JPS6325487B2 - - Google Patents

Info

Publication number
JPS6325487B2
JPS6325487B2 JP55003538A JP353880A JPS6325487B2 JP S6325487 B2 JPS6325487 B2 JP S6325487B2 JP 55003538 A JP55003538 A JP 55003538A JP 353880 A JP353880 A JP 353880A JP S6325487 B2 JPS6325487 B2 JP S6325487B2
Authority
JP
Japan
Prior art keywords
current
voltage
current transformer
output
measured
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
JP55003538A
Other languages
Japanese (ja)
Other versions
JPS56101726A (en
Inventor
Yoshimi Kurotaki
Kyoshi Nakamura
Yoshiaki Nanba
Tadao Kawai
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 JP353880A priority Critical patent/JPS56101726A/en
Publication of JPS56101726A publication Critical patent/JPS56101726A/en
Publication of JPS6325487B2 publication Critical patent/JPS6325487B2/ja
Granted 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
    • H01F38/20Instruments transformers
    • H01F38/40Instruments transformers for DC

Landscapes

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

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は直流変流器に関するもので、例えば、
直流送電などに用いられる大電流の測定に好適な
直流変流器の改良に係るものである。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a DC current transformer, for example,
This invention relates to the improvement of a DC current transformer suitable for measuring large currents used in DC power transmission.

〔従来の技術〕[Conventional technology]

直流変流器としては、実開昭53−141322号公報
の外、 昭和38年4月20日に第5刷が発行された「磁気
増幅器入門」(宮沢永次郎、穴山武共著、電気書
院)の第2章第12頁に磁気増幅器の基本形が開示
されている。この基本形に整流回路を接続した第
1図に示す直流変流器が知られている。
As for DC current transformers, in addition to Utility Model Application Publication No. 141322/1963, there is also a book called ``Introduction to Magnetic Amplifiers'' (co-authored by Eijiro Miyazawa and Takeshi Anayama, published by Denki Shoin), the fifth edition of which was published on April 20, 1962. Chapter 2, page 12 discloses the basic form of a magnetic amplifier. A DC current transformer shown in FIG. 1 in which a rectifier circuit is connected to this basic type is known.

第1図において、直流変流器100は単相交流
電源200で励振されて直流電流を測定する。直
流変流器100は、2個の鉄心5及び6に貫通す
る一次巻線1,2と、鉄心5,6に巻装された二
次巻線3,4を有する2個のリアクトルを差動で
直列となるように接続し、その二次側回路中に単
相交流電源200と全波整流器7及び負荷抵抗8
を接続することで構成される。このような直流変
流器100は一次巻線に流れる被測定電流±c
による入力起磁力±Fcに対し、その出力電流iL
平均値で見ると第2図のような関係となる。
In FIG. 1, a DC current transformer 100 is excited by a single-phase AC power source 200 to measure DC current. The DC current transformer 100 has two reactors that have primary windings 1 and 2 that pass through two iron cores 5 and 6, and secondary windings 3 and 4 that are wound around the iron cores 5 and 6. are connected in series, and a single-phase AC power supply 200, a full-wave rectifier 7, and a load resistor 8 are connected in the secondary circuit.
It consists of connecting. Such a DC current transformer 100 has a measured current flowing through the primary winding ± c
With respect to the input magnetomotive force ±F c , the output current i L has a relationship as shown in Fig. 2 when viewed as an average value.

すなわち、前記文献の第4章第5頁に述べられ
ているように、被測定電流が予定値以下では、出
力電流が正確に被測定電流に比列するが、被測定
電流が予定値を越えると各半サイクル毎の変流器
作用期間を狭めるように飽和期間が拡大して来る
ので、非線形特性となる。更に、被測定電流が増
大すると、遂には、出力電流は飽和する。
That is, as stated in Chapter 4, page 5 of the above-mentioned document, when the current to be measured is less than the scheduled value, the output current is accurately proportional to the current to be measured, but if the current to be measured exceeds the scheduled value. The saturation period expands so as to narrow the current transformer operating period for each half cycle, resulting in nonlinear characteristics. Furthermore, as the current to be measured increases, the output current finally saturates.

直流電流を精度よく測定するためには、第2図
の比例領域を用いることが望ましく、この比例領
域の中心起磁力±Fc1が、予定の被測定電流の中
心値で得られるように設計することが望ましい。
従つて、予定の被測定電流中心値によつて得られ
る変流器100の出力電源iLはiL1となる。
In order to accurately measure direct current, it is desirable to use the proportional region shown in Figure 2, and the design is such that the central magnetomotive force ±F c1 of this proportional region can be obtained at the center value of the planned current to be measured. This is desirable.
Therefore, the output power i L of the current transformer 100 obtained from the planned center value of the current to be measured is i L1 .

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

ところが、このように設計された変流器100
に、±Fc2の起磁力を与えるような過大電流Icが流
れ込んだとすると、その出力電流iLは、iL2という
数倍の大きさとなつてしまう。
However, the current transformer 100 designed in this way
If an excessive current I c that gives a magnetomotive force of ±F c2 flows into the magnet, the output current i L will be several times as large as i L2 .

このような直流変流器100は、一次巻線に過
大な被測定電流が流れると出力電流iLも過大とな
り、二次巻線が過熱したり、最悪の場合には焼損
する等の問題があつた。
In such a DC current transformer 100, if an excessively large current to be measured flows through the primary winding, the output current iL will also become excessive, causing problems such as overheating of the secondary winding or, in the worst case, burning out. It was hot.

本発明の目的は、従来技術での上記した問題点
を解決し、被測定電流が過大になつても二次巻線
を過熱や焼損等から防止することのできる直流変
流器を提供するにある。
SUMMARY OF THE INVENTION An object of the present invention is to provide a DC current transformer that can solve the above-mentioned problems in the prior art and can prevent the secondary winding from overheating, burning out, etc. even when the current to be measured becomes excessive. be.

〔問題点を解決するための手段〕[Means for solving problems]

本発明の特徴とするところは、直流変流器の交
流電源として、電流が予定値を越えると電圧が急
低下する電流電圧特性をもつ交流電源を備えたこ
とである。
A feature of the present invention is that the AC power source for the DC current transformer is provided with an AC power source having current-voltage characteristics such that the voltage suddenly drops when the current exceeds a predetermined value.

〔作用〕[Effect]

このように構成すれば、被測定電流が予定値を
越えたとき、交流電源電圧の低下によつて、各サ
イクルでの変流器作用期間が狭められ飽和期間が
拡大し、平均出力電流は急減少する。
With this configuration, when the current to be measured exceeds the scheduled value, the current transformer operating period in each cycle is narrowed due to the drop in the AC power supply voltage, the saturation period is expanded, and the average output current is suddenly reduced. Decrease.

この作用は、前記文献の第4,4図が、被測定
(制御)電流の増大を表現しているのに対し、被
測定電流を一定として、交流電源電圧を低下させ
ても、それらの相対的大小関係から、同様の現象
が生じて出力電流の増大が抑制されることは明白
である。
Although Figures 4 and 4 of the above-mentioned document express an increase in the measured (control) current, this effect shows that even if the measured current is held constant and the AC power supply voltage is decreased, the relative It is clear from the magnitude relationship that a similar phenomenon occurs and the increase in output current is suppressed.

〔実施例〕〔Example〕

以下図面により本発明を説明する。 The present invention will be explained below with reference to the drawings.

第3図は、第1図に示したと同様な直流変流器
100の単相交流電源に、第4図に示すような、
電流電圧特性を持つ単相交流電源201を用いた
ものである。いま、単相交流電源201の出力電
流Iと出力電圧Vの特性が第4図のように、単相
交流電源201の出力電流Iがある予定電流I0
なると出力電圧Vが急激に低減するものとする。
このような電流電圧特性を持つ単相交流電源20
1を、直流変流器100の電源に使用した時の変
流器としての入力−出力平均値特性は第5図のよ
うになる。いま、一次巻線の被測定電流Icが増加
して入力起磁力Fcが大きくなると、それに比例し
た変流器の出力電流iLが増加していき、そして入
力起磁力がさらに増加すると出力電流iLも増加す
る。しかし、出力電流iLを供給する単相交流電源
201は予定電流I0以上になると電圧が急低下す
るため、出力電流iLはI0以上に増加することがで
きない。即ち、第6図のa,bは、正常な大きさ
の被測定電流が流れているときの交流電源201
の出力電圧es、二次巻線電流iaおよび負荷抵抗8
の出力電流iL波形である。図は、上側の可飽和リ
アクトルの鉄心5のセツト、リセツト(電圧・時
間積が同一)の様子を示している。時刻t1〜t2
期間が変流器動作(非飽和)期間であり、それ以
外は飽和期間(下側の可飽和リアクトルの変流器
動作期間)である。
FIG. 3 shows a single-phase AC power source of a DC current transformer 100 similar to that shown in FIG.
A single-phase AC power supply 201 having current-voltage characteristics is used. Now, as shown in FIG. 4, when the characteristics of the output current I and output voltage V of the single-phase AC power supply 201 reach a certain scheduled current I0 , the output voltage V suddenly decreases. shall be taken as a thing.
Single-phase AC power supply 20 with such current-voltage characteristics
1 is used as the power source of the DC current transformer 100, the input-output average value characteristic as a current transformer is as shown in FIG. Now, when the measured current I c of the primary winding increases and the input magnetomotive force F c increases, the output current i L of the current transformer increases in proportion to it, and when the input magnetomotive force further increases, the output The current i L also increases. However, since the voltage of the single-phase AC power supply 201 that supplies the output current i L suddenly drops when the current exceeds the scheduled current I 0 , the output current i L cannot increase above I 0 . That is, a and b in FIG. 6 show the AC power supply 201 when a normal magnitude of current to be measured is flowing.
output voltage es, secondary winding current ia and load resistance 8
This is the output current i L waveform. The figure shows how the iron core 5 of the upper saturable reactor is set and reset (the voltage/time product is the same). The period from time t 1 to t 2 is a current transformer operation (non-saturation) period, and the other periods are saturated periods (current transformer operation period of the lower saturable reactor).

同図のc,dには、被測定電流Icが予定値を越
え、これによつて交流電源201の出力電圧esが
低下した様子を示している。期間t2〜t3間で、上
側の可飽和リアクトルの鉄心5が、そのヒステリ
シス特性曲線上でセツトされる量(電圧・時間
積)が小さく、このため、期間t3〜t4の短時間で
鉄心5は飽和してしまう。従つて、変流器作用期
間はt2〜t4までに短縮され、出力電流iLの波高値
が高くなつても、幅が狭まり、平均出力電流は飽
和へ向い、増加しなくなる。
In c and d of the same figure, the current to be measured I c exceeds a predetermined value, and the output voltage es of the AC power supply 201 is thereby reduced. During the period t 2 - t 3 , the amount (voltage-time product) set on the hysteresis characteristic curve of the iron core 5 of the upper saturable reactor is small, and therefore, during the short period t 3 - t 4 The iron core 5 becomes saturated. Therefore, the current transformer operating period is shortened from t2 to t4 , and even if the peak value of the output current iL becomes high, the width becomes narrower, and the average output current tends toward saturation and does not increase.

結局、第5図に示すように、所望の領域では被
測定電流Icに正確に比例し、かつ、予定値を越え
る被測定電流に対しては出力電流iLが増えること
のない直流変流器特性が得られる。
In the end, as shown in Figure 5, the DC transformation is precisely proportional to the current to be measured I c in the desired region, and the output current i L does not increase for the current to be measured that exceeds the planned value. The characteristics of the instrument can be obtained.

この結果、出力電流がI0の時の入力起磁力Fc0
以上の過大な入力起磁力が直流変流器100に与
えられても、出力電流iLは一定値を越えて大きく
なることはなく、直流変流器二次巻線回路には過
大な電流が流れず、巻線過熱や焼損等を防止する
ことができる。
As a result, the input magnetomotive force F c0 when the output current is I 0
Even if the above-mentioned excessive input magnetomotive force is applied to the DC current transformer 100, the output current i L will not increase beyond a certain value, and the excessive current will flow through the DC current transformer secondary winding circuit. It does not flow and can prevent winding overheating and burnout.

本発明は第7図に示す前記実開昭53−141322号
公報に開示されたような回路構成を備えた直流変
流器101の場合にも適用できる。第7図におい
て、直流変流器101は、2個の鉄心15,16
を貫通する一次巻線11,12と、鉄心15,1
6に巻装した二次巻線13,14からなる2個の
リアクトルをダイオード17,18,19,20
で接続し、ダイオード17のカソードとダイオー
ド18のアノード間に制限抵抗21を、またダイ
オード19のカソードとダイオード20のアノー
ド間に負荷抵抗22を接続した閉回路で構成され
ており、そして前記と同様の特性を持つ単相交流
電源201が、ダイオード17のアノードとダイ
オード18のカソードを結んだ点とダイオード1
9のアノードとダイオード20のカソードを結ん
だ点の間に接続される。この時、直流交流器10
1の入力−出力特性は第8図のようになり、この
ような入力−出力特性を有する直流変流器101
の交流電源に第4図のような電流電圧特性を備え
た単相交流電源201を使用した場合、変流器の
入力−出力特性は第9図のようになる。即ち、一
次巻線に流れる被測定電流Icによる入力起磁力Fc
に比例する出力電流iLが、電流I0に達すると電源
電圧が急低下し、前記実施例は同様の原理によ
り、一次巻線に過大な被測定電流が流れても、変
流器の二次巻線回路には過大な電流が流れず、巻
線過熱や焼損等を防止することができる。
The present invention can also be applied to a DC current transformer 101 having a circuit configuration as disclosed in the above-mentioned Japanese Utility Model Application No. 53-141322 as shown in FIG. In FIG. 7, a DC current transformer 101 includes two iron cores 15 and 16.
The primary windings 11 and 12 passing through the cores 15 and 1
Two reactors consisting of secondary windings 13 and 14 wound around diodes 17, 18, 19, 20
It consists of a closed circuit in which a limiting resistor 21 is connected between the cathode of the diode 17 and the anode of the diode 18, and a load resistor 22 is connected between the cathode of the diode 19 and the anode of the diode 20. A single-phase AC power supply 201 having the characteristics of
The diode 20 is connected between the anode of the diode 9 and the cathode of the diode 20. At this time, the DC alternator 10
The input-output characteristics of the DC current transformer 101 having such input-output characteristics are as shown in FIG.
When a single-phase AC power source 201 having current-voltage characteristics as shown in FIG. 4 is used as an AC power source, the input-output characteristics of the current transformer will be as shown in FIG. 9. In other words, the input magnetomotive force F c due to the current to be measured I c flowing through the primary winding
When the output current i L , which is proportional to Excessive current does not flow through the next winding circuit, and winding overheating, burnout, etc. can be prevented.

第10図に電流リミツト特性を持つ単相交流電
源の一実施例回路図を、第11図にその動作説明
用の各部電圧波形図を示す。第10図において、
Esは入力交流電圧、Tr1,Tr2とトランス、SR
は全波整流回路、FL1はインダクタンスL1及
びコンデンサC1よりなる第1のフイルタ、
PWMはパルス幅変調インバータ(DC/ACイン
バータ)、GPSはゲート位相器、FL2はインダク
タンスL2及びコンデンサC2,C3よりなる第
2のフイルタ、C.Tは交流変流器であり、E1〜E4
はそれぞれ図示位置の電圧を示す。交流入力電圧
EsはトランスTr1で変圧され、全波整流回路SR
で全波整流されてE1となり、フイルタFL1で直
流電圧E2に変換される。この直流電圧E2がパル
ス幅変調インバータPWMで矩形波交流電圧E3
変換され、これがフイルタFL2を通過すること
で正弦波交流電圧となり、出力側のトランスTr
2で交流電圧E4となつて出力される。電流リミ
ツタ動作は次のように行なわれる。パルス幅変調
インバータPWMの出力電圧E3は第11図に示す
ように、休止期間を持つた矩形波電圧である。こ
の電圧E3をフイルタFL2で正弦波交流電圧に変
換した時の波高値は、矩形波電圧E3のパルス幅
θによつて変化する。そこで、パルス幅変調イン
バータPWMの出力電圧をフイルタFL2で正弦
波交流電圧に変過した回路の交流電流を交流変流
器C.Tで検出し、この電流値と設定電流値(この
設定電流値が電流上限値となる)とを比較して、
検出電流値の方が設定電流値を越えて大きくなつ
た場合にパルス幅変調インバータPWM用のゲー
ト位相器GPSを絞り込み、第11図のE3′のよう
にパルス幅変調インバータの出力電圧のパルス幅
θ′を小さくする。この矩形波電圧がE3′のように
なることで、フイルタFL2を通過した後の正弦
波交流電圧が減少し、過電流検出と同時に出力電
圧は垂下特性を持つた電流リミツタ機構となる。
FIG. 10 shows a circuit diagram of an embodiment of a single-phase AC power supply having current limit characteristics, and FIG. 11 shows voltage waveform diagrams of various parts for explaining its operation. In Figure 10,
E s is input AC voltage, Tr1, Tr2 and transformer, SR
is a full-wave rectifier circuit, FL1 is a first filter consisting of an inductance L1 and a capacitor C1,
PWM is a pulse width modulation inverter (DC/AC inverter), GPS is a gate phase shifter, FL2 is a second filter consisting of inductance L2 and capacitors C2 and C3, CT is an AC current transformer, and E 1 to E 4
indicate the voltage at the indicated position. AC input voltage
E s is transformed by transformer Tr1, and the full wave rectifier circuit SR
It is full-wave rectified into E 1 and converted into DC voltage E 2 by filter FL1. This DC voltage E 2 is converted into a rectangular wave AC voltage E 3 by the pulse width modulation inverter PWM, which becomes a sine wave AC voltage by passing through the filter FL 2, and is transferred to the output transformer Tr.
2, it is output as AC voltage E4 . The current limiter operation is performed as follows. The output voltage E3 of the pulse width modulation inverter PWM is a rectangular wave voltage with a rest period, as shown in FIG. The peak value when this voltage E 3 is converted into a sinusoidal AC voltage by the filter FL2 changes depending on the pulse width θ of the rectangular wave voltage E 3 . Therefore, the output voltage of the pulse width modulation inverter PWM is converted into a sinusoidal AC voltage by the filter FL2, and the AC current of the circuit is detected by the AC current transformer CT, and this current value and the set current value (this set current value is the current (which is the upper limit value),
When the detected current value exceeds the set current value, the gate phase shifter GPS for the pulse width modulation inverter PWM is narrowed down, and the output voltage pulse of the pulse width modulation inverter is adjusted as shown in E 3 ' in Figure 11. Reduce the width θ'. Since this rectangular wave voltage becomes E 3 ', the sine wave AC voltage after passing through the filter FL2 decreases, and the output voltage becomes a current limiter mechanism having drooping characteristics at the same time as overcurrent is detected.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、直流変流器に過大な被測定電
流が流れた場合にも、二次巻線の過熱や焼損等を
防止することができる。
According to the present invention, even when an excessively large current to be measured flows through a DC current transformer, overheating and burnout of the secondary winding can be prevented.

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

第1図は従来の直流変流器回路図、第2図は第
1図の直流変流器の入力−出力特性図、第3図は
本発明の一実施例による直流変流器の構成図、第
4図は本発明の一実施例に用いる交流電源の電流
−電圧特性図、第5図は第3図に示す本発明の構
成を採用した直流変流器の入力−出力特性図、第
6図は本発明の動作説明図、第7図は本発明の他
の実施例による直流変流器構成図、第8図は第7
図の直流変流器本来の入力−出力特性図、第9図
は第7図の直流変流器に本発明の交流電源を採用
した場合の入力−出力特性図、第10図は本発明
に採用して好適な交流電源の一実施例回路図、第
11図はその動作説明用の各部電圧信号波形図で
ある。 1,2,11,12……一次巻線、3,4,1
3,14……二次巻線、5,6,15,16……
可飽和鉄心、8,22……負荷抵抗、100,1
01……直流変流器、200……交流電源、20
1……電圧急低下特性をもつ交流電源。
Fig. 1 is a conventional DC current transformer circuit diagram, Fig. 2 is an input-output characteristic diagram of the DC current transformer shown in Fig. 1, and Fig. 3 is a configuration diagram of a DC current transformer according to an embodiment of the present invention. , FIG. 4 is a current-voltage characteristic diagram of an AC power supply used in an embodiment of the present invention, FIG. 5 is an input-output characteristic diagram of a DC current transformer adopting the configuration of the present invention shown in FIG. 3, and FIG. 6 is an explanatory diagram of the operation of the present invention, FIG. 7 is a block diagram of a DC current transformer according to another embodiment of the present invention, and FIG.
Figure 9 is an input-output characteristic diagram of the original DC current transformer shown in Figure 7. Figure 9 is an input-output characteristic diagram when the AC power supply of the present invention is used in the DC current transformer of Figure 7. FIG. 11 is a circuit diagram of an embodiment of an AC power supply suitable for use, and is a voltage signal waveform diagram of each part for explaining its operation. 1, 2, 11, 12...Primary winding, 3, 4, 1
3, 14... Secondary winding, 5, 6, 15, 16...
Saturable core, 8, 22...Load resistance, 100, 1
01...DC current transformer, 200...AC power supply, 20
1...An AC power supply with sudden voltage drop characteristics.

Claims (1)

【特許請求の範囲】 1 可飽和鉄心と被測定電流を流す一次巻線およ
び二次巻線とを有する一対の可飽和リアクトル
と、負荷抵抗と、一対の前記二次巻線と前記負荷
抵抗を通る回路中に接続され前記一対の可飽和リ
アクトルの互いに逆位相で交互に変流器作用期間
と飽和期間を持たせる交流電源とを備えた直流変
流器において、 前記交流電源として、電流が予定値を越えると
電圧が急低下する電流電圧特性をもつ交流電源を
備えたことを特徴とする直流変流器。
[Scope of Claims] 1. A pair of saturable reactors having a saturable iron core, a primary winding and a secondary winding through which a current to be measured flows, a load resistor, and a pair of the secondary windings and the load resistor. In a DC current transformer, the AC power source is connected in a circuit through which the pair of saturable reactors alternately have a current transformer operation period and a saturation period in opposite phases to each other. A DC current transformer characterized by being equipped with an AC power source that has current-voltage characteristics that cause the voltage to drop suddenly when the voltage exceeds a certain value.
JP353880A 1980-01-18 1980-01-18 Dc current transformer Granted JPS56101726A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP353880A JPS56101726A (en) 1980-01-18 1980-01-18 Dc current transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP353880A JPS56101726A (en) 1980-01-18 1980-01-18 Dc current transformer

Publications (2)

Publication Number Publication Date
JPS56101726A JPS56101726A (en) 1981-08-14
JPS6325487B2 true JPS6325487B2 (en) 1988-05-25

Family

ID=11560177

Family Applications (1)

Application Number Title Priority Date Filing Date
JP353880A Granted JPS56101726A (en) 1980-01-18 1980-01-18 Dc current transformer

Country Status (1)

Country Link
JP (1) JPS56101726A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0258614U (en) * 1988-10-18 1990-04-26

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0258614U (en) * 1988-10-18 1990-04-26

Also Published As

Publication number Publication date
JPS56101726A (en) 1981-08-14

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