JPH0569287B2 - - Google Patents

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Publication number
JPH0569287B2
JPH0569287B2 JP60277861A JP27786185A JPH0569287B2 JP H0569287 B2 JPH0569287 B2 JP H0569287B2 JP 60277861 A JP60277861 A JP 60277861A JP 27786185 A JP27786185 A JP 27786185A JP H0569287 B2 JPH0569287 B2 JP H0569287B2
Authority
JP
Japan
Prior art keywords
phase
winding
transformer
turns
coil
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP60277861A
Other languages
Japanese (ja)
Other versions
JPS62137815A (en
Inventor
Yoshifumi Mochinaga
Masaru Ono
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.)
Toshiba Corp
Railway Technical Research Institute
Original Assignee
Toshiba Corp
Railway Technical Research Institute
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 Toshiba Corp, Railway Technical Research Institute filed Critical Toshiba Corp
Priority to JP60277861A priority Critical patent/JPS62137815A/en
Publication of JPS62137815A publication Critical patent/JPS62137815A/en
Publication of JPH0569287B2 publication Critical patent/JPH0569287B2/ja
Granted legal-status Critical Current

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  • Ac-Ac Conversion (AREA)
  • Control Of Electrical Variables (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

〔発明の技術分野〕 本発明は中性点直接接地の三相送電系統におい
て使用され、特に二相側を改良した安定巻線方式
三相二相変換用変圧器に関する。 〔発明の技術的背景とその問題点〕 高速電気車に電力を供給するための、き電用変
圧器には第13図に示すような変形ウツドブリツ
ジ結線と呼ばれる三相二相変換用変圧器1と昇圧
用変圧器2とで構成されたものが使用されてい
る。 三相二相変換用変圧器1は1次巻線が星形結線
であり電圧E1で受電し、2次巻線はV相を並列
接続した二重三角結線である。 この2次巻線の1組の出力端子ac間の電圧を
E2とすれば、もう1組の出力端子b′d′間の電圧は
E2/√3となり、端子ac間と端子b′d′間の電圧の
位相差は90度となつている。 昇圧用変圧器2は入力端子b′d′間の電圧E2/√
3を昇圧し、出力端子bd間に電圧E2を発生する
単巻変圧器である。 この変形ウツドブリツジ結線変圧器方式では、
1次側中性点0が直接接地できるので、超高圧送
電系統からも直接受電ができ1次巻線の絶縁が大
幅に低減できる利点がある。 しかし三相二相変換用変圧器1ほかに昇圧用変
圧器2が必要となるため、大形化し、製造価格が
高くなり、かつ広い設置場所と多額の工事費が必
要となる欠点がある。 次に2次側の絶縁階級の低減について説明す
る。 第14図は変形ウツドブリツジ結線変圧器の片
座と等価である単相2巻線形のき電用変圧器3の
1次側に電源4を接続し、2次側にしや断器5を
介して単巻変圧器6A,6B,6Cを接続し、電
気車7に給電する従来の単巻変圧器き電方式
(AT方式)を示している。この方式ではき電用
変圧器3の2次側は非接地方式となつているた
め、単巻変圧器6A,6B,6Cが接続されてい
ない状態、すなわちしや断器5が開の時に、2次
側で地絡が発生することを考慮して、電気車電圧
ETの2倍である2次電圧E2に相当する絶縁階級
としている。 第15図は最近開発された新AT方式を示した
ものであり、そのき電用変圧器8は電気車電圧
ETに等しいE2/2である2組の2次巻線を有す
る単相3巻線形の変圧器であり、第1(変電所)
ATである単巻変圧器6が省略されている。 すなわち、1次巻線9には電圧E1の電源4が
接続され、2次巻線10T,10Fは直列に接続
され、その接続点Nはレール21と接続すると共
に放電器22を介して接地され、両端の端子T,
Fに、しや断器5を介して単巻変圧器6B,6C
を接続し、電気車7に給電する回路図である。 実際の使用では、これらの回路を両座分用意
し、それらの出力電圧の位相差を90度になるよう
に構成し、両座の負荷が同一であれば1次側の三
相電源からの電流は三相平衡が得られるようにし
たものである。 この新AT方式では、たとえ、しや断器5が開
の時にも接続点Nはレールと接続すると共に放電
器を介して接地されているので2次側の絶縁階級
は電気車電圧ET、すなわち2次巻線の一方の電
圧E2/2に相当する値でよく、従来方式の半分
にすることができる。 しかも、2次巻線は接続点Nで接地されている
単巻結線であるので、第1ATと呼ばれる単巻変
圧器6Aの作用も有するので、第15図に示すよ
うに単巻変圧器6Aは不要とすることもできる。 〔発明の目的〕 本発明の目的は以上説明したような新AT方式
に採用されるき電9変圧器であり、小形で製造価
格が低減できる安定巻線方式三相二相変換用変圧
器を提供することにある。 〔発明の概要〕 本発明によるき電用変圧器は、その1次巻線を
星形結線とし、その中性点を接地して使用でき、
その2次巻線は、第2相のコイルの巻回数を第1
相および第3相のコイルの巻回数より、少なく
し、第2相を共有する2個の星形結線をなし、か
つ第2相の中間から中性点Nを取出し接地できる
ようにし、その3次巻線は三角結線とし、2次負
荷電流により不平衡アンペアターンを打消すため
に流れる循環電流を通し、星形結線だけの場合に
必要である安定巻線の役目もさせることである。 〔発明の実施例〕 以下本発明を第1図に示す実施例について説明
する。本実施例の変圧器11は第1図に示すよう
に、1次巻線12が普通の星形結線であり、2次
巻線13は後述するように特殊の星形結線であ
り、3次巻線14はその一端子aを接地した普通
の三角結線であり、これらの巻線が鉄心(図示し
ていない)上に巻装された、一種の三巻線変圧器
である。 2次巻線は第1相(U相)および第3相(W
相)を巻回数Nとする、コイル各2個(13u1
13u2,13w1,13w2)と、第2相(V相)
を巻回数(√3−1)N/2とするコイル2個
(13v1,13v2)とから成り、第2相のコイル
13v1,13v2を直列に接続し、その接続点を中
性点Nとし、その下部端子θ1に第1相コイルの1
3u1と第3相コイルの13w1を、その上部端子
θ2に第1相コイルの13u2と第3相コイルの13
w2を、第2相コイル13v1,13v2と位相差が
各々120度になるように接続し、残りの他端子を
2次端子TA,FA,TB,FBとする。 上記のように、2次巻線の各コイルの巻回数を
定め結線すると、第1図において、例えば三角形
TA,θ1,Nは2辺の長さ(TA−θ1とθ1とN)が
わかり、その夾角(TA−θ1−N)が120度である
ので、角θ1−N−TAは45度となり、端子TA,N,
FAを結ぶ点線15Aは直線になり、これをA座
の誘起電圧と呼び、同様に端子TB,N,FBを結
ぶ点線15Bも直線になり、これをB座の誘起電
圧と呼ぶ。そしてA座の誘起電圧15AとB座の
誘起電圧15Bは互に直交することになり、2次
端子たとえばTAと中性点Nとの点線の長さ、す
なわち誘起電圧15Aの半分の大きさは巻回数
[Technical Field of the Invention] The present invention relates to a stable winding type three-phase to two-phase conversion transformer that is used in a three-phase power transmission system with a directly grounded neutral point, and in particular has an improved two-phase side. [Technical background of the invention and its problems] A three-phase to two-phase conversion transformer 1 called a modified Utsudo bridge connection as shown in Fig. 13 is used as a feeding transformer for supplying power to high-speed electric cars. and a step-up transformer 2 are used. In the three-phase to two-phase conversion transformer 1, the primary winding has a star connection and receives power at a voltage E1 , and the secondary winding has a double triangular connection in which V-phases are connected in parallel. The voltage between one set of output terminals ac of this secondary winding is
If E 2 , the voltage between the other set of output terminals b′d′ is
E 2 /√3, and the phase difference between the voltages between terminals ac and terminals b'd' is 90 degrees. Step-up transformer 2 has a voltage between input terminals b′d′ E 2 /√
This is an autotransformer that boosts E 3 and generates voltage E 2 between output terminals b and d. In this modified Utsudo bridge connection transformer system,
Since the primary side neutral point 0 can be directly grounded, there is an advantage that power can be directly received from the ultra-high voltage power transmission system, and the insulation of the primary winding can be significantly reduced. However, since a step-up transformer 2 is required in addition to the three-phase to two-phase conversion transformer 1, there are disadvantages in that the size is large, the manufacturing cost is high, and a large installation space and large construction costs are required. Next, the reduction of the insulation class on the secondary side will be explained. Fig. 14 shows a power supply 4 connected to the primary side of a single-phase two-winding feeding transformer 3, which is equivalent to a single seat of a modified Utsudo bridge-connected transformer, and a power supply 4 connected to the secondary side via a shear breaker 5. A conventional autotransformer feeding system (AT system) is shown in which autotransformers 6A, 6B, and 6C are connected to supply power to an electric car 7. In this system, the secondary side of the feeding transformer 3 is non-grounded, so when the autotransformers 6A, 6B, and 6C are not connected, that is, when the shield breaker 5 is open, Considering that a ground fault may occur on the secondary side, the electric vehicle voltage
The insulation class corresponds to the secondary voltage E2 , which is twice E T. Figure 15 shows a recently developed new AT system, in which the feeding transformer 8 is connected to the electric vehicle voltage.
It is a single-phase three-winding transformer with two sets of secondary windings with E 2 /2 equal to T , and the first (substation)
The autotransformer 6, which is an AT, is omitted. That is, the power source 4 of voltage E 1 is connected to the primary winding 9, the secondary windings 10T and 10F are connected in series, and the connection point N is connected to the rail 21 and grounded via the discharger 22. and the terminals T at both ends,
F, autotransformers 6B and 6C are connected to F via a disconnector 5.
2 is a circuit diagram for connecting the electric vehicle 7 and supplying power to the electric vehicle 7. FIG. In actual use, these circuits are prepared for both sides, configured so that the phase difference between their output voltages is 90 degrees, and if the loads on both sides are the same, the power from the three-phase power supply on the primary side is The current is such that three-phase balance is obtained. In this new AT system, even when the shield breaker 5 is open, the connection point N is connected to the rail and grounded via the discharger, so the insulation class on the secondary side is equal to the electric car voltage E T , That is, a value corresponding to the voltage E 2 /2 of one side of the secondary winding is sufficient, which can be half of that of the conventional system. Moreover, since the secondary winding is an auto-winding connection that is grounded at the connection point N, it also has the function of the auto-transformer 6A called 1st AT, so the auto-transformer 6A as shown in FIG. It can also be made unnecessary. [Object of the Invention] The object of the present invention is to provide a feeder 9 transformer to be adopted in the new AT system as explained above, and to provide a stable winding type three-phase to two-phase conversion transformer that is compact and can reduce manufacturing costs. It is about providing. [Summary of the Invention] The feeding transformer according to the present invention has its primary winding connected in a star shape, and can be used with its neutral point grounded.
The secondary winding has a number of turns of the second phase coil.
The number of windings is smaller than that of the phase and third phase coils, two star-shaped wires are formed that share the second phase, and the neutral point N is taken out from the middle of the second phase so that it can be grounded. The secondary winding is triangularly connected to pass the circulating current that flows to cancel out unbalanced ampere turns due to the secondary load current, and also serves as a stabilizing winding, which is required in the case of only star-shaped connections. [Embodiments of the Invention] The present invention will be described below with reference to an embodiment shown in FIG. In the transformer 11 of this embodiment, as shown in FIG. The winding 14 is a normal triangular connection with one terminal a grounded, and these windings are wound around an iron core (not shown), forming a type of three-winding transformer. The secondary winding is the first phase (U phase) and the third phase (W
2 coils each (13u 1 ,
13u 2 , 13w 1 , 13w 2 ) and the second phase (V phase)
It consists of two coils (13v 1 , 13v 2 ) with the number of turns (√3-1)N/2, and the second phase coils 13v 1 , 13v 2 are connected in series, and the connection point is connected to the neutral 1 of the first phase coil is connected to the lower terminal θ 1 of the point N.
3u 1 and 13w 1 of the third phase coil, and connect 13u 2 of the first phase coil and 13w of the third phase coil to its upper terminal θ 2 .
w 2 is connected to the second phase coils 13v 1 and 13v 2 so that the phase difference is 120 degrees, and the remaining terminals are designated as secondary terminals T A , F A , T B , and F B . As mentioned above, when the number of turns of each coil of the secondary winding is determined and the wires are connected, for example, a triangle is formed in Fig. 1.
For T A , θ 1 , and N, the lengths of the two sides (TA − θ 1 and θ 1 and N) are known, and the included angle (TA θ 1 − N) is 120 degrees, so the angle θ 1 − N-T A is 45 degrees, and terminals T A , N,
The dotted line 15A connecting F A is a straight line, and this is called the induced voltage at the A position. Similarly, the dotted line 15B connecting the terminals T B , N, and F B is also a straight line, and this is called the induced voltage at the B position. The induced voltage 15A at the A location and the induced voltage 15B at the B location are orthogonal to each other, and the length of the dotted line between the secondary terminal, for example, T A and the neutral point N, is half the magnitude of the induced voltage 15A. is the number of turns

【式】に相当する。故に、誘起電圧の大きさ でTA−N間をE2/2とすればTA−θ1間はCorresponds to [formula]. Therefore, if the magnitude of the induced voltage is E 2 /2 between T A and N, then between T A and θ 1 is

【式】θ1−N間はE2/2×√3−1/√6とな る。 他の2次端子FA,TB,FBと中性点Nとの各関
係も、2次端子TAと中性点Nとの関係に全く同
様である。 この変圧器11の巻線配列構成の一例を第2図
に示す。すなわち鉄心脚16に、1次巻線12の
内側と外側に3次巻線14を巻装し、さらに最内
側に2次巻線の1群13u1,13v1,13w1を、
そして最外側に2次巻線の2群13u2,13v2
13w2を各々巻装した、サンドイツチ配置と呼
ばれるものであり、第1相と第3相はその構成が
全く同一になるが、第2相は2次巻線のコイル1
3v1,13v2が他相に比べ、その巻回数が(√3
−1)/2倍と少なく、後述するようにその通電
電流が√2倍と大きくなるので、その構成は他相
と異なる。 第1図において、1次側端子UVWに三相電圧
E1を印加すれば、2次側の誘起電圧はA座のTA
−N−FAの単相電圧15Aと、B座のTB−N−
FBの単相電圧15Bが得られ、この両座の単相
電圧15A,15Bはその大きさE2が等しく、
90度の位相差を有していることになり、これらの
中央は中性点Nで一緒になり、接地できるよう
に、構成すれば、2次端子の対地電圧はE2/2
となり第15図に示す新AT方式の回路に適用で
きることになる。 次に本実施例の如き構成にすると、2次側の
A,B両座に単相負荷が平衡している場合に、1
次側三相電源に対しては三相平衡負荷となること
を説明する。 まず、各部に流れる電流について、その解折を
簡単にするために各巻線の巻回数を第3図に示す
ような比、すなわち、コイル13u1,13u2,1
3w1,13w2
[Formula] The distance between θ 1 and N is E 2 /2×√3−1/√6. The relationships between the other secondary terminals F A , T B , F B and the neutral point N are exactly the same as the relationship between the secondary terminal T A and the neutral point N. An example of the winding arrangement configuration of this transformer 11 is shown in FIG. That is, the tertiary winding 14 is wound around the core leg 16 on the inside and outside of the primary winding 12, and the first group of secondary windings 13u 1 , 13v 1 , 13w 1 is further placed on the innermost side.
Then, on the outermost side, two groups of secondary windings 13u 2 , 13v 2 ,
13w2 is wound on each side, which is called a sanderch arrangement, and the first and third phases have exactly the same configuration, but the second phase has coil 1 of the secondary winding.
Compared to other phases, the number of turns of 3v 1 and 13v 2 is (√3
-1)/2 times, and as will be described later, the conduction current is as large as √2 times, so its configuration is different from other phases. In Figure 1, the three-phase voltage is applied to the primary terminal UVW.
If E 1 is applied, the induced voltage on the secondary side is T A at A
-N-F A single phase voltage of 15A and B location T B -N-
A single-phase voltage 15B of F B is obtained, and the single-phase voltages 15A and 15B of both sides have the same magnitude E 2 ,
They have a phase difference of 90 degrees, and if they are configured so that their centers meet at the neutral point N and can be grounded, the voltage to ground of the secondary terminal will be E 2 /2
Therefore, it can be applied to the circuit of the new AT method shown in Fig. 15. Next, with the configuration as in this embodiment, when the single-phase load is balanced on both A and B on the secondary side, 1
It will be explained that there is a three-phase balanced load for the next three-phase power supply. First, in order to simplify the analysis of the current flowing through each part, the number of turns of each winding is set to the ratio shown in FIG .
3w 1 , 13w 2

〔発明の効果〕〔Effect of the invention〕

以上説明したように、本発明によれば、一時側
巻線は星形結線であるので、その中性点を引出し
直接接地できるので短絡容量の大きい超高圧線路
からも直接受電が可能であり、又、1次巻線は段
絶縁と低減絶縁にできる。そして2次側巻線は、
その中性点を引出し、接地できるので新AT方式
の回路に適用でき、2次側の絶縁階級が半減でき
る。 しかも特別な昇圧用変圧器を必要としないの
で、その構造が簡単で小形・軽量化が可能で製造
価格が低減でき、その据付面積を少なくて済む安
定巻線方式三相二相変換用変圧器を提供できる。
As explained above, according to the present invention, since the temporary side winding is star-shaped, the neutral point can be drawn out and directly grounded, so that it is possible to directly receive power even from an ultra-high voltage line with a large short circuit capacity. Also, the primary winding can be provided with stepped insulation or reduced insulation. And the secondary winding is
Since the neutral point can be extracted and grounded, it can be applied to new AT system circuits, and the insulation class on the secondary side can be halved. Moreover, since a special step-up transformer is not required, the structure is simple, compact and lightweight, reducing manufacturing costs, and the stable winding type three-phase to two-phase conversion transformer requires less installation space. can be provided.

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

第1図は本発明による安定巻線方式三相二相変
換用変圧器の一実施例を示す結線図、第2図は第
1図に示した変圧器の巻線配列の一例を示す概略
構成図、第3図は第1図に示した変圧器における
各巻線の巻数比を示す説明図、第4図から第6図
は第1図に示した変圧器においてA座のみに負荷
をとつた場合の電流分布を示す説明図、第7図は
第1図に示した変圧器においてB座のみに負荷を
とつた場合の電流分布を示す説明図、第8図は第
1図に示した変圧器においてA座、B座同時に同
一負荷をとつた場合の電流分布および各電流の正
方向を示す説明図、第9図は第8図における電流
のベクトル図、第10図は本発明の他の実施例の
2次巻線を示す結線図、第11図は第10図の変
圧器を適用するAT方式の回路構成図、第12図
は本発明の他の実施例の2次巻線とリアクタンス
補償用直列コンデンサと保護ギヤツプの接続を示
す説明図、第13図は従来の変形ウツドブリツジ
結線のき電用変圧器の結線図、第14図は従来の
変形ウツドブリツジ結線におけるAT方式の回路
構成図、第15図は新しい三相二相変換用変圧器
によるAT方式の回路構成図である。 1……変形ウツドブリツド結線の三相二相変換
用変圧器、2……変形ウツドブリツジ結線の昇圧
用変圧器、3,8……き電用変圧器、5……しや
断器、6A,6B,6C……単巻変圧器、7……
電気車、10T……トロリ線側に接続される2次
巻線、10F……フイーダ側に接続される2次巻
線、11……安定巻線方式三相二相変換用変圧
器、12……1次巻線、13u1,13u2,13
v1,13v2,13w1,13w2,13v11,13
v12,13v21,13v22……2次巻線の各コイル、
14……3次巻線、15A,15B……A座、B
座の誘起電圧、16……鉄心脚、17……三相電
源、18……2次側単相負荷、19……直列コン
デンサ、20……保護ギヤツプ、21……レー
ル、22……放電器。
Fig. 1 is a wiring diagram showing an embodiment of a stable winding type three-phase to two-phase conversion transformer according to the present invention, and Fig. 2 is a schematic configuration showing an example of the winding arrangement of the transformer shown in Fig. 1. Figure 3 is an explanatory diagram showing the turns ratio of each winding in the transformer shown in Figure 1, and Figures 4 to 6 are diagrams showing the transformer shown in Figure 1 with a load applied only to the A seat. Figure 7 is an explanatory diagram showing the current distribution when the transformer shown in Figure 1 is loaded only at the B seat. Figure 8 is an explanatory diagram showing the current distribution when the transformer shown in Figure 1 is loaded. An explanatory diagram showing the current distribution and the positive direction of each current when the same load is applied to the A and B locations at the same time, FIG. 9 is a vector diagram of the current in FIG. 8, and FIG. 10 is an illustration of another example of the present invention. A wiring diagram showing the secondary winding of the embodiment, Fig. 11 is a circuit diagram of an AT system to which the transformer of Fig. 10 is applied, and Fig. 12 shows the secondary winding and reactance of another embodiment of the present invention. An explanatory diagram showing the connection of a compensation series capacitor and a protective gap, Fig. 13 is a wiring diagram of a feeding transformer with a conventional modified Udo bridge connection, and Fig. 14 is a circuit configuration diagram of an AT method with a conventional modified Udo bridge connection. Figure 15 is a circuit diagram of an AT system using a new three-phase to two-phase conversion transformer. 1...Three-phase two-phase conversion transformer with modified mud bridge connection, 2...Step-up transformer with modified mud bridge connection, 3, 8...Feeding transformer, 5...Shield breaker, 6A, 6B , 6C...autotransformer, 7...
Electric car, 10T...Secondary winding connected to the contact wire side, 10F...Secondary winding connected to the feeder side, 11...Stable winding type three-phase to two-phase conversion transformer, 12... ...Primary winding, 13u 1 , 13u 2 , 13
v 1 , 13v 2 , 13w 1 , 13w 2 , 13v 11 , 13
v 12 , 13v 21 , 13v 22 ...each coil of the secondary winding,
14...Tertiary winding, 15A, 15B...A seat, B
Induced voltage at the seat, 16... Iron core leg, 17... Three-phase power supply, 18... Secondary side single-phase load, 19... Series capacitor, 20... Protective gap, 21... Rail, 22... Discharger .

Claims (1)

【特許請求の範囲】 1 1次巻線は三相とも同一巻回数である星形結
線とし、2次巻線は、第1相および第3相を巻回
数Nとするコイル各2個と、第2相を巻回数(√
3−1)Nとするコイル1個とから成り、 前記第2相コイルの両端に、前記第1相および
第3相のコイルの一端を第2相と位相差が各々
120度になるように接続し、他の一端を2次端子
とし、同じ大きさである2個の2次側誘起電圧
で、その位相差を90度になるように接続し、かつ
前記第2相コイルの中間から中性点リードを取出
す構成とし、 3次巻線は三相とも同一巻回数である三角結線
としたことを特徴とする安定巻線方式三相二相変
換用変圧器。 2 2次巻線は、第1相および第3相を巻回数N
とするコイル各2個と、 第2相を巻回数(√3−1)N/2とするコイ
ル4個とから成り、 前記第2相コイルに、前記第1相あるいは第3
相のコイルの各1個を位相差が120度となるよう
に各々を直列に接続し、その両端を2次端子と
し、同じ大きさである4個の2次側誘起電圧で、
それらの位相差を各々90度になるように接続した
ことを特徴とする特許請求の範囲第1項記載の安
定巻線方式三相二相変換用変圧器。
[Claims] 1. The primary winding has a star-shaped connection in which the number of turns is the same for all three phases, and the secondary winding has two coils each with the number of turns N for the first and third phases, The number of turns of the second phase (√
3-1) one coil of N, and one end of the first phase and third phase coils is connected to both ends of the second phase coil, and one end of the first phase coil and the third phase coil are connected to each other with a phase difference from the second phase.
120 degrees, the other end is used as a secondary terminal, two secondary side induced voltages of the same magnitude are connected so that their phase difference is 90 degrees, and the second A stable winding type three-phase to two-phase conversion transformer, characterized in that the neutral point lead is taken out from the middle of the phase coil, and the tertiary winding is a triangular connection with the same number of turns for all three phases. 2 The secondary winding has the number of turns of the first and third phases N.
and four coils each having a second phase with a number of turns (√3-1)N/2.
Each phase coil is connected in series so that the phase difference is 120 degrees, and both ends are used as secondary terminals, and the four secondary side induced voltages are the same size.
A stable winding type three-phase to two-phase conversion transformer according to claim 1, characterized in that these are connected so that their phase differences are 90 degrees.
JP60277861A 1985-12-12 1985-12-12 Stabilized winding type transformer for three-phase to two-phase conversion Granted JPS62137815A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60277861A JPS62137815A (en) 1985-12-12 1985-12-12 Stabilized winding type transformer for three-phase to two-phase conversion

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60277861A JPS62137815A (en) 1985-12-12 1985-12-12 Stabilized winding type transformer for three-phase to two-phase conversion

Publications (2)

Publication Number Publication Date
JPS62137815A JPS62137815A (en) 1987-06-20
JPH0569287B2 true JPH0569287B2 (en) 1993-09-30

Family

ID=17589307

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60277861A Granted JPS62137815A (en) 1985-12-12 1985-12-12 Stabilized winding type transformer for three-phase to two-phase conversion

Country Status (1)

Country Link
JP (1) JPS62137815A (en)

Also Published As

Publication number Publication date
JPS62137815A (en) 1987-06-20

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