JPS59103317A - Large current 3-phase electric circuit - Google Patents

Large current 3-phase electric circuit

Info

Publication number
JPS59103317A
JPS59103317A JP58215900A JP21590083A JPS59103317A JP S59103317 A JPS59103317 A JP S59103317A JP 58215900 A JP58215900 A JP 58215900A JP 21590083 A JP21590083 A JP 21590083A JP S59103317 A JPS59103317 A JP S59103317A
Authority
JP
Japan
Prior art keywords
conductors
conductor
current
phase
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.)
Pending
Application number
JP58215900A
Other languages
Japanese (ja)
Inventor
ペ−タ−・ヘンリシ
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.)
Transformatoren Union AG
Original Assignee
Transformatoren Union AG
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 Transformatoren Union AG filed Critical Transformatoren Union AG
Publication of JPS59103317A publication Critical patent/JPS59103317A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01BCABLES; CONDUCTORS; INSULATORS; SELECTION OF MATERIALS FOR THEIR CONDUCTIVE, INSULATING OR DIELECTRIC PROPERTIES
    • H01B5/00Non-insulated conductors or conductive bodies characterised by their form
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01BCABLES; CONDUCTORS; INSULATORS; SELECTION OF MATERIALS FOR THEIR CONDUCTIVE, INSULATING OR DIELECTRIC PROPERTIES
    • H01B9/00Power cables
    • H01B9/001Power supply cables for the electrodes of electric-welding apparatus or electric-arc furnaces
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F27/00Details of transformers or inductances, in general
    • H01F27/02Casings
    • H01F27/04Leading of conductors or axles through casings, e.g. for tap-changing arrangements
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F27/00Details of transformers or inductances, in general
    • H01F27/28Coils; Windings; Conductive connections
    • H01F27/2823Wires
    • H01F27/2828Construction of conductive connections, of leads

Abstract

1. An arrangement for the transmission of large electrical outputs comprising large currents with small voltage differences from a transformer to an adjacent load, for example a steel melting furnace or an electrolytic bath, by means of a three-phase power line comprising conductors which have a wide cross-section in relation to their thickness, characterised in that all the conductors (10, 15, 17, 18) of the three-phase power line from the transformer windings (5, 6, 7) to the load In the region of the winding output lines (10 to 15) and also in the region of an outlet (16) through the transformer casing (9) and also in a subsequent conductor section have their broader faces respectively opposite one another with adjacent conductors (10, 15, 17, 18) mutually overlapping over their full width, and in that the width of the conductors (10, 17, 18, 15) approximately equals the height of the winding in the transformer.

Description

【発明の詳細な説明】 〔発明の属する技術分野〕 この発明は、断面において厚さに較べて非常に幅の広い
導体を介して変圧器から隣接する負荷例えば鋼溶解炉又
は電解槽へ大電流低電圧の大電力を導くための大電流三
相電路にかかわる。
[Detailed Description of the Invention] [Technical Field to which the Invention Pertains] This invention relates to the application of large currents from a transformer to an adjacent load, such as a steel melting furnace or an electrolytic cell, through a conductor that is very wide in cross section compared to its thickness. It is concerned with high-current three-phase circuits for conducting low-voltage high-power.

〔従来技術とその問題点〕[Prior art and its problems]

かかる適用例のための電路は、例えば)9yス7オルマ
トーレy 5. wオン社(Tranaformato
ren UnionAG )から1978年4月に発行
されたトラ7オープリー7 (Trafo−Brief
 ) 829号第2頁に記載の電炉用変圧器の接続部か
ら知られるように、通常は個々の導体がほぼ三角柱の稜
を形成するように構成されている。その際板又は管から
なる導体の外側には回転する漏れ磁界が生じる。従って
全電路を金属製又は導電性のさやで囲むのを避けなけれ
ばならない。なぜならばかがるさやは常時始動電流が流
れる外側忙固定された短絡回転子と見なされるからであ
る。
Electrical circuits for such applications are, for example) w-on (Tranaformato)
Trafo-Brief 7, published in April 1978 by Ren Union AG
829, page 2, the individual conductors are usually constructed so as to form approximately the edges of a triangular prism. In this case, a rotating leakage field is generated on the outside of the plate or tube conductor. Therefore, surrounding the entire circuit with metallic or conductive sheaths should be avoided. This is because the braking sheath is considered to be a short-circuited rotor with an externally fixed current carrying a constant starting current.

一般に大きい変換電力を考慮して鋼溶解炉など忙給電す
る変圧器は油冷却される。従ってかかる変圧器の機能部
分は油を満たしたタンクの中忙組立てられ、巻線口出し
導体はその側壁を貫通して引き出されなければならない
。このブッシングの部分においても導体は厚さに較べて
非常に広い幅を有している。導体の広い側面は巻線軸自
身が平行であるゆえに相互に平行であ)、かつ同時に導
体断面の重心がほぼ正三角形の頂点を形成するので、ブ
ッシングの部分において紘導体の狭い側面が実際的に向
がい合っている。そのため現存する導体断面上て電流の
非常に不均一な分布が避けられず、かかる電路忙対して
は比較的小さい電力の場合でもかなシの熱的問題が生じ
る。その際特にブッシングの部分においては導体の向が
い合った狭い側面において非常に高い電流密度のために
狭く限られた局部の強い温度上昇が生じる。
Generally, in consideration of the large converted power, transformers that supply power to a steel melting furnace or the like are oil-cooled. The functional parts of such a transformer are therefore assembled in an oil-filled tank, and the winding lead-out conductors have to be led out through the side walls thereof. Also in this bushing portion, the conductor has a very wide width compared to its thickness. The wide sides of the conductor are parallel to each other since the winding axes themselves are parallel), and at the same time the center of gravity of the conductor cross section forms the vertex of an approximately equilateral triangle, so that the narrow side of the conductor in the bushing area is practically They are facing each other. This inevitably results in a highly non-uniform distribution of current over the existing conductor cross-section, resulting in severe thermal problems even at relatively small powers for such circuits. Due to the very high current densities on the opposite narrow sides of the conductors, particularly in the bushing area, strong localized temperature increases occur.

〔発明の目的〕[Purpose of the invention]

この発明は、電路のインダクタンスを小さく保ちながら
、組み込まれた導体のすべての断面部分の電流負荷がほ
ぼ等しくなるように、大変圧器から隣接する大負荷へ大
電流を導くための電路を構成することを目的とする。
This invention aims to configure an electric circuit for guiding a large current from a large voltage transformer to an adjacent large load so that the current load on all cross sections of the incorporated conductor is approximately equal while keeping the inductance of the electric path small. With the goal.

〔目的の達成手段〕 この目的は、変圧器の巻線から負荷への電路のすべての
導体が巻線口出し導体の部分においても変圧器タンク壁
を貫通するブッシングの部分においてもまたブッシング
部分に接続する導体部分においても、これら導体の幅の
広い側面が向がい合って重なるように位置すると共に、
これら導体の幅をほぼ巻線の高さに等しくすることによ
り達成される。
[Means for achieving the objective] This objective is such that all conductors of the electrical path from the transformer windings to the load are connected to the bushing section both at the section of the winding outlet conductor and at the section of the bushing penetrating the transformer tank wall. Also in the conductor parts, the wide sides of these conductors are positioned so that they face each other and overlap,
This is achieved by making the width of these conductors approximately equal to the height of the winding.

〔発明の実施態様〕[Embodiments of the invention]

この発明の有利な実施態様においては、端部鉄心脚上の
低圧巻線の中央鉄心脚に近い巻線口出し導体がこの導体
側にある中央鉄心脚上の低圧巻線の口出し導体と結合さ
れると共に、端部鉄心脚上の各低圧巻線の変圧器端部側
の口出し導体が単独に変圧器タンク壁を貫通して引き出
され、負荷装置の負荷回路の付近で相互に導電結合され
て三角結線の第3の頂点を形成するようにするとと忙よ
り、三相電路に給電する低圧巻線が三角結線される。そ
の際、導体の厚さに対する幅の比は50ないし150特
に100とするのが良く、また導体の相互間隔がこれら
導体の厚さより大であるのが良い。
In an advantageous embodiment of the invention, the winding lead conductor of the low-voltage winding on the end core leg, which is close to the central core leg, is connected to the lead conductor of the low-voltage winding on the central core leg located on this conductor side. At the same time, the lead conductors on the transformer end side of each low-voltage winding on the end core leg are individually led out through the transformer tank wall, and are conductively coupled to each other near the load circuit of the load device to form a triangular shape. By forming the third apex of the connection, the low voltage windings that feed the three-phase circuit are triangularly connected. In this case, the ratio of the width to the thickness of the conductors is preferably between 50 and 150, in particular 100, and the mutual spacing of the conductors is preferably greater than the thickness of these conductors.

外側の磁界が生じないよりに考慮されたこの発明の別の
有利な実施態様においては1両外側の導体が断面が錐状
の閉鎖用帯により上側及び下側で相互に結合されて他の
二つの導体を囲む管を形成しこの管の中を冷却媒体が貫
流する。
In a further advantageous embodiment of the invention, in which no external magnetic field is generated, the two external conductors are connected to each other on the upper and lower sides by means of a conical closure strip and the other two A tube is formed surrounding the two conductors, through which a cooling medium flows.

この発明の別の合理的な実施態様においては、個々の導
体が電気的に並列かつ空間的に平行罠ならんだ冷却媒体
の貫流する多数の管により集成されると共に、空間的に
隣接する各二つの導体間の電圧がそれぞれ単独に調整可
能にされる。
In another advantageous embodiment of the invention, the individual conductors are assembled by a plurality of tubes through which the cooling medium flows in electrically parallel and spatially parallel traps, and each of the two spatially adjacent The voltage between the two conductors is made individually adjustable.

この発明のさらに別の合理的な実施態様においては、大
電流電路が移行片に接続されて、この移行片の中で4本
の導体が断面の7字形の三つの導体によシ3光ぼうの星
形に集成された導体部分に導かれ、その際端部鉄心脚上
の巻線の変圧器端部側の二つの口出し導体が同一のV字
形導体に結合される。この各々のV字形導体の端部はそ
れぞれ三角板に′結合され、この三角板が可撓導体束又
は直列接続された管と可撓導体束とを介して負荷の接続
極と結合されるようにするのがよい。
In a further advantageous embodiment of the invention, the high-current conductor is connected to a transition piece in which the four conductors are connected to three conductors with a figure-7 cross-section. The two lead conductors on the transformer end side of the windings on the end core legs are connected to the same V-shaped conductor. The ends of each V-shaped conductor are respectively coupled to a triangular plate, and the triangular plate is coupled to the connection pole of the load via a flexible conductor bundle or a series-connected tube and flexible conductor bundle. It is better.

〔発明の実施例〕[Embodiments of the invention]

つぎKこの発明にもとづく大電流三相電路の実施例を示
す図面によりこの発明の詳細な説明する。
Next, the present invention will be explained in detail with reference to drawings showing embodiments of a high current three-phase electric circuit based on the present invention.

変圧器の水平断面を示す第1図において、鉄心はその中
央脚1及び端部脚2,3によシ半径方向内側にある高圧
側巻線4と半径方向外側に配置された低圧側巻線5.6
.7を支えている。低圧側巻線5,6.77−1.それ
ぞれ1ターンからなフ、その幅が下側継鉄8と図示され
てない上側継鉄との間の巻線長に等しい短冊板からなっ
ている。継鉄8は端部脚2.3の端を相互Kかっ中央脚
iの端と結合する。鉄心は高圧側巻線4及び低圧側巻a
5゜6.7と共に油を満たしたタンク側壁9付きタンク
の中に組立てられる。巻線口出し導体10.n。
In FIG. 1, which shows a horizontal cross-section of a transformer, the core has a central leg 1 and end legs 2, 3, with a high-voltage winding 4 located on the radially inner side and a low-voltage winding located on the radially outer side. 5.6
.. It supports 7. Low voltage side winding 5, 6.77-1. It consists of a strip plate each consisting of one turn, the width of which is equal to the length of the winding between the lower yoke 8 and the upper yoke (not shown). A yoke 8 connects the ends of the end legs 2.3 with the ends of the central leg i in a reciprocal manner. The iron core has high voltage side winding 4 and low voltage side winding a
5°6.7 is assembled in a tank with tank side walls 9 filled with oil. Winding lead conductor 10. n.

12、13.14及び15は各低圧側巻線5.’6.7
の巻線導体の延長部を開けて作られ、従って巻き付は軸
に沿った方向に巻線5.6.7と同じ@に形成される。
12, 13, 14 and 15 are each low voltage side winding 5. '6.7
is made by opening the extension of the winding conductor, so that the winding is formed in the same direction as the winding 5.6.7 in the axial direction.

巻線口出し導体loないし15は複合ブッシング16を
介してタンク側壁9を貫通しタンクから引き出される。
The winding lead conductors lo to 15 pass through the tank side wall 9 via the composite bushing 16 and are led out of the tank.

その際、低圧側巻線5.6. rの三角結線を形成する
ために、巻線口出し導体11と12及び13と14はそ
れぞれ相互に結合され、共通の厚い導体17及び18に
よりさらに導かれる。
At that time, the low voltage side winding 5.6. To form a triangular connection of r, the winding lead conductors 11 and 12 and 13 and 14 are respectively interconnected and further guided by a common thick conductor 17 and 18.

タンクの外では、導体17.18及び巻線口出し導体1
0.15の延長部は空間的に平行に走シ、その際それら
の全幅が相互に重なっている。この位置を固定するため
に、導体17.18及び巻線口出し導体10.15は、
図示されていない補助手段にょシ絶縁材料からなる間隔
片20に押圧される。
Outside the tank, conductors 17, 18 and winding lead conductor 1
The 0.15 extensions run parallel in space, their full widths overlapping each other. To fix this position, the conductor 17.18 and the winding lead conductor 10.15 are
Auxiliary means, not shown, press against the spacing piece 20 made of insulating material.

巻線口出し導体は、第2図に示すように、タンクの外で
錐状の閉鎖帯21にょシ捕われて管19を形成し、この
管は三角結線の第3の頂点の電圧を導く。管19は同時
に冷却液を導くのに用いられ、この電路冷却構造により
大電流電路の運転安全性がさらに高められる。給電すべ
き負初の接続端子が適切な構造の場合には、管19は導
体17.18と共に直接に負荷まで導かれる。
The winding lead conductor is captured outside the tank in a conical closure 21 to form a tube 19, which carries the voltage at the third vertex of the triangular connection, as shown in FIG. The tube 19 is also used to conduct the cooling liquid, and this circuit cooling structure further increases the operational safety of the high current circuit. If the negative first connection to be supplied is of suitable construction, the tube 19 is led together with the conductor 17.18 directly to the load.

しかしながら負荷の接続装置はしばしばその接続端子の
重心が#デぼ正三角形を形成するので、この発明にもと
づく電路から三角形電路への移行が必要となる。この目
的のために、第3.4.5図に示す移行片が用いられる
。この移行片にょシ、半導体17.18及び再び二つの
帯に戻った管19がそれぞれ半分だけ120’回転され
て、導体17.18及び管19が断面の7字形の導体2
2,23及び24と結合される。その際形成された断面
の7字形の導体22,23124は3光はうの星形に集
成される。
However, since load connection devices often have a center of gravity of their connection terminals forming an equilateral triangle, a transition from the electrical circuit according to the invention to a triangular electrical circuit is necessary. For this purpose, the transition piece shown in FIG. 3.4.5 is used. After this transition piece, the semiconductor 17.18 and the tube 19, which has returned to the two bands, are each rotated by half 120', so that the conductor 17.18 and the tube 19 form a figure 7-shaped conductor 2 in cross section.
2, 23 and 24. The conductors 22, 23124 having a figure 7 cross section formed at this time are assembled into a three-light star shape.

導体22.23.24の向がい合った脚の間には脈動す
る磁束が主として生じ、一方星形の外とその回シには回
転する漏れ磁界が生じる。しかしながら、星形に集成さ
れた導体22.23.24は、可撓の中間導体を介して
あらかじめ定められた負荷に問題なく接続できる。その
際、導体22.23.24の自由端を可撓な中間導体に
接続するために、大電流電路の長軸に直角に断面の7字
形の導体に取付けられた板を設けるのがよい。
A pulsating magnetic flux primarily occurs between the opposite legs of the conductors 22, 23, 24, while a rotating leakage field occurs outside the star and its turns. However, the star-shaped conductors 22, 23, 24 can be connected to a predetermined load via a flexible intermediate conductor without any problem. In order to connect the free ends of the conductors 22, 23, 24 to the flexible intermediate conductor, it is advantageous to provide a plate which is attached to the conductor with a figure 7 cross-section at right angles to the long axis of the high-current circuit.

〔発明の効果〕〔Effect of the invention〕

本発明においては上述のように1断面が厚さに較べて非
常に幅の広い導体を介して変圧器から隣接する負荷例え
ば鋼溶解炉又は電解槽へ大電流小電圧差の大電力を伝達
するための大電流三相電路において、変圧器の巻線から
負荷への電路のすべての導体が巻線口出し導体の部分に
おいても変圧器タンク壁を貫通するブッシング部分にお
いてもまたブッシング部分に接続する導体部分において
も、これら導体の幅の広い側面が向かい合って重なるよ
うに位置されると共に、これら導体の幅がほぼ巻線の高
さに等しくされるので、従来のように三相導体がその狭
い側を向かい合わせて配置される場合の導体中の電流の
不均一分布の問題が基本的に解消される。すなわち、従
来においては電流の不均一分布が導体の幅方向に生じて
いたのに対し、本発明における導体配置の場合は電流の
不均一分布は導体の厚さ方向にしか生ぜず、導体の厚さ
が幅方向寸法よりも1桁以上小さいので、電流の不均一
は実用上無視しうる程度に減少するからである。
In the present invention, as described above, large power with a large current and small voltage difference is transmitted from the transformer to an adjacent load, such as a steel melting furnace or an electrolytic cell, through a conductor whose cross section is very wide compared to its thickness. In high-current three-phase circuits, all conductors of the circuit from the transformer windings to the load are connected both at the winding lead-out conductor section, at the bushing section penetrating the transformer tank wall, and at the bushing section connecting to the bushing section. In this case, the wide sides of these conductors are placed opposite each other and overlapped, and the width of these conductors is made approximately equal to the height of the winding, so that the three-phase conductors are placed on their narrow sides as before. This basically eliminates the problem of non-uniform distribution of current in the conductor when the conductors are placed opposite each other. In other words, while in the past non-uniform distribution of current occurred in the width direction of the conductor, in the case of the conductor arrangement of the present invention, non-uniform distribution of current occurs only in the thickness direction of the conductor. This is because the non-uniformity of the current is reduced to a practically negligible level since the width is smaller than the width direction dimension by at least one order of magnitude.

また、この発明にもとづき構成された大電流三相電路は
、これら導体によシ囲まれた空間の外側にはこれら導体
によシ引き起こされる起磁力が実際上存在しないので、
非常に有利である。その際導体間の三つの中間空間にお
ける起磁力は対称である。断面の幅が広い側面が向かい
合っている千尋体間の磁束は容易に発生する渦電流のた
めに良好に導かれるので、導体の外側には実際上漏れは
ない。
Furthermore, in the high current three-phase circuit constructed based on the present invention, there is virtually no magnetomotive force caused by these conductors outside the space surrounded by these conductors.
Very advantageous. The magnetomotive forces in the three intermediate spaces between the conductors are then symmetrical. There is virtually no leakage outside the conductor, since the magnetic flux between the chihiro bodies with wide cross-sectional sides facing each other is well guided due to the easily generated eddy currents.

さらに円周上120°づつ相互にずらした導体が無いの
で、回転磁界は発生しない。その結果この発明にもとづ
き構成された導体束が変圧器タンク壁を貫通するブッシ
ングにおいて、任意の大電流に至るまで漂遊磁束による
困難さは生じない。対称な磁束にもとづき対称な電圧低
下も発生するので、個々の導体の中のインダクタンスに
よる電圧降下も絶対値が等しい。導体中の抵抗による電
圧降下は電流の位相において生じ電圧降下の対称性を支
える。
Furthermore, since there are no conductors that are mutually shifted by 120 degrees on the circumference, no rotating magnetic field is generated. As a result, in bushings constructed according to the invention in which the conductor bundle penetrates the transformer tank wall, difficulties due to stray magnetic flux do not arise up to arbitrarily high currents. Due to the symmetrical magnetic flux, symmetrical voltage drops also occur, so that the voltage drops due to the inductance in the individual conductors are also equal in absolute value. The voltage drop due to resistance in the conductor occurs in the phase of the current, supporting the symmetry of the voltage drop.

かかる磁束分布によシこの大電流三相電路においては特
にブッシングの部分においても導体のすべての断面部分
の電流負荷がtlぼ等しく従って温度上昇も一様でかつ
低い。
Due to such magnetic flux distribution, in this high-current three-phase circuit, the current load on all cross-sectional portions of the conductor is approximately equal to tl, especially in the bushing portion, and therefore the temperature rise is uniform and low.

この発明にもとづく電路のインダクタンスによる電圧降
下はまた非常に小さい。なぜならば導体の幅はその厚さ
よ)非常に大きく、同時に導体相互の間隔は導体の厚さ
よシ大きいとは言いながら絶対値を考えれば非常に小さ
いからである。従って導体が小さい駆動電圧しか必要と
しない限りはこの発明にもとづく大電流電路の長所がさ
らに生じ、負荷電力があらかじめ定められた場合変圧器
の定格容量は従来の導体配置にくらべて小さくて足シる
The voltage drop across the inductance of the circuit according to the invention is also very small. This is because the width of a conductor is very large (as compared to its thickness), and at the same time, although the spacing between conductors is larger than the thickness of the conductors, it is extremely small when considered in absolute value. Therefore, insofar as the conductors require only a small driving voltage, the advantages of the high current circuit according to the invention arise even further, and for a given load power the rated capacity of the transformer is small compared to conventional conductor arrangements. Ru.

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

第1図はこの発明にもとづく大電流三相回路の1実施例
を示す変圧器の水平断面図、第2図は第1図に示す電路
の横断面図、第3図は移行片の1実施例の平面図、第4
図は第3図に示す移行片の横断面図、第5図は第3図に
示す移行片の側面図である。 図面において、1.2.3は鉄心脚、5.6.7は低圧
側巻線、9は変圧器タンク壁、10.11.12.13
゜14、15は低圧側巻線、17.18は導体、19は
管、21は゛閉鎖用帯、22.23.24はV字形導体
である。 FIG 4 FIG 5
Fig. 1 is a horizontal sectional view of a transformer showing one embodiment of a high current three-phase circuit based on the present invention, Fig. 2 is a cross sectional view of the electric circuit shown in Fig. 1, and Fig. 3 is an embodiment of a transition piece. Example plan, 4th
The figure is a cross-sectional view of the transition piece shown in FIG. 3, and FIG. 5 is a side view of the transition piece shown in FIG. 3. In the drawing, 1.2.3 is the core leg, 5.6.7 is the low voltage side winding, 9 is the transformer tank wall, 10.11.12.13
14 and 15 are low-voltage side windings, 17 and 18 are conductors, 19 is a tube, 21 is a closing band, and 22, 23, and 24 are V-shaped conductors. FIG 4 FIG 5

Claims (1)

【特許請求の範囲】 1)断面において厚さに較べて非常に幅の広い導体を介
して変圧器から隣接する負荷へ大電流小電圧差の大電力
を伝達する念めの大電流三相電路において、変圧器の巻
線から負荷への電路のすべての導体が、巻線口出し導体
の部分においても変圧器タンク壁を貫通するブッシング
の部分においてもまたブッシング部分に接続する導体部
分においても、これら導体の幅の広い側面が向かい合っ
て相互に重なるように位置されると共に、これら導体の
幅がほぼ巻線の高さに等しくされたことを特徴とする大
電流三相電路。 2、特許請求の範囲第1項に記載の電路において、変圧
器タンク壁を貫通するブッシングに接続し幅の広い側面
が相互に重なるように位置する導体からなる前記導体部
分が直接に負荷まで延びていることを特徴とする大電流
三相電路。 3)特許請求の範囲第1項又は第2項に記載の電路にお
いて、端部鉄心脚上の低圧巻線の中央鉄心脚に近い巻線
口出し導体がこの導体側にある中央鉄心脚上の低圧巻線
の口出し導体と結合されると共に、端部鉄心脚上の各低
圧巻線の変圧器端部側の口出し導体が単独で変圧器タン
ク壁を貫通して引き出され、負荷装置の負荷回路付近で
相互に導電結合されて三角結線の第3の頂点を形成し、
三相電路に給電する低圧巻線が三角結線されることを特
徴とする大電流三相電路。 4)′特許請求の範囲第1項から第3項までのいずれか
に記載の電路において、前記導体の厚さに対する幅の比
が50ないし150特に100であることを特徴とする
大電流三相回路。 5)特許請求の範囲第1項から第4項までのいずれかに
記載の電路において、前記導体間の相互間隔がこれら導
体の厚さより大きくされた仁とを特徴とする大電流三相
電路。 6)特許請求の範囲第1項から第5項までのいずれかに
記載の電路において、両外側の導体が断面が鎌状の閉鎖
用帯によシ上側及び下側で相互に結合されて他の二つの
導体を囲む管を形成し、この管の中を冷却媒体が貫流さ
れることを特徴とする大電流三相電路。 7)特許請求の範囲第1項から第5項までのいずれかに
記載の電路において、前記の個々の導体が電気的に並列
かつ空間的に平行にならんだ冷却媒体の貫流する多数の
管により集成されることを特徴とする大電流三相電路。 8)特許請求の範囲第1項から第7項までのいずれかに
記載の電路において、空間的に隣接する6二つの導体間
の電圧がそれぞれ単独に調整可能であることを特徴とす
る大電流三相電路。 9)特許請求の範囲第1項から第8項までのいずれかに
記載の電路において、前記4本の導体(10゜17、1
8.15 )が大電流電路の移行片において断面のV字
形の三つの導体(22,23,24)により3光はう星
形に集成された負荷接続用導体部分に導かれ、その際端
部鉄心脚上の巻線の変圧器端部側の二つの口出し導体が
一つの■字形溝体(24)に結合されることを特徴とす
る大電流三相電路。 10)%許請求の範囲第1項から第9項までのいずれか
に記載の電路において、前記各V字形導体(22゜23
.24)の端部がそれぞれ三角板に結合され、この三角
板が可撓導体束又は直列接続された管と可撓導体束とを
介して負荷の接続極と結合されることを特徴とする大電
流三相電路。
[Claims] 1) A high-current three-phase circuit for transmitting large power with a large current and small voltage difference from a transformer to an adjacent load through a conductor that is very wide in cross section compared to its thickness. , all conductors of the electrical path from the transformer windings to the load are connected, both at the winding lead-out conductor, at the bushing that penetrates the transformer tank wall, and at the conductor that connects to the bushing. A high-current three-phase electric circuit characterized in that the wide sides of the conductors are positioned so as to face each other and overlap each other, and the width of these conductors is made approximately equal to the height of the winding. 2. In the electric circuit according to claim 1, the conductor portion, which is connected to a bushing penetrating the transformer tank wall and is located such that its wide sides overlap each other, extends directly to the load. A high current three-phase circuit characterized by: 3) In the electric circuit according to claim 1 or 2, the winding lead conductor close to the center core leg of the low voltage winding on the end core leg is connected to the low voltage winding on the center core leg on the side of this conductor. At the same time, the lead conductor of the transformer end of each low voltage winding on the end core leg is connected to the lead conductor of the high-voltage winding wire, and is led out independently through the transformer tank wall, near the load circuit of the load device. are conductively coupled to each other to form the third vertex of the triangular connection,
A high-current three-phase circuit characterized by triangular connection of low-voltage windings that feed power to the three-phase circuit. 4)' A high-current three-phase electrical circuit according to any one of claims 1 to 3, characterized in that the conductor has a width to thickness ratio of 50 to 150, particularly 100. circuit. 5) A high current three-phase electric circuit according to any one of claims 1 to 4, characterized in that the mutual spacing between the conductors is greater than the thickness of these conductors. 6) In the electric circuit according to any one of claims 1 to 5, both outer conductors are connected to each other at the upper and lower sides by a closing band having a sickle-shaped cross section. A high-current three-phase electric circuit characterized by forming a tube surrounding two conductors, through which a cooling medium flows. 7) In the electrical circuit according to any one of claims 1 to 5, the individual conductors are formed by a number of electrically parallel and spatially parallel tubes through which a cooling medium flows. A high-current three-phase circuit characterized by being integrated. 8) In the electric circuit according to any one of claims 1 to 7, a large current characterized in that the voltage between six spatially adjacent conductors can be individually adjusted. Three-phase electrical circuit. 9) In the electric circuit according to any one of claims 1 to 8, the four conductors (10°17, 1
8.15) is guided by three conductors (22, 23, 24) with a V-shaped cross section in the transition piece of the high current circuit to the load connection conductor part assembled in a star shape, and the end A high current three-phase electric circuit characterized in that two lead conductors on the transformer end side of the winding on the core leg are connected to one ■-shaped groove body (24). 10)% Allowance In the electric circuit according to any one of claims 1 to 9, each of the V-shaped conductors (22°23
.. 24), the ends of which are respectively coupled to triangular plates, and the triangular plates are coupled to connection poles of the load via a flexible conductor bundle or a series-connected tube and flexible conductor bundle. Phase circuit.
JP58215900A 1982-11-16 1983-11-16 Large current 3-phase electric circuit Pending JPS59103317A (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
DE32424388 1982-11-16
DE19823242438 DE3242438A1 (en) 1982-11-16 1982-11-16 HIGH CURRENT LINE FOR THREE-PHASE

Publications (1)

Publication Number Publication Date
JPS59103317A true JPS59103317A (en) 1984-06-14

Family

ID=6178301

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58215900A Pending JPS59103317A (en) 1982-11-16 1983-11-16 Large current 3-phase electric circuit

Country Status (4)

Country Link
EP (1) EP0109024B1 (en)
JP (1) JPS59103317A (en)
AT (1) ATE26038T1 (en)
DE (2) DE3242438A1 (en)

Families Citing this family (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3411141C2 (en) * 1984-03-26 1986-07-31 Transformatoren Union Ag, 7000 Stuttgart Transformer with high current bushing
DE3629310A1 (en) * 1986-08-28 1988-03-10 Transformatoren Union Ag High-current conductor for special transformers
CH671902A5 (en) * 1987-02-09 1989-10-13 Elpatronic Ag
DE9105967U1 (en) * 1991-05-14 1992-09-17 Siemens Ag, 8000 Muenchen, De
DE19947917A1 (en) * 1999-10-06 2001-04-12 Abb Research Ltd Transformer has high voltage side enclosed at least in partly by low voltage side with coaxial inner conductor, tube forming housing with bridging cap connected to conductor
CN108922746B (en) * 2018-06-26 2023-12-22 河南森源电气股份有限公司 Three-phase transformer

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
AT148848B (en) * 1935-02-05 1937-03-10 Ludwig Gavanda Dr Ing Single or multi-phase high current line.
US3125622A (en) * 1960-07-25 1964-03-17 Conductors for arc furnaces
DE2501510C3 (en) * 1975-01-16 1979-02-15 Transformatoren Union Ag, 7000 Stuttgart Winding for transformers and chokes
US4174509A (en) * 1977-12-29 1979-11-13 General Electric Company Furnace transformer having a low-voltage internally-connected delta winding

Also Published As

Publication number Publication date
DE3242438A1 (en) 1984-05-17
ATE26038T1 (en) 1987-04-15
EP0109024B1 (en) 1987-03-18
EP0109024A1 (en) 1984-05-23
DE3370400D1 (en) 1987-04-23

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