JPH02146708A - Transformer - Google Patents
TransformerInfo
- Publication number
- JPH02146708A JPH02146708A JP29945488A JP29945488A JPH02146708A JP H02146708 A JPH02146708 A JP H02146708A JP 29945488 A JP29945488 A JP 29945488A JP 29945488 A JP29945488 A JP 29945488A JP H02146708 A JPH02146708 A JP H02146708A
- Authority
- JP
- Japan
- Prior art keywords
- windings
- winding
- superconductors
- transformer
- wound
- 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
Links
- 238000004804 winding Methods 0.000 claims abstract description 60
- 239000002887 superconductor Substances 0.000 claims abstract description 25
- 230000005291 magnetic effect Effects 0.000 abstract description 25
- 230000004907 flux Effects 0.000 abstract description 24
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical group [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 abstract description 6
- 238000001816 cooling Methods 0.000 abstract description 4
- 239000003507 refrigerant Substances 0.000 abstract 1
- 230000000694 effects Effects 0.000 description 4
- 239000004020 conductor Substances 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 239000002826 coolant Substances 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000005292 diamagnetic effect Effects 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 230000002265 prevention Effects 0.000 description 1
- 239000012779 reinforcing material Substances 0.000 description 1
Landscapes
- Regulation Of General Use Transformers (AREA)
Abstract
Description
【発明の詳細な説明】
[発明の目的]
(産業上の利用分野)
本発明は巻線の磁気シールド構造を改良した変圧器に関
するものである。DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Field of Industrial Application) The present invention relates to a transformer with improved magnetic shielding structure of the winding.
(従来の技術)
一般に変圧器は第3図に示すように鉄心1に対し同心状
に巻回した二次巻線2と、その外側に必要な絶縁距離だ
け離し巻回された一次巻線3を有する構成である。変圧
器は運転中もれ磁束を発生するが、このもれ磁束はエネ
ルギーが極小となるよう分布する。そのため磁束は巻線
の軸方向中央付近では、軸方向成分のみをもち、巻線の
空隙部付近にのみ存在するが、巻線の軸方向端部付近で
は、径方向の成分をもち巻線内にも広く分布するように
なる。(Prior Art) Generally, a transformer has a secondary winding 2 wound concentrically around an iron core 1, and a primary winding 3 wound outside of the secondary winding 2 at a required insulation distance, as shown in Fig. 3. The configuration has the following. A transformer generates leakage magnetic flux during operation, but this leakage flux is distributed so that its energy is minimized. Therefore, near the axial center of the winding, magnetic flux has only an axial component and exists only near the air gap of the winding, but near the axial ends of the winding, it has a radial component and is present inside the winding. become widely distributed.
(発明が解決しようとする課題)
磁束が巻線内を通ると巻線の各導体中には渦電流が生じ
損失を発生する。巻線の軸方向の端部付近では、第4図
の曲線Bのように磁束が広く分布し、巻線内を通る磁束
量が多くなるため大きな損失を発生していた。また、短
絡時には、短絡電流と、短絡電流に比例したもれ磁束の
間に働く電磁力により大きな機械力が巻線に働くため、
巻線および巻線支持構造を、この機械力に耐えるよう、
補強材を入れるのなど構造的に強固なものとする必要が
あり、変圧器の重量1寸法の増加につながっていた。(Problem to be Solved by the Invention) When magnetic flux passes through the winding, eddy currents occur in each conductor of the winding, causing loss. Near the ends of the winding in the axial direction, the magnetic flux is widely distributed as shown by curve B in FIG. 4, and the amount of magnetic flux passing through the winding increases, causing a large loss. In addition, in the event of a short circuit, a large mechanical force is applied to the winding due to the electromagnetic force acting between the short circuit current and the leakage flux proportional to the short circuit current.
The windings and winding support structure are designed to withstand this mechanical force.
It was necessary to make it structurally strong by adding reinforcing materials, which led to an increase in the weight of the transformer.
本発明は、もれ磁束の分布を変え、巻線と鎖交するもれ
磁束を減少することにより、損失を減少するとともに、
短絡時の機械力を低減する、磁気シールドを有する変圧
器を提供することを目的とする。The present invention reduces loss by changing the distribution of leakage magnetic flux and reducing leakage flux interlinking with the winding, and
An object of the present invention is to provide a transformer having a magnetic shield that reduces mechanical force during a short circuit.
[発明の構成]
(課題を解決するための手段)
上記の問題点を解決するため、本発明においては巻線の
内周、外周又は巻線の内部の少なくとも1ケ所に巻線と
同心状に条又は線状の超電導体を巻線の軸方向寸法に閉
回路を形成しないよう巻回し、超電導体を臨界温度以下
に冷却したことを特徴とする。[Structure of the Invention] (Means for Solving the Problems) In order to solve the above problems, in the present invention, a wire is provided concentrically with the winding at at least one location on the inner periphery of the winding, the outer periphery of the winding, or inside the winding. It is characterized in that a strip or linear superconductor is wound so as not to form a closed circuit in the axial dimension of the winding, and the superconductor is cooled to below a critical temperature.
(作用)
超電導体は、臨界温度以下では、マイスナ効果による反
磁性効果のため、超電導体付近の磁束と反対極性の磁極
を発生する。その結果、超電導体の付近に磁束が通りに
くくなり、超電導体の付近の磁束数が少なくなる。従っ
て超電導体が巻線の近傍に存在するとき、巻線の内部を
通る磁束は超電導体がない場合に比べ小さなものとなる
。(Function) At temperatures below a critical temperature, a superconductor generates a magnetic pole with a polarity opposite to the magnetic flux near the superconductor due to the diamagnetic effect caused by the Meissner effect. As a result, it becomes difficult for magnetic flux to pass near the superconductor, and the number of magnetic fluxes near the superconductor decreases. Therefore, when a superconductor exists near a winding, the magnetic flux passing through the inside of the winding becomes smaller than when there is no superconductor.
(実施例)
第1図に本発明の実施例を示す。鉄心1に−次巻線2.
二次巻線3を巻回して変圧器本体を構成する。この変圧
器本体には、−次巻線3の外側。(Example) FIG. 1 shows an example of the present invention. Iron core 1 - next winding 2.
The secondary winding 3 is wound to form a transformer body. This transformer body has a - outer side of the secondary winding 3.
二次巻線2と鉄心1の間にそれぞれ閉回路を形成しない
よう超電導体5.5′を巻線と同心状にかつ巻線軸方向
寸法以上に巻回しである。そしてこの変圧器本体を冷却
容器6に入れ冷却媒体により超電導体5.5を臨界温度
以下に冷却する。The superconductor 5,5' is wound concentrically with the winding and with a dimension greater than the axial dimension of the winding so as not to form a closed circuit between the secondary winding 2 and the iron core 1. The transformer body is then placed in a cooling container 6, and the superconductor 5.5 is cooled to below the critical temperature by a cooling medium.
臨界温度以下の超電導体5.5′は、マイスナー効果に
より付近の磁束と反対磁極を発生する。The superconductor 5.5' below the critical temperature generates a magnetic pole opposite to the nearby magnetic flux due to the Meissner effect.
そのため、超電導体5.5近傍は磁束が通りくくなり、
磁束は超電導体を避けて通るようになる。Therefore, the magnetic flux becomes difficult to pass around the superconductor 5.5,
The magnetic flux will now avoid the superconductor.
従ってこのときの磁束線図は第1図に見られるよう巻線
の軸方向端部でも径方向成分は小さく、はとんどが軸方
向を向く。よって、巻線の軸方向端部における磁束分布
は第4図の曲線Aのようになり、巻線と鎖交するもれ磁
束量が第4図の曲線B(従来の場合)よりも小さくでき
る。Therefore, in the magnetic flux line diagram at this time, as shown in FIG. 1, the radial component is small even at the axial end of the winding, and most of the magnetic flux lines are oriented in the axial direction. Therefore, the magnetic flux distribution at the axial end of the winding becomes like curve A in Figure 4, and the amount of leakage magnetic flux interlinking with the winding can be made smaller than curve B in Figure 4 (conventional case). .
このように巻線と鎖交するもれ磁束が減少できるため、
渦電流による損失を低減するとともに短絡時に巻線に働
く機械力が小さくできるので、巻線および巻線の支持構
造が簡略化でき、重量1寸法を小さくした変圧器が提供
できる。In this way, the leakage magnetic flux interlinking with the winding can be reduced, so
Since losses due to eddy currents can be reduced and the mechanical force acting on the windings during a short circuit can be reduced, the windings and the support structure for the windings can be simplified, and a transformer with one dimension of weight reduced can be provided.
また第2図に示すように、超電導体5の巻回位置を一次
、二次巻線2,3間としても同様の効果がある。このと
き超電導体5を接地すれば、超電導体5を混触防止板と
兼用することも可能である。Further, as shown in FIG. 2, the same effect can be obtained by winding the superconductor 5 between the primary and secondary windings 2 and 3. At this time, if the superconductor 5 is grounded, the superconductor 5 can also be used as a contact prevention plate.
[発明の効果コ
以上のように本発明は巻線の内周、外周、内部の少なく
とも1ケ所に起電導体を巻回することにより、もれ磁束
によって生ずる渦電流損失を低減できるほか、短絡時に
生ずる短絡機械力を低減できるため巻線および巻線支持
構造を簡略化し、変圧器の重量寸法を小さくすることが
できる。[Effects of the Invention] As described above, the present invention can reduce eddy current loss caused by leakage magnetic flux by winding an electromotive conductor at at least one location on the inner periphery, outer periphery, and inside of the winding. Since the short-circuit mechanical force that sometimes occurs can be reduced, the winding and the winding support structure can be simplified, and the weight and size of the transformer can be reduced.
第1図は本発明による変圧器を示す概略断面図、第2図
は本発明の他の実施例を示す概略断面図、第3図は従来
の構成における変圧器の概略断面図、第4図は、変圧器
の軸方向端部での磁束分布の様子を示す分布図である。
1・・・鉄心、 2・・・二次巻線、 3・・・−
次巻線。
5.5−・・・超電導体。
6・・・冷却容器。
第3図FIG. 1 is a schematic sectional view showing a transformer according to the present invention, FIG. 2 is a schematic sectional view showing another embodiment of the invention, FIG. 3 is a schematic sectional view of a transformer in a conventional configuration, and FIG. 2 is a distribution diagram showing the state of magnetic flux distribution at the axial end of the transformer. FIG. 1... Iron core, 2... Secondary winding, 3...-
Next winding. 5.5-...Superconductor. 6...Cooling container. Figure 3
Claims (1)
と同心状に条または線状の超電導体を巻線の軸方向寸法
以上の寸法にかつ閉回路を構成しないように巻回して臨
界温度以下に冷却したことを特徴とする変圧器。A superconductor in the form of a strip or wire is wound concentrically with the winding at at least one location on the inner circumference, outer circumference, or inside the winding to a dimension greater than or equal to the axial dimension of the winding, and so as not to form a closed circuit. A transformer characterized by being cooled below temperature.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP29945488A JPH02146708A (en) | 1988-11-29 | 1988-11-29 | Transformer |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP29945488A JPH02146708A (en) | 1988-11-29 | 1988-11-29 | Transformer |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH02146708A true JPH02146708A (en) | 1990-06-05 |
Family
ID=17872785
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP29945488A Pending JPH02146708A (en) | 1988-11-29 | 1988-11-29 | Transformer |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH02146708A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2000016350A3 (en) * | 1998-09-14 | 2000-06-08 | Siemens Ag | High temperature superconducting transformer |
-
1988
- 1988-11-29 JP JP29945488A patent/JPH02146708A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2000016350A3 (en) * | 1998-09-14 | 2000-06-08 | Siemens Ag | High temperature superconducting transformer |
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