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JPS5929132B2 - rectifier transformer - Google Patents
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JPS5929132B2 - rectifier transformer - Google Patents

rectifier transformer

Info

Publication number
JPS5929132B2
JPS5929132B2 JP52112150A JP11215077A JPS5929132B2 JP S5929132 B2 JPS5929132 B2 JP S5929132B2 JP 52112150 A JP52112150 A JP 52112150A JP 11215077 A JP11215077 A JP 11215077A JP S5929132 B2 JPS5929132 B2 JP S5929132B2
Authority
JP
Japan
Prior art keywords
winding
windings
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
JP52112150A
Other languages
Japanese (ja)
Other versions
JPS5445734A (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 JP52112150A priority Critical patent/JPS5929132B2/en
Publication of JPS5445734A publication Critical patent/JPS5445734A/en
Publication of JPS5929132B2 publication Critical patent/JPS5929132B2/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し各陽極は(2
π/3+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。ここ
で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衝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。
In a double star-connected rectifier circuit with an interphase reactor, the two three-phase groups operate like independent three-phase rectifiers, and each anode (2
It operates for a period of π/3+u), and overlap commutation of the anode current due to the leakage reactance of each group of transformers takes place. Here, u indicates the overlapping angle. Therefore, if the leakage reactance of each group is different, the anode currents become unbalanced, causing problems such as direct current bias magnetization of the interphase reactor. Therefore, the DC winding of this type of transformer must be constructed to minimize the difference in leakage reactance between each group. FIGS. 1 and 2a show cross sections of concentrically arranged windings of a conventionally used double star-connected rectifier transformer.

1は鉄ノ仄2は交流巻線、3a、3bは直流巻線の第1
群の巻線、4a、4bは直流巻線の第2群の巻線である
1 is the iron wire, 2 is the AC winding, and 3a and 3b are the first DC windings.
Group windings 4a, 4b are windings of the 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。第2図bは第2図aの直流巻
線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
多く必要とし、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
プを設けにくいこと、直流巻線が交流巻線2に対してJ
i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。
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. FIG. 2b is a front view showing the DC winding 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 high current, low voltage windings, but it requires a lot of effort to connect externally to the windings, and generally the AC winding 2 is connected inside because of the external connection of the DC winding. Therefore, it is difficult to install a voltage adjustment tap on the AC side, and the DC winding is J
Since the winding capacity is i times larger, there is a disadvantage that the winding material is larger than when the DC winding is arranged 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 are adjacent to each other, the second group of windings 3b and 4b are adjacent to each other.
The insulation treatment between the sections 4b must be performed using a solid insulator, which has the drawback of requiring a lot of effort and 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図に示すように二群の巻線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、第二群の巻線の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。
On the other hand, as a winding structure in which the secondary windings of a transformer are divided into two groups, the two groups of windings 3c and 4c are divided into multiple layers and these are arranged concentrically, as shown in Fig. 3. be. This structure simplifies the processing of the windings, but due to the reasons explained below, there is a large difference in leakage reactance between the first and second group windings. cannot be carried out. In other words, the leakage reactance of the concentrically arranged transformer windings is expressed by the following equation.

XェーHXI+X2・・・・・・ (1)X1■■■■
6、’れ’、I門釜((n−i)ι・rk−gk)・・
・・・・ (2)A工 上式において X゜漏洩リアクタンス Xl゜空隙部分で生じる漏洩リアクタンスX2: コイ
ル内部で生じる漏洩リアクタンスEg.漏洩磁束による
誘起電圧I 巻線電流 F.周波数 (n−1)k:層あたりのアンペアターンh :巻線の
高さ Rk:空隙の平均半径 Rk′:巻線の平均半径 Gk:空隙の巾 Dk:巻線の巾 である。
X-HXI+X2... (1)X1■■■■
6, 're', Imonkama ((n-i)ι・rk-gk)...
...... (2) In the construction type A, X゜Leakage reactance Xl゜Leakage reactance generated in the gap X2: Leakage reactance generated inside the coil Eg. Induced voltage I due to leakage magnetic flux Winding current F. Frequency (n-1)k: Ampere turns per layer h: Height of the winding Rk: Average radius of the gap Rk': Average radius of the winding Gk: Width of the gap Dk: Width of the winding.

第3図aは直流巻線の二群の巻線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と直流巻線第一群の巻線
3cとの起磁力分布図、第3図cは交流巻線2と直流巻
線第二群の巻線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んる
Figure 3a shows a winding structure in which two groups of windings 3c and 4c of the DC winding are wound with equal ampere turns (n 1) k in each layer, and Figure 3b shows the winding structure of the AC winding 2 and FIG. 3c shows a magnetomotive force distribution diagram between the AC winding 2 and the winding 4c of the second DC winding group. (1),
From equations (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. Winding wire 3c
, 4c are not equal. An object of the present invention is 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を複数層に分割し、これ
らを同心的に配置するとともに各層の巻回数を異ならせ
る。
FIG. 4 shows an embodiment of the present invention, in which FIG. Make the number of times different.

すなわちアンペアターン(n−1)kを異ならせるよう
にしたものである。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層の巻線
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。
That is, the ampere turns (n-1)k are made different. 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. In Equations 1, 2, and 3, since the average radius Rk' of the windings in each layer and the average radius Rk of the air gaps are different in the concentrically arranged windings, the magnetomotive force distribution is adjusted according to these values.

すなわち(n−1)kの値を調整すれば二群の巻線13
,14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各層の巻回数を変えることで、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。
In other words, by adjusting the value of (n-1)k, the second group of windings 13
, 14 can be made equal.
The present invention, which is configured to equalize the leakage reactance of two groups of windings by changing the number of turns in each layer of the DC winding, simplifies the insulation treatment of the DC winding and reduces the number of connections between the windings. It is possible to obtain a winding wire that is easy to work with.

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。
It should be noted that although the description has been based on the case where the DC winding is located on the inside, it goes without saying that it 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 drawings]

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は第二群の起磁力分布図、
第4図aは本発明の−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
の起磁力分布図である。 1・・・・・・鉄′収2・・・・・・交流巻線、13・
・・・・・直流巻線第=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 the magnetomotive force distribution diagram of the second group.
FIG. 4a is a sectional view of a winding according to an embodiment of the present invention;
FIG. 4b is a magnetomotive force distribution diagram of the first group of windings, and FIG. 4c is a magnetomotive force distribution diagram of the second group. 1... Iron collection 2... AC winding, 13.
...DC winding 1st group, 14...DC winding 2nd group.

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二群の直流巻線を
それぞれ複数層に分割しこれらを同心的に配置したもの
において、二群の巻線の各層の巻回数を異ならせること
によつ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. Two groups of DC windings in a double star connection with an interphase reactor are each divided into multiple layers and these are arranged concentrically, by varying the number of turns in each layer of the two groups of windings. A rectifier transformer characterized in that two groups of windings have equal leakage reactance.
JP52112150A 1977-09-20 1977-09-20 rectifier transformer Expired JPS5929132B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP52112150A JPS5929132B2 (en) 1977-09-20 1977-09-20 rectifier transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP52112150A JPS5929132B2 (en) 1977-09-20 1977-09-20 rectifier transformer

Publications (2)

Publication Number Publication Date
JPS5445734A JPS5445734A (en) 1979-04-11
JPS5929132B2 true JPS5929132B2 (en) 1984-07-18

Family

ID=14579477

Family Applications (1)

Application Number Title Priority Date Filing Date
JP52112150A Expired JPS5929132B2 (en) 1977-09-20 1977-09-20 rectifier transformer

Country Status (1)

Country Link
JP (1) JPS5929132B2 (en)

Also Published As

Publication number Publication date
JPS5445734A (en) 1979-04-11

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