JPH02155208A - High series-capacitance disc winding - Google Patents

High series-capacitance disc winding

Info

Publication number
JPH02155208A
JPH02155208A JP30917288A JP30917288A JPH02155208A JP H02155208 A JPH02155208 A JP H02155208A JP 30917288 A JP30917288 A JP 30917288A JP 30917288 A JP30917288 A JP 30917288A JP H02155208 A JPH02155208 A JP H02155208A
Authority
JP
Japan
Prior art keywords
disc
winding
conductors
conductor
disk
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
JP30917288A
Other languages
Japanese (ja)
Inventor
Masaaki Kosaka
正明 高坂
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.)
Fuji Electric Co Ltd
Original Assignee
Fuji 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 Fuji Electric Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP30917288A priority Critical patent/JPH02155208A/en
Publication of JPH02155208A publication Critical patent/JPH02155208A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To simplify winding work, and to improve reliability by composing a high series-capacitance disc winding of a central-section disc winding having an even number of parallel conductors, an upper-end section disc winding, which is installed to the upper end section of the central-section disc winding and parallel conductors of which are halved, and a lower-end section disc winding, which is mounted to the lower end section of the central-section disc winding and parallel number and the number of turns of which are made the same as the upper-end section disc winding. CONSTITUTION:Two conductors 1c, 1d are branched from an upper terminal 22 for their connection, and the conductor 1c is positioned on the outside diameter side of the disc coil 15 and the conductor 1d on the inside diameter side of a disc coil 16. The conductor 1c reaches to the inside diameter side in the disc coil 15 and is connected to the conductor 9c of the disc coil 16. Adjacent disc coils are mutually connected in series in a connecting section 34 on the outside diameter side and a connecting section 35 on the inside diameter side in the same manner as a normal disc winding up to immediately before the conductors 9c and 1d are unified on the inside diameter side of the disc coil 16 and connected to a disc coil 21. Lastly, two parallel conductors are integrally bonded electrically by a lower terminal 23 by a connection system reverse to the disc coil 15 in the disc coil 21.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は雷などの衝撃電圧に対する変圧器の高電圧円
板巻線の、絶縁耐力を向上させた巻線として使用される
高直列容量円板巻線に関する。
[Detailed Description of the Invention] [Field of Industrial Application] This invention is a high-series capacitance circular winding used as a high-voltage disc winding of a transformer with improved dielectric strength against shock voltages such as lightning. Regarding plate winding.

〔従来の技術〕[Conventional technology]

変電所などに設置される電力用変圧器が接続されている
電力系統に雷が直接落下する直接雪や、近くでの落雷や
雷雲内での放電によって送電線に誘導される誘導雷など
によって、電力系統に急激に変化する衝撃電圧が発生す
るという現象がある。
Lightning can be caused by direct snowfall, where lightning falls directly onto power systems connected to power transformers installed at substations, or induced lightning, which is induced into power transmission lines by nearby lightning strikes or discharges within thunderclouds. There is a phenomenon in which a sudden change in shock voltage occurs in a power system.

この衝撃電圧は電力系統の送電線や接続されている変圧
器や遮断器などの電気機器に侵入して送電線や電気機器
を絶縁破壊に到らしめることがあるので、これを回避す
るために、避雷器を設置したりして電気機器に許容され
る衝撃電圧以上の高い電圧が印加されないように保護を
するという方式%式% 変圧器や遮断器などの電気機器は電力系統の電圧の高さ
に応じた衝撃電圧に耐えるよう規格に定められており、
この絶縁耐力を確認するために、雷によって発生する衝
撃電圧を模擬することのできる衝撃電圧発生器によって
発生させた電圧をこれら電気機器に印加するという試験
が行われ、この試験は衝*a圧試験と呼ばれている。
This shock voltage can invade power system transmission lines and connected electrical equipment such as transformers and circuit breakers, causing dielectric breakdown in power transmission lines and electrical equipment, so to avoid this, A method of protecting electrical equipment from applying a voltage higher than the permissible shock voltage by installing lightning arresters, etc. Electrical equipment such as transformers and circuit breakers are used to protect electrical equipment from the high voltage of the power system. It is specified in the standard to withstand the shock voltage according to the
In order to confirm this dielectric strength, a test was conducted in which a voltage generated by a shock voltage generator capable of simulating the shock voltage generated by lightning was applied to these electrical devices. It's called a test.

変圧器の場合、衝撃電圧が印加された巻線がこの衝撃電
圧に共振して巻線内部で局部的な電圧の集中が生ずると
いう問題があることが知られており、このような現象は
一般に電位振動と呼ばれている。特に超高圧の変圧器巻
線の場合、電位振動を抑制して巻線内の衝撃電圧の分布
がなるべく−様になるようにして局部的に電圧が集中す
ることのないようにすることが重要で、そのための巻線
内の電位振動をシミュレーションするためのコンピュー
タによる技術計算プログラムが開発されており、精度の
よい計算技術を基礎にして最適巻線構成の研究開発が進
められている。
In the case of transformers, it is known that there is a problem in which the windings to which an impact voltage is applied resonate with the impact voltage, causing local voltage concentration inside the windings, and this phenomenon generally occurs. This is called potential oscillation. Particularly in the case of ultra-high voltage transformer windings, it is important to suppress potential oscillations and make the distribution of shock voltage within the windings as uniform as possible to avoid local concentration of voltage. For this purpose, a computer-based technical calculation program has been developed to simulate the potential oscillations within the winding, and research and development of the optimal winding configuration is progressing based on highly accurate calculation technology.

円板巻線は他の高圧巻線、たとえば、多層円筒巻線など
に比べて構造が簡単なことから外部短絡による11磁力
に対する機械的強度が大きいとか、製作が容易であると
か、設計上の自由度が高いなどの重要な利点があること
から、500KVの超々高圧変圧器にも使用されている
。その代わり、電位振動を抑制して衝%l電圧に対する
絶縁耐力の高い円板巻線が使用される。このような円板
S線として最も一般に使用されるものの中に高直列容量
円板巻線と呼ばれている円板巻線がある。
Disk windings have a simpler structure than other high-voltage windings, such as multilayer cylindrical windings, so they have greater mechanical strength against the magnetic force caused by external short circuits, are easier to manufacture, and have design considerations. Because it has important advantages such as high degree of freedom, it is also used in 500KV ultra-high voltage transformers. Instead, a disk winding is used which suppresses potential oscillations and has a high dielectric strength against voltage. Among the most commonly used disk S wires is a disk winding called a high series capacitance disk winding.

円板巻線に衝撃電圧が印加されたときの巻線内部に発生
する電位振動の大きさは衝撃電圧が印加された直後の巻
線内に生ずる電位分布の様相によっておおよその判断が
可能である。この電位分布は初期電位分布と呼ばれてい
るが、この初期電位分布は主に円板巻数の対地静電容量
としての並列容量と円板巻数内の静電容量としての直列
容量の比率から決まる分布をする。その分布は印加端が
印加電圧に等しく巻線内部に侵入するほど減衰する分布
をし、減衰の激しい分布の場合、略指数関数状の減衰関
数となる。この関数を数学的に表現し変数を円板コイル
の個数にすると、指数部の変数である円板コイルの個数
にかかる係数は一般にαで表現され、このαは前述の並
列容量Cの直列容量Kに対する比の平方根で表される。
When an impact voltage is applied to a disk winding, the magnitude of the potential oscillation that occurs inside the winding can be approximately determined by the appearance of the potential distribution that occurs within the winding immediately after the impact voltage is applied. . This potential distribution is called the initial potential distribution, and this initial potential distribution is mainly determined by the ratio of the parallel capacitance as the ground capacitance of the number of disc turns and the series capacitance as the capacitance within the number of disc turns. Make a distribution. The distribution is such that the applied end is equal to the applied voltage and is attenuated as it penetrates into the winding, and in the case of a distribution with severe attenuation, it becomes a substantially exponential attenuation function. When this function is expressed mathematically and the variable is the number of disc coils, the coefficient on the number of disc coils, which is the variable in the exponent part, is generally expressed as α, and this α is the series capacitance of the parallel capacitance C mentioned above. It is expressed as the square root of the ratio to K.

αが大きい初期電位分布が急激は減衰する分布となり、
αが0の場合は平等分布となる。αが大きくまた円板コ
イルの数が充分大きい場合には、印加端での円板コイル
間にかかる電圧は電位分布が−様な場合のα倍になる0
円板巻線の衝撃電圧による電位振動を抑制するにはこの
αの値を小さくする゛ことが最も基本的な対策であり、
高直列容量円板巻線とはこのαを小さくするために、直
列容量が大きくなるような接続方式とした円板巻線の一
種である。
The initial potential distribution with a large α suddenly becomes a distribution that attenuates.
When α is 0, the distribution is equal. If α is large and the number of disc coils is large enough, the voltage applied between the disc coils at the application end will be α times the voltage when the potential distribution is −-like.
The most basic measure to suppress the potential vibration caused by the impact voltage of the disk winding is to reduce the value of α.
A high series capacitance disk winding is a type of disk winding that uses a connection method that increases the series capacitance in order to reduce α.

直列容量は、隣合う円板コイル間や導体間などの幾何学
的配置によって定まる静電容量に蓄積される静電エネル
ギーの総和に一致する等価的な静電容量として定義され
る。このような直列容量の定義に基づく計算方式は蓄積
エネルギー法と呼ばれることがある。
Series capacitance is defined as an equivalent capacitance that corresponds to the sum of electrostatic energy stored in the capacitance determined by the geometrical arrangement, such as between adjacent disk coils or conductors. A calculation method based on such a definition of series capacitance is sometimes called a stored energy method.

静電容量に蓄積される静電エネルギーは、周知のように
、静電容量と電圧の二乗の積の2分の1となる。したが
って幾何学的配置から定まる静電容量が同じであっても
、接続方式を工夫してこの静電容量にかかる電圧を大き
くすることにより、等価的な静電容量としての直列容量
を増大することができる。
As is well known, the electrostatic energy stored in the capacitance is one half of the product of the capacitance and the square of the voltage. Therefore, even if the capacitance determined from the geometric arrangement is the same, by devising the connection method and increasing the voltage applied to this capacitance, the series capacitance as an equivalent capacitance can be increased. Can be done.

第2図は従来技術の高直列容量円板巻線の例を示す巻数
の断面概略図でもある導体配列図である。
FIG. 2 is a conductor arrangement diagram which is also a cross-sectional schematic diagram of the number of turns showing an example of a conventional high series capacitance disc winding.

この図は2並列導体からなる高直列容量円板巻線を示し
たものであり、それぞれの導体の参照符号は、数値が上
部端子22から数えた巻数であり、この数値の後に付し
た英字a、bは連続する導体の区別を表している。すな
わち、英字aを付した導体は全て直列に接続されて電気
的に1本の導体となる導体断面を示したものであり、英
字すを付した導体も同様である。すなわち、この回の晶
直列容量円板巻線はa、l!:bを付した2本の導体か
らなる2並列導体の円板巻線である。
This figure shows a high series capacitance disk winding consisting of two parallel conductors. , b represents the distinction between continuous conductors. That is, the conductors marked with the letter a are all connected in series to form a single electrical conductor, and the same applies to the conductors marked with the letter a. That is, the crystal series capacitance disk windings of this time are a, l! : It is a disk winding of two parallel conductors consisting of two conductors marked with b.

上部端子22から分岐した2本の導体は最初に円板巻線
11の巻き始めの1ターンとしての導体la、lbとな
り、その後、2a、2b、3a3bという順序で電気的
に接続されている。導体la、lbと導体5a、5bと
は4本まとめて巻回された構成となっており、2タ一ン
巻回されて円板コイル11を形成している。同じように
して円板コイル12.13.14も構造的には4本の導
体をまとめて2タ一ン巻回することによりそれぞれの円
板コイルが形成されている。2ターンというのは作図上
最少の巻数で表示したものであって実際の円板コイルで
は種々の巻数のものがあり、5ターンかそれ以上あるの
か普通である。
The two conductors branched from the upper terminal 22 first become conductors la and lb as one turn at the beginning of winding of the disc winding 11, and are then electrically connected in the order of 2a, 2b, and 3a3b. The conductors la, lb and the conductors 5a, 5b have a configuration in which four conductors are wound together, and are wound in two turns to form a disk coil 11. Similarly, the disk coils 12, 13, and 14 are structurally formed by winding four conductors together with two turns. 2 turns is the minimum number of turns shown in the drawing, and actual disk coils have various numbers of turns, usually 5 turns or more.

このように形成された円板コイル11.12は図に示す
ように、内径側である図の左側の接続部31で円板コイ
ル11と12のそれぞれ4本の導体が接続され、外径側
の接続部32で円板コイル】2の導体4a、4bと円板
コイル11の導体5a、5bとが接続される。このよう
な接続によって、上部端子22から始まって導体1a、
lbを巻き始めの導体として、円板コイル11と12と
を2回転して最後に導体8a、8bに至る接続方式にな
る。
As shown in the figure, the disc coils 11 and 12 formed in this way have four conductors connected to each of the disc coils 11 and 12 at the connection part 31 on the left side of the figure, which is the inner diameter side, and The conductors 4a, 4b of the disc coil [2] and the conductors 5a, 5b of the disc coil 11 are connected at the connecting portion 32 of the disc coil 11. With such a connection, starting from the upper terminal 22, the conductor 1a,
The connection method is such that the disk coils 11 and 12 are rotated twice with lb as the conductor at the beginning of winding, and finally the conductors 8a and 8b are reached.

同じようにして円板コイル13.14も円iコイル11
.12の巻き終わりの導体8a、8bに接続部33で接
続された導体9a、9bを巻き始め導体として、円板コ
イル11.12と同じ接続方式で接続される。このよう
にして、2つの円板コイルを1組にした接続が行われる
とともに、それぞれの組が直列接続されることにより1
つの高直列容量円板巻線が形成される6回では円板コイ
ルを7つしか図示していないが、実際の高直列容量円板
巻線は数十個の円板コイルからなっているのが普通であ
る。
In the same way, the disk coils 13 and 14 are also connected to the circular i coil 11.
.. The conductors 9a and 9b connected to the winding end conductors 8a and 8b of No. 12 at the connecting portion 33 are used as winding start conductors and are connected in the same connection method as the disc coils 11 and 12. In this way, the two disc coils are connected as one set, and each set is connected in series, so that one
Although only seven disc coils are shown in the figure in which two high series capacitance disc windings are formed, an actual high series capacitance disc winding consists of several dozen disc coils. is normal.

このように導体が巻数の増加に伴って2つの円板コイル
の中を回転するようにその位rを変えることにより、巻
き始めの導体と1回転してきた導体とが一緒になっても
う1回転するという接続方式が高直列容量円板巻線の特
徴である。この図では2並列導体の例を示しであるが、
1本の導体だけの場合や2並列2重の4本導体の高直列
容量円板巻線なども実用されている。
In this way, by changing the degree r so that the conductor rotates in the two disk coils as the number of turns increases, the conductor at the beginning of winding and the conductor that has made one rotation can rotate one more time together. This connection method is a characteristic of high series capacity disc windings. This figure shows an example of two parallel conductors, but
High series capacitance disk windings with only one conductor or two parallel double conductors with four conductors are also in practical use.

高直列容量円板巻線特有の接続方式によって、隣合う導
体間の誘起電圧が1ターンの誘起電圧の複数倍になる部
分が生ずる6円板コイル11の例によると、導体1bの
隣の導体5aとは4タ一ン分の誘起電圧の差が生ずる。
According to the example of the six-disc coil 11, where the induced voltage between adjacent conductors is multiple times the induced voltage of one turn due to the connection method peculiar to high series capacitance disk windings, the conductor next to the conductor 1b 5a, there is a difference in induced voltage of 4 tanns.

同じようにして、他の円板コイル12.13.14にお
いても各導体の参照符号の数値の差がそれぞれの隣合う
導体間の誘起電圧の1ターンに対する倍率を表している
Similarly, in the other disc coils 12, 13, and 14, the difference in the numerical values of the reference symbols of each conductor represents the magnification of the induced voltage between each adjacent conductor for one turn.

このような接続方式の高直列容量円板SvAにおける2
つの円板コイルからなる1111の円板コイル当たりの
直列容量は、誘起電圧が1ターンの複数倍になっている
導体間の静電エネルギーの総和を1組の円板コイルの誘
起電圧で除して2倍したものになる。lターン当たりの
誘起電圧は除される値と除する値との双方に含まれてい
るので、この1ターン当たりの誘起電圧が幾らであるか
は直列容量計算の上で関係ない値となる0円板コイル間
の静電容量は高直列容量円板巻線の場合には、直列容量
に占める割合が小さいので、ここでは無視する。
2 in the high series capacitance disk SvA of this connection method.
The series capacitance per 1111 disc coil consisting of two disc coils is calculated by dividing the sum of electrostatic energy between conductors whose induced voltage is multiple times that of one turn by the induced voltage of one set of disc coils. It becomes twice as much. Since the induced voltage per l turn is included in both the value to be divided and the value to be divided, the induced voltage per turn is a value that is irrelevant when calculating the series capacitance. In the case of a high series capacitance disk winding, the capacitance between the disk coils accounts for a small proportion of the series capacitance, so it is ignored here.

円板コイル11.12の1組の円板コイルの場合につい
て、具体的な数値でM積エネルギー法を適用すると次の
ようになる。
When the M product energy method is applied to the case of a set of disc coils 11 and 12 using specific numerical values, the result is as follows.

円板コイル11.12で隣合う導体間の誘起電圧の差が
4タ一ン分になるのが導体1bと5a、2bと6a、8
aと4b、7aと3bの4箇所、3タ一ン分になるのが
5bと2a、4aと7bの2箇所である。静電エネルギ
ーは幾何学的配置によって決まる静電容量と電圧の二乗
の積の2分の1であるから、総静電エネルギーに相当す
る値は、4の二乗である16の4倍の64と3の二乗で
ある9の2倍の18との和である82が得られる。
In the disc coil 11.12, the difference in induced voltage between adjacent conductors is 4 tans for conductors 1b and 5a, 2b and 6a, and 8.
There are four locations, a and 4b, and 7a and 3b, and two locations, 5b and 2a, and 4a and 7b, that correspond to three tangs. Since electrostatic energy is one-half of the product of capacitance and voltage squared, which is determined by the geometrical arrangement, the value corresponding to the total electrostatic energy is 4 times 16, which is 4 squared, which is 64. 82, which is the sum of 9, which is the square of 3, and 18, which is twice the number, is obtained.

これは円板コイル11.12が図示のような接続方式で
なく通常の円板コイルの接続方式の場合のように、隣合
う導体間の誘起電圧はlター7分にしかならない場合の
82箇所分に相当する。第2図と同じ導体配置の通常の
円板コイルの場合には、1つの円板コイル当たりlり゛
−ン分の誘起電圧となる導体間は3箇所であり、1組の
円板コイルとしては6箇所になるから、このときの静電
エネルギーに相当する値は6となる。したがって、第2
図のような高直列容量円板巻線の接続方式を採用したこ
とにより直列容量は82を6で除した約14倍となる。
This is 82 points when the induced voltage between adjacent conductors is only 1.7 times, as in the case where the disk coils 11 and 12 are connected not as shown but in the normal disk coil connection mode. equivalent to minutes. In the case of a normal disc coil with the same conductor arrangement as shown in Fig. 2, there are three locations between the conductors where the induced voltage of 1 line per disc coil is generated. Since there are 6 locations, the value corresponding to the electrostatic energy at this time is 6. Therefore, the second
By adopting the high series capacitance disk winding connection method as shown in the figure, the series capacitance is approximately 14 times 82 divided by 6.

実際の円板コイル2つ当たりの直列容量はこの数値に隣
合う導体の静電容量の積を円板コイル2つ分の巻数の二
乗で除し2倍したものである。ここでは実際の静電容量
や直列容量の値は関係ないので具体的な数値は省略する
The actual series capacitance per two disc coils is this value multiplied by the product of the capacitances of adjacent conductors divided by the square of the number of turns for the two disc coils. Since the actual values of capacitance and series capacitance are not relevant here, specific numerical values are omitted.

第2図の円板コイル1つの巻数は4ターンであるが、実
際の円板コイルの巻数はもつと大きいのが普通であるの
で、高直列容量円板巻線の接続方式によって隣合う導体
間の誘起電圧の倍率も大きいので、このような直列容量
の差は更に大きいものとなる。
The number of turns of one disc coil in Figure 2 is 4 turns, but since the number of turns of an actual disc coil is usually large, the connection method of high series capacitance disc windings is used to connect adjacent conductors. Since the magnification of the induced voltage is also large, this difference in series capacitance becomes even larger.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

前述のように、高直列容量円板巻線は特有の接続方式を
採用することにより直列容量が増大する。
As mentioned above, the series capacitance of the high series capacitance disk winding is increased by employing a unique connection method.

したがって、衝撃電圧が印加された際の電位振動の程度
を決める係数αの値が低減され、その結果、電位分布が
−様な分布に近づき隣合う円板コイル間が負担する#J
siit圧が軽減されて円板巻線としての衝撃電圧に対
する絶縁耐力が増大することになる。しかし、第2図で
明らかなように、電気的には2本の導体が並列に使用さ
れているのにかかわらず、円板コイルは4本の導体が並
列になるように巻回した構成になっており、円板巻線の
製作がより困難になるという問題がある。更に巻数が下
から上に増大する接続部32があるために、円板巻線全
体を図の上から下に連続して巻回する連続巻きを採用し
て導体の溶接接続する箇所を無くするという構成を採用
することができず、この接続部32で円板コイル11と
12との双方の導体を溶接接続する必要があるという問
題がある。溶接接続部があるために、溶接作業が必要で
あるという製作工数が増大するという問題ばかりでなく
、溶接部の信頼性が、変圧器全体の信頼性に影響すると
いう重要な問題がある。
Therefore, the value of the coefficient α that determines the degree of potential oscillation when an impact voltage is applied is reduced, and as a result, the potential distribution approaches a −-like distribution and the #J
The siit pressure is reduced and the dielectric strength against impact voltage as a disk winding is increased. However, as shown in Figure 2, although electrically two conductors are used in parallel, a disk coil has a configuration in which four conductors are wound in parallel. Therefore, there is a problem that manufacturing the disk winding becomes more difficult. Furthermore, since there is a connection part 32 where the number of turns increases from bottom to top, continuous winding is adopted in which the entire disk winding is wound continuously from top to bottom in the figure, eliminating the welded connection point of the conductor. However, there is a problem in that the conductors of both the disc coils 11 and 12 must be connected by welding at the connecting portion 32. The presence of welded connections not only increases the number of manufacturing steps due to the need for welding operations, but also poses an important problem in that the reliability of the welds affects the reliability of the entire transformer.

この発明は、このような問題を解決し、円板巻線の巻回
時の導体の並列数が電気的な並列数と同じでよく、かつ
導体の溶接接続を必要としない連続巻きが可能な高直列
容量円板巻線を提供することを目的とする。
This invention solves these problems, and allows the number of conductors in parallel when winding a disc winding to be the same as the number of electrical parallels, and allows continuous winding without the need for welded connections of the conductors. The purpose is to provide a high series capacitance disk winding.

〔課題を解決するための手段〕[Means to solve the problem]

上記課題を解決するために、この発明によれば、偶数本
の並列導体からなる円板コイルを所定の段数積み重ねて
直列接続してなる中央部円板巻線と、この中央部円板巻
線の軸方向の上端部に同軸に設け前記中央部円板巻線の
2分の1の本数の並列導体からなる下端部円板巻線と、
前記中央部円板巻線の下端部に設け並列本数と巻数とが
前記下端部円板巻線と同じ下端部円板巻線とからなり、
前記中央部円板巻線の並列導体の2分の1の上端を上端
部内i巻線の終端に接続し、中央部円板巻線の残る2分
の1の並列導体の下端を下端部円板巻線の始端に接続し
、下端部円板巻線の始端と中央部円板巻線の下端部円板
巻線と接続されない残りの並列導体とを上部端子に接続
し、下端部円板巻線の終端と中央部円板S線の下端部円
板巻線と接続されない残りの並列導体を下部端子に接続
するものとする。
In order to solve the above problems, the present invention provides a central disk winding formed by stacking a predetermined number of stages of disk coils each having an even number of parallel conductors and connecting them in series; a lower end disc winding consisting of parallel conductors of half the number of the central disc winding, which are coaxially disposed at the upper end in the axial direction of the central disc winding;
A lower end disc winding is provided at the lower end of the central disc winding and has the same number of parallel windings and turns as the lower end disc winding,
The upper end of one half of the parallel conductor of the central disc winding is connected to the terminal end of the i winding in the upper end, and the lower end of the remaining one half of the parallel conductor of the central disc winding is connected to the lower end of the parallel conductor of the central disc winding. Connect to the starting end of the plate winding, connect the starting end of the lower end disc winding, the lower end disc winding of the central disc winding and the remaining parallel conductors that are not connected to the upper terminal, and connect the lower end disc winding to the upper terminal, The remaining parallel conductors that are not connected to the end of the winding and the lower end disk winding of the central disk S wire are connected to the lower terminal.

〔作用〕[Effect]

この発明の構成において、偶数本の並列導体からなる円
板コイルを所定の段数積み重ねて直列接続してなる中央
部円板巻線と、この中央部円板巻線の軸方向の上端部に
同軸に設け前記中央部円板巻線の2分の1の本数の並列
導体からなる下端部円板巻線と、前記中央部円板巻線の
下端部に設け並列本数と巻数とが前記下端部円板巻線と
同じ下端部円板巻線とからなり、前記中央部円板巻線の
並列導体の2分の1の上端を下端部円板巻線の終端に接
続し、中央部門Vi、S線の残る2分の1の並列導体の
下端を下端部円板巻線の始端に接続し、下端部円板巻線
の始端と中央部円板巻線の下端部円板巻線と接続されな
い残りの並列導体とを上部端子に接続し、下端部円板巻
線の終端と中央部円板巻線の下端部円板巻線と接続され
ない残りの並列導体を下部端子に接続する構成としたこ
とにより、上部端子から下端部円板巻線と中央部円板巻
線の2分の1の並列導体に接続されて下部端子に接続さ
れる1組の並列導体と、上部端子から中央部円板巻線の
残る2分の1の並列導体に接続されて下端部円板巻線に
接続されて上部端子に接続される組との2つの並列導体
の組とが形成される。
In the configuration of this invention, there is a central disc winding formed by stacking a predetermined number of stages of disc coils each having an even number of parallel conductors and connecting them in series; A lower end disc winding is provided at the lower end of the central disc winding, and the number of parallel conductors and the number of turns are equal to each other at the lower end. It consists of a disk winding and the same lower end disk winding, the upper end of one half of the parallel conductor of the central disk winding is connected to the terminal end of the lower end disk winding, and the central section Vi, Connect the lower end of the remaining half of the parallel conductor of the S wire to the starting end of the lower end disc winding, and connect the starting end of the lower end disc winding to the lower end disc winding of the central disc winding. The remaining parallel conductors that are not connected to the lower end disk winding are connected to the upper terminal, and the remaining parallel conductors that are not connected to the lower end disk winding of the lower end disk winding and the center disk winding are connected to the lower terminal. As a result, a pair of parallel conductors are connected from the upper terminal to the parallel conductors of the lower end disk winding and half of the center disk winding, and are connected to the lower terminal, and Two sets of parallel conductors are formed, one set being connected to the parallel conductors of the remaining half of the disk winding, the other being connected to the lower end disk winding and connected to the top terminal.

下端部円板巻線と下端部円板巻線との巻数は同じである
ので、これら2&[Iの並列導体の巻数は等しくなると
ともに、中央部円板巻線の内部でこれら2組の導体同士
が隣合う構成となりしかも上下端部円板巻線の巻数に相
当する巻数差を持つことになる。この巻数差の二乗に比
例して静電エネルギーが増大し等価静電容量としての直
列容量が増大することから、衝撃電圧が印加された際の
電位振動が抑制される高直列容量円板巻線となる。中央
部円板巻線は偶数並列導体数の普通の円板巻線で構成さ
れるので巻回作業時の並列導体数はこの電気的な並列導
体数と同じでよいので、巻回作業が容易となり、普通の
円板巻線に採用される導体の溶接接続箇所のない連続巻
きが可能になる。
Since the number of turns of the lower end disc winding and the lower end disc winding are the same, the number of turns of these 2 & [I parallel conductors is equal, and the two sets of conductors are The windings are arranged adjacent to each other, and there is a difference in the number of windings corresponding to the number of windings of the upper and lower end disc windings. The electrostatic energy increases in proportion to the square of the difference in the number of turns, and the series capacitance as the equivalent capacitance increases, so the high series capacitance disc winding suppresses potential oscillations when an impact voltage is applied. becomes. The central disc winding is composed of ordinary disc windings with an even number of parallel conductors, so the number of parallel conductors during winding work can be the same as the number of electrical parallel conductors, making winding work easy. This enables continuous winding of the conductor without the welded joints used in ordinary disc windings.

〔実施例〕〔Example〕

以下この発明を実施例に基づいて説明する。第1図はこ
の発明の実施例を示す高直列容量円板巻線の巻線断面の
概略図でもある導体配列図である。
The present invention will be explained below based on examples. FIG. 1 is a conductor arrangement diagram which is also a schematic diagram of a winding cross section of a high series capacitance disc winding showing an embodiment of the present invention.

この図において、導体の参照符号は第2図と同様に上部
端子22からの巻数としての数値と直列接続された導体
の区別としての英字c、dからなっており、同じ英字の
導体は電気的に1本につながった導体であることを示し
ている。
In this figure, the reference numbers for the conductors are the same as in Figure 2, consisting of numerical values representing the number of turns from the upper terminal 22 and letters c and d to distinguish between conductors connected in series, and conductors with the same letter are electrically This indicates that the conductor is connected to one conductor.

上部端子22から分岐して2本の導体1c。Two conductors 1c branch from the upper terminal 22.

1dが接続されており、導体ICは円板コイル15の外
径側に、導体1dは円板コイル16の内径側にそれぞれ
入る。導体1cは円板コイル15の中を内径側に到って
導体8cとなり、円板コイル16の導体9 cに接続さ
れる。この円板コイル16の内径側で導体9cとldが
一緒になって、以後円板コイル21に接続される直前ま
で、普通の円板巻線と同じようにして外径側の接続部3
4と内径側の接続部35で隣合う円板コイル同士が直列
に接続される0円板コイル21は円板コイル15と反対
の接続方式で、最後に下部端子23によって2本の並列
導体が電気的に一体に接続される。この図では高直列容
量円板巻線の下半分は上半分と対称配置で構成されてい
るので、円板コイル19,20.21などの下部の円板
コイルの導体の参照符号を省略しである0図で明らかな
ように、全ての接続部34.35は2本の導体が接続さ
れる構成であり、これは普通の円板巻線と同様であって
、この高直列容量円板巻線全体を上下の端子との接続以
外に導体同士の溶接接続の一切ない連続巻の円板S線と
して製作することができる。
1d is connected, the conductor IC enters the outer diameter side of the disc coil 15, and the conductor 1d enters the inner diameter side of the disc coil 16. The conductor 1c reaches the inner diameter side of the disc coil 15, becomes a conductor 8c, and is connected to the conductor 9c of the disc coil 16. The conductors 9c and ld are connected together on the inner diameter side of this disc coil 16, and from then on, until just before being connected to the disc coil 21, the connecting portion 3 on the outer diameter side is
The 0-disk coil 21 has a connection method opposite to that of the disk coil 15, in which adjacent disk coils are connected in series at the connecting portion 35 on the inner diameter side.Finally, the two parallel conductors are connected by the lower terminal 23. electrically connected together. In this figure, the lower half of the high series capacitance disc winding is arranged symmetrically with the upper half, so reference numbers for the conductors of the lower disc coils, such as disc coils 19, 20, and 21, are omitted. As is clear from a certain figure, all the connection parts 34 and 35 have a configuration in which two conductors are connected, and this is similar to a normal disk winding, and this high series capacitance disk winding The entire wire can be manufactured as a continuous-wound disc S wire without any welded connections between conductors other than connections with upper and lower terminals.

円板コイル15と21は2本の導体が内径側と外径側か
らそれぞれ別個に上下端子22.23に接続された構成
であり、その他の円板コイル16ないし20は構造的に
は半径方向に重ねられた2本の並列導体からなる最も基
本的な円板巻線となっている。しかし、この中央部の円
板コイル16ないし20から構成される中央部円板巻線
100の特徴は、例えば円板コイル16の内径側の導体
1dと90で8ターン、その隣の導体9cと2dで7タ
ーンの巻数差が生じていることである。
The disc coils 15 and 21 have two conductors connected to upper and lower terminals 22 and 23 separately from the inner diameter side and the outer diameter side, respectively, and the other disc coils 16 to 20 are structurally connected in the radial direction. This is the most basic disk winding consisting of two parallel conductors stacked on top of each other. However, the feature of the central disc winding 100 composed of the central disc coils 16 to 20 is that, for example, the conductors 1d and 90 on the inner diameter side of the disc coil 16 have 8 turns, and the adjacent conductor 9c There is a difference in the number of turns of 7 turns at 2d.

このように、中央部巻線100の導体間は全て7ターン
か8ターンの巻数差になっている。このことは、前述の
直列容量を増大するために隣合う導体間の巻数差を大き
くする接続方式となっており、この中央部円板巻数10
0の直列容量が従来技術と同じように高直列容量を実現
していることを示している。第2図の例と同じようにし
て円板コイル16.17のからなる1°組の円板コイル
の群について静電エネルギーの割合を計算すると、7タ
ーン差の部分が6箇所、8ターン差の部分が8箇所ある
から、7の二乗掛ける6が294.8の二乗掛ける8が
512、合計806となる0通常の円板コイルの場合、
この値は前述のように、6であるから、中央部巻!%1
R100は約100倍の静電エネルギーになることが分
かる。ただ、第2図の場合のこの値が82であったのに
対して、第1図ではこの約10倍になっているのはたま
たま適用した円板コイルの巻数の関係や第2図の高直列
容量円板巻線として採用した構成からこのような結果が
出たということであって、第2図の従来技術の場合でも
静電エネルギーの値第2図よりも大きくする接続方式が
あり、前述の第2図に対して第1図の静電エネルギーの
値が大きいという点がこの発明ガ効果であるという訳で
はない。
In this way, all the conductors of the central winding 100 have a difference in the number of turns of 7 or 8 turns. This means that the connection method increases the difference in the number of turns between adjacent conductors in order to increase the series capacitance mentioned above, and the number of turns on the central disk is 10.
It is shown that a series capacitance of 0 realizes a high series capacitance as in the prior art. When calculating the electrostatic energy ratio for a 1° group of disk coils consisting of disk coils 16 and 17 in the same way as the example in Figure 2, there are 6 areas with a 7-turn difference, and 6 areas with an 8-turn difference. There are 8 parts, so 7 squared times 6 is 294.8 squared times 8 is 512, totaling 806.0 In the case of a normal disk coil,
As mentioned above, this value is 6, so the central part volume! %1
It can be seen that R100 has about 100 times the electrostatic energy. However, while this value in the case of Fig. 2 was 82, the reason why it is about 10 times this in Fig. 1 is due to the relationship with the number of turns of the disc coil that was applied, and the height in Fig. 2. This result was obtained from the configuration adopted as a series capacitive disk winding, and even in the case of the prior art shown in Fig. 2, there is a connection method that increases the electrostatic energy value higher than that shown in Fig. 2. The fact that the electrostatic energy value in FIG. 1 is larger than that in FIG. 2 described above is not necessarily an effect of this invention.

第1図では上下端部円板巻線15.21を1つの円板コ
イルだけで構成したが、2つの円板コイルで形成し、こ
れを第2図の円板コイル11゜12と類似の1本の導体
による通常の高直列容量円板巻線の接続方式を採用し、
導体1bを上から3つ目の円板コイルから始めるという
方式を採用することもできる。また、高直列容量円板巻
線の並列数を2に限定するものではなく2の倍数である
偶数であればこの発明を適用することができる。
In Fig. 1, the upper and lower end disc windings 15, 21 are composed of only one disc coil, but they can be formed of two disc coils, which are similar to the disc coils 11 and 12 in Fig. 2. Adopting the normal high series capacitance disk winding connection method using a single conductor,
It is also possible to adopt a method in which the conductor 1b starts from the third disc coil from the top. Further, the number of parallel high series capacitance disc windings is not limited to 2, but the present invention can be applied as long as it is an even number that is a multiple of 2.

この場合は、上下端部円板巻線15.21は並列本数の
2分の1の本数で構成し、これを中央部円板巻線の2分
の1の本数に接続することによりこの発明と同じ効果を
上げることができる。
In this case, the upper and lower end disc windings 15 and 21 are configured with half the number of parallel windings, and are connected to half the number of central disc windings, thereby achieving the invention. can achieve the same effect.

下端部円板巻線と下端部円板巻線とは同じ構成とする必
要は必ずしもなく、並列導体数と巻数が同じであれば、
この発明を適用する上で全く同じ構成を採る必要はない
0例えば、上部端子22が星形結線の線路側で下部端子
23が中性点側である場合、衝撃電圧は常に線路側から
印加されることになり、印加側がらり大きな電圧が掛か
ることから、下端部円板巻線15を下端部円板巻線21
に比べて衝撃電圧耐力の優れた巻数構成を採用すること
が必要な場合がある。
It is not necessarily necessary that the lower end disc winding and the lower end disc winding have the same configuration; as long as the number of parallel conductors and the number of turns are the same,
It is not necessary to adopt exactly the same configuration when applying this invention. For example, if the upper terminal 22 is on the line side of a star-shaped connection and the lower terminal 23 is on the neutral point side, the impulse voltage is always applied from the line side. Since a large voltage is applied to the application side, the lower end disc winding 15 is replaced by the lower end disc winding 21.
In some cases, it may be necessary to adopt a winding structure with superior impact voltage resistance compared to the conventional windings.

〔発明の効果〕〔Effect of the invention〕

この発明は前述のように、並列導体が偶数本の中央部円
板巻線と、この中央部円板巻線上端部に設けた並列導体
が2分の1の下端部円板巻線と、中央部円板巻線の下端
部に設けた並列本数と巻数とが下端部円板巻線と同じ下
端部円板巻線とで高直列容量円板巻線を構成する。そし
て、中央部円板巻線の並列導体の2分の1の上端を下端
部円板巻線の終端に接続して1組の並列導体を形成して
その両端を上部端子と下部端子に接続する。また、中央
部円板巻線の残る2分の1の並列導体の下端を下端部円
板巻線の始端に接続してもう111の並列導体を形成し
てその両端を上部端子と下部端子に接続する。このよう
にして形成した2組の並列導体は、下端部円板巻線と下
端部円板巻線との巻数が同じであることから巻数が互い
に等しくなるとともに、中央部円板巻線の内部でこれら
2&[lの導体同士が隣合う構成となりしかもこの隣合
う導体間に上下端部円板巻線の巻数に相当する巻数差が
生ずることになる。この巻数差の二乗に比例して静電エ
ネルギーが増大し等価静電容量としての直列容量が増大
することから、衝wit圧が印加された際の電位振動が
抑制される高直列容量円板巻線となる。中央部円板巻線
は偶数並列導体数の普通の円板巻線で構成されるので巻
回作業時の並列導体数はこの電気的な並列導体数と同じ
でよいので、巻回作業が容易となり、作業時間が短縮さ
れて変圧器の価格低減に資することになる。更に、普通
の円板巻線に採用される連続巻きが可能になることから
、溶接箇所が上下部端子と高直列容量円板巻線の導体と
を接続する部分以外の溶接接続箇所を無くすることがで
きるので、溶接の不良に起因する事故の可能性が低くな
るために、変圧器としての信鯨性の向上に寄与するとい
う効果も生ずる。
As described above, the present invention includes a central disk winding having an even number of parallel conductors, a lower end disk winding having one half of the parallel conductors provided at the upper end of the central disk winding; A high series capacitance disk winding is constituted by the lower end disk winding provided at the lower end of the central disk winding in which the number of parallel windings and the number of turns are the same as the lower end disk winding. Then, the upper end of one half of the parallel conductor of the central disc winding is connected to the terminal end of the lower end disc winding to form a set of parallel conductors, and both ends of the parallel conductor are connected to the upper terminal and the lower terminal. do. Also, connect the lower ends of the remaining 1/2 parallel conductors of the central disc winding to the starting ends of the lower end disc windings to form another 111 parallel conductors, and connect both ends to the upper and lower terminals. Connecting. The two sets of parallel conductors formed in this way have the same number of turns since the lower end disk winding and the lower end disk winding have the same number of turns, and the inside of the center disk winding has the same number of turns. These 2&[l conductors are arranged adjacent to each other, and a difference in the number of turns corresponding to the number of turns of the upper and lower end disc windings occurs between the adjacent conductors. Since electrostatic energy increases in proportion to the square of the difference in the number of turns, and the series capacitance as the equivalent capacitance increases, high series capacitance disc winding suppresses potential oscillation when an impulse wit pressure is applied. It becomes a line. The central disc winding is composed of ordinary disc windings with an even number of parallel conductors, so the number of parallel conductors during winding work can be the same as the number of electrical parallel conductors, making winding work easy. Therefore, the work time is shortened and the cost of the transformer is reduced. Furthermore, since continuous winding, which is used in ordinary disk windings, is possible, there are no welded connection points other than those where the upper and lower terminals connect the conductor of the high series capacity disk winding. As a result, the possibility of accidents due to poor welding is reduced, which also has the effect of contributing to improved reliability as a transformer.

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

第1図はこの発明の実施例を示す導体配列図、第2図は
従来技術の例を示す導体配列図である。 15・・・円板コイル(下端部円板巻線)、16.17
.1B、19.20・・・円板コイル、100・・・中
央部円板巻線、 21・・・円板コイル(下部円板巻線)、22・・・上
部端子、23・・・下部端子。
FIG. 1 is a conductor arrangement diagram showing an embodiment of the present invention, and FIG. 2 is a conductor arrangement diagram showing an example of the prior art. 15... Disc coil (lower end disc winding), 16.17
.. 1B, 19.20... Disc coil, 100... Center disc winding, 21... Disc coil (lower disc winding), 22... Upper terminal, 23... Lower part terminal.

Claims (1)

【特許請求の範囲】[Claims] 1)偶数本の並列導体からなる円板コイルを所定の段数
積み重ねて直列接続してなる中央部円板巻線と、この中
央部円板巻線の軸方向の上端部に同軸に設け前記中央部
円板巻線の2分の1の本数の並列導体からなる上端部円
板巻線と、前記中央部円板巻線の下端部に設け並列本数
と巻数とが前記上端部円板巻線と同じ下端部円板巻線と
からなり、前記中央部円板巻線の並列導体の2分の1の
上端を上端部円板巻線の終端に接続し、中央部円板巻線
の残る2分の1の並列導体の下端を下端部円板巻線の始
端に接続し、上端部円板巻線の始端と中央部円板巻線の
上端部円板巻線と接続されない残りの並列導体とを上部
端子に接続し、下端部円板巻線の終端と中央部円板巻線
の下端部円板巻線と接続されない残りの並列導体を下部
端子に接続したことを特徴とする高直列容量円板巻線。
1) A central disc winding formed by stacking a predetermined number of stages of disc coils each consisting of an even number of parallel conductors and connecting them in series; an upper end disc winding consisting of parallel conductors with half the number of parallel conductors of the central disc winding; and a lower end of the central disc winding, the number of parallel conductors and the number of turns being equal to the upper end disc winding. The upper end of one half of the parallel conductor of the central disc winding is connected to the terminal end of the upper end disc winding, and the remaining part of the central disc winding is connected to the terminal end of the upper end disc winding. Connect the lower end of the 1/2 parallel conductor to the starting end of the lower end disc winding, and connect the remaining parallel conductors that are not connected to the starting end of the upper end disc winding and the upper end disc winding of the middle disc winding. The conductor is connected to the upper terminal, and the remaining parallel conductor that is not connected to the terminal end of the lower end disc winding and the lower end disc winding of the central disc winding is connected to the lower terminal. Series capacitive disc winding.
JP30917288A 1988-12-07 1988-12-07 High series-capacitance disc winding Pending JPH02155208A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP30917288A JPH02155208A (en) 1988-12-07 1988-12-07 High series-capacitance disc winding

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP30917288A JPH02155208A (en) 1988-12-07 1988-12-07 High series-capacitance disc winding

Publications (1)

Publication Number Publication Date
JPH02155208A true JPH02155208A (en) 1990-06-14

Family

ID=17989801

Family Applications (1)

Application Number Title Priority Date Filing Date
JP30917288A Pending JPH02155208A (en) 1988-12-07 1988-12-07 High series-capacitance disc winding

Country Status (1)

Country Link
JP (1) JPH02155208A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106024335A (en) * 2016-07-21 2016-10-12 江西变压器科技股份有限公司 Odd-number-section continuous coil

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106024335A (en) * 2016-07-21 2016-10-12 江西变压器科技股份有限公司 Odd-number-section continuous coil

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