JPS5878405A - Coil for electrical apparatus - Google Patents

Coil for electrical apparatus

Info

Publication number
JPS5878405A
JPS5878405A JP17639881A JP17639881A JPS5878405A JP S5878405 A JPS5878405 A JP S5878405A JP 17639881 A JP17639881 A JP 17639881A JP 17639881 A JP17639881 A JP 17639881A JP S5878405 A JPS5878405 A JP S5878405A
Authority
JP
Japan
Prior art keywords
coil
sections
unit plate
conductors
conductor
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
JP17639881A
Other languages
Japanese (ja)
Inventor
Hiroshi Shioda
広 塩田
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
Toshiba Corp
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 Toshiba Corp, Tokyo Shibaura Electric Co Ltd filed Critical Toshiba Corp
Priority to JP17639881A priority Critical patent/JPS5878405A/en
Publication of JPS5878405A publication Critical patent/JPS5878405A/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
    • H01F27/343Preventing or reducing surge voltages; oscillations

Landscapes

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

Abstract

PURPOSE:To improve an initial voltage distribution and workability, and to obtain high quality, highly reliable coil for electric apparatus by forming a coil with four sections considered as a unit through connection between the first and fourth sections to a high cell cap coil for which two sections have been considered as a unit. CONSTITUTION:In the case of this coil, the conductors 1-16 and conductors 17-32 are wound in parallel forming a continuous plate coil of 2-column and 1- row. When the four sections are shunted, the one conductor 16 of the fourth section is cut and is connected to the conductor 17 of the first section at the point A'. In the same way, a coil is formed by repeating such process until the desired number of turns is obtained with the four sections of continuous plate coil of 2-column and 1-row considered as a unit. Therefore, a number of turns of one section is doubled, a number of all sections is reduced to 1/2, a series static capacitance is increased up to 4 times. As a result, the initial voltage distribution comes closer to a steady voltage distribution. Insulation between sections is alleviated by about 7% than that of the conventional high cell cap coil.

Description

【発明の詳細な説明】 1)発明の技術公費 本発明は高直列静電容量を持つ電気機器用=イ・ルに係
D、41に直列静電容量の一層の増加をはかつえ電気機
器用コイルに関する・ 2)ll来技術 変圧器などO′:1イルに波頭の極めて急峻な進行#I
Lが印加され九と自、電圧印加初期のコイル内の電位分
布は直列分布静電容量にと、コイルと対地関O分布静電
容量・によって決定される。ζ0初期電位分布と、コイ
ルのインダクタンスで決まる定常電位分布とt)@に@
因して、コイル内には過度電位振動を生じる。:1イル
内の局部的な絶縁及びコイル対地間の絶縁は、この電位
振動に大きく支配される・従って、フィルの絶縁を合理
化するに線電位振動を可*Ilな@シ小さくする区とが
肝要であ〉、その九めには初期電位分布を定常電位分布
に近ずけることが必要である。
[Detailed Description of the Invention] 1) Technique of the Invention Publicly Funded The present invention is for electrical equipment with high series capacitance = D, 41, for electrical equipment with further increase in series capacitance. Regarding coils, 2) Next technology transformers, etc.O': Extremely steep progression of wave crest in 1 line #I
When L is applied, the potential distribution within the coil at the initial stage of voltage application is determined by the series distributed capacitance and the distributed capacitance between the coil and the ground. ζ0 initial potential distribution, steady potential distribution determined by coil inductance, and t) @ to @
Therefore, transient potential oscillations occur within the coil. :The local insulation within one coil and the insulation between the coil and the ground are largely controlled by this potential oscillation.Therefore, in order to rationalize the insulation of the fill, it is necessary to minimize the line potential oscillation. The ninth step is to bring the initial potential distribution close to the steady-state potential distribution.

今、第illのように、コイルに電圧Vの方形液が印加
され九とき、コイル接地端νよ1)Axの点O初期電位
Vxは(1)式で表わされる。
Now, when a rectangular liquid with a voltage V is applied to the coil as shown in ill.9, the initial potential Vx at point O of the coil grounding end ν is expressed by equation (1).

但し、t:全コイル長、C!Σ・、K!ΣにαをIダラ
メータとしてV菫/VとXの関係は、第2110ように
1kD、αが小さい薯初期電位分布は定常電位分布に近
ずくことがわかる。αを小1くするには、直列静電容量
藍を大きくするか、対地静電容量Cを小さくする必要が
ある。この点に着目して、直列静電容量を大暑〈壜るよ
うに工夫したコイルにハイセルキャップコイルがある。
However, t: total coil length, C! Σ・,K! It can be seen that the relationship between V sumi/V and X, where α is an I darameter in Σ, is 1 kD as shown in the 2110th line, and the initial potential distribution approaches the steady potential distribution when α is small. In order to reduce α to 1, it is necessary to increase the series capacitance or to decrease the ground capacitance C. Focusing on this point, the HiCell Cap Coil is a coil designed to greatly reduce the series capacitance.

ハイセル中ヤッlコイルの基本構成を第3図に示す、第
311に示すように、1〜80導体と9〜16の導体(
数字は各ターン゛の導体を示す)を並列に4[、互いに
インターリーブするよう構成1れている。ハイセルキャ
ップコイルの巻自方を説明すると1先ず、2本の導体(
211本の構成が可能であるが、以下o*vta簡単の
丸め2本とする)を並列に巻−し、2R−列の連続板状
コイルからなる七タシーンを作)、最外ターンにおいて
一方O導体を切断し、セクシ冒ン関で8と90導体をム
点で接続する。以下同様に、所望するターンになる壜で
これを繰如返し点B、C,D″e*続し、第311のよ
うに構威する。
The basic configuration of the high cell medium coil is shown in Figure 3.As shown in Figure 311, conductors 1 to 80 and conductors 9 to 16 (
The numbers indicate the conductors in each turn) are arranged in parallel and interleaved with each other. To explain the winding process of the Hi-Cell Cap Coil, 1. First, there are two conductors (
A configuration of 211 coils is possible, but in the following, we will use o Cut the O conductor and connect the 8th and 90th conductors at the M point using a sexy connector. In the same manner, this is repeated until the desired turn is reached, continuing at points B, C, D''e*, and constructed as in No. 311.

3)従来技110問題点 ヒO構威によれば、最低で42セクシ璽ンにつき1個所
の接続作業を要し、導体を複数本構成とするならば、そ
の並列本数倍だけ接続個所が増加する。辷れは、インタ
ーリーブさせない連続円板コイルに比べ、コイル巻量作
業が大巾に増加し、品質面におiても接続作業が多い1
、製品の信頼性が低下し中すいという問題がある。
3) According to the prior art 110 problem HiO configuration, at least one connection is required for every 42 conductors, and if a plurality of conductors are used, the number of connection points is multiplied by the number of parallel conductors. To increase. Compared to continuous disc coils that are not interleaved, the amount of coil winding work is greatly increased, and in terms of quality, there is also a lot of connection work1.
, there is a problem that the reliability of the product decreases and the product becomes unusable.

次に、ハイ竜ル中ヤ11fコイルの直列静電容量区e計
算法について述べ石、先ず、2セクシ璽ンを一つO単位
として、例えばムB間の静電容量に′を求め、これが(
全セクシ■ン数/2)個だけ直列につながっているとす
ればKが求まる。巻回間の静電容量X′は、波llの急
峻なサージに対して杜、1〜8の導体と9〜160導体
O間に、4I形コンデンナのように分布すると考えられ
るので、(2)式で表わすことかで龜る。
Next, I will explain how to calculate the series capacitance section of the 11f coil.First, let's take a 2-sex coil as a unit of 0 and find the capacitance between M and B, for example. (
Assuming that the total number of sexes/2) are connected in series, K can be found. The electrostatic capacitance X' between turns is considered to be distributed like a 4I type capacitor between conductors 1 to 8 and conductors 9 to 160 in response to a steep surge of wave 11, so (2 ) Expression is difficult.

−−−−−−−−−−−(2) jjで、−:素線絶縁物O誘電率、r : @ IIa
O平均半働、b :素線幅、t;素−絶縁の両側厚1、
n:セクシ璽ン幽シの巻回数。
−−−−−−−−−−−(2) jj, −: dielectric constant of strand insulator O, r: @ IIa
O average half-work, b: Width of wire, t: Thickness on both sides of bare insulation 1,
n: Number of turns of the sexy seal.

従りて、全直列静電容量区はに′が直列K(全セクシ■
ン歇/2)個つながっているとして、但し、N:全セク
シ冒ン数 ζζで、@gtabg%線一つOコイルについて紘定数
であるから、Kは(m/N)Kはぼ比例することになる
Therefore, the total series capacitance section is
Assuming that 2) are connected, where N is the total number of sexy connections ζζ, @gtabg% is the Hiro constant for one O coil, so K is approximately proportional to (m/N). It turns out.

因に、連続円@ y 4 k O(1は20〜2sli
jI!テToj+、^イ七ルキャップーイルでは、これ
が2.5〜3. S Ii度に改善されるものの未だ不
満足な値である。
Incidentally, continuous circle @ y 4 k O (1 is 20 to 2sli
jI! In TeToj+, ^I7 Le Cap Ile, this is 2.5 to 3. Although it has been improved to SII degrees, it is still an unsatisfactory value.

4)発明の目的 本発明は、従来コイルと巻線の平均半117%素線幅1
1素纏絶縁の両側厚さt1セタシ冒ン尚)の巻回数n1
全セクシ■ン数Nは全く同一としながらも、直列静電容
量を従来のハイセルキャvfクイルに対し増加させるこ
とによシ、αをよ〕減少し、初期電位分布を大幅に改善
すると共に、作**を改善し、高品質、高信頼性の電気
機器用コイルを提供することを目的とする。
4) Purpose of the Invention The present invention aims to reduce the average wire width of conventional coils and windings by 117%.
Thickness on both sides of 1 piece of insulation t1 Number of turns n1
By increasing the series capacitance compared to the conventional high cell capacitor VF quill while keeping the total number of sexes N exactly the same, α can be greatly reduced, and the initial potential distribution can be greatly improved. The purpose is to improve the ** and provide high quality, highly reliable coils for electrical equipment.

5)発明の構成 ζOIi的を達成するため、本発9II線、従来2セク
シ冒ンt I Jlffiとしていたハイセルキャッ!
コイkfC対し、嬉11第4七クシ■ン間において接続
を行うことによ〉、4セタシ冒ンを1単位としてコイル
を構威しえことを特徴とする特6)発@O実施例 以下、本発明を図の実施例を参照して説−する。
5) Structure of the Invention In order to achieve the purpose of ζOIi, the 9II line of the present invention has been changed to a high cell cap, which had previously been 2-sexy.
By connecting between the 4th and 7th wires of the coil kfC, a coil can be constructed with 4 sets of wires as one unit 6) Example @O Example below , the invention will be explained with reference to the embodiments shown in the figures.

第4図線本発明による;イルの基本構成を示したもので
、このコイルの巻き方は1〜16の導体と17〜320
導体(並列K11lして2段1列の連続板状コイルを作
)、これを4−にクシ曽ン分巻IN、九とζろで第4セ
クシ曹ンの一方の導体16を切断し、第1セクシ曹ンの
導体17にム′点で接続する。以下同様に、2段1列O
連続板状コイル4セクシ冒ンを単位として所望するター
ンになる壜で繰勤返し、図示コイルを構成する。
Figure 4 shows the basic structure of the coil according to the present invention, and the winding method of this coil is 1 to 16 conductors and 17 to 320 conductors.
Conductor (parallel K11l to make two stages and one row of continuous plate-like coils), wind this into 4-circle winding IN, cut one conductor 16 of 4th winder at 9 and ζ-ro, It is connected to the conductor 17 of the first conductor at point M'. Similarly, 2 rows 1 row O
The coil shown in the figure is constructed by repeating the continuous plate-shaped coil in units of 4 squares to form a desired turn.

本発@による;イルの静電容量を考える丸め、第5Il
lをかかげる。第51Iは第411における偶数番目の
竜タシ曹ンを奇数II目のセクシ■ンに並べて画いてい
るが、直列静電容量0分布について紘第4図と等価であ
る。第3図と第5図を比較すると、l七りシ謬ン幽)の
ターン数は2倍KID食セクシーン数紘1/2 Kなっ
て11:いる、従りて、前記(3)式よ)直列静電容量
区ははぼ4倍増し、ヒO艙呆、αは1/2 K tす、
初期電位分布が定常電位分布に近ずくととが判る。
According to the original @; Rounding considering the capacitance of Il, 5th Il
Hold up l. No. 51I is drawn with the even-numbered sections of No. 411 lined up with the odd-numbered sections II, and is equivalent to FIG. 4 with respect to the zero distribution of series capacitance. Comparing Figure 3 and Figure 5, the number of turns in 17rishimanyu) is doubled as KID food sexy number 1/2 K becomes 11: Therefore, the above formula (3) ) The series capacitance increases by about 4 times, and α becomes 1/2 Kt.
It can be seen that the initial potential distribution approaches the steady potential distribution.

次に、本発@によるフィルの絶縁について検討してみる
Next, let's consider the insulation of the fill using the present invention.

板状コイルではターン間絶縁、七りシ冒ン間絶縁及び対
地絶縁が主な検討対象となる。そζで、先ずターン間に
りいて考える。定常状部において、第3![と第4園を
比較すると、第3図″cdターン関KFil−−ン幽J
)0鱒起電圧を・として211@の電圧がかかるOK対
し、第4図で紘その2倍の4m@0電圧がかかる。但し
、これは後で述べる初期電位分布で龜する分担電圧に比
べ十分に低いもOfあnS*に問題とはならない0次に
?−ジに対する初期−位分布によ 担は第1セタシ冒ン0@き始めのターン間に生じ、その
大11さV■a(4)式で表わされる。
For plate-shaped coils, the main considerations are insulation between turns, insulation between windshields, and ground insulation. So, first, think about it between turns. In the steady state part, the third! [If you compare the 4th garden with
) In contrast to OK, where a voltage of 211 @ is applied, assuming the electromotive voltage of 0, a voltage of 4 m @ 0, which is twice that, is applied in Fig. 4. However, although this is sufficiently low compared to the shared voltage caused by the initial potential distribution, which will be described later, it does not pose a problem for OfAnS*. Due to the initial position distribution for -ji, the charge occurs during the first turn of the first set-up, and its magnitude is expressed by the equation (4).

(4)弐に従来のハイ竜ルキャッfプイルの代表的な数
値として111111130. %wtm@ Q、 α
+++x3を代入すると、 これに対し、本発WIAKよるコイルではα#1.sで
*=60.N−30に等しいので、 ・・・・・・−・・・・・・・(6) となシ、(6)と(5)を比較すると、り131、たか
だかlG−しか増加しない。
(4) 2. A typical value for the conventional high dragon le cap f pool is 111111130. %wtm@Q, α
By substituting +++x3, on the other hand, in the coil based on the original WIAK, α#1. *=60 in s. Since it is equal to N-30, (6) and (6), comparing (6) and (5), it increases by only 131, at most 1G-.

次に、セクタ璽ン関の絶縁を考える。第3図、第4図に
おいてわかるように、従来のハイセル今ヤツf:Iイル
では第2セクシ璽ンと1s3セクシ■ンのコイル内側に
おいても最も高い電圧を生じ、本発明によるコイルでは
第4セクシ■ンと第5セクシ■ンの間に最も高い電圧を
生じる。この値線、従来のハイセル中ヤツf:1イルO
場合は(8)式、本発明によるコイルでは(9)式で示
される。
Next, consider the insulation of the sector seal. As can be seen in FIGS. 3 and 4, the highest voltage is generated inside the coils of the second sex and the 1s3 sex in the conventional HiCell F:I coil, and in the coil according to the present invention, the highest voltage is generated inside the coil in the fourth sex. The highest voltage is generated between sex 1 and the 5th sex. This value line, the conventional high cell middle guy f: 1 il O
The case is expressed by equation (8), and the coil according to the present invention is expressed by equation (9).

先1と同じ(N+am180 G、 1103 Gを両
式に代入すゐと、 ・・−・・・・・・・・・・・(2) となり、輪と軸を比較すると、 つまb1本発14によるフィル社、7−@変従来のハイ
セルキャッf−:1イルよクセクシ1フ間O飴縁が軽減
されることになる。
Same as above 1 (substituting N+am180 G, 1103 G into both equations, we get ・・・-・・・・・・・・・・・・(2), and comparing the ring and the shaft, we get: 14) According to Phil, Inc., 7-@ change conventional Heiserukyaf-: 1 Illustrated between 1 and 1 F O candy edges will be reduced.

以上、ターン間、セクシ冒ン間の絶縁に対しては、本発
明によるコイルが従来のハイセルキャップコイルとほぼ
同等であることを示し九が、最後に;イルと鉄心との間
の寸法中、油入変圧11KThけるフィルとタンク間の
寸法を支配し、機器全体の大きさに最も大暑く影響する
対地絶縁について考察する。
The above shows that the coil according to the present invention is almost equivalent to the conventional high cell cap coil in terms of insulation between turns and between the iron core. We will consider ground insulation, which governs the dimensions between the fill and tank of an oil-immersed transformer of 11KTh, and which has the greatest effect on the overall size of the equipment.

対地絶縁にりいては、コイルの両端からイン/1ルス波
形を印加するいわゆる非接地インdルス試験が条件的に
最も厳しく、Δ結線の場合であれば*mの中央の電位が
、を九人結線であれば中性点の電位が電位振動によ)印
加電圧よ)も高い最大値をとる。
Regarding ground insulation, the so-called ungrounded in-d pulse test in which an in/1 pulse waveform is applied from both ends of the coil is the most severe in terms of conditions. If it is a human connection, the potential at the neutral point (as well as the applied voltage) will take a high maximum value due to potential oscillation.

本発1によるコイルでは、上記電位振動が抑制されてい
るので、対地絶縁の軽減を社かること−で自1例えば油
入変圧1)KTh叶るタンク−コイル間の距離の縮み、
タップ切換IIO対地絶縁の軽減など電気機量O小形軽
量化に寄与す、&ヒとができる・ 一方、=イル巻llO際、導体の切断及び接続作業が半
減される丸め、加工工数の大巾な削減と、信**の向上
にも多大な効果がある・ D発明の変形例 嬉・図は本発$10他O実施例を示し、第4図とは逆に
接続線の方を外側にしたものである。このようにしても
、本発@0効果を何ら損うものではない、を九、本文中
の説明は全て1ターンあ九シ1本の導体について説−し
たが、lターンあ九如2m本であってもこれと同勢の効
果があることは言う迄もない。
In the coil according to the present invention 1, the above-mentioned potential vibration is suppressed, so by reducing the ground insulation, the distance between the tank and the coil can be reduced.
Tap switching IIO contributes to the miniaturization and weight reduction of electric equipment, such as reducing the need for ground insulation.On the other hand, during coil winding, the cutting and connecting work of the conductor is halved, and the number of machining steps is greatly reduced. It is also very effective in reducing the amount of damage and improving reliability**. ・Modified example of the D invention. This is what I did. Even if this is done, the main @0 effect will not be impaired in any way.The explanation in the main text is based on one conductor with one turn and one conductor. Needless to say, it has the same effect as this.

8)発−の効果 以上Oように本発明によれば、従来のハイセル中ヤツ!
コイルに対し、電位振動特性を向上させ、411にセク
タ1冫間絶縁及び対地絶縁を軽減し、更に、作業性を改
善し、高信頼性にして、機器全体の小拳帳量化に貢献す
る電気機器用コイルを得ることができる。
8) According to the present invention, the effect of the release is more than that of the conventional high cell medium!
The electric potential oscillation characteristics of the coil are improved, the insulation between sectors 1 and ground insulation is reduced, and the workability is improved and reliability is improved, contributing to the miniaturization of the entire device. A coil for equipment can be obtained.

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

第1図は電位振動を説明する丸めの等価回路図、第2図
はαをdラメータとして第11IIKおける電位分布を
示すグラフ図、第3図は従来のハイセルキャップコイル
のターン構成を示す断面図、第4図は本発明の一実施例
を示す断面図、第5固状第4図におけ為直列静電容量を
求めるための説明図、gasは本発明の他の実施例を示
す断面図である。 l〜64・・・導体のターン、ム、 B 、 C、D、
A′。 B′・・・接続箇所。 第1図 第2図 )(、jX、4 第3図 第4図 第5図 第6図
Fig. 1 is a rounded equivalent circuit diagram explaining potential oscillations, Fig. 2 is a graph showing the potential distribution at No. 11IIK with α as a d parameter, and Fig. 3 is a cross section showing the turn configuration of a conventional high cell cap coil. Figure 4 is a sectional view showing one embodiment of the present invention, 5th solid state is an explanatory diagram for determining the series capacitance in Fig. 4, and gas is a cross-sectional view showing another embodiment of the present invention. It is a diagram. l~64...Conductor turn, M, B, C, D,
A'. B'...Connection point. (Fig. 1, Fig. 2) (, jX, 4, Fig. 3, Fig. 4, Fig. 5, Fig. 6)

Claims (1)

【特許請求の範囲】[Claims] 2m本(1は自然数)の導体をコイル外側よ〉内側へ向
りて巻回し九第1の単位板状コイルと、コイル内側にお
いて全導体を切断することなく第1の単位板状コイルか
ら第2の単位板状コイル内側に弧長しえわた勤加工部と
、コイル内側から外側へ向ってIIIした第2の単位板
状フィルと、コイル外側において全導体を切断すること
な(第2の単位板状コイルから第3の単位板状コイル外
側に砥長しえわ九)加工部と、フィル外側から内側へ肉
って巻回し九第3の単位板状コイルと、コイル内側にお
匹て全導体を切断することなく第3の単位板状;イルか
も第40単位板状コイル内儒に延長し九わ九〉加工部と
、フィル内側から外側へ向りて巻回しえ第4の単位板状
コイルとからなるフィル群を複数個備え、IQOwイル
群の第40単位板状ツイルの最外ターンの導体のうち1
本′は切断せずに隣接する他のコイル群へのわたプとし
、1111)の1本はjllo単位板状コイル0最外タ
ーンの導体のうち1本と接続したことを特徴とする電気
機饅コイル。
A 2m conductor (1 is a natural number) is wound from the outside of the coil to the inside to form a first unit plate coil. A second unit plate-like fill is formed by forming an arc-length cutting part on the inside of the second unit plate-like coil, and a second unit plate-like fill that extends from the inside of the coil toward the outside. 9) Grind the unit plate coil to the outside of the third unit plate coil. 9) Wind the fill from the outside to the inside. Without cutting the whole conductor, extend the third unit plate-shaped coil to the inside of the 40th unit plate-shaped coil and wind it from the inside of the fill to the outside. One of the conductors of the outermost turn of the 40th unit plate-like twill of the IQOw coil group.
This electric machine is characterized in that the main coil is connected to another adjacent coil group without being cut, and one of the coils of 1111) is connected to one of the conductors of the outermost turn of the jllo unit plate coil 0. Steamed rice coil.
JP17639881A 1981-11-05 1981-11-05 Coil for electrical apparatus Pending JPS5878405A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17639881A JPS5878405A (en) 1981-11-05 1981-11-05 Coil for electrical apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17639881A JPS5878405A (en) 1981-11-05 1981-11-05 Coil for electrical apparatus

Publications (1)

Publication Number Publication Date
JPS5878405A true JPS5878405A (en) 1983-05-12

Family

ID=16012965

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17639881A Pending JPS5878405A (en) 1981-11-05 1981-11-05 Coil for electrical apparatus

Country Status (1)

Country Link
JP (1) JPS5878405A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0311707A (en) * 1989-06-09 1991-01-21 Toshiba Corp Superconductive magnet

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0311707A (en) * 1989-06-09 1991-01-21 Toshiba Corp Superconductive magnet

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