JPH043093B2 - - Google Patents
Info
- Publication number
- JPH043093B2 JPH043093B2 JP58202632A JP20263283A JPH043093B2 JP H043093 B2 JPH043093 B2 JP H043093B2 JP 58202632 A JP58202632 A JP 58202632A JP 20263283 A JP20263283 A JP 20263283A JP H043093 B2 JPH043093 B2 JP H043093B2
- Authority
- JP
- Japan
- Prior art keywords
- winding
- conductor
- conductors
- parallel
- insulation
- 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 - Lifetime
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
- H01F27/28—Coils; Windings; Conductive connections
- H01F27/32—Insulating of coils, windings, or parts thereof
- H01F27/323—Insulation between winding turns, between winding layers
-
- 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
- H01F27/28—Coils; Windings; Conductive connections
- H01F27/2871—Pancake coils
-
- 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
- H01F27/343—Preventing or reducing surge voltages; oscillations
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Insulating Of Coils (AREA)
Description
【発明の詳細な説明】
〔発明の技術分野〕
本発明は変圧器の低電圧大電流巻線に多用され
るヘリカル巻線を採用した変圧器巻線に関する。DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a transformer winding employing a helical winding, which is often used as a low voltage, high current winding of a transformer.
変圧器の低圧巻線は、高圧巻線と較らべて巻回
数が少なく、かつ大電流が流れるので、多くの本
数の平角導体を並列にして、らせん状に形成する
いわゆるヘリカル巻線が多用されている。この場
合、並列導体間の分流アンバランスを改良するた
め、各並列導体と対向巻線間のインピーダンスを
平衡させる必要があり、この目的で並列導体間で
は、その相対的な位置の入替が行なわれており、
これを転位と称している。
The low-voltage winding of a transformer has fewer turns than the high-voltage winding, and a large current flows through it, so so-called helical winding, in which a large number of rectangular conductors are connected in parallel to form a spiral, is often used. has been done. In this case, in order to improve the shunt imbalance between the parallel conductors, it is necessary to balance the impedance between each parallel conductor and the opposing winding, and for this purpose, the relative positions of the parallel conductors are swapped. and
This is called dislocation.
第1図は8本の並列導体の場合における最も一
般的に行なわれている転位の仕方を示している。
鉄心脚11にヘリカル巻線12を、その外側に対
向する巻線13を同心的に巻回した状態を示して
いる。ヘリカル巻線12の全高さH(巻線スタツ
クと称す)の中央で全並列導体位置を裏返すよう
な標準転位を1回、またスタツクの1/4Hと3/4H
の2個所で、並列導体の内側4本づつの2群間の
入れ替えを行なう特別転位を行なつている。この
転位の概念を第2図に示しているが、低圧のヘリ
カル巻線12の並列導体を内側と外側の2群A,
Bに分けて、各群のスタツク方向での占める位置
が示されている。このような転位を行なえば、各
並列導体の対向巻線13との間のインピーダンス
がほぼ等しくなり、その結果各並列導体に等分の
負荷電流が分流される。 FIG. 1 shows the most commonly performed transposition method in the case of eight parallel conductors.
A helical winding 12 is shown concentrically wound around the core leg 11, and a winding 13 facing the outside thereof is wound concentrically. One standard transposition that flips all parallel conductor positions in the center of the total height H of the helical winding 12 (referred to as the winding stack), and also 1/4H and 3/4H of the stack.
At two locations, special transposition is performed to swap between two groups of four inner parallel conductors. The concept of this dislocation is shown in Figure 2, where the parallel conductors of the low-voltage helical winding 12 are
The positions occupied by each group in the stack direction are shown in B. If such a transposition is performed, the impedance between each parallel conductor and the opposing winding 13 becomes approximately equal, and as a result, an equal load current is shunted to each parallel conductor.
一方、近年の省エネルギー思想の高まりに伴な
い、変圧器に対しても発生する全損失の低減が強
く要請されており、このため変圧器のコンパクト
化が一段と必要になつている。変圧器コンパクト
化の手段としては、絶縁技術の進歩による絶縁寸
法の削減とともに、導体の占積率の向上が大きな
比重を占めており、ヘリカル巻線においては各並
列導体の絶縁被覆を極小にすることが極めて有効
である。 On the other hand, with the recent rise in energy saving ideas, there has been a strong demand for reducing the total loss generated in transformers, and for this reason, it has become increasingly necessary to make transformers more compact. As a means of making transformers more compact, improvements in the space factor of the conductors are important as well as reductions in insulation dimensions due to advances in insulation technology.In helical windings, the insulation covering of each parallel conductor is minimized. This is extremely effective.
この目的で並列導体の被覆に極薄絶縁紙を使用
したり、ホルマールなどの被膜絶縁にすることが
行なわれている。ヘリカル巻線は、本来同電位の
導体を並列にして巻き上げるので、導体間の絶縁
は多くを要しないとされていた。しかしながら、
導体絶縁の極小化を進めてゆくと、導体付着の微
小な異物により、導体絶縁が局部的に破れ、導体
間に導通を生じるという不測の事態が懸念され
る。 For this purpose, the parallel conductors are covered with ultra-thin insulating paper, or with insulation films such as formal. Since helical winding originally involves winding conductors of the same potential in parallel, it was thought that there was no need for much insulation between the conductors. however,
As the conductor insulation continues to be miniaturized, there is a concern that the conductor insulation may be locally broken due to minute foreign matter attached to the conductor, resulting in conduction between the conductors.
このように各並列導体は、もともと同電位とな
るべき導体であるから、多少の導体間導通は、許
容できる場合もあるが、詳細に検討してみると、
第1図および第2図に示すようなヘリカル巻線1
2においては、負荷電流の通電時に並列導体群
A,B間には、巻線内部で約100Vのオーダーの
誘起電圧が生じることが判る。したがつて、万一
前記不測の導体間の導通が巻線内部のA,B群間
に起ると、この部分に過大な電流が流れて巻線を
焼損するおそれがある。 In this way, each parallel conductor is originally a conductor that should have the same potential, so some degree of conduction between conductors may be tolerated, but if you examine it in detail,
Helical winding 1 as shown in Figures 1 and 2
In No. 2, it can be seen that an induced voltage on the order of about 100 V is generated inside the winding between the parallel conductor groups A and B when the load current is applied. Therefore, if unexpected electrical conduction occurs between groups A and B inside the winding, an excessive current may flow through this portion and burn out the winding.
本発明の目的は、導体占積率の向上を押し進
め、変圧器のコンパクト化、低損失化を果すとと
もに異物などの附着による導体絶縁の破壊を防止
し得る変圧器巻線を提供するにある。
SUMMARY OF THE INVENTION An object of the present invention is to provide a transformer winding that can improve the conductor space factor, make the transformer more compact and reduce loss, and prevent breakdown of the conductor insulation due to adhesion of foreign matter.
本発明による変圧器巻線は、複数本の並列導体
の各々転位される並列導体群間に一般の導体絶縁
とは別個の追加絶縁を施こして巻いたことを特徴
とするものである。
The transformer winding according to the present invention is characterized in that a plurality of parallel conductors are wound with additional insulation separate from general conductor insulation between each transposed parallel conductor group.
以下本発明を第3図に示す実施例について説明
する。第3図に示す実施例の場合でも、8本の並
列導体1〜8を巻回したヘリカル巻線12を示し
ている。そして従来と同様にそのヘリカル巻線1
2の全高さHとし、そのスタツクの1/4Hづつを
下方から巻回単位1T、2T、3T、4Tとし、その
並列導体の内側4本づつ1〜4および5〜8の2
群AおよびBとして転位を行なつている。すなわ
ち、ヘリカル高さHの中央である巻回単位2Tか
ら巻回単位3Tでは、全並列導体位置を1、2、
3、4から4、3、2、1および5、6、7、8
から8、7、6、5に裏返すような標準的な転位
を1回、また巻回単位1Tから巻回単位2Tの間お
よび巻回単位3Tから巻回単位4Tの間の2個所
で、並列導体の内外4本づつの2群A,B間の入
れ替えた第2図と同様に行なう特別転位を行なつ
ている。
The present invention will be described below with reference to an embodiment shown in FIG. The embodiment shown in FIG. 3 also shows a helical winding 12 in which eight parallel conductors 1 to 8 are wound. As before, the helical winding 1
The total height of the stack is H, and each 1/4H of the stack is wound in units of 1T, 2T, 3T, and 4T from the bottom, and the inner four of the parallel conductors are 1 to 4 and 5 to 8.
Rearrangements are carried out as groups A and B. In other words, from winding unit 2T to winding unit 3T, which is the center of helical height H, all parallel conductor positions are 1, 2,
3, 4 to 4, 3, 2, 1 and 5, 6, 7, 8
A standard transition such as flipping from 8 to 7 to 6 to 5 is carried out once, and in parallel at two locations: between 1T and 2T and between 3T and 4T. A special transposition is performed in the same way as in FIG. 2, in which two groups A and B of four conductors are swapped inside and outside.
このように転位されて巻回したヘリカル巻線1
2においては、負荷電流の通電時に並列導体群
A,Bの間に100Vのオーダーの誘起電圧が生じ
ることになる。本発明においては、転位される各
導体群1〜4のA群と導体群5〜8のB群の間に
巻線全長にわたつて絶縁物14を追加挿入したこ
とを特徴としている。このように構成すれば、各
導体の絶縁被覆の極小化を進めていつても、並列
導体群A,Bの間には、別な絶縁物14を配置し
ているので、A,B群間での不測の導通の危険性
は、全くなく、ヘリカル巻線12の導体占積率向
上、しいては変圧器全体のコンパクト化と低損失
化を計ることができる。 Helical winding 1 wound in such a transposed manner
In No. 2, an induced voltage on the order of 100V is generated between the parallel conductor groups A and B when the load current is applied. The present invention is characterized in that an insulator 14 is additionally inserted over the entire length of the winding between group A of conductor groups 1 to 4 and group B of conductor groups 5 to 8 to be transposed. With this configuration, even if the insulation coating of each conductor is minimized, another insulator 14 is placed between the parallel conductor groups A and B, so There is no risk of unexpected conduction, and the conductor space factor of the helical winding 12 can be improved, and the transformer as a whole can be made more compact and have lower losses.
なお、第3図では、導体絶縁とは別個の絶縁物
14の挿入を示したが、この代りに各群A,B間
の隣接位置になる導体1,4,5および8に一般
導体とは別の追加絶縁を施こして補強しても良
い。 In addition, although FIG. 3 shows the insertion of an insulator 14 separate from the conductor insulation, instead of this, conductors 1, 4, 5, and 8 located adjacent to each group A and B are inserted with a general conductor. It may be reinforced with additional insulation.
また第3図では、各群A,B間の絶縁を巻線ス
タツクの全長にわたつて挿入したが、厳密に云う
と導体1〜8は両端で一括されるのであるから、
実際に巻線内部での導通が問題になるのは、導体
1と導体8が隣接する部分すなわち巻回単位2T
および3Tの1/2H区間であるので、この巻回単位
2T、3T部分の巻線群A,B間だけに絶縁物14
を挿入するか、あるいは導体1および8だけを他
の導体と別の追加絶縁を施す方法でも良い。さら
に並列導体数が多くなつて第4図に示すように並
列導体群A〜Dの4群に分けて転位するような場
合には、各群間に絶縁物14を挿入すれば、全く
同様の効果を得ることができる。 Furthermore, in Fig. 3, the insulation between each group A and B is inserted over the entire length of the winding stack, but strictly speaking, conductors 1 to 8 are bundled at both ends, so
Actually, the problem of conduction inside the winding is the part where conductor 1 and conductor 8 are adjacent, that is, the unit of winding 2T.
Since it is a 1/2H section of 3T, this winding unit
Insulator 14 only between winding groups A and B of 2T and 3T parts
Alternatively, conductors 1 and 8 may be additionally insulated from other conductors. Furthermore, when the number of parallel conductors increases and they are divided into four parallel conductor groups A to D as shown in Figure 4 and transposed, an insulator 14 can be inserted between each group to achieve exactly the same result. effect can be obtained.
以上のように本発明によれば、複数本の並列導
体の各々転位される並列導体群間に、一般の導体
絶縁とは別個の追加絶縁を施こしたことにより、
導体絶縁被覆の極小化を進め、導体占積率の向上
を計つたヘリカル巻線を得ることができ、異物な
どによる不測の導通不具合に対しても危惧なく製
作することができ、変圧器のコンパクト化および
低損失化を計ることができる。
As described above, according to the present invention, by providing additional insulation separate from general conductor insulation between each transposed parallel conductor group of a plurality of parallel conductors,
By minimizing the conductor insulation coating, it is possible to obtain a helical winding that improves the conductor space factor, and it can be manufactured without worrying about unexpected conduction problems due to foreign objects, making the transformer more compact. It is possible to reduce the loss and reduce the loss.
第1図は従来のヘリカル巻線とその転位状態を
示す概略構成図、第2図はその導体転位を説明す
るための概念図、第3図は本発明による変圧器巻
線の転位状態を示す概略構成図、第4図は本発明
の変圧器巻線の他の実施例による導体転位を説明
するための概念図である。
1,2……8……導体番号、11……鉄心脚、
12……ヘリカル巻線、13……対向巻線、14
……導体間挿入絶縁物。
Fig. 1 is a schematic configuration diagram showing a conventional helical winding and its transposition state, Fig. 2 is a conceptual diagram for explaining its conductor transposition, and Fig. 3 shows a transposition state of a transformer winding according to the present invention. The schematic configuration diagram, FIG. 4, is a conceptual diagram for explaining conductor transposition according to another embodiment of the transformer winding of the present invention. 1, 2...8...Conductor number, 11...Iron core leg,
12...Helical winding, 13...Opposed winding, 14
...Insulator inserted between conductors.
Claims (1)
らせん状に形成し、これら複数本の並列導体を複
数の導体群に分け、この導体群の巻線半径方向の
相対的位置の入替えにより転移を行うようにした
変圧器巻線において、各々転移される導体群間に
追加絶縁を施こしたことを特徴とする変圧器巻
線。1 A plurality of insulated conductors are arranged in parallel and formed into a spiral shape, these parallel conductors are divided into a plurality of conductor groups, and the relative positions of these conductor groups in the winding radial direction are swapped to cause transfer. A transformer winding characterized in that additional insulation is provided between groups of conductors that are transferred.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP20263283A JPS6095908A (en) | 1983-10-31 | 1983-10-31 | Winding of transformer |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP20263283A JPS6095908A (en) | 1983-10-31 | 1983-10-31 | Winding of transformer |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6095908A JPS6095908A (en) | 1985-05-29 |
| JPH043093B2 true JPH043093B2 (en) | 1992-01-22 |
Family
ID=16460559
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP20263283A Granted JPS6095908A (en) | 1983-10-31 | 1983-10-31 | Winding of transformer |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6095908A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2010109043A (en) * | 2008-10-29 | 2010-05-13 | Railway Technical Res Inst | Method of dislocating superconducting coil, and superconducting coil |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS58150208A (en) * | 1982-03-02 | 1983-09-06 | 株式会社東芝 | Dislocated wire for induction device |
-
1983
- 1983-10-31 JP JP20263283A patent/JPS6095908A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6095908A (en) | 1985-05-29 |
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