Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPH0213806B2 - - Google Patents
[go: Go Back, main page]

JPH0213806B2 - - Google Patents

Info

Publication number
JPH0213806B2
JPH0213806B2 JP57066915A JP6691582A JPH0213806B2 JP H0213806 B2 JPH0213806 B2 JP H0213806B2 JP 57066915 A JP57066915 A JP 57066915A JP 6691582 A JP6691582 A JP 6691582A JP H0213806 B2 JPH0213806 B2 JP H0213806B2
Authority
JP
Japan
Prior art keywords
impedance
transformer
iron core
impedance adjustment
increases
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 - Lifetime
Application number
JP57066915A
Other languages
Japanese (ja)
Other versions
JPS58182809A (en
Inventor
Seiji Oku
Hiroshi Yamaguchi
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.)
Kansai Electric Power Co Inc
Daihen Corp
Original Assignee
Daihen Corp
Kansai Denryoku 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 Daihen Corp, Kansai Denryoku KK filed Critical Daihen Corp
Priority to JP57066915A priority Critical patent/JPS58182809A/en
Publication of JPS58182809A publication Critical patent/JPS58182809A/en
Publication of JPH0213806B2 publication Critical patent/JPH0213806B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F27/00Details of transformers or inductances, in general
    • H01F27/34Special means for preventing or reducing unwanted electric or magnetic effects, e.g. no-load losses, reactive currents, harmonics, oscillations, leakage fields
    • H01F27/38Auxiliary core members; Auxiliary coils or windings

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Coils Of Transformers For General Uses (AREA)
  • Regulation Of General Use Transformers (AREA)

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、高調波に対するインピーダンスを従
来より低くして、出力電圧波形に生じる歪を少な
くすることができるようにした高調波低インピー
ダンス変圧器に関するものである。
[Detailed Description of the Invention] [Industrial Application Field] The present invention provides a harmonic low impedance transformer that has lower impedance to harmonics than conventional ones and can reduce distortion occurring in the output voltage waveform. It is related to.

[従来技術及び発明が解決しようとする課題] 最近、サイリスタによりスイツチ制御される負
荷が多くなつてきている。そのため負荷に給電し
ている変圧器には大きな高調波電流が流れて大き
な電圧降下が生じ、この高調波電流による電圧降
下が変圧器の出力電圧波形を大きく歪ませる。変
圧器の出力電圧波形が歪むと、負荷側に接続され
た進相用コンデンサ、制御機器等に悪影響が及ん
で給電される電力の質が低下するだけでなく、高
調波の発生源でない負荷(電力需要家)にもその
影響が波及して電力供給上好ましくない状態とな
る。
[Prior Art and Problems to be Solved by the Invention] Recently, more and more loads have been controlled by switches using thyristors. Therefore, a large harmonic current flows through the transformer supplying power to the load, causing a large voltage drop, and the voltage drop due to this harmonic current greatly distorts the output voltage waveform of the transformer. If the output voltage waveform of the transformer is distorted, it not only adversely affects the phase advancing capacitors and control equipment connected to the load side, reducing the quality of the supplied power, but also harming the load (which is not the source of harmonics). The impact also spreads to electricity consumers (power consumers), creating an unfavorable situation in terms of power supply.

第1図は、従来の変圧器の簡略化した等価回路
を示したもので、この等価回路において抵抗を
R、インダクタンスをL、角周波数をωとする
と、変圧器のインピーダンスZ〓は、Z〓=R+jωLと
なる。
Figure 1 shows a simplified equivalent circuit of a conventional transformer. In this equivalent circuit, if resistance is R, inductance is L, and angular frequency is ω, the impedance Z〓 of the transformer is Z〓 =R+jωL.

上記の変圧器に交流電流I〓が流れた場合の電圧
降下E〓Tは、E〓T=I〓(R+jωL)となり、この電圧

下E〓Tは周波数の増加に伴つて増加していく。従
つて負荷電流に高調波成分が含まれていると該高
調波電流により大きな電圧降下E〓Tが生じ、この
電圧降下により出力電圧に歪みが生じる。この歪
みは負荷電流に含まれている高調波の次数が高く
なる程増大する。
The voltage drop E〓 T when an alternating current I〓 flows through the above transformer is E〓 T = I〓 (R + jωL), and this voltage drop E〓 T increases as the frequency increases. Therefore, if the load current contains a harmonic component, the harmonic current causes a large voltage drop ET , and this voltage drop causes distortion in the output voltage. This distortion increases as the order of harmonics included in the load current increases.

本発明の目的は、高調波に対する変圧器のイン
ピーダンスを従来よりも低くすることにより高調
波電流による電圧降下を抑制して出力電圧波形の
歪を抑えることができるようにした高調波低イン
ピーダンス変圧器を提供することにある。
An object of the present invention is to provide a harmonic low impedance transformer that is capable of suppressing voltage drop due to harmonic current and suppressing distortion of the output voltage waveform by lowering the impedance of the transformer relative to harmonics than before. Our goal is to provide the following.

[課題を解決するための手段] 本発明においては、上記の目的を達成するた
め、インピーダンス調節用鉄心と該インピーダン
ス調節用鉄心を囲むように設けられたインピーダ
ンス調節用閉回路とを備えたインピーダンス調節
装置を1次巻線と2次巻線との間に配設した。
[Means for Solving the Problem] In order to achieve the above object, the present invention provides an impedance adjustment comprising an impedance adjustment iron core and an impedance adjustment closed circuit provided so as to surround the impedance adjustment iron core. The device was placed between the primary and secondary windings.

上記インピーダンス調節用閉回路は、インピー
ダンス調節用鉄心を囲むように設けられて両端が
電気的に接続された短絡導体により構成したり、
インピーダンス調節用鉄心を囲むように設けられ
た導体と該導体の両端間に接続されたコンデンサ
とにより構成したりすることができる。
The closed circuit for impedance adjustment is constituted by a short-circuited conductor that is provided to surround the iron core for impedance adjustment and is electrically connected at both ends,
It can be constructed by a conductor provided so as to surround the impedance adjusting iron core and a capacitor connected between both ends of the conductor.

[作 用] 上記のようにインピーダンス調節用鉄心と、該
鉄心を囲むインピーダンス調節用閉回路とを備え
たインピーダンス調節装置を1次巻線と2次巻線
との間に配設すると、インピーダンス調節用鉄心
の存在により1次巻線と2次巻線との間の間隙を
磁束が通り易くなるため、1次巻線と2次巻線と
の間を流れる漏洩磁束が増加し、この漏洩磁束の
増加が変圧器のインピーダンスを増大させる方向
に働く。
[Function] When an impedance adjustment device including an impedance adjustment iron core and an impedance adjustment closed circuit surrounding the iron core is disposed between the primary winding and the secondary winding as described above, impedance adjustment is performed. The presence of the iron core makes it easier for magnetic flux to pass through the gap between the primary and secondary windings, increasing the leakage magnetic flux flowing between the primary and secondary windings. This increases the impedance of the transformer.

また上記インピーダンス調節用鉄心に漏洩磁束
が流れると、該鉄心を囲むように設けられている
閉回路に電圧が誘起して該閉回路に電流が流れ、
この電流によりインピーダンス調節用鉄心に漏洩
磁束が入るのを妨げるように働く反発磁界が生じ
る。周波数が低い領域では、閉回路を流れる電流
が小さく、反発磁界が小さいため、インピーダン
ス調節用鉄心を多くの漏洩磁束が通るが、周波数
が高くなつていくと、閉回路を流れる電流が増大
していつて、反発磁界が次第に大きくなつていく
ため、インピーダンス調節用鉄心に流れ込む漏洩
磁束が少なくなつていく。従つて変圧器のインピ
ーダンスは周波数の上昇に伴つて増加していく
が、その増加割合は周波数の上昇に伴つて次第に
小さくなつていく。
Furthermore, when leakage magnetic flux flows through the impedance adjusting iron core, a voltage is induced in a closed circuit provided so as to surround the iron core, and a current flows through the closed circuit.
This current generates a repulsive magnetic field that acts to prevent leakage magnetic flux from entering the impedance adjusting iron core. In the low frequency range, the current flowing through the closed circuit is small and the repulsive magnetic field is small, so a lot of leakage magnetic flux passes through the impedance adjustment iron core, but as the frequency increases, the current flowing through the closed circuit increases. As the repulsion magnetic field gradually increases, the leakage magnetic flux flowing into the impedance adjusting iron core decreases. Therefore, the impedance of the transformer increases as the frequency increases, but the rate of increase gradually decreases as the frequency increases.

このように、本発明によれば、周波数が高くな
るにしたがつて変圧器のインピーダンスの増加割
合を小さくすることができるため、基本周波数
(例えば商用周波数)における変圧器インピーダ
ンスを従来のものと同じにするように設計した場
合、高調波成分に対する変圧器インピーダンスを
従来のものより低く抑えることができる。従つて
負荷電流の高調波成分による変圧器での電圧降下
を低く抑えることができ、その出力電圧の歪みを
抑制することができる。
As described above, according to the present invention, it is possible to reduce the rate of increase in the impedance of the transformer as the frequency increases, so that the impedance of the transformer at the fundamental frequency (for example, commercial frequency) can be kept the same as that of the conventional one. When designed to do so, the transformer impedance to harmonic components can be suppressed lower than that of conventional transformers. Therefore, the voltage drop in the transformer due to harmonic components of the load current can be suppressed to a low level, and the distortion of the output voltage can be suppressed.

[実施例] 以下図面を参照して本発明の実施例を詳細に説
明する。
[Examples] Examples of the present invention will be described in detail below with reference to the drawings.

第2図は、本発明の一実施例の平面図であつ
て、同図において1は脚部1a,1bと継鉄部1
c,1cとを有する環状の鉄心、2は鉄心1の脚
部1a,1bにそれぞれ巻回された2次巻線、3
は2次巻線2の外側に、該2次巻線と同心的に巻
回された1次巻線である。4は2次巻線2と1次
巻線3との間に配設された波形ダクトスペーサ
で、このダクトスペーサにより両巻線間に冷却用
のダクトが形成されている。
FIG. 2 is a plan view of one embodiment of the present invention, in which 1 indicates leg portions 1a, 1b and yoke portion 1.
2 is a secondary winding wound around the legs 1a and 1b of the core 1, respectively;
is a primary winding wound concentrically with the secondary winding 2 outside the secondary winding 2. Reference numeral 4 denotes a wave-shaped duct spacer disposed between the secondary winding 2 and the primary winding 3, and this duct spacer forms a cooling duct between both windings.

5は2次巻線2と1次巻線3との間に挿入され
たインピーダンス調節装置である。このインピー
ダンス調節装置は2個設けられて、両インピーダ
ンス調節装置5,5が、鉄心1を間にして継鉄部
1cの長さ方向に相対向するような位置関係にし
て配設されている。
5 is an impedance adjustment device inserted between the secondary winding 2 and the primary winding 3. Two impedance adjusting devices are provided, and both impedance adjusting devices 5, 5 are arranged in a positional relationship such that they face each other in the length direction of the yoke portion 1c with the iron core 1 in between.

各インピーダンス調節装置5の長さ寸法(第2
図において紙面と直角な方向の寸法)は、1次巻
線3または2次巻線の軸長寸法に略等しく設定さ
れ、各インピーダンス調節装置5の両端部が1次
及び2次巻線の端部を略面一の状態で配置され
て、両巻線の少なくとも一方に固定されている。
Length dimension of each impedance adjustment device 5 (second
(in the figure, the dimension perpendicular to the plane of the paper) is set approximately equal to the axial length dimension of the primary winding 3 or the secondary winding, and both ends of each impedance adjustment device 5 are the ends of the primary and secondary windings. The windings are fixed to at least one of the two windings with their parts substantially flush with each other.

第3図及び第4図を参照すると、上記インピー
ダンス調節装置5の一例が示してあり、第3図は
正面図、第4図は第3図のA―A線断面図ある。
Referring to FIGS. 3 and 4, an example of the impedance adjustment device 5 is shown, with FIG. 3 being a front view and FIG. 4 being a sectional view taken along the line AA in FIG. 3.

インピーダンス調節装置5は、巻線の軸長寸法
に略等しい長さlと適宜の幅寸法dとを有する短
冊状のけい素鋼板を複数枚(通常は4〜5枚)積
層したインピーダンス調節用鉄心5aと、このイ
ンピーダンス調節用鉄心5aを囲むように設けて
両端を電気的に接続した短絡導体5bとからなつ
ており、短絡導体5bにより鉄心5aを囲むイン
ピーダンス調節用閉回路が構成されている。
The impedance adjustment device 5 includes an impedance adjustment iron core made by laminating a plurality of rectangular silicon steel plates (usually 4 to 5 pieces) each having a length l approximately equal to the axial length of the winding and an appropriate width d. 5a, and a short-circuiting conductor 5b provided so as to surround the impedance-adjusting iron core 5a and having both ends electrically connected, and the short-circuiting conductor 5b constitutes an impedance-adjusting closed circuit surrounding the iron core 5a.

短絡導体5bは、インピーダンス調節用鉄心5
aの長さlよりやや短い幅寸法l′を有する銅板
を、インピーダンス調節用鉄心5aを囲むように
成形してその両端を接合することにより形成さ
れ、鉄心5aと短絡導体5bとは互いに離反しな
いように接着または溶着等により一体化されてい
る。
The shorting conductor 5b is the impedance adjusting iron core 5.
It is formed by molding a copper plate having a width l' slightly shorter than the length l of a so as to surround the impedance adjusting iron core 5a and joining both ends thereof, so that the iron core 5a and the shorting conductor 5b are not separated from each other. They are integrated by gluing or welding, etc.

上記のように構成した本発明の高調波低インピ
ーダンス変圧器では、1次巻線3と2次巻線2と
の間にインピーダンス調節用鉄心5aと配設した
ことにより両巻線間を流れる漏洩磁束が従来より
も増加し、この漏洩磁束の増加が変圧器インピー
ダンスを増加させるように働く。一方鉄心5aに
漏洩磁束が流れると、短絡導体5b(インピーダ
ンス調節用閉回路)に誘起電圧が生じ、該誘起電
圧により短絡導体5bに短絡電流が流れる。この
短絡電流により、鉄心5aに漏洩磁束が入るのを
妨げる反発磁界が生じる。この場合、短絡導体5
bに誘起される電圧eは、e=k(dφ/dt)(但
しkは定数、φは漏洩磁束、tは時間)であり、
この誘起電圧eは周波数の増加に伴つて、即ち高
調波の次数が高くなるに従つて大きくなる。従つ
て反発磁界は、周波数が高くなるに従つて強くな
つていく。
In the harmonic low impedance transformer of the present invention configured as described above, since the impedance adjusting iron core 5a is disposed between the primary winding 3 and the secondary winding 2, leakage flowing between the two windings can be prevented. The magnetic flux increases compared to before, and this increase in leakage magnetic flux acts to increase the transformer impedance. On the other hand, when leakage magnetic flux flows through the iron core 5a, an induced voltage is generated in the short-circuit conductor 5b (closed circuit for adjusting impedance), and a short-circuit current flows through the short-circuit conductor 5b due to the induced voltage. This short-circuit current generates a repulsive magnetic field that prevents leakage magnetic flux from entering the iron core 5a. In this case, the short circuit conductor 5
The voltage e induced in b is e=k(dφ/dt) (where k is a constant, φ is leakage magnetic flux, and t is time),
This induced voltage e increases as the frequency increases, that is, as the harmonic order increases. Therefore, the repulsive magnetic field becomes stronger as the frequency becomes higher.

周波数が低い間は、反発磁界が弱いため、イン
ピーダンス調節用鉄心5aを通して多くの漏洩磁
束が流れるが、周波数が高くなつて反発磁界が強
くなるとインピーダンス調節用鉄心に流れる漏洩
磁束は少なくなる。
While the frequency is low, the repulsion magnetic field is weak, so much leakage magnetic flux flows through the impedance adjustment iron core 5a, but as the frequency increases and the repulsion magnetic field becomes stronger, the leakage magnetic flux flowing through the impedance adjustment iron core decreases.

変圧器のインピーダンスは周波数の上昇に伴つ
て増加していくが、周波数の上昇に伴つて反発磁
界が強くなつていき、鉄心5aに流れ込む漏洩磁
束が少なくなつていくと、変圧器インピーダンス
の増加割合は次第に小さくなる。
The impedance of the transformer increases as the frequency increases, but as the repulsive magnetic field becomes stronger and the leakage magnetic flux flowing into the iron core 5a decreases, the rate of increase in the transformer impedance increases. gradually becomes smaller.

従つて、本発明の変圧器では、周波数が高くな
るほど、即ち高調波の次数が高くなるほど変圧器
インピーダンスの増加率を小さくすることができ
る。
Therefore, in the transformer of the present invention, the rate of increase in transformer impedance can be made smaller as the frequency becomes higher, that is, the order of the harmonics becomes higher.

上記の変圧器の等価回路は第5図のように表現
できる。ここで変圧器の巻線抵抗をR1、インピ
ーダンス調節装置の鉄心5a以外を通る漏洩磁束
(以下この漏洩磁束を主漏洩磁束という。)による
インダクタンスをL1、インピーダンス調節装置
の鉄心5aを通る漏洩磁束によるインピーダンス
の抵抗分及びインダクタンス分をそれぞれR2
びL2とする。この場合主漏洩磁束によるインピ
ーダンスZ〓1はZ〓1=R1+jωL1となり、インピーダ
ンス調節装置の鉄心5aを通る漏洩磁束によるイ
ンピーダンスZ〓2は、Z〓2=jωL2×R2/(R2
jωL2)となる。このインピーダンスZ〓2の値は高
調波の次数の増加(周波数の増加)と共に単調に
増加するが、周波数の上昇に伴つてその増加率は
小さくなつていく。
The equivalent circuit of the above transformer can be expressed as shown in FIG. Here, R 1 is the winding resistance of the transformer, L 1 is the inductance due to the leakage magnetic flux passing through other than the iron core 5a of the impedance adjustment device (hereinafter, this leakage magnetic flux is referred to as main leakage flux), and L 1 is the inductance due to the leakage flux passing through the iron core 5a of the impedance adjustment device. Let the resistance and inductance components of impedance due to magnetic flux be R 2 and L 2 , respectively. In this case, the impedance Z〓 1 due to the main leakage magnetic flux is Z〓 1 = R 1 + jωL 1 , and the impedance Z〓 2 due to the leakage magnetic flux passing through the iron core 5a of the impedance adjustment device is Z〓 2 = jωL 2 ×R 2 / (R 2+
jωL 2 ). The value of this impedance Z〓 2 increases monotonically as the harmonic order increases (frequency increases), but the rate of increase decreases as the frequency increases.

上記のように1次巻線と2次巻線との間にイン
ピーダンス調節装置5を配設すると、該調節装置
を配設しない場合に比べて当然インピーダンスが
増加する。従つて基本周波数(例えば商用周波
数)における変圧器インピーダンスを従来と同じ
にするためには、主漏洩磁束によるインピーダン
スZ〓1を低くするように変圧器を設計する必要があ
るのは当然である。
When the impedance adjustment device 5 is provided between the primary winding and the secondary winding as described above, the impedance naturally increases compared to the case where the adjustment device is not provided. Therefore, in order to keep the transformer impedance at the fundamental frequency (for example, commercial frequency) the same as before, it is natural that the transformer must be designed to lower the impedance Z〓 1 due to the main leakage flux.

基本周波数における変圧器インピーダンスを同
じとした場合、本発明に係わる変圧器では、周波
数が高い領域で変圧器インピーダンスの増加割合
が少なくなる分だけ従来の変圧器よりも高い周波
数領域でのインピーダンスが低くなり、負荷電流
の高調波成分による電圧降下が小さくなる。
Assuming that the transformer impedance at the fundamental frequency is the same, the transformer according to the present invention has a lower impedance in the high frequency region than a conventional transformer because the rate of increase in transformer impedance in the high frequency region is smaller. Therefore, the voltage drop due to harmonic components of the load current becomes smaller.

第6図は、基本周波数を60Hzとして、基本周波
数において変圧器インピーダンスZ0を等しくする
ように設計した上記実施例の変圧器と従来の変圧
器とについて、変圧器インピーダンスZ0が周波数
F[Hz]に対してどのように変化するかを実測し
た結果を示したものである。第6図において曲線
aは従来の変圧器を示し、曲線bは本発明に係わ
る高調波低インピーダンス変圧器を示している。
この測定結果から判るように、従来の変圧器では
周波数の増加とともにインピーダンスZ0が急激に
増加するが、本発明の高調波低インピーダンス変
圧器では、周波数の増加に伴つてインピーダンス
Z0が漸増する傾向になる。そして基本周波数60Hz
の第9高調波540Hzでのインピーダンスを比較す
ると、本発明の変圧器のインピーダンスZ0は従来
の変圧器のそれの略1/2にまで減少していること
が分かる。周波数の増加に伴つて、従来の変圧器
のインピーダンスと本発明の変圧器のインピーダ
ンスとの比は更に大きくなる。
FIG. 6 shows that the transformer of the above embodiment and a conventional transformer are designed to have the same transformer impedance Z 0 at the fundamental frequency, with the fundamental frequency being 60 Hz, and that the transformer impedance Z 0 is equal to the frequency F [Hz ] shows the results of actual measurements of how it changes. In FIG. 6, curve a represents a conventional transformer, and curve b represents a harmonic low impedance transformer according to the present invention.
As can be seen from this measurement result, in the conventional transformer, the impedance Z 0 increases rapidly as the frequency increases, but in the harmonic low impedance transformer of the present invention, the impedance Z 0 increases as the frequency increases.
Z 0 tends to increase gradually. and fundamental frequency 60Hz
Comparing the impedance at the ninth harmonic of 540 Hz, it can be seen that the impedance Z 0 of the transformer of the present invention is reduced to approximately 1/2 of that of the conventional transformer. As the frequency increases, the ratio of the impedance of the conventional transformer to the impedance of the transformer of the present invention becomes even larger.

第7図は、本発明で用いるインピーダンス調節
装置の他の構成例を示したもので、このインピー
ダンス調節装置では、複数枚のけい素鋼板を積層
して形成した矩形状の鉄心部材7a,7b…,7
fを、それぞれの長辺を横向きとして所定の間〓
6を介して縦列配置することによりインピーダン
ス調節用鉄心5aが構成されている。そしてこの
インピーダンス調節用鉄心5aを囲むように銅板
を1ターン巻回することにより短絡導体5bが形
成され、インピーダンス調節用鉄心5aと短絡導
体部5bとが接着等により一体化されてインピー
ダンス調節装置5が構成されている。この例でも
短絡導体5bによりインピーダンス調節用閉回路
が構成されている。
FIG. 7 shows another configuration example of the impedance adjustment device used in the present invention. In this impedance adjustment device, rectangular core members 7a, 7b, . . . are formed by laminating a plurality of silicon steel plates. ,7
f for a given period with each long side facing horizontally 〓
The impedance adjusting iron core 5a is constructed by arranging the impedance adjustment iron cores 5a in tandem with each other. A short-circuiting conductor 5b is formed by winding a copper plate for one turn so as to surround this impedance-adjusting core 5a, and the impedance-adjusting core 5a and the short-circuiting conductor portion 5b are integrated by adhesive or the like to form an impedance adjusting device 5. is configured. In this example as well, the short-circuit conductor 5b constitutes a closed circuit for adjusting impedance.

このインピーダンス調節装置によれば、インピ
ーダンス調節用鉄心5aの漏洩磁束通路の途中に
間〓6が形成されているため、インピーダンス調
節用鉄心5aの磁気飽和を防止することができ
る。したがつて変圧器に過大な電流が流れた場合
に、電流波形の尖頭値付近でも磁気飽和せず、変
圧器のインピーダンスが変化することを防止する
ことができる。
According to this impedance adjustment device, since the gap 6 is formed in the middle of the leakage magnetic flux path of the impedance adjustment iron core 5a, magnetic saturation of the impedance adjustment iron core 5a can be prevented. Therefore, when an excessive current flows through the transformer, magnetic saturation does not occur even near the peak value of the current waveform, and the impedance of the transformer can be prevented from changing.

上記の実施例では、インピーダンス調節装置5
を巻線の内部に固定するとしたが、巻線の軸線方
向に沿つてインピーダンス調節装置を摺動させ得
る構造にして、変圧器のインピーダンスを可変に
することもできる。このように構成すれば、負荷
側に接続されているコンデンサの接続、切離し等
によつて生じる共振電流の増加を検出してインピ
ーダンス調節装置を摺動させることにより、電源
の高調波から変圧器を含む給電線路の共振周波数
を外すことができるので、給電線路の共振現象を
効果的に抑制して高調波低インピーダンス変圧器
の機能を一段と発揮させることができ、良質の電
力を供給することができる。
In the above embodiment, the impedance adjustment device 5
Although it is assumed that the impedance adjustment device is fixed inside the winding, the impedance of the transformer can also be made variable by having a structure in which the impedance adjustment device can be slid along the axial direction of the winding. With this configuration, by detecting an increase in resonant current caused by connection or disconnection of a capacitor connected to the load side and sliding the impedance adjustment device, the transformer can be protected from harmonics of the power supply. Since the resonant frequency of the power supply line can be removed, the resonance phenomenon of the power supply line can be effectively suppressed and the function of the harmonic low impedance transformer can be further demonstrated, allowing the supply of high quality power. .

上記の各実施例では、インピーダンス調節装置
5を1次,2次巻線間の周方向の一部分に配設し
ているが、両巻線間に、略全周に亘つて配設して
もよい。
In each of the above embodiments, the impedance adjustment device 5 is disposed in a part of the circumferential direction between the primary and secondary windings, but it may also be disposed between both windings over substantially the entire circumference. good.

上記実施例では、インピーダンス調節装置5の
鉄心5aを囲むように短絡導体5bを設けて、こ
の短絡導体によりインピーダンス調節用閉回路を
構成したが、インピーダンス調節用鉄心5aを囲
むように両端が接合されていない(短絡状態にな
い)導体を設け、該導体の両端部間に適宜のコン
デンサを接続するようにしても同様の効果を得る
ことができる。このように構成した場合、基本周
波数ではコンデンサのリアクタンスが大きいた
め、インピーダンス調節用閉回路を流れる電流が
少なく、反発磁界はほとんど生じないが、周波数
が高くなるとコンデンサのリアクタンスが小さく
なるため、インピーダンス調節用閉回路を流れる
電流が増加して反発磁界が生じ、変圧器インピー
ダンスの増加率が小さくなる。
In the above embodiment, the short-circuit conductor 5b is provided so as to surround the iron core 5a of the impedance adjustment device 5, and the short-circuit conductor constitutes a closed circuit for impedance adjustment. A similar effect can be obtained by providing a conductor that is not short-circuited (not short-circuited) and connecting an appropriate capacitor between both ends of the conductor. With this configuration, the reactance of the capacitor is large at the fundamental frequency, so the current flowing through the closed circuit for impedance adjustment is small, and almost no repulsion magnetic field is generated.However, as the frequency increases, the reactance of the capacitor becomes smaller, so the impedance adjustment becomes more difficult. The current flowing through the closed circuit increases, creating a repelling magnetic field and reducing the rate of increase in transformer impedance.

このように構成すると、周波数が低いときにイ
ンピーダンス調節用閉回路を流れる電流を小さく
することができるため、該閉回路での発熱を抑制
することができる。
With this configuration, it is possible to reduce the current flowing through the impedance adjustment closed circuit when the frequency is low, so that heat generation in the closed circuit can be suppressed.

[発明の効果] 以上のように、本発明によれば、1次巻線及び
2次巻線間に、インピーダンス調節用鉄心と該鉄
心を囲むインピーダンス調節用閉回路とを備えた
インピーダンス調節装置を配設して、周波数の上
昇に対する変圧器インピーダンスの増加割合を小
さくしたので、負荷電流に含まれる高調波成分に
り変圧器内で生じる電圧降下を小さくすることが
でき、変圧器の出力電圧波形の歪を少なくして良
質の電力を負荷に供給することができる利点があ
る。
[Effects of the Invention] As described above, according to the present invention, an impedance adjustment device including an impedance adjustment iron core and an impedance adjustment closed circuit surrounding the iron core is provided between a primary winding and a secondary winding. This reduces the rate of increase in the transformer impedance as the frequency increases, making it possible to reduce the voltage drop that occurs within the transformer due to harmonic components included in the load current, thereby improving the output voltage waveform of the transformer. This has the advantage that high-quality power can be supplied to the load with less distortion.

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

第1図は従来の変圧器の等価回路図、第2図は
本発明の一実施例の平面図、第3図は第2図の実
施例で用いるインピーダンス調節装置の一例を示
す正面図、第4図は第3図のA−A線断面図、第
5図は本発明の高調波低インピーダンス変圧器の
等価回路図、第6図は従来の変圧器及び本発明の
変圧器についてインピーダンスの周波数に対する
特性の実測結果を示す線図、第7図は本発明で用
いるインピーダンス調節装置の他の構成例を示す
正面図である。 1…鉄心、2…2次巻線、3…1次巻線、5…
インピーダンス調節装置、5a…インピーダンス
調節用鉄心、5b…短絡導体、6…間〓、7a〜
7f…鉄心部材。
FIG. 1 is an equivalent circuit diagram of a conventional transformer, FIG. 2 is a plan view of an embodiment of the present invention, FIG. 3 is a front view showing an example of an impedance adjustment device used in the embodiment of FIG. Figure 4 is a sectional view taken along the line A-A in Figure 3, Figure 5 is an equivalent circuit diagram of the harmonic low impedance transformer of the present invention, and Figure 6 is the impedance frequency of the conventional transformer and the transformer of the present invention. FIG. 7 is a front view showing another configuration example of the impedance adjustment device used in the present invention. 1... Iron core, 2... Secondary winding, 3... Primary winding, 5...
Impedance adjustment device, 5a... Iron core for impedance adjustment, 5b... Short circuit conductor, 6... Between, 7a~
7f...Iron core member.

Claims (1)

【特許請求の範囲】 1 鉄心に巻回した1次巻線と該1次巻線と同心
的に巻回した2次巻線とを備えた変圧器におい
て、 インピーダンス調節用鉄心と、該インピーダン
ス調節用鉄心を囲むように設けられたインピーダ
ンス調節用閉回路とを備えたインピーダンス調節
装置を前記1次巻線と2次巻線との間に配設した
ことを特徴とする高調波低インピーダンス変圧
器。 2 前記インピーダンス調節用閉回路は、前記イ
ンピーダンス調節用鉄心を囲むように設けられて
両端が電気的に接続された短絡導体からなつてい
る特許請求の範囲第1項に記載の高調波低インピ
ーダンス変圧器。 3 前記インピーダンス調節用閉回路は、前記鉄
心を囲むように設けられた導体と、該導体の両端
間に接続されたコンデンサとからなつている特許
請求の範囲第1項に記載の高調波低インピーダン
ス変圧器。
[Scope of Claims] 1. A transformer including a primary winding wound around an iron core and a secondary winding wound concentrically with the primary winding, comprising: an impedance adjusting iron core; and a secondary winding wound concentrically with the primary winding. A harmonic low impedance transformer, characterized in that an impedance adjustment device including a closed circuit for impedance adjustment provided so as to surround the iron core is disposed between the primary winding and the secondary winding. . 2. The harmonic low impedance transformer according to claim 1, wherein the impedance adjustment closed circuit is formed of a short-circuited conductor that is provided to surround the impedance adjustment core and is electrically connected at both ends. vessel. 3. The harmonic low impedance according to claim 1, wherein the impedance adjustment closed circuit is comprised of a conductor provided to surround the iron core and a capacitor connected between both ends of the conductor. transformer.
JP57066915A 1982-04-21 1982-04-21 Higher harmonic low impedance transformer Granted JPS58182809A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57066915A JPS58182809A (en) 1982-04-21 1982-04-21 Higher harmonic low impedance transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57066915A JPS58182809A (en) 1982-04-21 1982-04-21 Higher harmonic low impedance transformer

Publications (2)

Publication Number Publication Date
JPS58182809A JPS58182809A (en) 1983-10-25
JPH0213806B2 true JPH0213806B2 (en) 1990-04-05

Family

ID=13329739

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57066915A Granted JPS58182809A (en) 1982-04-21 1982-04-21 Higher harmonic low impedance transformer

Country Status (1)

Country Link
JP (1) JPS58182809A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109192467A (en) * 2018-10-11 2019-01-11 佛山市欧立电子有限公司 A kind of single-phase big impedance transformer and its manufacturing method for inverter

Also Published As

Publication number Publication date
JPS58182809A (en) 1983-10-25

Similar Documents

Publication Publication Date Title
JP4930596B2 (en) Transformer and power supply using the same
US11133142B2 (en) Power switch
JPH08203736A (en) Coil device with core
JP7196306B2 (en) air circuit breaker current transformer
US3504318A (en) Three-phase transformer with four legged magnetic core
US3509507A (en) Grounded y - y three-phase transformer
KR100881364B1 (en) Current transformer for power supply and manufacturing method thereof
JP5520613B2 (en) Magnetic flux control type variable transformer
EP1559120A1 (en) Transformer
JPH0213806B2 (en)
CN115602430B (en) Harmonic suppression device and method based on iron core magnetization compensation
JPH11219832A (en) Choke coil for noise filter
JP3789333B2 (en) Electromagnetic equipment
JP4867053B2 (en) Reactor
JP3402573B2 (en) Transformer and power supply
EP3633814B1 (en) Harmonic mitigation arrangement for an electromagnetic device
US4390941A (en) Static magnetic frequency multiplies
JP2002134328A (en) coil
JP3283783B2 (en) Flux control type variable transformer
CN223784998U (en) A three-phase to single-phase transformer
US6782513B1 (en) High power factor integrated controlled ferroresonant constant current source
De Leon et al. Transformer based solutions to power quality problems
JPH03241719A (en) Ac reactor
KR101193408B1 (en) A transformer for an inverter
JPS59229809A (en) Triangular three-leg type three-phase reactor