JPH0945553A - Transformer with tap winding - Google Patents

Transformer with tap winding

Info

Publication number
JPH0945553A
JPH0945553A JP19138495A JP19138495A JPH0945553A JP H0945553 A JPH0945553 A JP H0945553A JP 19138495 A JP19138495 A JP 19138495A JP 19138495 A JP19138495 A JP 19138495A JP H0945553 A JPH0945553 A JP H0945553A
Authority
JP
Japan
Prior art keywords
winding
tap
magnetic field
transformer
tap winding
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.)
Withdrawn
Application number
JP19138495A
Other languages
Japanese (ja)
Inventor
Keizo Kawanishi
敬造 川西
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 JP19138495A priority Critical patent/JPH0945553A/en
Publication of JPH0945553A publication Critical patent/JPH0945553A/en
Withdrawn legal-status Critical Current

Links

Abstract

PROBLEM TO BE SOLVED: To relax a leakage magnetic field component in the direction of radius near a tap winding of an outer winding by locating a magnetic shield along the inner diameter of the tap winding. SOLUTION: An inner winding 3 and outer windings 4, 5 divided into upper and lower parts are wound about an iron core 2 accommodated in a tank. A tap winding 6 is provided between the outer windings 4, 5. A magnetic shield 10 is provided along the inner diameter of the tap winding 6. Thus, a leakage flux 9 in a region 6A is collected toward the magnetic shield 10, and magnetic field components in the radial direction on the side of region 6A of the outer windings 4, 5 are relaxed. It is not necessary to divide the conductors of the outer windings 4, 5 in the axial direction or to enlarge a cooler, and the electromagnetic and mechanical forces on the outer windings 4, 5 is also relaxed. Therefore, the force for tightening the outer windings 4, 5 in the axial direction may be smaller, and reduction in the cost of the device can be realized.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】この発明は、主巻線にタップ巻線
が埋め込まれた変圧器に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a transformer having a main winding and a tap winding embedded therein.

【0002】[0002]

【従来の技術】変圧器には、タップ巻線が主巻線に埋め
込まれた方式と、主巻線とは半径方向の絶縁間隙を介し
て独立にタップ巻線が配置された方式とがあり、ここで
は、前者の方式の変圧器について扱う。タップ巻線から
は複数のタップリードが引き出され、タップ切換器へ接
続されている。このタップを選択することにより変圧器
の変圧比を変え、電力線の送電電圧を常に一定に保って
いる。
2. Description of the Related Art There are two types of transformers, one in which the tap winding is embedded in the main winding, and the other in which the tap winding is arranged independently of the main winding via an insulating gap in the radial direction. , Here, we will deal with the former type of transformer. A plurality of tap leads are drawn from the tap winding and connected to the tap changer. By selecting this tap, the transformation ratio of the transformer is changed and the transmission voltage of the power line is always kept constant.

【0003】図5(A)は従来のタップ巻線付変圧器の
構成を示す片側断面図であり、図5(B)は図5(A)
のA部拡大断面図である。図5(A)において、タンク
1内に収納された鉄心2に内側巻線3と上下に二分割さ
れた外側巻線4、5とが巻回されている。また、図5
(B)のように外側巻線4、5の間にはタップ巻線6が
介装されている。ただし、タップリードは図示が省略さ
れている。
FIG. 5 (A) is a one-sided sectional view showing the structure of a conventional transformer with a tap winding, and FIG. 5 (B) is shown in FIG. 5 (A).
It is an A section expanded sectional view of. In FIG. 5 (A), an inner winding 3 and outer windings 4 and 5 which are vertically divided into two are wound around an iron core 2 housed in a tank 1. Also, FIG.
A tap winding 6 is interposed between the outer windings 4 and 5 as shown in FIG. However, the illustration of the tap lead is omitted.

【0004】図6(A)は従来の異なるタップ巻線付変
圧器の構成を示す片側断面図であり、図6(B)は図6
(A)のB部拡大断面図である。タンク1内に収納され
た鉄心2に内側巻線3と外側巻線7とが巻回されてい
る。また、図6(B)のように外側巻線7の上下端部に
タップ巻線8が配置されている。
FIG. 6 (A) is a one-sided sectional view showing the structure of a conventional transformer with a different tap winding, and FIG. 6 (B) is shown in FIG.
It is an B section expanded sectional view of (A). An inner winding 3 and an outer winding 7 are wound around an iron core 2 housed in a tank 1. Further, as shown in FIG. 6B, tap windings 8 are arranged at the upper and lower ends of the outer winding 7.

【0005】[0005]

【発明が解決しようとする課題】しかしながら、前述し
たような従来の装置は、外側巻線のタップ巻線近傍にお
ける半径方向の漏れ磁界成分が大きいという問題があっ
た。すなわち、タップ巻線にはタップの選定位置によっ
て電流の流れている部分があるので、この部分の漏れ磁
束が半径方向に広がるようになる。そのために、外側巻
線のタップ巻線近傍には半径方向の漏れ磁界成分が形成
される。
However, the conventional device as described above has a problem that the leakage magnetic field component in the radial direction near the tap winding of the outer winding is large. That is, the tap winding has a portion in which current flows depending on the selected position of the tap, so that the leakage flux in this portion spreads in the radial direction. Therefore, a leakage magnetic field component in the radial direction is formed near the tap winding of the outer winding.

【0006】図7(A)は図5の構成における磁界分布
図であり、図7(B)は図7(A)のA1部(点線の範
囲)拡大磁界分布図である。図7において、9が漏れ磁
束である。タップ巻線の配されている領域6Aは、電流
が流れていないので単なる空間として磁界計算された。
図7(B)より判るように、領域6Aで漏れ磁束9が半
径方向に広がるので、外側巻線4、5のタップ巻線側に
半径方向の漏れ磁界成分が形成される。
FIG. 7A is a magnetic field distribution diagram in the configuration of FIG. 5, and FIG. 7B is an enlarged magnetic field distribution diagram of the A1 portion (dotted line range) of FIG. 7A. In FIG. 7, 9 is a leakage magnetic flux. In the area 6A where the tap windings are arranged, since no current flows, the magnetic field was calculated as a mere space.
As can be seen from FIG. 7B, the leakage magnetic flux 9 spreads in the radial direction in the region 6A, so that a leakage magnetic field component in the radial direction is formed on the tap winding side of the outer windings 4 and 5.

【0007】また、図8(A)は図6の構成における磁
界分布図であり、図8(B)は図8(A)のB1部(点
線の範囲)拡大磁界分布図である。図8において、9が
漏れ磁束である。タップ巻線の配されている領域8A
は、電流が流れていないので単なる空間として磁界計算
された。図8(B)より判るように、領域8Aで磁束が
半径方向に広がるので、外側巻線7の端部に半径方向の
漏れ磁界成分が形成される。
FIG. 8 (A) is a magnetic field distribution diagram in the configuration of FIG. 6, and FIG. 8 (B) is an enlarged magnetic field distribution diagram of the B1 portion (dotted line range) of FIG. 8 (A). In FIG. 8, 9 is a leakage magnetic flux. Area 8A where tap windings are arranged
Was calculated as a mere space because no current was flowing. As can be seen from FIG. 8 (B), since the magnetic flux spreads in the radial direction in the region 8A, a leakage magnetic field component in the radial direction is formed at the end of the outer winding 7.

【0008】一般に、うず電流は、磁界に直角な方向の
導体幅の二乗に比例して増加する。したがって、このう
ず電流を抑えるためには、軸方向の漏れ磁界に対しては
外側巻線の半径方向の導体幅を小さくし、半径方向の漏
れ磁界に対しては外側巻線の軸方向の導体幅を小さくす
ればよい。そのために、従来の外側巻線では、導体が半
径方向に分割されるとともに、軸方向にも分割されてい
た。導体を軸方向に分割すると製作工数が増すので、導
体を分割する方法の代りに冷却器を大きくし、うず電流
によるタップ巻線近傍の局部加熱を抑える方法もある。
しかし、冷却器を大きくすると装置が大型化し、結局は
コストアップにつながってしまう。
Generally, the eddy current increases in proportion to the square of the conductor width in the direction perpendicular to the magnetic field. Therefore, to suppress this eddy current, the radial conductor width of the outer winding is reduced with respect to the axial leakage magnetic field, and the axial conductor width of the outer winding is reduced with respect to the radial leakage magnetic field. The width should be reduced. Therefore, in the conventional outer winding, the conductor is divided not only in the radial direction but also in the axial direction. Since dividing the conductor in the axial direction increases the number of manufacturing steps, instead of dividing the conductor, there is also a method of enlarging the cooler to suppress local heating near the tap winding due to eddy current.
However, if the cooler is enlarged, the size of the device becomes large, which eventually leads to an increase in cost.

【0009】この発明の目的は、外側巻線のタップ巻線
近傍における半径方向の漏れ磁界成分を緩和させること
にある。
An object of the present invention is to reduce the leakage magnetic field component in the radial direction near the tap winding of the outer winding.

【0010】[0010]

【課題を解決するための手段】上記目的を達成するため
に、この発明によれば、鉄心を軸にして巻回される内側
巻線と外側巻線とを備え、外側巻線がタップ巻線を介し
て軸方向に二分割された変圧器において、磁気シールド
をタップ巻線の内径側に沿って配置したものとする。
In order to achieve the above object, according to the present invention, an inner winding and an outer winding wound around an iron core are provided, and the outer winding is a tap winding. In the transformer divided in two in the axial direction via the magnetic shield, the magnetic shield is arranged along the inner diameter side of the tap winding.

【0011】または、鉄心を軸にして巻回される内側巻
線と外側巻線とを備え、外側巻線の軸方向端部にタップ
巻線が配置された変圧器において、磁気シールドをタッ
プ巻線の反外側巻線側に配置したものとしてもよい。ま
た、前記の各構成において、前記磁気シールドを、磁性
粉がバインダーを介して成形されてなるものとすれば、
なお好適である。
Alternatively, in a transformer having an inner winding and an outer winding that are wound around an iron core, and a tap winding is arranged at an axial end portion of the outer winding, the magnetic shield is tap-wound. It may be arranged on the side opposite to the outer side of the wire. Further, in each of the above-mentioned configurations, if the magnetic shield is formed of magnetic powder via a binder,
It is still preferable.

【0012】[0012]

【作用】この発明の構成によれば、外側巻線の間に介装
されたタップ巻線の内径側に沿って,磁気シールドを配
置する。これにより漏れ磁束が磁気シールド側に集まっ
て来るので、漏れ磁束の広がりが抑えられる。そのため
に、外側巻線のタップ巻線近傍における半径方向の漏れ
磁界成分が緩和される。
According to the structure of the present invention, the magnetic shield is arranged along the inner diameter side of the tap winding interposed between the outer windings. As a result, the leakage flux gathers on the magnetic shield side, so that the spread of the leakage flux can be suppressed. Therefore, the leakage magnetic field component in the radial direction near the tap winding of the outer winding is relaxed.

【0013】また、外側巻線の端部に設けられたタップ
巻線の反外側巻線側に磁気シールドを配置する。これに
よっても漏れ磁束が磁気シールド側に集まって来るの
で、漏れ磁束の広がりが抑えられる。そのために、外側
巻線のタップ巻線近傍における半径方向の漏れ磁界成分
が緩和される。また、磁気シールドを、磁性粉がバイン
ダーを介して成形されてなるものとすれば、その磁性粉
の充填率の調整により任意の比透磁率μを有する磁気シ
ールドを形成することができる。従って、種々のタップ
巻線付変圧器に対して、外側巻線のタップ巻線近傍にお
ける半径方向の漏れ磁界成分を緩和するためのそれぞれ
最適な比透磁率μを有する磁気シールドを容易に作るこ
とができる。
Further, a magnetic shield is arranged on the side opposite to the outer winding of the tap winding provided at the end of the outer winding. This also causes the leakage magnetic flux to gather on the magnetic shield side, so that the spread of the leakage magnetic flux can be suppressed. Therefore, the leakage magnetic field component in the radial direction near the tap winding of the outer winding is relaxed. If the magnetic shield is formed by molding magnetic powder through a binder, it is possible to form a magnetic shield having an arbitrary relative magnetic permeability μ by adjusting the filling rate of the magnetic powder. Therefore, for various types of transformers with tap windings, it is possible to easily create magnetic shields having optimum relative magnetic permeability μ for mitigating radial leakage magnetic field components in the vicinity of the tap windings of the outer windings. You can

【0014】[0014]

【実施例】以下、この発明を実施例に基づいて説明す
る。図1は、この発明の実施例にかかるタップ巻線付変
圧器の構成を示す要部拡大断面図である。タップ巻線6
の内径側に沿って磁気シールド10が配されている。そ
の他の構成は、図5で説明された従来の構成と同じであ
る。同じ部分には、同一参照符号を付けることにより詳
細な説明を繰り返すことは省略する。
EXAMPLES The present invention will be described below based on examples. FIG. 1 is an enlarged sectional view of an essential part showing the configuration of a transformer with a tap winding according to an embodiment of the present invention. Tap winding 6
The magnetic shield 10 is arranged along the inner diameter side of the. The other configuration is the same as the conventional configuration described in FIG. The same portions will be denoted by the same reference symbols and repeated detailed description will be omitted.

【0015】図1の磁気シールド10としては、例え
ば、磁性を有する粉体(磁性粉)がバインダーを介して
成形されたものであり磁粉鉄心とも呼ばれているものを
採用することができる。磁気シールド10として前記の
磁粉鉄心を採用した場合には、この磁気シールド10の
比透磁率μとしては、その磁性粉の充填率の調整によっ
て任意のものを作ることができる。外側巻線4,5内に
形成される半径方向の漏れ磁界を緩和するための磁気シ
ールド10の最適な比透磁率μは鉄心・巻線の構造によ
って異なるが、タップ巻線が主巻線に埋め込まれたタッ
プ巻線付変圧器の場合、変圧器の機種間の差異を考慮し
ても、μを10ないし100程度にすることによって外
側巻線4、5内に形成される半径方向の漏れ磁界を緩和
することができる。
As the magnetic shield 10 in FIG. 1, for example, a magnetic powder (magnetic powder) molded through a binder, which is also called a magnetic iron core, can be adopted. When the above-mentioned magnetic iron core is adopted as the magnetic shield 10, the relative magnetic permeability μ of the magnetic shield 10 can be arbitrarily adjusted by adjusting the filling rate of the magnetic powder. Although the optimum relative permeability μ of the magnetic shield 10 for relaxing the radial leakage magnetic field formed in the outer windings 4 and 5 differs depending on the structure of the iron core / winding, the tap winding is the main winding. In the case of an embedded transformer with tap winding, radial leakage formed in the outer windings 4 and 5 by setting μ to about 10 to 100, even in consideration of differences between transformer models. The magnetic field can be relaxed.

【0016】図3(A)は、図1の構成における磁界分
布図であり、図3(B)は図3(A)のA2部(点線の
範囲)拡大磁界分布図である。図3において9が漏れ磁
束であり、タップ巻線の配されている領域6Aは、電流
が流れていないので単なる空間として磁界計算された。
また、磁気シールド10の比透磁率μは10として計算
された。図3(B)の領域6Aにおける漏れ磁束9が磁
気シールド10側に寄せ集められ、図7(B)における
従来の場合より外側巻線4、5の領域6A側における半
径方向磁界成分が緩和されているのが判る。
FIG. 3 (A) is a magnetic field distribution diagram in the configuration of FIG. 1, and FIG. 3 (B) is an enlarged magnetic field distribution diagram of the portion A2 (dotted line range) of FIG. 3 (A). In FIG. 3, 9 is the leakage magnetic flux, and the region 6A in which the tap windings are arranged has no current flowing, so the magnetic field was calculated as a mere space.
The relative permeability μ of the magnetic shield 10 was calculated as 10. The leakage magnetic flux 9 in the area 6A of FIG. 3B is gathered closer to the magnetic shield 10 side, and the radial magnetic field component on the area 6A side of the outer windings 4 and 5 is relaxed as compared with the conventional case in FIG. 7B. You can see that

【0017】図2は、この発明の異なる実施例にかかる
タップ巻線付変圧器の構成を示す要部拡大断面図であ
る。タップ巻線8の上端部に磁気シールド11が配され
ている。その他の構成は図6の従来の構成と同じであ
る。磁気シールド11の材質は、図1の磁気シールド1
0のものと同一である。なお、磁気シールド11は、外
側巻線7の下端部に配されているタップ巻線の下面側に
も設けられている。
FIG. 2 is an enlarged sectional view of the essential parts showing the structure of the transformer with tap winding according to another embodiment of the present invention. A magnetic shield 11 is arranged on the upper end of the tap winding 8. Other configurations are the same as the conventional configuration of FIG. The material of the magnetic shield 11 is the magnetic shield 1 of FIG.
It is the same as that of 0. The magnetic shield 11 is also provided on the lower surface side of the tap winding arranged at the lower end of the outer winding 7.

【0018】図4(A)は、図2の構成における磁界分
布図であり、図4(B)は図4(A)のB2部(点線の
範囲)拡大磁界分布図である。図4において、9が漏れ
磁束であり、タップ巻線の配されている領域8Aは、電
流が流れていないので単なる空間として磁界計算され
た。また、磁気シールド11の比透磁率μは10として
計算された。図4(B)の領域8Aにおける漏れ磁束9
は磁気シールド11側に寄せ集められ、図8(B)にお
ける従来の場合より外側巻線7の端部における半径方向
磁界成分が緩和されているのが判る。
FIG. 4 (A) is a magnetic field distribution diagram in the configuration of FIG. 2, and FIG. 4 (B) is an enlarged magnetic field distribution diagram of B2 portion (dotted line range) of FIG. 4 (A). In FIG. 4, 9 is the leakage magnetic flux, and the region 8A in which the tap windings are arranged has no current flowing therein, so the magnetic field was calculated as a mere space. The relative permeability μ of the magnetic shield 11 was calculated as 10. Leakage magnetic flux 9 in region 8A of FIG. 4 (B)
Are gathered closer to the magnetic shield 11 side, and it can be seen that the radial magnetic field component at the end portion of the outer winding 7 is relaxed as compared with the conventional case in FIG.

【0019】[0019]

【発明の効果】この発明は前述のように、外側巻線の間
に介装されたタップ巻線の内径側に沿って、あるいは、
外側巻線の端部に設けられたタップ巻線の反外側巻線側
に、磁気シールドを配置する。これにより、外側巻線の
タップ巻線近傍における半径方向の漏れ磁界成分が緩和
される。したがって、外側巻線の導体を軸方向に分割し
たり、冷却器を大きくしたりする必要がなく、装置のコ
ストが低減される。また、半径方向の漏れ磁界成分が緩
和されると外側巻線の軸方向に働く電磁機械力も緩和さ
れる。そのために、外側巻線を軸方向に締め付ける力も
少なくて済み、この点からも装置のコストダウンがはか
れる。
As described above, the present invention is provided along the inner diameter side of the tap winding interposed between the outer windings, or
The magnetic shield is arranged on the side opposite to the outer winding of the tap winding provided at the end of the outer winding. As a result, the leakage magnetic field component in the radial direction near the tap winding of the outer winding is relaxed. Therefore, it is not necessary to divide the conductor of the outer winding in the axial direction or increase the size of the cooler, and the cost of the device is reduced. Further, when the leakage magnetic field component in the radial direction is relaxed, the electromagnetic mechanical force acting in the axial direction of the outer winding is also relaxed. Therefore, less force is required to tighten the outer winding in the axial direction, and the cost of the device can be reduced from this point as well.

【0020】また、磁気シールドを、磁性粉がバインダ
ーを介して成形されてなるものとする。これにより、種
々のタップ巻線付変圧器に対応して、外側巻線のタップ
巻線近傍における半径方向の漏れ磁界成分を緩和するた
めのそれぞれ最適な比透磁率μを有する磁気シールドを
容易に作ることが可能となる。
Further, the magnetic shield is formed by molding magnetic powder through a binder. This facilitates the magnetic shield having the optimum relative permeability μ for mitigating the radial leakage magnetic field component near the tap winding of the outer winding, corresponding to various tap winding transformers. It becomes possible to make.

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

【図1】この発明の実施例にかかるタップ巻線付変圧器
の構成を示す要部拡大断面図
FIG. 1 is an enlarged sectional view of an essential part showing the configuration of a transformer with tap winding according to an embodiment of the present invention.

【図2】この発明の異なる実施例にかかるタップ巻線付
変圧器の構成を示す要部拡大断面図
FIG. 2 is an enlarged sectional view of an essential part showing the configuration of a transformer with tap winding according to another embodiment of the present invention.

【図3】(A)は図1の磁界分布図であり、(B)は図
3(A)のA2部拡大磁界分布図
3A is a magnetic field distribution diagram of FIG. 1, and FIG. 3B is an enlarged magnetic field distribution diagram of an A2 portion of FIG. 3A.

【図4】(A)は図2の磁界分布図であり、(B)は図
4(A)のB2部拡大磁界分布図
4A is a magnetic field distribution diagram of FIG. 2, and FIG. 4B is an enlarged magnetic field distribution diagram of B2 part of FIG. 4A.

【図5】(A)は従来のタップ巻線付変圧器の構成を示
す片側断面図であり、(B)は図5(A)のA部拡大断
面図
5A is a one-sided cross-sectional view showing the configuration of a conventional transformer with tap winding, and FIG. 5B is an enlarged cross-sectional view of part A of FIG. 5A.

【図6】(A)は従来の異なるタップ巻線付変圧器の構
成を示す片側断面図であり、(B)は図6(A)のB部
拡大断面図
6A is a one-sided cross-sectional view showing the structure of a conventional transformer with a different tap winding, and FIG. 6B is an enlarged cross-sectional view of a B part in FIG. 6A.

【図7】(A)は図5の磁界分布図であり、(B)は図
7(A)のA1部拡大磁界分布図
7A is a magnetic field distribution diagram of FIG. 5, and FIG. 7B is an enlarged magnetic field distribution diagram of an A1 portion of FIG. 7A.

【図8】(A)は図6の磁界分布図であり、(B)は図
8(A)のB1部拡大磁界分布図
8A is a magnetic field distribution diagram of FIG. 6, and FIG. 8B is an enlarged magnetic field distribution diagram of a B1 portion of FIG. 8A.

【符号の説明】 2:鉄心、3:内側巻線、4,5,7:外側巻線、6,
8:タップ巻線、9:漏れ磁束、10,11:磁気シー
ルド
[Explanation of symbols] 2: Iron core, 3: Inner winding, 4, 5, 7: Outer winding, 6,
8: Tap winding, 9: Leakage magnetic flux, 10, 11: Magnetic shield

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】鉄心を軸にして巻回される内側巻線と外側
巻線とを備え、外側巻線がタップ巻線を介して軸方向に
二分割された変圧器において、磁気シールドをタップ巻
線の内径側に沿って配置したことを特徴とするタップ巻
線付変圧器。
Claim: What is claimed is: 1. A transformer comprising an inner winding and an outer winding wound around an iron core, the outer winding being axially divided into two parts by tapping the magnetic shield. A transformer with a tap winding, which is arranged along the inner diameter side of the winding.
【請求項2】鉄心を軸にして巻回される内側巻線と外側
巻線とを備え、外側巻線の軸方向端部にタップ巻線が配
置された変圧器において、磁気シールドをタップ巻線の
反外側巻線側に配置したことを特徴とするタップ巻線付
変圧器。
2. A transformer, comprising an inner winding and an outer winding wound around an iron core, wherein the outer winding has a tap winding arranged at an axial end portion thereof. A transformer with a tap winding, characterized in that it is arranged on the side opposite to the winding side of the wire.
【請求項3】請求項1ないし請求項2に記載のものにお
いて、前記磁気シールドは、磁性粉をバインダーを介し
て加圧成形されてなるものであることを特徴とするタッ
プ巻線付変圧器。
3. The transformer with tap winding according to claim 1 or 2, wherein the magnetic shield is formed by press-molding magnetic powder through a binder. .
JP19138495A 1995-07-27 1995-07-27 Transformer with tap winding Withdrawn JPH0945553A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19138495A JPH0945553A (en) 1995-07-27 1995-07-27 Transformer with tap winding

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19138495A JPH0945553A (en) 1995-07-27 1995-07-27 Transformer with tap winding

Publications (1)

Publication Number Publication Date
JPH0945553A true JPH0945553A (en) 1997-02-14

Family

ID=16273708

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19138495A Withdrawn JPH0945553A (en) 1995-07-27 1995-07-27 Transformer with tap winding

Country Status (1)

Country Link
JP (1) JPH0945553A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20160086726A1 (en) * 2014-09-19 2016-03-24 Hitachi, Ltd. Transformer

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20160086726A1 (en) * 2014-09-19 2016-03-24 Hitachi, Ltd. Transformer
US9812250B2 (en) * 2014-09-19 2017-11-07 Hitachi, Ltd. Transformer

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