JPS5934614A - Leakage transformer for high frequency - Google Patents

Leakage transformer for high frequency

Info

Publication number
JPS5934614A
JPS5934614A JP57144075A JP14407582A JPS5934614A JP S5934614 A JPS5934614 A JP S5934614A JP 57144075 A JP57144075 A JP 57144075A JP 14407582 A JP14407582 A JP 14407582A JP S5934614 A JPS5934614 A JP S5934614A
Authority
JP
Japan
Prior art keywords
core
shunt
main
winding
high frequency
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
JP57144075A
Other languages
Japanese (ja)
Inventor
Tadashi Mitsui
正 三井
Hiroshi Imaizumi
啓 今泉
Kohei Yuhara
湯原 恒平
Mochikiyo Nobuhara
以清 延原
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.)
Toshiba Electric Equipment Corp
TDK Corp
Toshiba Denzai KK
Original Assignee
Toshiba Electric Equipment Corp
TDK Corp
Toshiba Denzai KK
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 Toshiba Electric Equipment Corp, TDK Corp, Toshiba Denzai KK filed Critical Toshiba Electric Equipment Corp
Priority to JP57144075A priority Critical patent/JPS5934614A/en
Publication of JPS5934614A publication Critical patent/JPS5934614A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F38/00Adaptations of transformers or inductances for specific applications or functions
    • H01F38/08High-leakage transformers or inductances

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Transformers For Measuring Instruments (AREA)

Abstract

PURPOSE:To reduce the eddy-current loss due to leakage flux by a method wherein a primary winding and a secondary winding are provided in parallel with each other with a gap between the main core and said windings, and a shunt core is provided in one body with the intermediate part between the primary and the secondary windings on the main core. CONSTITUTION:A main core consists of U type cores 1-1 and 1-2, and I type core 1-3 which is arranged between each leg part of said U type cores 1-1 and 1-2, and a gap is formed at each butting part of the U type cores 1-1, 1-2 and I type core 1-3. The shunt core 4 is provided in one body with the intermediary part of the primary winding 2 and the secondary winding 3 on the main core 1. As the shunt core 4 is provided at the I type core 1-3 of the main core 1, the number of interlinkage of the leakage flux phi1 flowing the shunt core 4 and the windings 2 and 3 is relatively small.

Description

【発明の詳細な説明】 本発明は高周波インバータの出カドランスなどに用いら
れる高周波用漏れ変圧器に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a high frequency leakage transformer used as an output transformer of a high frequency inverter.

従来、放電灯を高周波点灯するものは多数提案されてお
り、また、このような点灯装置における高周波発生装置
としてインバータを用いるものも多数提案されている。
Conventionally, many devices have been proposed for lighting discharge lamps at high frequencies, and many devices using inverters as high frequency generators in such lighting devices have also been proposed.

このようなインバータの出カドランスとして高周波用漏
れ変圧器が用いられている。すなわち、漏れインダクタ
ンスを放電灯の限流装置として利用しようとするもので
ある。
A high frequency leakage transformer is used as an output transformer of such an inverter. That is, the leakage inductance is used as a current limiting device for a discharge lamp.

そして、従来の高周波用漏れ変圧器はフェライト材から
なる複数個の鉄心を突合わせて主磁路を形成するととも
に、突合わせ部に間隙を形成し、巻線の巻数および前記
間隙長などを調整して所望の漏れインダクタンスを得る
ようにしていた。高周波用漏れ変圧器において、上記の
ようにして漏れインダクタンスを得られるのは、高周波
用であるから必要なインピーダンスを得るだめのインダ
クタンスは商用周波数などに比して非富に小さくてよい
からである。すなわち、巻線の巻数を少なくするかおる
いは間隙長を比、く的大きくすることによって、主イン
ダクタンスに対する漏れインダクタンスを大きくできる
ものである。
In conventional high-frequency leakage transformers, a main magnetic path is formed by butting together multiple iron cores made of ferrite material, and a gap is formed at the butt part to adjust the number of turns of the winding and the length of the gap. to obtain the desired leakage inductance. The reason why leakage inductance can be obtained in the above manner in a high frequency leakage transformer is because it is used for high frequencies, so the inductance needed to obtain the necessary impedance can be extremely small compared to commercial frequencies. . That is, the leakage inductance relative to the main inductance can be increased by reducing the number of turns of the winding or by increasing the gap length.

しかしながら、上述した従来の高周波用漏れ変圧器は電
力損失が多いという問題を有するものであった、すなわ
ち、上述したように漏れインダクタンスを得るために間
隙を比較的大きく形成しているが、この間隙を中心とし
て漏れ磁束が広く分布しておジ、この漏れ磁束が巻線と
鎖交することによってうず電流積を生じるのである。う
す電流積は周波数の2乗に比例するから、商用周波数よ
りはるかに高い101(Hz程度以上の交番磁束が生じ
る高周波用漏れ変圧器においては前記うず゛電流積が極
めて大きくなるのである。このような問題は、上述した
ように主磁路を形成する複数個の鉄心の突合わせ部の間
隙を利用して漏れインダクタンスを得ようとする高周波
用漏れ変圧器特有の問題であって、分路鉄心を設けてな
る商用周波など低周波用の漏れ変圧器においては実質的
に問題とならないものである。
However, the conventional high-frequency leakage transformer described above has a problem of high power loss.In other words, as described above, in order to obtain leakage inductance, a relatively large gap is formed, but this gap The leakage magnetic flux is widely distributed around the winding, and this leakage flux interlinks with the windings, causing an eddy current product. Since the thin current product is proportional to the square of the frequency, the eddy current product becomes extremely large in high frequency leakage transformers where alternating magnetic flux of 101 (Hz or more), which is much higher than the commercial frequency, is generated. As mentioned above, this problem is unique to high-frequency leakage transformers that attempt to obtain leakage inductance by using the gaps between the abutting parts of multiple cores that form the main magnetic path. In a leaky transformer for low frequencies such as commercial frequencies, which is provided with a leakage transformer, there is virtually no problem.

本発明は、上記従来装置の欠点を解消するためになされ
たもので、漏れ磁束によるうす電流積を低減して全体と
しての電力損失を減少できる高周波用漏れ変圧器を提供
することを目的とするものである。
The present invention has been made in order to eliminate the drawbacks of the conventional devices described above, and an object of the present invention is to provide a high frequency leakage transformer that can reduce the product of thin current due to leakage magnetic flux and reduce overall power loss. It is something.

本発明は、所望の漏れインダクタンスを得られながら、
漏れ磁束と巻線との鎖交数を少なくすることを追求して
なされたもので、主磁路を形成する主鉄心に互いに間隙
を有して一次巻線および二次巻線を並設し、前記主鉄心
における前記−次巻線および前記二次巻線の中間部分と
一体的に分路鉄心を設けたことを特徴とするものである
The present invention provides the desired leakage inductance while achieving the desired leakage inductance.
This was done in pursuit of reducing the number of linkages between leakage magnetic flux and the windings, and the primary winding and secondary winding are arranged side by side with a gap between them on the main iron core that forms the main magnetic path. , a shunt core is provided integrally with an intermediate portion of the secondary winding and the secondary winding in the main core.

本発明は、前記分路鉄心を設けたことによって漏れ磁束
を前記分路鉄心を介して通流することができ、しかも、
分路鉄心は主鉄心における一次巻線および二次巻線が巻
装されている部分と一体的に設けられているから、各巻
線と鎖交する漏れ磁束を大幅に減少できるものである。
In the present invention, by providing the shunt core, leakage magnetic flux can be passed through the shunt core, and further,
Since the shunt core is provided integrally with the part of the main core around which the primary and secondary windings are wound, it is possible to significantly reduce the leakage flux interlinking with each winding.

すなわち、一般に巻線は巻装される鉄心側に多く巻回き
れるもものである。たとえば主鉄心が一対のE形鉄心を
突合わせてなる場合を考えると、各E形鉄心の側脚側よ
シ巻線を巻装する中失脚仙に巻線が位置しているもので
ある。したがって、巻線を巻装する主鉄心部分と一体的
に分路鉄心を設けることにより、巻線と鎖交する漏れ磁
束を一層少なくできるのである。ここで、本発明におい
て分路鉄心を設けるのは従来において広く分布していた
漏れ磁束を集中的に通流させるためであって、低周波用
漏れ変圧器が漏れ磁束を生じさせるために分路鉄心を設
けているのとは全く異なるものでおる。なお、従来の高
周波用漏れ変圧器にその′1.1分路鉄心を設けると、
漏れ磁束が多くなりすぎることがあるので、主鉄心にお
ける間隙および分路鉄心の形状などのlij iを必要
とするが、このような調整は当楽者において容易でろろ
う。
That is, in general, the winding can be wound in large numbers on the side of the core to be wound. For example, if the main core is made up of a pair of E-shaped cores butted against each other, the windings are located on the side legs of each E-shaped core where the windings are wound. Therefore, by providing a shunt core integrally with the main core portion around which the windings are wound, leakage magnetic flux interlinking with the windings can be further reduced. Here, the reason why the shunt iron core is provided in the present invention is to make the leakage magnetic flux, which was widely distributed in the past, flow in a concentrated manner. This is completely different from having an iron core. In addition, if the '1.1 shunt core is installed in a conventional high frequency leakage transformer,
Since the leakage flux may become too large, it is necessary to adjust the gap in the main core and the shape of the shunt core, but such adjustments will be easy for the musician.

不発明において、高周波とは10KHz以上である。In the invention, high frequency is 10 KHz or higher.

また、不発明において主鉄心および分路鉄心としてフェ
ノイト、rモルファスlどからなる鉄心を用いるCとか
でさる。しかし、けい素鋼板のようにl0KI(z以上
の高周波で用いるとtL電力損失増大するものは避ける
べきである。−また、主鉄心および分路鉄心のル状は任
意であろうたとえば主鉄心として一対の1」形鉄心と、
これら口形鉄心の各脚部間に挟持された工形鉄心とで侮
成されるものを用いることができる。さらに、分路鉄心
と主鉄心の一部とは一体成形されていてもよいものであ
る。この場合、組nてか容易であるとともに、主鉄心1
分路鉄心および巻線の位置関係の積度を高くすることが
できる。
Further, in the non-invention, iron cores made of phenoite, r-morphous l, etc. are used as the main iron core and the shunt iron core. However, silicon steel sheets, which increase tL power loss when used at high frequencies of 10KI (z or higher), should be avoided. - Also, the shape of the main core and shunt core may be arbitrary. a pair of 1” iron cores;
It is possible to use a molded iron core which is made up of a rounded iron core held between the legs of the necked iron core. Furthermore, the shunt core and a portion of the main core may be integrally formed. In this case, it is easy to assemble, and the main core 1
It is possible to increase the degree of integration of the positional relationship between the shunt core and the winding.

さらに、本発明は放電灯を負荷とするインノζ−タの出
カドランスとして用いることができる。この場合、漏れ
インダクタンスを前記放′市灯の限流装置として利用で
さるものである。しかし、本発明の用途は前記のものに
限られるもので4よない。
Furthermore, the present invention can be used as an output transformer for an inverter whose load is a discharge lamp. In this case, the leakage inductance is used as a current limiting device for the public market lamp. However, the uses of the present invention are not limited to the above-mentioned ones.

以下、本発明の一実施例を第1図〜第3図を参照して説
明する。(1)は主鉄心で、複数個たとえば3個の鉄心
を突合わせて悔成され主磁路を形成するものである。す
なわち、本実施例において一対のLl形鉄心(1−旬、
 (1−2)と、これら1−」形鉄心(1−1)。
Hereinafter, one embodiment of the present invention will be described with reference to FIGS. 1 to 3. (1) is the main core, which is made by butting together a plurality of cores, for example three cores, to form a main magnetic path. That is, in this embodiment, a pair of Ll type iron cores (1-1,
(1-2) and these 1-'' type cores (1-1).

(1−2)の各脚部間に配置された■形鉄心(1−)と
からなる。これらL」形鉄心(1−1)、 (]、−2
)、[形鉄心(1−3)の各突合わせ部に間隙を形成し
ている。
It consists of a ■-shaped iron core (1-) placed between each leg of (1-2). These L” shaped cores (1-1), (], -2
), [A gap is formed at each abutting portion of the shaped iron core (1-3).

これら間隙には周知のスベーダを介在させることができ
る。t2) 、 (3)は−次巻線および二次巻線で、
前記主鉄心(1)の■形鉄心(1−3)に互に間隔を有
して並設されているものである。(4)は分路鉄心で、
前記主鉄心(1)ICおける前記−次巻線(2)および
二次巻線(3)の中間部分と一体的に設けられているも
のでめる。すなわち、本実施例において前記■形鉄心の
中間部分に設けられている。この分路鉄心(4)は主鉄
心(1)の■形鉄心(1−3)と一体成杉されていても
よい。あるいは実質的に漏れ(B′1束を生じないよう
な間隙を有L2て設けら力、ていてもよい。
A well-known subedator can be interposed in these gaps. t2), (3) is the -order winding and the secondary winding,
The square iron cores (1-3) of the main iron core (1) are arranged in parallel with each other at intervals. (4) is the shunt core,
The main iron core (1) is provided integrally with an intermediate portion of the secondary winding (2) and the secondary winding (3) in the IC. That is, in this embodiment, it is provided at the middle portion of the ■-shaped iron core. This shunt core (4) may be made of cedar integrally with the ■-shaped core (1-3) of the main core (1). Alternatively, a gap L2 may be provided that does not substantially cause leakage (B'1 bundle).

つき゛に作用」を述べる。分路鉄心(4)が上b12の
ような関係で主鉄心(1)のI形鉄心(1−3)に設け
られているから、この分路鉄心(4)を通流する漏れ磁
束(為)と巷、腺(2)、(3)との鎖交数は相対的に
少ない。
It is said that it has a unique effect. Since the shunt core (4) is installed on the I-type core (1-3) of the main core (1) in the relationship shown in b12 above, the leakage magnetic flux (because of the leakage magnetic flux flowing through this shunt core (4) ), and the number of linkages between glands (2) and (3) is relatively small.

すなわち、第3図および第4図を参照して述べると、第
4図のように分路鉄心(4)を巻線(2)、 (3)が
巻装されていないtlfliの主鉄心(j−1’)に設
けた場合、分路鉄心前を通ωLしたθζ[iれ脩果(z
2)と巻線(4)、(j)との鎖交数は第3図のものよ
り多くなる。これは、巻線が巻装される鉄心11i!+
に偏位しでいるため、分路鉄心L4) 、 (Jに同じ
踊れ磁束(為)、(メ2)が通流しても巻線との鎖交数
が異なるのである。
That is, referring to FIGS. 3 and 4, as shown in FIG. 4, the shunt core (4) is connected to the tlfli main core (j -1'), the output (z
2) and the windings (4) and (j), the number of interlinkages is greater than that in FIG. This is the iron core 11i on which the winding is wound! +
Therefore, even if the same magnetic flux (for) and (me2) flows through the shunt core L4) and (J), the number of linkages with the winding will be different.

上記実施例のものを第5図示のトランジスタインバータ
(in)の出力トジンス(T)としてハ」いることがで
きる。第5図において(Fl、)は負荷としての放電灯
である。第5図のトランジスタインバータ(In)の回
路栴成そのものは周知であるので説明を省略する。なお
、第5図示のものにおいて(Wb)はベース巻装てるる
か、このヘース巻線(sb)は第1図のものにおいて入
力巻線(2)の上層に巻回することができる一、また、
第5図中(N f )はフィラメント巻線であるが、こ
のものは第1図のものにおいてのものに適用した場合の
漏れ変圧器における重力損失の実測値を示す。
The above embodiment can be used as the output voltage (T) of the transistor inverter (in) shown in FIG. In FIG. 5, (Fl,) is a discharge lamp as a load. Since the circuit structure of the transistor inverter (In) shown in FIG. 5 is well known, its explanation will be omitted. In the case shown in Fig. 5, (Wb) can be wound on the base, or this Heess winding (sb) can be wound on the upper layer of the input winding (2) in the case shown in Fig. 1. Also,
In FIG. 5, (N f ) is a filament winding, which shows the actual measured value of gravity loss in a leaky transformer when applied to the one in FIG. 1.

主鉄心材料=フエライ) 製H7C3 (東京電気化学工業抹式会社製) 主鉄心外形寸法:40(楠×58(横×230!7) 
 (−m’)周波数: 40Kl−12 負荷: 110wけい光ランプ2灯直列入力巻線(よシ
線:直径0.08mmX60本)数σ)/出力巻線(よ
シ纒:直径0.12#X 20本)敬σ)ニア4/99
巻線と主鉄心(1−3)または<1−3’)間の距離:
約1mm巻線と主鉄心(1−t)または(1−、’)間
の距離:約3關分路鉄心(4) tたは(4)主鉄心と
の間隙長:2wn第6図および第7図は本発明の他の実
施例な示すものである。本実施例において主鉄心(kG
は一対のE形鉄心(10−1)、 (10−2)とから
なシ、一方のE形鉄心(10−1)の各側脚は中央脚よ
シ短く形成されている。そして、これらE形鉄心(10
−1)、 (10−2)の中央脚の接合部に分路鉄心Q
υ、(1υを接着などによシ固定してなるものである。
Main core material = Ferrai) H7C3 (manufactured by Tokyo Denki Kagaku Kogyo Machishiki Company) Main core external dimensions: 40 (campus x 58 (width x 230!7)
(-m') Frequency: 40Kl-12 Load: 2 110W fluorescent lamps Series input winding (width wire: diameter 0.08 mm x 60 wires) number σ) / output winding (width wire: diameter 0.12#) X 20 pieces) σ) Near 4/99
Distance between winding and main core (1-3) or <1-3':
Approximately 1 mm Distance between winding and main core (1-t) or (1-,'): Approximately 3 Shunt core (4) t or (4) Gap length with main core: 2wn Figure 6 and FIG. 7 shows another embodiment of the invention. In this example, the main iron core (kG
consists of a pair of E-shaped cores (10-1) and (10-2), and each side leg of one E-shaped core (10-1) is formed shorter than the central leg. And these E type iron cores (10
-1), (10-2) at the joint of the central leg with shunt core Q
υ, (1υ) is fixed by adhesive etc.

その他、第1の実施例と同じ部分には同じ符号を付しで
ある。本実施例の作用は第1の実施例と同様であるので
説明を省略する。
Other parts that are the same as those in the first embodiment are given the same reference numerals. The operation of this embodiment is similar to that of the first embodiment, so the explanation will be omitted.

第8図は本発明のさらに他の実施例を示すものである。FIG. 8 shows still another embodiment of the present invention.

本実施例はいわゆる内鉄形のもので、主鉄心(至)は工
形およびl形鉄心(20−1)、 <2O−2)を突合
わせてなるものでbる。分路鉄心(2])は上記のもの
と同様な関係に設けられている。本実施例においても第
1図と同じ部分に同じ符号を付すとともに、作用も第1
図のものと同様であるので説明を省略する。
The present embodiment is of the so-called internal iron type, and the main iron core (to) is formed by butting together the core type and the l-shaped iron core (20-1), <2O-2). The shunt core (2]) is provided in a similar relationship to that described above. In this embodiment as well, the same parts as in FIG.
Since it is the same as that shown in the figure, the explanation will be omitted.

以上詳述したように本発明は、主磁路を形成する主鉄心
に一次巻線および二次巻線を互いに間隔を有して並設し
、前記主鉄心における前記−次巻線および前記二次巻線
の中間部分と一体的に分路鉄心を設けたから、巻線と鎖
交する漏れ磁束を大幅に低減できて、前記漏れ磁束によ
るうず竜流損を減少でき、もって全体として′重力損失
が少ない高周波用漏れ変圧器を提供できるものである。
As described in detail above, the present invention provides a primary winding and a secondary winding that are arranged side by side with a space between them on a main core that forms a main magnetic path, and the secondary winding and the secondary winding on the main core. Since the shunt core is provided integrally with the middle part of the next winding, the leakage magnetic flux interlinking with the winding can be significantly reduced, and the eddy current loss due to the leakage magnetic flux can be reduced, resulting in the overall 'gravitational loss'. Therefore, it is possible to provide a high frequency leakage transformer with less leakage.

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

第1図は本発明の一実施例を示す一部断面正面図、第2
図は同じく鉄心を示す斜視図、第3図は第1図の一部を
拡大して示す図、第4図は本発明の作用を示すために第
3図と対応させて示す図、第5図は本発明の一適用でお
るトランジスタインバータを示す回路図、第6図は本発
明の他の実施例を示す一部断面正面図、第7図は同じく
鉄心を示す斜視図、第8図は本発明のさらに他の実施例
を示す一部断面正面図である。 (1)、(LQ)、四・・・主鉄心、(2)・・・−次
巻線、(3)・・・二次巻線、(4)、Qυ、 (21
>・・・分路鉄心、特許出願人 東京電気化学工業株式
会社東芝電材株式会社 A′1   目 才 ・、p(A’  4  (イ) 才 夕 閃 b 才   乙   ?1
FIG. 1 is a partially sectional front view showing one embodiment of the present invention, and FIG.
3 is a perspective view showing the iron core, FIG. 3 is an enlarged view of a part of FIG. 1, FIG. 4 is a view corresponding to FIG. Figure 6 is a circuit diagram showing a transistor inverter to which the present invention is applied, Figure 6 is a partially sectional front view showing another embodiment of the present invention, Figure 7 is a perspective view also showing the iron core, and Figure 8 is FIG. 7 is a partially sectional front view showing still another embodiment of the present invention. (1), (LQ), 4...Main core, (2)...-Next winding, (3)...Secondary winding, (4), Qυ, (21
>...Shunt core, patent applicant Tokyo Denki Kagaku Kogyo Co., Ltd. Toshiba Electric Materials Co., Ltd.

Claims (4)

【特許請求の範囲】[Claims] (1)  複数個の鉄心を突合わせて構成され主磁路を
形成した主鉄心と; この主鉄心に間隔を有して並設された一次巻線および二
次巻線と; 上記主鉄心における上記−次巻線および」二記二次巻線
の中間部分と一体的に設けられた分路鉄心と; を具備したことを特徴とする高周波用漏れ変圧器。
(1) A main core formed by butting together a plurality of cores to form a main magnetic path; A primary winding and a secondary winding arranged in parallel on this main core at intervals; A high frequency leakage transformer comprising: a shunt core integrally provided with an intermediate portion of the secondary winding and the secondary winding.
(2)前記分路鉄心は前記鉄心の一部と一体成形された
ものであることを特徴とする特許請求の範囲(1)記載
の高周波用漏れ変圧器。
(2) The high frequency leakage transformer according to claim (1), wherein the shunt core is integrally formed with a part of the core.
(3)  前記主鉄心は一対の1」形鉄心と、これら1
」形鉄心の脚部間に配置された工形鉄心とからなり、前
記分路鉄心は上記工形鉄心の中間部に設けられているも
のであることを特徴とする特許請求の範囲(1)または
(2)記載の高周波用漏れ変圧器。
(3) The main core has a pair of 1" type cores, and these 1
Claim (1) characterized in that the shunt core is provided at an intermediate portion of the shaped iron core, and the shunt core is disposed between the legs of the shaped iron core. Or the high frequency leakage transformer described in (2).
(4)前記主鉄心および前記分路鉄心はフェライト材か
らなるものであることを特徴とする特許請求の範囲(1
)〜(3)のいずれか一記載の高周波用漏れ変圧器。
(4) Claim (1) characterized in that the main iron core and the shunt iron core are made of ferrite material.
The high frequency leakage transformer according to any one of ) to (3).
JP57144075A 1982-08-20 1982-08-20 Leakage transformer for high frequency Pending JPS5934614A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57144075A JPS5934614A (en) 1982-08-20 1982-08-20 Leakage transformer for high frequency

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57144075A JPS5934614A (en) 1982-08-20 1982-08-20 Leakage transformer for high frequency

Publications (1)

Publication Number Publication Date
JPS5934614A true JPS5934614A (en) 1984-02-25

Family

ID=15353689

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57144075A Pending JPS5934614A (en) 1982-08-20 1982-08-20 Leakage transformer for high frequency

Country Status (1)

Country Link
JP (1) JPS5934614A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63182519U (en) * 1987-05-19 1988-11-24
CN108899182A (en) * 2018-04-15 2018-11-27 珠海市富源电子有限公司 High voltage short circuit protects transformer

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS55110017A (en) * 1979-02-15 1980-08-25 Matsushita Electric Works Ltd Electromagnetic unit

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS55110017A (en) * 1979-02-15 1980-08-25 Matsushita Electric Works Ltd Electromagnetic unit

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63182519U (en) * 1987-05-19 1988-11-24
CN108899182A (en) * 2018-04-15 2018-11-27 珠海市富源电子有限公司 High voltage short circuit protects transformer
CN108899182B (en) * 2018-04-15 2021-01-05 珠海市富源电子有限公司 High-voltage short-circuit protection transformer

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