JPS59204220A - Stationrary induction electric apparatus - Google Patents

Stationrary induction electric apparatus

Info

Publication number
JPS59204220A
JPS59204220A JP58078164A JP7816483A JPS59204220A JP S59204220 A JPS59204220 A JP S59204220A JP 58078164 A JP58078164 A JP 58078164A JP 7816483 A JP7816483 A JP 7816483A JP S59204220 A JPS59204220 A JP S59204220A
Authority
JP
Japan
Prior art keywords
magnetic shielding
winding
phase
shielding plates
magnetic shield
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
JP58078164A
Other languages
Japanese (ja)
Inventor
Yoshio Hamadate
良夫 浜館
Tatsu Saito
斉藤 達
Yasunori Ono
康則 大野
Yoshiaki Inui
乾 芳彰
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 JP58078164A priority Critical patent/JPS59204220A/en
Publication of JPS59204220A publication Critical patent/JPS59204220A/en
Pending 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
    • H01F27/36Electric or magnetic shields or screens
    • 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
    • H01F27/36Electric or magnetic shields or screens
    • H01F27/366Electric or magnetic shields or screens made of ferromagnetic material

Landscapes

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

Abstract

PURPOSE:To reduce the number of sheets of the magnetic shielding plates of a stationary induction electric apparatus by a method wherein a pair of the magnetic shielding plates projected obliquely having the prescribed angles in the outer direction of a window at every phase from a magnetic shielding plate arranged extending over another phase are combined to the latter. CONSTITUTION:Even when leakage flux generated between a high-voltage winding 1 and a low-voltage winding 2 intends to invade in a tank or another structural material, the greater part thereof is attracted at first to magnetic shielding plates 40 split and juxtaposed along the shape of the winding, and after then, according to action of magnetic flux to flow transferring to a magnetic shielding plate 20 provided extending over another phase, reduction of loss at the respective parts of a transformer can be attained. Moreover, a pair of the magnetic shielding plates 40 protruded obliquely having the prescribed agnles theta in the outer direction of a core window are arranged as to along the outermost diametrical winding as much as possible. Accordingly, because the magnetic shielding plates can be concentrated to one piece making the central part of the phase of the winding as a boundary, the number of sheets of the wiring is reduced sharply.

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明は静止誘導電器の鉄心締付金具に取付けらj、る
磁気シールド板に(糸り、、 %に、大容量化さj、た
静II:、誘導霜;器の改良に関する。
[Detailed Description of the Invention] [Field of Application of the Invention] The present invention is directed to a magnetic shield plate attached to an iron core fastening fitting of a stationary induction electric appliance. II: Induced frost; Concerning improvements in vessels.

〔発明の背景〕[Background of the invention]

近年、静止誘47も、器、たとえば、変圧器は益々大容
弗化される一向にあり、それに伴い、巻線からの漏れ磁
束も増大している。このため、d雨れ磁束が原因で生じ
る徐遊損の増加と構造材に訪起される局部的な温度上昇
を磁気シールド板を用いることで出来る限り小さくする
努力がなされている。
In recent years, the static induction 47, such as a transformer, has become increasingly larger in capacity, and leakage flux from the windings has also increased accordingly. For this reason, efforts are being made to minimize the increase in stray loss caused by rain magnetic flux and the local temperature rise occurring in structural materials by using magnetic shield plates.

これを第1図の従来の変圧器の一相分の平面図により説
明する。図中、1.2は一8線、3 (ti’鉄IL・
、20.30は巻線端部に配揄さt、た磁気シールド根
である。このうち、磁気シールド4反20は他相にまた
がっているが、磁気シールド板30d]各+1−1毎に
鉄心窓外方向へ面角にほぼ巻線形状に沿って分割並置さ
れてお・す、これら両ネ;は端部で磁気的に結合されて
た構成となっている。
This will be explained with reference to a plan view of one phase of a conventional transformer shown in FIG. In the figure, 1.2 is the 18th line, 3 (ti' iron IL・
, 20.30 is a magnetic shield root placed at the end of the winding. Among these, the magnetic shield 4 anti-20 straddles other phases, and the magnetic shield plates 30d are divided and arranged parallel to each other along the winding shape at a face angle toward the outside of the iron core window every +1-1. , these two wires are magnetically coupled at their ends.

この構成の変圧器では、高圧軽酊1と低圧巻線2の間に
生じた漏れ磁束がタンク(図示せず)や他の構造材に侵
入しようとしても巻線形状に沿って分割並置された磁気
シールド根30に、その大部分がます吸引され、その後
、磁束が他相に聾:る磁気シールド板20へ移行して流
れる作用により、変圧器各部の損失低減が図れる。なお
、磁気/−ルド叛30を複数分割並置するのは、磁気シ
ールド板30が大形化した際に生ずるシールド板自身の
発生損失を最小限に押え、このような購造での磁気シー
ルド効果全十分に発揮式せるためである。
In a transformer with this configuration, even if the leakage magnetic flux generated between the high-voltage winding 1 and the low-voltage winding 2 tries to enter the tank (not shown) or other structural materials, it will be divided and juxtaposed along the winding shape. Most of the magnetic flux is attracted to the magnetic shield root 30, and then the magnetic flux moves to the magnetic shield plate 20, which is deaf to other phases, and flows, thereby reducing losses in each part of the transformer. The reason why the magnetic shield plate 30 is divided into multiple pieces and arranged in parallel is to minimize the loss of the shield plate itself that occurs when the magnetic shield plate 30 becomes larger, and to improve the magnetic shielding effect in such a purchase. This is so that it can be fully demonstrated.

しかし、変圧器が大容量化するにつれて、必然的に巻線
径も大きくなり、上述の効果を達成しようとするには、
各相毎に鉄jlJ窓外方向に直角に突出させる磁気/−
ルド板30の本数をとうしても増加させる必要が生じて
、これが経済的な変圧器を供給する上での欠点となって
いた。
However, as the capacity of transformers increases, the winding diameter also inevitably increases, and in order to achieve the above effects,
Magnetism that projects perpendicularly to the outside of the window for each phase /-
It became necessary to increase the number of lead plates 30, which was a disadvantage in providing an economical transformer.

〔発明の目的〕[Purpose of the invention]

本発明の目的は磁気シールド板のシールド効果を低下さ
せることなく、磁気シールド板の本数を低σ諺・し7、
製作工数やコストを低下させる経済的な静止誇導東器全
提供するすこある。
The purpose of the present invention is to reduce the number of magnetic shield plates without reducing the shielding effect of the magnetic shield plates.
We offer a complete range of economical stationary guide tools that reduce manufacturing man-hours and costs.

〔発明の概要〕[Summary of the invention]

本発明の侠点は、他相にわたって配置する磁気シールド
叛から谷相栂に窓外方向へ所定の角度ケもって斜めに突
出させる一対の磁気シールド叛を組合せ目己懺したこと
にある。
The advantage of the present invention lies in the combination of a pair of magnetic shield shields that protrude diagonally from the magnetic shield shields arranged across the other phases toward the outside of the window at a predetermined angle.

〔発明の実施例〕[Embodiments of the invention]

以下、本発明の一実施例を図面を参照しながら説明する
。第2図は第1図と同様の変圧器の要部平面図である。
An embodiment of the present invention will be described below with reference to the drawings. FIG. 2 is a plan view of the main parts of the transformer similar to FIG. 1.

従来の構造と異なる点は鉄心窓外方向へ所定の角度θを
もって斜めに突出した一対の磁気シールド板40が最外
径巻線にできるたけ沿うように配置される点である。
The difference from the conventional structure is that a pair of magnetic shield plates 40 that project obliquely at a predetermined angle θ toward the outside of the iron core window are arranged so as to follow the outermost diameter winding as much as possible.

この構造では、鉄心窓外方向に突出した磁気シールド板
40の長さを十分に長く確保することができるので、従
来、鉄心窓外方向に曲角に突出した磁気シールド叛30
が複数本必幾たったものか、巻線の相中上部を境に一本
に集約することがでさるため、その装置本数か大幅に低
減する。なお、磁気・/−ルド板40で巻倫全偵う面積
もその版幅fK:最適に運ぶことで従来とほぼ同一にで
きるため磁束の吸引効果もこntでのものとelは同一
にすることができる。
With this structure, the length of the magnetic shield plate 40 protruding outward from the iron core window can be ensured to be sufficiently long.
However, the number of devices required can be reduced significantly by consolidating them into one at the upper part of the phase of the winding. In addition, the area covered by the magnetic//- lead plate 40 can be made almost the same as the conventional one by carrying the plate width fK optimally, so the magnetic flux attraction effect and el should be the same as in this case. Can be done.

第3図は本発明の第二の実施例を示す。鉄心窓外方向へ
斜めに突出させた一対の磁気シールド叛50が最外径巻
線に近接せずに、巻線1,2の内側に食い込んだ場合で
、鉄心窓外方向への角度θ′が第2図の場合のθに比べ
大となる。この構造の場合は、磁気シールド板50の長
さが第2図の揚台に比べ煙かくなるが、磁気シールド叛
の暢を若干広けるなどの最適化を施こすことで第2図で
述べたとはクヨ同様な効果を十分に発揮することができ
る。
FIG. 3 shows a second embodiment of the invention. In the case where a pair of magnetic shielding members 50 diagonally protruding toward the outside of the core window do not approach the outermost diameter winding but bite into the inside of the windings 1 and 2, the angle θ' toward the outside of the core window is is larger than θ in the case of FIG. In the case of this structure, the length of the magnetic shield plate 50 is longer than that of the platform shown in Fig. 2, but by making optimizations such as slightly widening the range of the magnetic shield, the length of the magnetic shield plate 50 is longer than that shown in Fig. 2. It can fully demonstrate the same effect as Kuyo.

第4図は本発明の第三の実施例の変圧器端部相の狭部平
面図である。
FIG. 4 is a plan view of a narrow portion of a transformer end phase according to a third embodiment of the present invention.

41D相に配置した磁気シールド板20および斜めに突
出した磁気シールド板60や鉄心3等で覆イクれない端
部相では鉄心窓外方向へ所定の角度θ金もって斜めに突
出せしめる磁気シールド板の一方70を他に比べて長く
して端部で露出する巻線の一部も含めてこの磁気シール
ド&70で榎える構造となっている。
In the end phase that cannot be covered by the magnetic shield plate 20 disposed in the 41D phase, the magnetic shield plate 60 protruding diagonally, and the iron core 3, etc., the magnetic shield plate protrudes obliquely at a predetermined angle θ toward the outside of the iron core window. On the other hand, the structure is such that the magnetic shield 70 is longer than the others, and a part of the winding wire exposed at the end can be protected by the magnetic shield &70.

この構造にすれは、従来、端部相でタンク(図示せず)
や他の構造材に侵入していた大量の磁束全磁気シールド
&70で積極的に吸引して磁気7−ルド板20へ移行し
て流すために第2図で述べた本発明の効果が一層確実な
ものとなる。
Traditionally, this structure has a tank (not shown) at the end phase.
The effect of the present invention described in FIG. 2 is even more certain because the large amount of magnetic flux that has penetrated into the magnetic flux and other structural materials is actively attracted by the total magnetic shield &70 and transferred to the magnetic field plate 20 and flows. Become something.

第5図は本発明の第四の実施例を示し、第2図と同様の
変圧器の要部平面である。
FIG. 5 shows a fourth embodiment of the present invention, and is a plan view of the main part of a transformer similar to FIG. 2.

従来の構造と異なる点は、鉄心窓外方向へ所定の角度θ
をもって斜めに突出した一対のa気/−ルド板80のタ
ンク側の端面が相中心部全境に平行配置されている点で
ある。図中4はタンクである。なお、本発明では磁気シ
ールド叛全鉄心窓外方向へ所定の角度をもって斜めに突
出させたが本発明はこれに限定されることU′なく、三
角形の侭気ンールド板で構成しても本発明の効果を奏す
ることができる。
The difference from the conventional structure is that the iron core is set at a predetermined angle θ toward the outside of the window.
The point is that the tank-side end surfaces of the pair of a-air/-old plates 80 that protrude obliquely are arranged parallel to the entire border of the phase center. 4 in the figure is a tank. In the present invention, the entire magnetic shield core protrudes obliquely toward the outside of the window at a predetermined angle, but the present invention is not limited to this, and the present invention may also be constructed with a triangular winding plate. It is possible to achieve the following effects.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、損失が過大となる斜線で示す相中上部
付近のタンクではわずかの間隙を設けるだけで巻線が磁
気シールドに穆われることになるため、タンクに対する
シールド効果か向上する。
According to the present invention, in the tank near the upper part of the phase indicated by the diagonal line where the loss is excessive, the winding is surrounded by the magnetic shield just by providing a small gap, so that the shielding effect for the tank is improved.

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

第1図は従来の変圧器の一相分の平面図、第2図は本発
明の一実施例の一相分の平面図、第3図、第4図は本発
明のそれぞれ第二、第三の実施例で一相分の平面図、第
5囚は本発明の第四の実施例で変圧器端部の平面図であ
る。 20.30,40,50,60,70.80・・・磁気
シー2     / 茅4図 茅S口
Fig. 1 is a plan view of one phase of a conventional transformer, Fig. 2 is a plan view of one phase of an embodiment of the present invention, and Figs. The third embodiment is a plan view of one phase, and the fifth embodiment is a plan view of the end of the transformer in the fourth embodiment of the present invention. 20.30, 40, 50, 60, 70.80...Magnetic sea 2 / Kaya 4 figure Kaya S mouth

Claims (1)

【特許請求の範囲】 1、巻線の上・下端に漏れ磁束を導くために、他相へわ
たって配量される磁気シールド板をもつ静止誘導電器に
おいて、 各相舟に鉄心窓外方向へ所定の角度をもって斜めに突出
させる一対の前記磁気シールド板を組合せて配鵬゛した
ことを特徴とする静止誘導電器。
[Claims] 1. In a stationary induction electric appliance having a magnetic shield plate distributed over other phases in order to guide leakage magnetic flux to the upper and lower ends of the winding, each phase is provided with a magnetic shield plate extending toward the outside of the iron core window. A stationary induction electric appliance characterized in that a pair of magnetic shield plates as described above are disposed in combination and are protruded obliquely at a predetermined angle.
JP58078164A 1983-05-06 1983-05-06 Stationrary induction electric apparatus Pending JPS59204220A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58078164A JPS59204220A (en) 1983-05-06 1983-05-06 Stationrary induction electric apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58078164A JPS59204220A (en) 1983-05-06 1983-05-06 Stationrary induction electric apparatus

Publications (1)

Publication Number Publication Date
JPS59204220A true JPS59204220A (en) 1984-11-19

Family

ID=13654285

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58078164A Pending JPS59204220A (en) 1983-05-06 1983-05-06 Stationrary induction electric apparatus

Country Status (1)

Country Link
JP (1) JPS59204220A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102315004A (en) * 2010-06-30 2012-01-11 特变电工沈阳变压器集团有限公司 Magnetic shielding structure and method of transformer

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102315004A (en) * 2010-06-30 2012-01-11 特变电工沈阳变压器集团有限公司 Magnetic shielding structure and method of transformer

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