person δ,
? ---Core/2-/Burning/J

Claims (2)

【特許請求の範囲】[Claims] (1)コアと、1次巻線と、各々独立して構成された少
なくとも2つの2次巻線とを備え、前記2次巻線は、並
列かつ同一極性に接続する高周波トランス。
(1) A high frequency transformer comprising a core, a primary winding, and at least two secondary windings each configured independently, the secondary windings being connected in parallel and with the same polarity.
(2)2次巻線を平行してコアに配置し、各々の2次巻
線間に空間を設けた特許請求の範囲第1項記載の高周波
トランス。
(2) The high frequency transformer according to claim 1, wherein the secondary windings are arranged in parallel on the core, and a space is provided between each secondary winding.
JP6227586A 1986-03-20 1986-03-20 High-frequency transformer Pending JPS62219605A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6227586A JPS62219605A (en) 1986-03-20 1986-03-20 High-frequency transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6227586A JPS62219605A (en) 1986-03-20 1986-03-20 High-frequency transformer

Publications (1)

Publication Number Publication Date
JPS62219605A true JPS62219605A (en) 1987-09-26

Family

ID=13195428

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6227586A Pending JPS62219605A (en) 1986-03-20 1986-03-20 High-frequency transformer

Country Status (1)

Country Link
JP (1) JPS62219605A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0516415A2 (en) * 1991-05-31 1992-12-02 Kabushiki Kaisha Toshiba Planar transformer
CN104282422A (en) * 2013-07-08 2015-01-14 康舒科技股份有限公司 High-efficiency transformer

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0516415A2 (en) * 1991-05-31 1992-12-02 Kabushiki Kaisha Toshiba Planar transformer
US5430424A (en) * 1991-05-31 1995-07-04 Kabushiki Kaisha Toshiba Planar transformer
CN104282422A (en) * 2013-07-08 2015-01-14 康舒科技股份有限公司 High-efficiency transformer

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