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JPS5946409B2 - rectifier transformer - Google Patents
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JPS5946409B2 - rectifier transformer - Google Patents

rectifier transformer

Info

Publication number
JPS5946409B2
JPS5946409B2 JP52112149A JP11214977A JPS5946409B2 JP S5946409 B2 JPS5946409 B2 JP S5946409B2 JP 52112149 A JP52112149 A JP 52112149A JP 11214977 A JP11214977 A JP 11214977A JP S5946409 B2 JPS5946409 B2 JP S5946409B2
Authority
JP
Japan
Prior art keywords
windings
winding
group
groups
force distribution
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
JP52112149A
Other languages
Japanese (ja)
Other versions
JPS5445733A (en
Inventor
良朗 望月
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 Corp
Original Assignee
Tokyo Shibaura Electric Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP52112149A priority Critical patent/JPS5946409B2/en
Publication of JPS5445733A publication Critical patent/JPS5445733A/en
Publication of JPS5946409B2 publication Critical patent/JPS5946409B2/en
Expired legal-status Critical Current

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Description

【発明の詳細な説明】 本発明は相間リアクトル付二重星形結線の整流器用変圧
器の直流巻線の構造に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to the structure of a DC winding of a double star-connected rectifier transformer with an interphase reactor.

相間リアクトル付二重星形結線の整流回路では2組の三
相群は独立した三相整流器のように動作2πし各陽極は
(/+u)の期間動作し変圧器の各群の漏洩リアクタン
スによる陽極電流の重なり転流が行なわれる。
In a double star-connected rectifier circuit with an interphase reactor, the two three-phase groups operate like independent three-phase rectifiers, 2π, and each anode operates for a period of (/+u), depending on the leakage reactance of each group of the transformer. An overlap commutation of the anode current takes place.

ここではuは重なり角を示す。従つて各群の漏洩リアク
タンスが異なると陽極電流が不平衡となり相間リアクト
ルの直流偏磁等の障害をひき起す。そのため、この種の
変圧器の直流巻線は各群の漏洩リアクタンスの差を極力
なくす構造としなければならない。第1図、第2図aに
従来用いられている二重星形結線の整流器用変圧器の同
心配置形の巻線の断面を示す。
Here, u indicates the overlapping angle. Therefore, if the leakage reactance of each group is different, the anode current becomes unbalanced, causing problems such as direct current bias magnetization of the interphase reactor. Therefore, the DC winding of this type of transformer must be structured to minimize the difference in leakage reactance between the groups. FIGS. 1 and 2a show cross sections of concentrically arranged windings of a conventionally used double star-connected rectifier transformer.

1は鉄心、2は交流巻線、3a、3bは直流巻線の第一
群の巻線、4a、4bは直流巻線の第二群の巻線である
1 is an iron core, 2 is an AC winding, 3a and 3b are windings of a first group of DC windings, and 4a and 4b are windings of a second group of DC windings.

第1図の直流巻線は各群の巻線3a、4aを円板状に細
かく分割して交互に配列し並列接続した構造である。
The DC winding shown in FIG. 1 has a structure in which the windings 3a and 4a of each group are finely divided into disk shapes, arranged alternately, and connected in parallel.

第2図aの直流巻線は二群の巻線3b、4bを一括に筒
状に巻回した構造である。
The DC winding shown in FIG. 2a has a structure in which two groups of windings 3b and 4b are wound together into a cylindrical shape.

第2図bは第2図aの直流巻線3b、4bを示す正面図
である。以上に述べた構造は直流巻線の容量、絶縁レベ
ル冷却方式によつて長所短所があり、次のような特徴を
持つている。第1図の構造は大電流低電圧の巻線に多く
用いられるが巻線外部での接続の手間を多く必要とする
ばかりか、一般に直流巻線の外部接続のつごうから交流
巻線2を内側に設けるため交流側の電圧調整タップが設
けにくく、さらには、直流巻線が交流巻線2に対してV
丁倍の巻線容量を持つている理由から直流巻線が内側配
置の場合より巻線材料がかさむ欠点がある。第2の構造
は、中小電流の巻線に用いられている構造であるが直流
巻線の二群の巻線3b、4bが隣接することから二群の
巻線3b、4b間の絶縁処理を個体絶縁物で行なわなく
てはならず、絶縁処理の手間、及び絶縁材料を多く必要
とする欠点がある。
FIG. 2b is a front view showing the DC windings 3b and 4b of FIG. 2a. The structure described above has advantages and disadvantages depending on the capacity of the DC winding and the insulation level cooling method, and has the following characteristics. The structure shown in Figure 1 is often used for windings with large currents and low voltages, but not only does it require a lot of effort to connect externally to the windings, but it is also common to use AC windings 2 due to the external connections of DC windings. Since it is installed on the inside, it is difficult to install a voltage adjustment tap on the AC side, and furthermore, the DC winding has a V
Because the winding capacity is twice as large, there is a disadvantage that the winding material is more bulky than when the DC winding is placed inside. The second structure is a structure used for windings of medium and small currents, but since the two groups of windings 3b and 4b of the DC winding are adjacent to each other, insulation treatment between the two groups of windings 3b and 4b is required. This method has the disadvantage of requiring a solid insulating material, requiring a lot of time and effort for insulation treatment, and requiring a large amount of insulation material.

一方、変圧器の二次側巻線を二群とする巻線構造として
、第3図に示すような第一群、第二群の巻線3c、4c
を複数層に分割しこれらを同心的に配置したものがある
。この構造によれば巻線の加工は簡単になるが、以下説
明する理由により第一群、第二群の巻線3c、4cC7
)漏洩リアクタンスの差が大きく、二重星形結線の整流
器用変圧器の巻線に実施することは出来ない。すなわち
同心配置の変圧器巻線の漏洩リアクタンスは次式で表わ
される。X■ ? =X1+X。
On the other hand, as a winding structure in which the secondary windings of a transformer are divided into two groups, the first group and the second group of windings 3c and 4c as shown in FIG.
There is one in which the layer is divided into multiple layers and these layers are arranged concentrically. This structure simplifies the processing of the windings, but for the reasons explained below, the windings 3c, 4cC7 of the first group and the second group
) Due to the large difference in leakage reactance, it cannot be applied to the windings of a double star-connected rectifier transformer. In other words, the leakage reactance of the concentrically arranged transformer windings is expressed by the following equation. X■? =X1+X.

・・・・・・・・・(1)である。第3図aは直流巻線
の二群3c,4cの各層のアンペアターン(n−1)k
が等しく巻回された巻線構造を示し、第3図bは交流巻
線2と直流巻線の第一群3cとの起磁力分布図、第3図
cは交流巻線2と直流巻線第二群4cとの起磁力分布図
を示す。(1)、(2)、(3)式より、漏洩リアクタ
ンスは漏洩磁束に比例し、巻線及び巻線間空隙内部の磁
束分布は起磁力分布と相似であるから、第3図の巻線構
造の二群の巻線3c,4cの漏洩リアクタンスは等しく
ならないからである。本発明は直流巻線の起磁力分布の
操作によつて従来の直流巻線の持つ欠点を改良した整流
器用変圧器を提供することを目的とするもので、以下図
面によつて説明する。
......(1). Figure 3a shows the ampere turns (n-1)k of each layer of the two groups 3c and 4c of the DC winding.
Fig. 3b shows a magnetomotive force distribution diagram of the AC winding 2 and the first group 3c of DC windings, and Fig. 3c shows the magnetomotive force distribution diagram of the AC winding 2 and the DC winding. A magnetomotive force distribution diagram with the second group 4c is shown. From equations (1), (2), and (3), the leakage reactance is proportional to the leakage magnetic flux, and the magnetic flux distribution inside the windings and the air gap between the windings is similar to the magnetomotive force distribution. This is because the leakage reactances of the two groups of windings 3c and 4c in the structure are not equal. The present invention aims to provide a rectifier transformer that improves the drawbacks of conventional DC windings by manipulating the magnetomotive force distribution of the DC windings, and will be explained below with reference to the drawings.

第4図は本発明の一実施例を示すもので、第4図aは直
流巻線の二群の巻線13,14を複数の筒状の巻回層に
分割し、これら複数の巻回層を異なる群の巻線13,1
4の巻回層が対向するように同心的に配置するとともに
各巻回層の空隙の巾Gkを異ならせた巻線構造を示す。
FIG. 4 shows one embodiment of the present invention, and FIG. Windings 13, 1 in different groups of layers
4 shows a winding structure in which four winding layers are arranged concentrically so as to face each other, and the width Gk of the gap in each winding layer is different.

第4図bは交流巻線2と直流巻線第一群の巻線13との
起磁力分布図、第4図cは交流巻線2と直流巻線第二群
の巻線14との起磁力分布図を示す。(1)、(2)、
(3)、式において同心配置の巻線では各巻回層の平均
半径Rk′、空隙の平均半径Rkが異なるので、その値
に応じて起磁力分布を調整する。
Figure 4b is a magnetomotive force distribution diagram between the AC winding 2 and the winding 13 of the first group of DC windings, and Figure 4c is a diagram of the magnetomotive force distribution between the AC winding 2 and the winding 14 of the second group of DC windings. A magnetic force distribution diagram is shown. (1), (2),
(3), in the case of concentrically arranged windings, the average radius Rk' of each winding layer and the average radius Rk of the air gap are different, so the magnetomotive force distribution is adjusted according to these values.

すなわち、Gkの値を調整すれば、二群の巻線13,1
4の漏洩リアクタンスは等しくすることができる。この
ように、直流巻線の二群の巻線をそれぞれ複数の筒状の
巻回層に分割してこれらを同心的に配置する場合に各巻
回層間の空隙の巾を変えることで、二群の巻線の漏洩リ
アクタンスを等しくするように構成した本発明では、直
流巻線の絶縁処理が簡単になり巻線の接続個所も少なく
工作の容易な巻線を得ることができる。
That is, by adjusting the value of Gk, the second group of windings 13, 1
The leakage reactances of 4 can be made equal. In this way, when two groups of DC windings are each divided into a plurality of cylindrical winding layers and these are arranged concentrically, the two groups can be divided by changing the width of the gap between each winding layer. According to the present invention, which is configured to equalize the leakage reactance of the windings, the insulation treatment of the DC winding becomes simple, and the winding can be easily machined with fewer connection points.

尚、説明は直流巻線が内側にあるものによつたが、外側
にあるものにも実施できることは云うまでもない。
Although the explanation has been based on the case where the DC winding is located on the inside, it goes without saying that the present invention can also be applied to a case where the DC winding is located on the outside.

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

第1図、第2図aは従来の巻線を示す断面図、第2図b
は第2図aの直流巻線を示す正面図、第3図aは起磁力
分布を考慮しない巻線の断面図、第3図bは第一群の巻
線の起磁力分布図、第3図cは第二群の巻線の起磁力分
布図、第4図aは本発明の一実施例による巻線の断面図
、第4図bは第一群の巻線の起磁力分布図、第4図cは
第二群の巻線の起磁力分布図である。 1・・・・・・鉄心、2・・・・・・交流巻線、13・
・・・・・直流巻線第一群、14・・・・・・直流巻線
第二群。
Figures 1 and 2a are cross-sectional views showing conventional windings, Figure 2b
is a front view showing the DC winding in Fig. 2a, Fig. 3a is a cross-sectional view of the winding without considering the magnetomotive force distribution, Fig. 3b is a magnetomotive force distribution diagram of the first group of windings, Figure c is a magnetomotive force distribution diagram of the second group of windings, Figure 4a is a sectional view of the winding according to an embodiment of the present invention, Figure 4b is a magnetomotive force distribution diagram of the first group of windings, FIG. 4c is a magnetomotive force distribution diagram of the second group of windings. 1...Iron core, 2...AC winding, 13.
...First group of DC windings, 14... Second group of DC windings.

Claims (1)

【特許請求の範囲】[Claims] 1 相間リアクトル付二重星形結線の直流巻線が二群の
巻線からなり、かつ各群の巻線がそれぞれ複数の筒状の
巻回層を有していて同心的に配置されたものにおいて、
前記二群の巻線の各巻回層の空隙の巾を異ならせて二群
の巻線の漏洩リアクタンスを等しくしたことを特徴とす
る整流器用変圧器。
1 A double star-connected DC winding with an interphase reactor consisting of two groups of windings, each group of windings having a plurality of cylindrical winding layers arranged concentrically. In,
A transformer for a rectifier, characterized in that the width of the gap in each winding layer of the two groups of windings is made different to equalize the leakage reactance of the two groups of windings.
JP52112149A 1977-09-20 1977-09-20 rectifier transformer Expired JPS5946409B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP52112149A JPS5946409B2 (en) 1977-09-20 1977-09-20 rectifier transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP52112149A JPS5946409B2 (en) 1977-09-20 1977-09-20 rectifier transformer

Publications (2)

Publication Number Publication Date
JPS5445733A JPS5445733A (en) 1979-04-11
JPS5946409B2 true JPS5946409B2 (en) 1984-11-12

Family

ID=14579451

Family Applications (1)

Application Number Title Priority Date Filing Date
JP52112149A Expired JPS5946409B2 (en) 1977-09-20 1977-09-20 rectifier transformer

Country Status (1)

Country Link
JP (1) JPS5946409B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61138230U (en) * 1985-02-19 1986-08-27

Also Published As

Publication number Publication date
JPS5445733A (en) 1979-04-11

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