JPS5947721A - Stationary induction apparatus - Google Patents
Stationary induction apparatusInfo
- Publication number
- JPS5947721A JPS5947721A JP57156543A JP15654382A JPS5947721A JP S5947721 A JPS5947721 A JP S5947721A JP 57156543 A JP57156543 A JP 57156543A JP 15654382 A JP15654382 A JP 15654382A JP S5947721 A JPS5947721 A JP S5947721A
- Authority
- JP
- Japan
- Prior art keywords
- winding
- lead wire
- magnetic shielding
- magnetic
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F27/00—Details of transformers or inductances, in general
- H01F27/34—Special means for preventing or reducing unwanted electric or magnetic effects, e.g. no-load losses, reactive currents, harmonics, oscillations, leakage fields
- H01F27/36—Electric or magnetic shields or screens
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F27/00—Details of transformers or inductances, in general
- H01F27/34—Special means for preventing or reducing unwanted electric or magnetic effects, e.g. no-load losses, reactive currents, harmonics, oscillations, leakage fields
- H01F27/36—Electric or magnetic shields or screens
- H01F27/366—Electric or magnetic shields or screens made of ferromagnetic material
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Regulation Of General Use Transformers (AREA)
Abstract
Description
【発明の詳細な説明】
本発明は変圧器やりアクドル等の静止誘導電器に係り、
特に巻線からの漏れ磁束を制御するだめの磁気シールド
に関する。[Detailed Description of the Invention] The present invention relates to stationary induction electric appliances such as transformers and accelerators.
In particular, it relates to a magnetic shield for controlling leakage magnetic flux from windings.
近年、静止誘導電器たとえば変圧器は益々大容量化され
る傾向にあり、それに伴い巻線からの漏れ磁束も増大し
ている1、漏れ磁束の増大と共に変圧器構造物の局部温
度上昇の防市、発生損失の低減が性能、耐用性の観点か
ら問題視されている1、変圧器の締金具もその一例であ
る。In recent years, the capacity of stationary induction electric devices such as transformers has been increasing, and leakage flux from the windings has also increased. , reduction of generated loss is seen as a problem from the viewpoint of performance and durability 1. Fasteners for transformers are an example of this.
これを第J図、第2図に示す従来の変圧器内部構造図に
より説明する。鉄心U脚部3ノー継鉄部4゜5とを組合
わせて構成さオ]ている1、この脚部3の両側面に鉄心
あて板10が尚てらtl、貫通ホルト又iJ:バインド
テープにより締付f、tらilている。鉄心継鉄部4及
び5は鉄心脚部3のトートに配備さtlており、その両
側には鉄心締付金具6,7が当てられ締付ける構造とな
っている。この締月金具6゜7は鉄心継鉄部4,5を締
付けると共に、鉄心脚部3の周囲に巻回された、内側巻
線1及び外側巻+li!i!2’を押圧する作用も行っ
ている1、以」二の如き構成から成る変圧器では、従来
第1図中矢印で示すような巻線からの漏わ、磁束の相当
量全吸引するように高透磁率の磁気シールド板8゜9が
上部鉄心締付金具6及び丁″部鉄心締付金具7の巻線側
の面に配備されており、この磁気シールド板8及び9で
吸引された漏れ磁束を磁気抵抗の小さい紙面に垂直な方
向に導く作用をしている。This will be explained with reference to the internal structure diagrams of a conventional transformer shown in FIG. J and FIG. 2. The iron core is constructed by combining the U leg part 3 and the yoke part 4. It is tightened. The core yoke parts 4 and 5 are arranged on the tote of the core leg part 3, and core clamping fittings 6 and 7 are applied to both sides of the core yoke parts 4 and 5 to tighten them. This clamping fitting 6°7 tightens the core yoke parts 4 and 5, and also the inner winding 1 and the outer winding +li! wound around the core leg part 3! i! Conventionally, in a transformer having a structure such as 1 or 2, which also has the effect of pressing the magnetic flux 2', a considerable amount of the magnetic flux leaking from the windings as shown by the arrow in Fig. 1 is completely absorbed. A magnetic shielding plate 8゜9 with high magnetic permeability is provided on the winding side surface of the upper core clamping bracket 6 and the bottom core clamping bracket 7, and leakage is absorbed by the magnetic shielding plates 8 and 9. It acts to guide magnetic flux in a direction perpendicular to the plane of the paper where magnetic resistance is low.
このような磁気シールド板に吸引される漏れ磁束の性質
を、第2図(a)に示すようなU、V、W相から成る3
相変圧器で見てみると、各相からの漏れ磁束φ8.φ7
.φ7が120度の位相差をもちベクトル的ニハランス
し、大部分の漏れ磁束が磁気シールド板中に閉じこめら
れる流れとなる。さらに、この磁気シールド板中を長手
方向に流れる磁束分布の形態を見てみると、第2図中)
K示すようにU。The properties of the leakage magnetic flux attracted by such a magnetic shield plate can be expressed as 3, consisting of U, V, and W phases, as shown in Figure 2 (a).
Looking at the phase transformer, leakage magnetic flux from each phase is φ8. φ7
.. φ7 has a phase difference of 120 degrees and exhibits vectorial Nihalance, resulting in a flow in which most of the leakage magnetic flux is confined within the magnetic shield plate. Furthermore, if we look at the shape of the magnetic flux distribution flowing in the longitudinal direction in this magnetic shield plate, we can see that (in Figure 2)
U as shown in K.
V相及び■、W相の巻線相関部付近で累積されてピーク
値となる特徴も有している。It also has the characteristic that it accumulates and reaches a peak value near the winding correlation portions of the V phase, ■, and W phases.
かかる磁気シールド板の磁束吸引効果は一般に漏れ磁束
の発生源となる巻線1,2にできるだけ近接させること
で向上できるものであるが、絶縁性能上、必然的に制約
されてくる。The magnetic flux attracting effect of such a magnetic shield plate can generally be improved by placing it as close as possible to the windings 1 and 2, which are the sources of leakage magnetic flux, but this is inevitably limited in terms of insulation performance.
特に第1図中ハツチングを施こしたA部、すなわち内側
巻線からの口出し線11に近接する磁気シールド板の外
側端部で、かつ第2図中ハツチングを施こしたB部、す
なわち各相の中心部fC−C)付近で電界の集中が著し
くなり放電が起りやすくなる問題が生じてくる。Particularly, the hatched part A in FIG. 1, that is, the outer end of the magnetic shielding plate close to the lead wire 11 from the inner winding, and the hatched part B in FIG. 2, that is, each phase. A problem arises in that the electric field is significantly concentrated near the center fC-C), making it easy for discharge to occur.
したがってこの力側巻線からの口出し線11に対する電
界集中を防ぐためには、磁気シールド板8ないし9と巻
線1,2との間’#、’+に太きくシ、なければならず
、そのために変圧器の形状が必然的に大きくなると共に
磁気シールド板での磁束吸引効果も低下するという欠点
があった。Therefore, in order to prevent electric field concentration from the force side winding to the lead wire 11, thick wires must be placed between the magnetic shield plates 8 to 9 and the windings 1 and 2. However, the shape of the transformer inevitably becomes larger, and the magnetic flux attraction effect of the magnetic shield plate also decreases.
本発明の目的は1、上記した従来技術の欠点をなくシ、
巻線からの口出し線に対向する付近での磁気シールド部
材の電界集中を防止すると共に、磁気シールド部材の磁
束吸引効果全充分忙発挿し得る静止誘導電器を提供する
ことにある。The purpose of the present invention is 1 to eliminate the above-mentioned drawbacks of the prior art;
To provide a stationary induction electric appliance which can prevent electric field concentration in a magnetic shield member in the vicinity opposite to a lead wire from a winding, and can sufficiently generate the magnetic flux attracting effect of the magnetic shield member.
この目的全達成するため、本発明は、磁気シールド部材
における口出し線に対向する部分に、口出し線の形状に
ほぼ沿うような切欠き部を設りたことを特徴とする。In order to achieve all of these objects, the present invention is characterized in that a notch portion that substantially follows the shape of the lead wire is provided in a portion of the magnetic shielding member that faces the lead wire.
以下、本発明を図示の各実施例について詳細に説明する
。DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be described in detail below with respect to each of the illustrated embodiments.
第3図は本発明の一実施例であり、第2図と同一部分を
示す3相変圧器の上部正面図である。図中第2図と同一
符号は同一の部分を示している。FIG. 3 is an embodiment of the present invention, and is a top front view of a three-phase transformer showing the same portion as FIG. 2. In the figure, the same reference numerals as in FIG. 2 indicate the same parts.
この実施例が従来の変圧器と異なる点は、磁気シールド
板20が、内側巻線からの口出し線11と対向する相中
心部<C−C>付近で、はぼ口出し線形状に沿って一様
に切欠かれている点である。This embodiment differs from conventional transformers in that the magnetic shield plate 20 is aligned along the shape of the lead wire near the phase center <C-C> facing the lead wire 11 from the inner winding. It is a point that is notched like this.
しかも、この磁気シールド板2oの切欠き部21の範囲
は3相巻線に渡る磁気シールド板の磁路を遮断するもの
でないため、磁気シールド中を長手方向に流れる漏れ磁
束の通路は確保され一層いる。Moreover, since the range of the notch 21 of the magnetic shield plate 2o does not block the magnetic path of the magnetic shield plate extending over the three-phase winding, the path of leakage magnetic flux flowing in the longitudinal direction in the magnetic shield is ensured. There is.
かかる構造によれば、磁気シールド板20と巻線の距離
を大としなくとも、内側巻線からの口出し線に対する電
界集中を防止することができるため、従来の磁気シール
ド板で生じていた前述の如き多くの欠点を改善できるこ
とになる。According to this structure, it is possible to prevent electric field concentration from the inner winding to the lead wire without increasing the distance between the magnetic shield plate 20 and the winding, so that the above-mentioned problem that occurs with the conventional magnetic shield plate can be prevented. Many of these shortcomings can be improved.
なおこの切欠き部21は、通常はとんどが相中心部に位
置するために、第2図(b)から明らかな如く磁気シー
ルド板中′@:流れる磁束量も小さい所である。そのた
めこのような切欠き部21を設けても、磁気シールド板
中の磁束密度がむしろ均一化されることになり、磁束吸
引効果弔などにケま全く障害となるものではない。Since most of the notches 21 are normally located at the center of the phase, the amount of magnetic flux flowing through the magnetic shield plate is also small, as is clear from FIG. 2(b). Therefore, even if such a notch 21 is provided, the magnetic flux density in the magnetic shield plate is rather made uniform, and the magnetic flux attraction effect is not hindered at all.
第4図から第8図tよ本発明の他の各実施例λ:示すも
のであり、いずれも変圧器」一部付近での磁気シールド
板の切欠き部のたて断面図で、第3図の実施例で述べた
磁気シールド板2oの磁束吸引効果が一層助長できるよ
うに配局:さJ′)た構造となっている。FIG. 4 to FIG. 8 t show other embodiments of the present invention. The arrangement is such that the magnetic flux attracting effect of the magnetic shield plate 2o described in the embodiment shown in the figure can be further enhanced.
第4図は磁気シールド板3oの切欠き部31の形状を、
第3図の実施例のようT?Z a熱シールド板の幅方向
において一様とせずに2、内側巻線からの口出し線11
の高さ方向の形状にほぼ沿う、Lうに形成したもので、
巻線1.2の径方向内側部で磁気シールド板30が、第
8図の磁気シールド板20よりも巻線に近接した構造と
なっている21本構造では巻線からの径方向漏れ磁束が
、通常最大となる巻線内側部で磁気シールド板3oが巻
糸?1゜2に近接しでいることから、この磁気シーツト
ド板30による漏れ磁束の吸引効果がむし2ろ一層助長
されることになるだけで、口出し線11に対する電界集
中を防止できる効果、作用は第3図に述べた例と何ら変
るものではない、
第5図は第4図の磁気シールド板30の製作を容易とす
るために、高さ方向に磁気シールド板を40.41.4
1!:分割した例であり、また第6図は径方向に磁気シ
ールド板’e50,5]、、52と分割した例である。FIG. 4 shows the shape of the notch 31 of the magnetic shield plate 3o.
T like the embodiment in Figure 3? Z aThe wires 11 are drawn out from the inner winding without being uniform in the width direction of the heat shield plate.
It is formed in an L shape that roughly follows the shape in the height direction.
In the 21-wire structure in which the magnetic shield plate 30 is closer to the winding than the magnetic shield plate 20 shown in FIG. , is the magnetic shielding plate 3o the winding thread at the inner side of the winding, which is usually the largest? 1°2, the effect of attracting leakage magnetic flux by the magnetic sheet plate 30 is only further promoted, and the effect and action of preventing electric field concentration on the lead wire 11 is secondary. This is no different from the example shown in FIG. 3. In order to facilitate the production of the magnetic shield plate 30 shown in FIG. 4, FIG.
1! Figure 6 shows an example in which the magnetic shield plates are divided into magnetic shield plates 'e50,5], 52 in the radial direction.
さらに第7図は磁気シールド板を60〜63と高さ方向
及び径方向に分割配置した例、第8図は鉄心締付金具6
が平板1枚で構成ふれた場合に磁気シールド板70の取
付は構造全示す例であるが、いずれの場合においてもそ
の電界緩和効果及び磁束吸引効果とも第3図、第4図で
示した例と本質的に何ら変るものではない。Furthermore, Fig. 7 shows an example in which the magnetic shield plates are divided into 60 to 63 in the height direction and radial direction, and Fig. 8 shows the iron core tightening bracket 6.
This is an example in which the magnetic shield plate 70 is installed to show the entire structure when the magnetic shield plate 70 is composed of a single flat plate, but in any case, both the electric field relaxation effect and the magnetic flux attraction effect are the same as those shown in Figs. 3 and 4. There is essentially no difference.
以上説明したように、本発明によれば、巻線からの口出
し線に起因する磁気シールド部材の電界集中を効果的に
抑えることができるばかりでなく、磁気シールド部材に
よる巻線からの漏れ磁束の吸引効果を一層向上すること
ができる。As explained above, according to the present invention, it is possible not only to effectively suppress electric field concentration in the magnetic shielding member caused by lead wires from the winding, but also to reduce magnetic flux leakage from the winding due to the magnetic shielding member. The suction effect can be further improved.
第1図は従来の変圧器の内部たて断面図、第2図(a)
、 (b)は同変圧器の上部側面図及び磁気シールド板
の磁束分布図、第3図は本発明の一実施例に係る変圧器
の上部側面図、第4 fr21〜!+;8図は本発明の
他の名実棚側に係る変圧器の要部たて断面図である。
1.2・・・内側及び列側巻線、;1・・・鉄心脚部、
4゜5・・・鉄心継鉄部、11・・・し目Jil、線、
zo、:3o。
40〜42.50〜52.60へ・63.70・・・磁
気シールド板、21,3]・・・切欠き部。
第 1 図
ム
第 2 図
(0−)
Cb)
yFJ5 図
第 6 図
第 7 口
肩 8 図
白
l 2Figure 1 is an internal vertical sectional view of a conventional transformer, Figure 2 (a)
, (b) is a top side view of the transformer and a magnetic flux distribution diagram of the magnetic shield plate, FIG. 3 is a top side view of the transformer according to an embodiment of the present invention, and 4th fr21~! +; Figure 8 is a vertical sectional view of the main part of a transformer according to another nominal shelf side of the present invention. 1.2... Inner and row side winding; 1... Iron core legs;
4゜5...Iron core yoke part, 11...Jil, wire,
zo, :3o. 40 to 42.50 to 52.60・63.70...Magnetic shield plate, 21,3]...Notch part. Figure 1 Figure 2 (0-) Cb) yFJ5 Figure 6 Figure 7 Mouth shoulder 8 Figure white l 2
Claims (1)
置されて鉄心脚部間全磁気的に結合する鉄心継鉄部と、
前記鉄心脚部圧巻回された巻線と、この巻線の上下端に
位相の異なる各巻線間に渡って設けられた磁気シールド
部材とを備え、前記巻線からの口出し線を前記巻線と前
記磁気シールド部材との間隙を通して巻線の径方向外側
に引き出(7たものにおいて、前記磁気シールド部、l
における前記口出し線に対向する部分に、前記口出し線
の形状にほぼ沿うような切欠き部を設けたことを特徴と
する静止誘導電器。1. A plurality of core legs, and core yoke parts disposed at both ends of these core legs to fully magnetically couple the core legs;
The iron core leg includes a winding that is wrapped around the core leg, and a magnetic shielding member that is provided at the upper and lower ends of the winding between the windings having different phases. The winding is drawn outward in the radial direction through a gap with the magnetic shielding member (7).
A stationary induction electric appliance characterized in that a cutout portion that substantially follows the shape of the lead wire is provided in a portion facing the lead wire.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57156543A JPS5947721A (en) | 1982-09-10 | 1982-09-10 | Stationary induction apparatus |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57156543A JPS5947721A (en) | 1982-09-10 | 1982-09-10 | Stationary induction apparatus |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS5947721A true JPS5947721A (en) | 1984-03-17 |
Family
ID=15630092
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP57156543A Pending JPS5947721A (en) | 1982-09-10 | 1982-09-10 | Stationary induction apparatus |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5947721A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2002226170A (en) * | 2001-01-31 | 2002-08-14 | Ishikawajima Harima Heavy Ind Co Ltd | Automatic operating method for changing gate position by gantry crane |
JP2020043217A (en) * | 2018-09-11 | 2020-03-19 | 富士電機株式会社 | Transformer |
-
1982
- 1982-09-10 JP JP57156543A patent/JPS5947721A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2002226170A (en) * | 2001-01-31 | 2002-08-14 | Ishikawajima Harima Heavy Ind Co Ltd | Automatic operating method for changing gate position by gantry crane |
JP2020043217A (en) * | 2018-09-11 | 2020-03-19 | 富士電機株式会社 | Transformer |
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