JPS6348409B2 - - Google Patents
Info
- Publication number
- JPS6348409B2 JPS6348409B2 JP57030582A JP3058282A JPS6348409B2 JP S6348409 B2 JPS6348409 B2 JP S6348409B2 JP 57030582 A JP57030582 A JP 57030582A JP 3058282 A JP3058282 A JP 3058282A JP S6348409 B2 JPS6348409 B2 JP S6348409B2
- Authority
- JP
- Japan
- Prior art keywords
- winding
- conductor
- conductors
- section
- sections
- 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
Links
- 239000004020 conductor Substances 0.000 claims description 63
- 238000004804 winding Methods 0.000 claims description 51
- 230000007704 transition Effects 0.000 description 7
- 238000000034 method Methods 0.000 description 5
- 238000010586 diagram Methods 0.000 description 3
- 230000017105 transposition Effects 0.000 description 3
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical group [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 2
- 238000007796 conventional method Methods 0.000 description 2
- 238000001816 cooling Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000002542 deteriorative effect Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000000945 filler Substances 0.000 description 1
- 230000008707 rearrangement Effects 0.000 description 1
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
- H01F27/2871—Pancake coils
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Coils Of Transformers For General Uses (AREA)
Description
【発明の詳細な説明】
〔本発明の技術的分野〕
本発明は連続円板巻線に係り、特に内鉄形変圧
器巻線に多用される連続円板巻線の転位構造に関
する。DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a continuous disk winding, and more particularly to a transposed structure of a continuous disk winding often used in core type transformer windings.
内鉄形変圧器に使用される巻線には、その巻線
の電圧、電流に応じて種々の巻き方が選択適用さ
れているが、中でも連続円板巻線は構成の単純性
による工作の容易さ、および、電気的、機械的特
性の優秀さなどから、広範囲の電圧クラスの巻線
として多用されている。これは、連続円板巻線
が、その名に示すように巻始めから巻終り迄導体
を途中で切ることなく連続的に巻き上げて形成さ
れ、巻線途中での導体接続作業を不要とすること
に依る。その連続円板巻線の導体としては、その
必要な電流容量に応じて平角導体(矩形断面をも
つた最も一般的な導体)を1本あるいは複数本並
列に使用したり、更に電流の大きな巻線に対して
は複数本の平角導体を撚り合わせた転位電線を1
本あるいは複数本並列に使用したりしている。
Various winding methods are selected and applied to the windings used in core type transformers depending on the voltage and current of the windings, but continuous disk windings are particularly easy to work with due to their simple structure. Due to its ease of use and excellent electrical and mechanical properties, it is widely used as a winding wire for a wide range of voltage classes. As the name suggests, continuous disk winding is formed by winding the conductor continuously from the beginning to the end without cutting it in the middle, eliminating the need to connect the conductor midway through the winding. Depends on. As the conductor for the continuous disc winding, one or more rectangular conductors (the most common conductor with a rectangular cross section) may be used in parallel, depending on the required current capacity, or windings with larger currents may be used. For wires, one transposed wire is made by twisting multiple rectangular conductors.
A book or multiple books are used in parallel.
第1図のaは2本の導体を並列に使用した連続
円板巻線1の導体配置を示しており、同図bに示
す巻線A部断面図中の数字は巻回番号を、アルフ
アベツトa,bは並列の2本の導体を示してい
る。図から明らかなように巻線の1つのセクシヨ
ン2から次のセクシヨン3へ移る(これを渡りと
称している)際には並列導体はその半径方向位置
の入替が行われる。尚、図中4は鉄心脚5側に巻
回された巻線1に対向する巻線を示している。 Figure 1a shows the conductor arrangement of a continuous disk winding 1 using two conductors in parallel, and the numbers in the cross-sectional view of the winding A part shown in Figure 1b indicate the winding numbers. a and b indicate two parallel conductors. As is clear from the figure, when passing from one section 2 of the winding to the next section 3 (this is referred to as a crossing), the parallel conductors change their radial positions. In addition, 4 in the figure shows the winding opposite to the winding 1 wound on the iron core leg 5 side.
第2図は外側渡り部の斜視図である。この図か
らも判るように導体の渡りは1本毎に行われる。
こうすることにより、巻線セクシヨン2あるいは
3の半径方向寸法d(これをビルドと称している)
をその上下のセクシヨンから極端に変化させずに
巻くことができる。また、渡り時に並列導体の半
径方向位置を入替えることにより、各導体の対向
する巻線4との相対距離を平等にすることができ
る。これにより、各導体と対向する巻線間の相互
インダクタンスが等しくなり、並列導体の分流を
平等にすることができるようになる。 FIG. 2 is a perspective view of the outer transition section. As can be seen from this figure, the conductors are crossed one by one.
By doing this, the radial dimension d of winding section 2 or 3 (this is called the build)
can be wound without extreme changes from its upper and lower sections. Furthermore, by exchanging the radial positions of the parallel conductors during crossing, the relative distances between each conductor and the opposing winding 4 can be equalized. This equalizes the mutual inductance between each conductor and the opposing windings, making it possible to equalize the shunting of parallel conductors.
渡りは巻線セクシヨンの内側および外側で行わ
れるが、これらの相互位置を並列導体本数や導体
太さに応じて調整することにより、渡り部での凸
張りをなくし、内外径共ほぼ真円に巻き上げるこ
とが可能となる。 The transition takes place on the inside and outside of the winding section, but by adjusting the mutual positions of these according to the number of parallel conductors and the thickness of the conductors, the convexity at the transition section is eliminated, and the inside and outside diameters are almost perfectly round. It is possible to roll it up.
しかしながら、この従来の連続円板巻線の巻き
方には次のような不具合があつた。即ち、並列導
体が2本の場合には前述のような渡り毎の導体半
径方向位置の入替により、対向巻線に対する導体
転位が完全に行われるが、セクシヨン内の並列導
体が3本になつた場合は、導体間転位が不完全と
なり、並列導体間の分流にアンバランスが生じ、
これが巻線負荷損失を増大させ、ひいては巻線温
度を上昇させてしまうというものである。以下、
これについて説明する。
However, this conventional continuous disk winding method has the following drawbacks. In other words, when there are two parallel conductors, the conductor transposition to the opposing winding is completed by exchanging the radial position of the conductors at each crossing as described above, but when the number of parallel conductors in the section is reduced to three. In this case, the dislocation between the conductors becomes incomplete, causing an imbalance in the shunt between the parallel conductors.
This increases the winding load loss and, in turn, increases the winding temperature. below,
This will be explained.
第3図は並列導体3本、セクシヨン当りの巻回
数が2回の場合の従来の巻き方でのセクシヨン内
各導体配置を示している。図において、各並列導
体はセクシヨン毎にその半径方向位置の入替が行
われており、対向巻線に対する相互位置も一見平
等に見えるが、実は次のような不具合がある。即
ち、導体aと導体cは両者が各セクシヨン毎に対
称な位置を占めるため、転位は安全であるが導体
bは常に導体aおよびcの中間に配置される。導
体bが常に中間を占めるということは一見各導体
の配置の平均化を思わせ、事実各導体の全長はほ
ぼ同等(即ち、抵抗分は同等)になるのである
が、対向巻線に対する相互インダクタンスには無
視できない差が生じる。各導体の分流は、各導体
と対向巻線間のインピーダンスで決まるので、た
とえ相互インダクタンスに多少の差があつても抵
抗分が同等であれば分流にさほどのアンバランス
を生じない場合もあるが、特に大容量変圧器にな
るほど鉄心が太くなり、巻回線が減り、抵抗分と
インダクタンス分の比が小さくなるので極端なア
ンバランスが生じることになる。 FIG. 3 shows the arrangement of each conductor in a section in a conventional winding method in which there are three parallel conductors and the number of turns per section is two. In the figure, the radial positions of the parallel conductors are changed for each section, and although their mutual positions with respect to the opposing windings appear to be equal at first glance, there is actually the following problem. That is, since conductors a and c occupy symmetrical positions in each section, transposition is safe, but conductor b is always located between conductors a and c. The fact that conductor b always occupies the middle suggests that the arrangement of each conductor is averaged, and in fact the total length of each conductor is almost the same (that is, the resistance is the same), but the mutual inductance with respect to the opposing winding There is a difference that cannot be ignored. The shunt current of each conductor is determined by the impedance between each conductor and the opposing winding, so even if there is a slight difference in mutual inductance, if the resistance components are the same, there may not be much unbalance in the shunt current. In particular, as the transformer becomes larger in capacity, the core becomes thicker, the number of windings decreases, and the ratio of resistance to inductance becomes smaller, resulting in extreme imbalance.
この分流アンバランスは負荷損を増加させ、巻
線温度を上昇させるため変圧器特性を悪化させる
ほか、極端な場合は巻線を焼損させる等の問題が
あるため、是非とも回避する必要がある。 This shunt imbalance increases load loss and increases winding temperature, deteriorating transformer characteristics, and in extreme cases can cause winding burnout, so it must be avoided at all costs.
本発明は上記の点に鑑み、セクシヨン内並列導
体が3本の場合でも分流が平等になるような改良
された連続円板巻線を提供することを目的とす
る。
In view of the above points, it is an object of the present invention to provide an improved continuous disk winding in which the shunt current is equal even when there are three parallel conductors in a section.
この目的を達成するため、本発明は、連続円板
巻線を構成する3本の並列導体のうち、隣り合う
2本の導体を1組として残り1本の導体と半径方
向の位置を入れ替えてセクシヨン間を渡すことに
より転位を行い、全体としていずれの導体も半径
方向に占める位置の割合が等しくなるようにした
ことを特徴とする。
In order to achieve this objective, the present invention combines two adjacent conductors among the three parallel conductors constituting the continuous disk winding into one set, and swaps the positions in the radial direction with the remaining one conductor. The conductor is characterized in that the transposition is performed by passing between the sections, so that the proportion of the position occupied by each conductor in the radial direction is equal as a whole.
以下、本発明を図面を参照して説明する。 Hereinafter, the present invention will be explained with reference to the drawings.
第4図は本発明の一実施例に係る連続円板巻線
の各導体配置図を示したもので、一般の渡りは従
来方法と同一であるが、巻始めから1/3および2/3
に相当するセクシヨン間の渡り部で新規な渡り方
法をとつている。即ち、この個所の渡りは3本の
導体のうち2本は一度に渡らせ、ここでの半径方
向位置の入替は行わず、残り1本との間で位置の
入替を行い渡らせるというものである。このよう
な渡り方法とすることにより、それまで中間に位
置していた導体は渡り後には後部へ、逆に端部に
位置していた導体の一方が中央に位置することに
なる。 Figure 4 shows the arrangement of each conductor in a continuous disk winding according to an embodiment of the present invention.The general crossing is the same as in the conventional method, but from the beginning of winding to 1/3 and 2/3
A new crossing method is used at the transition between sections corresponding to . In other words, two of the three conductors are crossed at this point, and the radial position is not swapped here, but the position is swapped with the remaining one. be. By using such a crossing method, the conductor that was previously located in the middle will be moved to the rear after crossing, and conversely, one of the conductors that was located at the end will be located in the center.
従つて、巻始めから1/3と2/3でこの新規な渡り
を行うことにより、各導体が巻線の1/3ずつでそ
れぞれの中間の位置を占めるようにできる。中間
を占める区間がそれぞれ平等になれば一般のセク
シヨン間では、従来通りの渡りで両端の導体は完
全に対称配置となるので、結局巻線全長にわたつ
て各導体の占める位置が平等になり、従つて転位
が完全に行われ正しい分流が行われることにな
る。 Therefore, by making this new transition at 1/3 and 2/3 from the beginning of the winding, each conductor can be made to occupy a middle position in each of the 1/3 of the winding. If the sections occupying the middle become equal, between the general sections, the conductors at both ends will be arranged completely symmetrically with the conventional crossing, so in the end, the positions occupied by each conductor will be equal over the entire length of the winding, Therefore, the rearrangement will be completed and the current will be divided correctly.
尚、以上の説明で新規な転位を1/3、2/3に限定
したが、この位置はおよそ目安として略1/3、略
2/3とすれば十分であり、またその位置にこだわ
らずこの新規渡りを数回行つて、全体として各導
体の中間位置を占める区分がそれぞれ略1/3ずつ
になるようにすれば良いことは明白である。ま
た、2本同時に渡ることで上下のセクシヨンと半
径方向寸法差が従来方法より大きくなるが、内外
渡り位置の調整と絶縁物の詰物を入れてやること
で支障なくできる。 In addition, in the above explanation, new dislocations are limited to 1/3 and 2/3, but as a rough guide, it is sufficient to set the new dislocations to approximately 1/3 and approximately 2/3, and it is not necessary to be particular about the position. It is obvious that this new crossing can be made several times so that the sections occupying the middle positions of each conductor as a whole are approximately 1/3 each. Also, by crossing two wires at the same time, the difference in radial dimension between the upper and lower sections becomes larger than in the conventional method, but this can be done without any problem by adjusting the position of the transition between the inside and outside and inserting an insulating filler.
以上のように本発明によれば、セクシヨン内並
列導体が3本の場合でも各導体の分流が平等な連
続円板巻線が得られる。この結果、低損失で冷却
装置などを小さくしたコンパクトな変圧器を得る
ことができるようになる。
As described above, according to the present invention, even when there are three parallel conductors in a section, a continuous disk winding can be obtained in which the branch currents of each conductor are equal. As a result, a compact transformer with low loss and a small cooling device etc. can be obtained.
第1図は並列導体2本で構成された連続円板巻
線の導体配置説明図で、aはその断面斜視図、b
はそのA部拡大図、第2図は外側渡り部での導体
入替を示す斜視図、第3図は並列導体3本で構成
された従来の連続円板巻線の導体配置図、第4図
は並列導体3本で構成された本発明の一実施例を
示す連続円板巻線の導体配置図である。
1……連続円板巻線、2,3……巻線セクシヨ
ン、4……対向巻線、5……鉄心脚。
Figure 1 is an explanatory diagram of the conductor arrangement of a continuous disc winding composed of two parallel conductors, where a is a cross-sectional perspective view, and b
is an enlarged view of part A, Figure 2 is a perspective view showing conductor replacement at the outer transition section, Figure 3 is a conductor arrangement diagram of a conventional continuous disk winding composed of three parallel conductors, and Figure 4. 1 is a conductor layout diagram of a continuous disc winding wire, which is an embodiment of the present invention, and is constructed of three parallel conductors. 1... Continuous disk winding, 2, 3... Winding section, 4... Opposing winding, 5... Iron core leg.
Claims (1)
向の配置位置を対称に入れ替えて転位させながら
連続的に巻回していくことにより形成する連続円
板巻線において、少なくとも2個所のセクシヨン
間で前記3本の並列導体のうち隣接する2本の導
体を1組として残り1本の導体と半径方向の位置
を入れ替えてセクシヨン間を渡すことにより、3
本の導体の半径方向配置を平均化したことを特徴
とする連続円板巻線。1. In a continuous disk winding formed by continuously winding three parallel conductors while symmetrically changing their radial positions between sections and transposing them, the above-mentioned conductors are formed between at least two sections. By using two adjacent conductors among the three parallel conductors as one set and replacing the radial position with the remaining one conductor and passing between the sections,
A continuous disk winding characterized by an averaged radial arrangement of conductors.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3058282A JPS58148414A (en) | 1982-03-01 | 1982-03-01 | Continuous disc winding |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3058282A JPS58148414A (en) | 1982-03-01 | 1982-03-01 | Continuous disc winding |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS58148414A JPS58148414A (en) | 1983-09-03 |
JPS6348409B2 true JPS6348409B2 (en) | 1988-09-29 |
Family
ID=12307841
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP3058282A Granted JPS58148414A (en) | 1982-03-01 | 1982-03-01 | Continuous disc winding |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS58148414A (en) |
Families Citing this family (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2003105165A1 (en) * | 2002-06-11 | 2003-12-18 | 株式会社エス・エッチ・ティ | Air-core coil and manufacturing method thereof |
FI121098B (en) * | 2008-03-04 | 2010-06-30 | Abb Technology Ag | Disc Winding |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5814592Y2 (en) * | 1977-02-24 | 1983-03-23 | 株式会社ダイヘン | High series capacity transformer winding |
-
1982
- 1982-03-01 JP JP3058282A patent/JPS58148414A/en active Granted
Also Published As
Publication number | Publication date |
---|---|
JPS58148414A (en) | 1983-09-03 |
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