JP3343083B2 - Linkage flux control type transformer device - Google Patents
Linkage flux control type transformer deviceInfo
- Publication number
- JP3343083B2 JP3343083B2 JP31462098A JP31462098A JP3343083B2 JP 3343083 B2 JP3343083 B2 JP 3343083B2 JP 31462098 A JP31462098 A JP 31462098A JP 31462098 A JP31462098 A JP 31462098A JP 3343083 B2 JP3343083 B2 JP 3343083B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic circuit
- cut core
- winding
- shaped cut
- phase
- 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 - Fee Related
Links
- 230000004907 flux Effects 0.000 title claims description 179
- 238000004804 winding Methods 0.000 claims description 215
- 230000007423 decrease Effects 0.000 description 25
- 238000010586 diagram Methods 0.000 description 15
- 230000005284 excitation Effects 0.000 description 9
- 230000000087 stabilizing effect Effects 0.000 description 4
- 230000006641 stabilisation Effects 0.000 description 2
- 238000011105 stabilization Methods 0.000 description 2
- 238000005299 abrasion Methods 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 230000005611 electricity Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000012423 maintenance Methods 0.000 description 1
- 238000010079 rubber tapping Methods 0.000 description 1
Landscapes
- Control Of Electrical Variables (AREA)
- Ac-Ac Conversion (AREA)
Description
【0001】[0001]
【発明の属する技術分野】この発明は、電力系統の変電
所や、需要家の受電設備の変圧器装置等に適用され、電
力系統の電圧変動や、負荷変動による電圧変動を自動的
に補償し二次(負荷)電圧を安定化することができる鎖
交磁束制御形変圧器装置に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention is applied to a substation of a power system, a transformer device of a power receiving facility of a customer, and the like, and automatically compensates for a voltage fluctuation of a power system and a voltage fluctuation due to a load fluctuation. The present invention relates to a flux linkage control type transformer device capable of stabilizing a secondary (load) voltage.
【0002】[0002]
【従来の技術】近年の経済発展に伴う電力需要の増大、
負荷の多様化等により電圧の変動等に対応できるフレキ
シブルな電力設備が求められつつある。電力系統の電圧
の安定化に寄与する従来の技術は、図16に示すような
変圧器のタップ切換形電圧調整器で対処していた。この
変圧器のタップ切換形電圧調整器は、タップ接触部とタ
ップ切換機構があり、タップ接触部の摩耗、接触不良等
の他、タップ切換機構の動作による電圧制御の時間的遅
れや機構の摩耗など、保守・性能上から基本的に使用上
の制約があった。2. Description of the Related Art In recent years, the demand for electricity has increased due to economic development,
Flexible power equipment that can cope with voltage fluctuations and the like due to diversification of loads and the like is being demanded. The conventional technology that contributes to stabilization of the voltage of the power system has been dealt with by a tap- switching voltage regulator of a transformer as shown in FIG. The tap switching type voltage regulator of this transformer has a tap contact portion and a tap switching mechanism, and in addition to the abrasion of the tap contact portion, poor contact, etc., time delay of voltage control due to the operation of the tap switching mechanism and wear of the mechanism. Basically, there were restrictions on use in terms of maintenance and performance.
【0003】これに対し、本出願人は先に一次巻線と二
次巻線の鎖交磁束を制御する磁束制御形可変変圧器(特
願平9−83793号)について提案した。図17は、
本出願人が先に提案した磁束制御形可変変圧器の一実施
例を示す斜視図で、この磁束制御形可変変圧器は、図1
7に示すように、一次巻線14と二次巻線19、変圧器
用磁気回路21及び捩じれ方向に90度回転させて接触
させたU形カットコア11,13並びに制御巻線12で
構成される。On the other hand, the present applicant has previously proposed a magnetic flux control type variable transformer (Japanese Patent Application No. 9-83793) for controlling the interlinkage magnetic flux between the primary winding and the secondary winding. FIG.
FIG. 1 is a perspective view showing an embodiment of a magnetic flux control type variable transformer previously proposed by the present applicant.
As shown in FIG. 7, the primary winding 14 and the secondary winding 19, a transformer magnetic circuit 21, U-shaped cut cores 11 and 13, which are in contact with each other by being rotated by 90 degrees in the torsion direction, and a control winding 12. .
【0004】この変圧器の二次電圧e2は、一次巻線1
4により磁束φ1−1,φ1−2の内二次巻線19と鎖
交するφ1−2の値によって決まるが、二次巻線に負荷
電流i2が流れるとφ1−2と逆方向に磁束φ2が生
じ、φ1−2はφ1−1の磁気回路側へシフトして減少
し、二次電圧は低下する。そこで、制御巻線12に励磁
電流icを流すことによりU形カットコアの接触部15
で磁気飽和しφ1−1の磁気回路の磁気抵抗が大きくな
り、φ1−1,φ1−2の磁束配分が変化するので二次
電圧を上昇させることができる。[0004] The secondary voltage e2 of the transformer is the primary winding 1
4 is determined by the value of φ1-2 interlinked with the secondary winding 19 of the magnetic fluxes φ1-1 and φ1-2, but when the load current i2 flows through the secondary winding, the magnetic flux φ2 in the opposite direction to φ1-2. Occurs, φ1-2 shifts to the magnetic circuit side of φ1-1 and decreases, and the secondary voltage decreases. Therefore, the exciting current ic is passed through the control winding 12 to make the contact portion 15 of the U-shaped cut core.
, The magnetic resistance of the magnetic circuit of φ1-1 increases, and the magnetic flux distribution of φ1-1 and φ1-2 changes, so that the secondary voltage can be increased.
【0005】しかし、この変圧器は、無負荷の場合、一
次巻線電流による磁束φ1−2を打消す磁束φ2が生じ
無い。そして、磁束φ1−1とφ1−2の配分はそれぞ
れの磁気回路の磁気抵抗に反比例するが、φ1−1の磁
気回路はU形カットコアの接触部15を含んでおり磁気
抵抗が大きく、制御巻線12の励磁電流が無い場合でも
φ1−2に集中して配分される。このため二次電圧e2
は高めになるが、制御巻線12に励磁電流を流しても二
次電圧e2を高める方向しか制御できないので、これを
考慮しないで設計すると二次電圧e2の調整範囲が狭く
なる。However, in this transformer, when there is no load, no magnetic flux φ2 cancels out the magnetic flux φ1-2 due to the primary winding current. The distribution of the magnetic fluxes φ1-1 and φ1-2 is inversely proportional to the magnetic resistance of each magnetic circuit. However, the magnetic circuit of φ1-1 includes the contact portion 15 of the U-shaped cut core, and the magnetic resistance is large. Even when there is no exciting current of the winding 12, the current is concentrated and distributed to φ1-2. Therefore, the secondary voltage e2
However, even if an exciting current is supplied to the control winding 12, only the direction in which the secondary voltage e2 is increased can be controlled. Therefore, if the secondary voltage e2 is designed without taking this into consideration, the adjustment range of the secondary voltage e2 is narrowed.
【0006】また、二次巻線19に進み負荷電流が流れ
た場合は、一次巻線14の漏洩リアクタンス部分で電圧
が上昇しφ1−2の磁束が増加して、二次電圧e2は高
くなり、また、制御巻線12の励磁電流を増加してφ1
−1の磁気回路の磁気抵抗を高め、一次巻線14の漏洩
リアクタンスを減少させて電圧上昇を抑制するとφ1−
2の磁束増加要因となり調整範囲が狭くなる。When a load current flows through the secondary winding 19, the voltage rises in the leakage reactance portion of the primary winding 14 and the magnetic flux φ1-2 increases, so that the secondary voltage e2 increases. The exciting current of the control winding 12 is increased to
-1 to increase the magnetic resistance of the magnetic circuit and reduce the leakage reactance of the primary winding 14 to suppress the voltage rise.
2, which causes an increase in magnetic flux, and the adjustment range is narrowed.
【0007】[0007]
【発明が解決しようとする課題】本出願人が先に提案し
た上記磁束制御形可変変圧器は、磁気回路構成から無負
荷時と進み負荷時の電圧調整幅が狭くなる特性上の課題
を有する。The magnetic flux control type variable transformer previously proposed by the present applicant has a characteristic problem that the voltage adjustment width at the time of no load and at the time of the load becomes narrow due to the magnetic circuit configuration. .
【0008】そこで、本発明は、負荷の状態に関係なく
電圧の調整範囲を広げるため、一次巻線と二次巻線の鎖
交磁束を能動的に制御する鎖交磁束制御形変圧器装置を
提供することを目的とする。Accordingly, the present invention provides a flux linkage control type transformer device for actively controlling the flux linkage between the primary winding and the secondary winding in order to widen the voltage adjustment range irrespective of the load condition. The purpose is to provide.
【0009】[0009]
【課題を解決するための手段】請求項1の発明は、第1
の磁気回路と第2の磁気回路を有し、第1の磁気回路
は、第1のU形カットコアと第2のU形カットコアと
を、そのカット面同志を互いに対向させ、かつ、一方の
カットコアに対して他方のカットコアを捩じれ方向に9
0度回転させて接触させた磁気回路で構成し、第2の磁
気回路は、第3のU形カットコアと第4のU形カットコ
アとを、そのカット面同志を互いに対向させ、かつ、一
方のカットコアに対して他方のカットコアを捩じれ方向
に90度回転させて接触させた磁気回路で構成し、第1
の磁気回路の第1のU形カットコアと第2の磁気回路の
第3のU形カットコアに共通の一次巻線を巻回し、第2
の磁気回路の第3のU形カットコアには二次巻線を巻回
し、第1の磁気回路の第2のU形カットコアには漏洩磁
束制御巻線を巻回し、第2の磁気回路の第4のU形カッ
トコアには主磁束制御巻線を巻回し、前記主磁束制御巻
線と前記漏洩磁束制御巻線の励磁電流の値を変え、一次
巻線の第1の磁気回路と第2の磁気回路の磁気抵抗を変
化させて、前記一次巻線と前記二次巻線の鎖交磁束を制
御し、二次巻線電圧を連続的に可変することを特徴とし
たものである。According to the first aspect of the present invention, there is provided the following:
And a second magnetic circuit, wherein the first magnetic circuit has a first U-shaped cut core and a second U-shaped cut core with their cut surfaces facing each other, and The other cut core is twisted 9
The second magnetic circuit includes a third U-shaped cut core and a fourth U-shaped cut core, the cut surfaces of which are opposed to each other, The first cut core is constituted by a magnetic circuit in which the other cut core is rotated by 90 degrees in a torsion direction and brought into contact with one cut core, and
A primary winding wound around a first U-shaped cut core of the first magnetic circuit and a third U-shaped cut core of the second magnetic circuit;
A secondary winding is wound around a third U-shaped cut core of the magnetic circuit, and a leakage flux control winding is wound around a second U-shaped cut core of the first magnetic circuit. The fourth U-shaped cut core has a main magnetic flux control winding wound thereon, and changes the values of the exciting currents of the main magnetic flux control winding and the leakage magnetic flux control winding. The magnetic resistance of the second magnetic circuit is changed to control the interlinkage magnetic flux between the primary winding and the secondary winding, thereby continuously varying the secondary winding voltage. .
【0010】請求項2の発明は、第1の三相磁気回路と
第2の三相磁気回路を有し、第1の三相磁気回路は、第
1のE形カットコアと第1のU形カットコアとを、その
カット面同志を互いに対向させ、かつ、一方のカットコ
アに対して他方のカットコアを捩じれ方向に90度回転
させて接触させた磁気回路で構成し、第2の三相磁気回
路は、第2のE形カットコアと第2のU形カットコアと
を、そのカット面同志を互いに対向させ、かつ、一方の
カットコアに対して他方のカットコアを捩じれ方向に9
0度回転させて接触させた磁気回路で構成し、第1の三
相磁気回路の第1のE形カットコアと第2の三相磁気回
路の第2のE形カットコアに共通の三相一次巻線を巻回
し、第2の三相磁気回路の第2のE形カットコアには三
相二次巻線を巻回し、第1の三相磁気回路の第1のU形
カットコアには漏洩磁束制御巻線を巻回し、第2の三相
磁気回路の第2のU形カットコアには主磁束制御巻線を
巻回し、前記主磁束制御巻線と前記漏洩磁束制御巻線の
励磁電流の値を変え、一次巻線の第1の三相磁気回路と
第2の三相磁気回路の磁気抵抗を変化させて、前記三相
一次巻線と前記三相二次巻線の鎖交磁束を一括制御し、
三相二次巻線電圧を連続的に可変することを特徴とした
ものである。According to a second aspect of the present invention, there is provided a first three-phase magnetic circuit and a second three-phase magnetic circuit, wherein the first three-phase magnetic circuit comprises a first E-shaped cut core and a first U-shaped cut core. A second cut core is formed by a magnetic circuit in which cut surfaces of the cut cores are opposed to each other, and one cut core is brought into contact with the other cut core by rotating the cut core by 90 degrees in a twisting direction. The phase magnetic circuit is configured such that the second E-shaped cut core and the second U-shaped cut core have their cut surfaces opposed to each other, and the other cut core is twisted in the torsional direction with respect to one cut core.
A three-phase magnetic circuit constituted by a magnetic circuit rotated and contacted by 0 degrees and common to a first E-shaped cut core of a first three-phase magnetic circuit and a second E-shaped cut core of a second three-phase magnetic circuit A primary winding is wound, a three-phase secondary winding is wound around a second E-shaped cut core of the second three-phase magnetic circuit, and a first U-shaped cut core of the first three-phase magnetic circuit is wound. Is wound with a leakage flux control winding, a main flux control winding is wound around a second U-shaped cut core of a second three-phase magnetic circuit, and the main flux control winding and the leakage flux control winding are By changing the value of the exciting current and changing the magnetic resistance of the first three-phase magnetic circuit and the second three-phase magnetic circuit of the primary winding, the chain of the three-phase primary winding and the three-phase secondary winding is changed. Collectively control the magnetic flux,
It is characterized in that the three-phase secondary winding voltage is continuously varied.
【0011】請求項3の発明は、請求項1の発明におい
て、第1の磁気回路の第1のU形カットコアに補助巻線
を巻回したことを特徴としたものである。According to a third aspect of the present invention, in the first aspect, an auxiliary winding is wound around the first U-shaped cut core of the first magnetic circuit.
【0012】請求項4の発明は、請求項2の発明におい
て、第1の三相磁気回路の第1のE形カットコアに補助
巻線を巻回したことを特徴としたものである。According to a fourth aspect of the present invention, in the second aspect, an auxiliary winding is wound around the first E-shaped cut core of the first three-phase magnetic circuit.
【0013】[0013]
【0014】[0014]
【0015】[0015]
【0016】[0016]
【0017】[0017]
【0018】[0018]
【発明の実施の形態】本発明は、変圧器の一次巻線と二
次巻線の鎖交磁束量を変化させ、二次巻線の誘起電圧を
制御するものである。本発明の基本構成は、第1の磁気
回路と第2の磁気回路に共通の一次巻線を巻回し、第1
の磁気回路は、第1のU形カットコアと第2のU形カッ
トコアとを、そのカット面同志を互いに対向させ、か
つ、一方のカットコアに対して他方のカットコアを捩じ
れ方向に90度回転させて接触させた磁気回路で構成す
る。第2のU形カットコアには、漏洩磁束制御巻線を巻
回する。第2の磁気回路は第1の磁気回路と同様の構成
として第3のU形カットコアには二次巻線を巻回し、第
4のU形カットコアには主磁束制御巻線を巻回する。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention controls the induced voltage of a secondary winding by changing the amount of interlinkage magnetic flux between a primary winding and a secondary winding of a transformer. The basic configuration of the present invention is such that a primary winding common to a first magnetic circuit and a second magnetic circuit is wound,
The first U-shaped cut core and the second U-shaped cut core have their cut surfaces opposed to each other, and the other cut core is twisted 90 degrees with respect to one cut core. It is composed of a magnetic circuit rotated and contacted by degrees. A leakage flux control winding is wound around the second U-shaped cut core. The second magnetic circuit has the same configuration as the first magnetic circuit, and a secondary winding is wound around the third U-shaped cut core.
The main flux control winding is wound around the U-shaped cut core of No. 4.
【0019】三相変圧器の場合は、第1の三相磁気回路
と第2の三相磁気回路に共通の三相一次巻線を巻回し、
第1の三相磁気回路は、第1のE形カットコアと第1の
U形カットコアとを、そのカット面同志を互いに対向さ
せ、かつ、一方のカットコアに対して他方のカットコア
を捩じれ方向に90度回転させて接触させた磁気回路で
構成する。第1のU形カットコアには、漏洩磁束制御巻
線を巻回する。第2の三相磁気回路は第1の三相磁気回
路と同様の構成として第2のE形カットコアには三相二
次巻線を巻回し、第2のU形カットコアには主磁束制御
巻線を巻回する。In the case of a three-phase transformer, a three-phase primary winding common to the first three-phase magnetic circuit and the second three-phase magnetic circuit is wound,
The first three-phase magnetic circuit is configured such that the first E-shaped cut core and the first U-shaped cut core have their cut surfaces facing each other, and one cut core is connected to the other cut core. It is composed of a magnetic circuit rotated 90 degrees in the twisting direction and brought into contact. A leakage flux control winding is wound around the first U-shaped cut core. The second three-phase magnetic circuit has a configuration similar to that of the first three-phase magnetic circuit, in which a three-phase secondary winding is wound around a second E-shaped cut core, and a main magnetic flux is wound on a second U-shaped cut core. Wind the control winding.
【0020】上記のような構成によれば、まず、無負荷
時の電圧調整は、一次巻線に電圧e1を印加することに
より、第1の磁気回路に磁束φ1−1、第2の磁気回路
に磁束φ1−2が発生する。一次巻線には、第1の磁気
回路に磁束φ1−1、第二の磁気回路に磁束φ1−2が
発生するための励磁電流i1が流れる。第2の磁気回路
に巻回された二次巻線に誘起する電圧は、第2の磁気回
路の磁束に応じた電圧が誘起する。According to the above-described configuration, first, the voltage adjustment at the time of no load is performed by applying the voltage e1 to the primary winding so that the magnetic flux φ1-1 and the second magnetic circuit are applied to the first magnetic circuit. Generates a magnetic flux φ1-2. An exciting current i1 for generating a magnetic flux φ1-1 in the first magnetic circuit and a magnetic flux φ1-2 in the second magnetic circuit flows through the primary winding. The voltage induced in the secondary winding wound around the second magnetic circuit is induced by a voltage corresponding to the magnetic flux of the second magnetic circuit.
【0021】そして、第1の磁気回路と第2の磁気回路
の磁気抵抗は前記漏洩磁束制御巻線と主磁束制御巻線の
励磁電流によって調整できる。負荷がある場合は、二次
巻線に二次(負荷)電流i2が流れると第2の磁気回路
には一次巻線の磁束を打消す磁束を生じ、このとき一次
巻線には負荷電流の一部が流れるが、第2の磁気回路の
磁束を回復するには至らず二次電圧e2は低下する。こ
のとき、第1の磁気回路の磁束は、一次巻線の印加電圧
と誘起電圧が平衡するため、第2の磁気回路の磁束の減
少相当分増加する。ここで、第2のU形カットコアに巻
回された漏洩磁束制御巻線に励磁電流を流すと、その起
磁力で生じる磁束が第1の磁気回路の第1,第2のU形
カットコアの接触面を通り、第1,第2のU形カットコ
アの接触面の磁気抵抗が増加する。そのため一次巻線の
印加電圧による第1の磁気回路の磁束の通過が抑制され
て減少し、一次巻線の印加電圧と誘起電圧が平衡するた
め、第1の磁気回路の磁束の減少相当分に対応して第2
の磁気回路の磁束が増加して第2の磁気回路上に巻回さ
れた一次巻線と二次巻線の鎖交磁束が増加するので、二
次電圧e2は増加する。The magnetic resistances of the first magnetic circuit and the second magnetic circuit can be adjusted by exciting currents of the leakage magnetic flux control winding and the main magnetic flux control winding. When there is a load, when a secondary (load) current i2 flows through the secondary winding, a magnetic flux that cancels the magnetic flux of the primary winding is generated in the second magnetic circuit.
Although a part of the load current flows through the winding , the secondary voltage e2 decreases without recovering the magnetic flux of the second magnetic circuit. At this time, the magnetic flux of the first magnetic circuit increases by an amount corresponding to the decrease of the magnetic flux of the second magnetic circuit because the applied voltage of the primary winding and the induced voltage are balanced. Here, when an exciting current is applied to the leakage magnetic flux control winding wound around the second U-shaped cut core, the magnetic flux generated by the magnetomotive force causes the first and second U-shaped cut cores of the first magnetic circuit. , The magnetic resistance of the contact surfaces of the first and second U-shaped cut cores increases. Therefore, the passage of the magnetic flux of the first magnetic circuit due to the applied voltage of the primary winding is suppressed and reduced, and the applied voltage of the primary winding and the induced voltage are balanced. Correspondingly second
The magnetic flux of the magnetic circuit increases, and the interlinkage magnetic flux between the primary winding and the secondary winding wound on the second magnetic circuit increases, so that the secondary voltage e2 increases.
【0022】また、二次巻線の負荷が減少して二次電流
が減少すると、第2の磁気回路の二次巻線の磁束が増加
して一次巻線と二次巻線の鎖交磁束が増加し、二次電圧
e2は上昇する。ここで、漏洩磁束制御巻線の励磁電流
を減少させると、制御磁束が減少して、第1の磁気回路
の第1,第2のU形カットコアの接触面の前記共通磁路
の磁気抵抗が減少し、第1の磁気回路の磁束が増加し第
2の磁気回路の磁束が減少して、二次電圧e2は低下す
る。When the load on the secondary winding decreases and the secondary current decreases, the magnetic flux of the secondary winding of the second magnetic circuit increases, and the flux linkage between the primary and secondary windings increases. Increases, and the secondary voltage e2 increases. Here, when the exciting current of the leakage magnetic flux control winding is reduced, the control magnetic flux decreases, and the magnetic resistance of the common magnetic path at the contact surface between the first and second U-shaped cut cores of the first magnetic circuit. Decreases, the magnetic flux of the first magnetic circuit increases and the magnetic flux of the second magnetic circuit decreases, and the secondary voltage e2 decreases.
【0023】以上の漏洩磁束制御巻線の励磁電流による
制御は、二次巻線と鎖交しない磁束を調整するものであ
り、等価回路として見ると一次巻線の漏洩リアクタンス
値を調整し二次電圧を制御しているものといえる。The above-described control by the exciting current of the leakage flux control winding adjusts a magnetic flux that does not interlink with the secondary winding. When viewed as an equivalent circuit, the leakage reactance value of the primary winding is adjusted and the secondary winding is controlled. It can be said that the voltage is controlled.
【0024】二次(負荷)電流が零の無負荷の場合、漏
洩磁束制御巻線を励磁しても二次電圧を上昇させること
はできても低下させることはできない。そこで、第2の
磁気回路の第4のU形カットコアに巻回された主磁束制
御巻線に励磁電流を流すと、その起磁力で生じる磁束が
第2の磁気回路の第3,第4のU形カットコアの接触面
を通り、第3,第4のU形カットコアの接触面の磁気抵
抗が増加する。そうすると一次巻線の印加電圧による第
2の磁気回路の磁束の通過が抑制されて減少し、二次巻
線の鎖交磁束が減少することになり二次電圧は低下す
る。このように無負荷時の場合であっても漏洩磁束制御
巻線と共に、主磁束制御巻線に励磁電流を流し、両者の
励磁電流を調整することにより一次巻線による磁束の配
分を制御することができ、二次電圧を制御できる。進み
負荷電流時の場合は、一次巻線の漏洩リアクタンス部分
で進み電流成分による電圧が上昇するため、漏洩磁束制
御巻線の励磁電流を増加して漏洩リアクタンスを減少さ
せて電圧上昇の抑制をはかりつつ、一次巻線と二次巻線
の鎖交磁束を主磁束制御巻線の励磁電流で調整する。主
磁束制御巻線の励磁電流を増加すると変圧器の主磁路を
形成する第2の磁気回路の磁気抵抗が大きくなって励磁
リアクタンスが減少するので、負荷に遅相用のリアクト
ルが挿入されたのと等価になり一次側から見た進み力率
が改善され、電圧上昇は抑制される。When the secondary (load) current is zero and there is no load, the secondary voltage can be increased but not decreased even if the leakage flux control winding is excited. Therefore, when an exciting current is applied to the main magnetic flux control winding wound around the fourth U-shaped cut core of the second magnetic circuit, the magnetic flux generated by the magnetomotive force generates the third, fourth, and fourth magnetic fluxes of the second magnetic circuit. , The magnetic resistance of the contact surfaces of the third and fourth U-shaped cut cores increases. Then, the passage of the magnetic flux of the second magnetic circuit by the voltage applied to the primary winding is suppressed and reduced, and the flux linkage of the secondary winding is reduced, and the secondary voltage is reduced. As described above, even when no load is applied, the excitation current flows through the main flux control winding together with the leakage flux control winding, and the distribution of the magnetic flux by the primary winding is controlled by adjusting the excitation currents of the two. And the secondary voltage can be controlled. In the case of an advancing load current, the voltage due to the advancing current component rises in the leakage reactance portion of the primary winding, so the exciting current of the leakage flux control winding is increased to reduce the leakage reactance and suppress the voltage rise. Meanwhile, the flux linkage between the primary winding and the secondary winding is adjusted by the exciting current of the main magnetic flux control winding. When the exciting current of the main magnetic flux control winding is increased, the magnetic resistance of the second magnetic circuit forming the main magnetic path of the transformer is increased and the exciting reactance is reduced. The power factor of the lead as seen from the primary side is improved, and the voltage rise is suppressed.
【0025】上述のように、負荷の状態如何に拘らず、
前記漏洩磁束制御巻線、主磁束制御巻線の励磁電流の値
を変え、一次巻線の第1の磁気回路の磁気抵抗と第2の
磁気回路の磁気抵抗を能動的に変化させて、前記一次巻
線と前記二次巻線の鎖交磁束を制御し、二次巻線電圧を
連続的に可変することができる。三相変圧器においても
同様に、前記漏洩磁束制御巻線、主磁束制御巻線の励磁
電流の値を変え、一次巻線の第1の磁気回路の磁気抵抗
と第2の磁気回路の磁気抵抗を能動的に変化させて、前
記三相一次巻線と前記三相二次巻線の三相の鎖交磁束を
一括制御し、三相二次巻線電圧を連続的に可変すること
ができる。As described above, regardless of the state of the load,
Changing the value of the exciting current of the leakage flux control winding and the main flux control winding, and actively changing the magnetic resistance of the first magnetic circuit and the magnetic resistance of the second magnetic circuit of the primary winding, The flux linkage between the primary winding and the secondary winding is controlled, so that the secondary winding voltage can be continuously varied. Similarly, in the three-phase transformer, the value of the exciting current of the leakage flux control winding and the value of the exciting current of the main flux control winding are changed, and the magnetic resistance of the first magnetic circuit and the magnetic resistance of the second magnetic circuit of the primary winding are changed. , And the three-phase linkage magnetic flux of the three-phase primary winding and the three-phase secondary winding is collectively controlled, so that the three-phase secondary winding voltage can be continuously varied. .
【0026】(実施例)図1は、本発明による鎖交磁束
制御形変圧器装置の一実施例を説明するための斜視図
で、第1の磁気回路は第1のU形カットコア13と第2
のU形カットコア11とで構成し、第2の磁気回路は第
3のU形カットコア18と第4のU形カットコア16で
構成する。第1の磁気回路は、第1のU形カットコア1
3と第2のU形カットコア11とを、そのカット面同志
を互いに対向させ、かつ、一方のカットコアに対して他
方のカットコアを捩じれ方向に90度回転させて接触さ
せた磁気回路で構成し、第2の磁気回路は、第3のU形
カットコア18と第4のU形カットコア16とを、その
カット面同志を互いに対向させ、かつ、一方のカットコ
アに対して他方のカットコアを捩じれ方向に90度回転
させて接触させた磁気回路で構成する。(Embodiment) FIG. 1 is a perspective view for explaining an embodiment of a flux linkage control type transformer device according to the present invention, wherein a first magnetic circuit comprises a first U-shaped cut core 13 and Second
The second magnetic circuit includes a third U-shaped cut core 18 and a fourth U-shaped cut core 16. The first magnetic circuit includes a first U-shaped cut core 1
3 and the second U-shaped cut core 11 by a magnetic circuit in which the cut surfaces thereof are opposed to each other, and the other cut core is rotated by 90 degrees in the torsional direction with respect to one cut core to make contact therewith. In the second magnetic circuit, the third U-shaped cut core 18 and the fourth U-shaped cut core 16 are arranged such that their cut surfaces face each other, and one cut core has the other cut core. It consists of a magnetic circuit in which the cut core is rotated by 90 degrees in the twisting direction and brought into contact.
【0027】第1の磁気回路と第2の磁気回路の第1,
第3U形カットコア13,18に共通の一次巻線14を
巻回し、第2の磁気回路の第3のU形カットコア18に
二次巻線19を巻回する。第1の磁気回路の第2のU形
カットコア11には漏洩磁束制御巻線12を、第2の磁
気回路の第4のU形カットコア16には主磁束制御巻線
17を巻回する。The first magnetic circuit and the second magnetic circuit have first and second magnetic circuits.
The primary winding 14 is wound around the third U-shaped cut cores 13 and 18, and the secondary winding 19 is wound around the third U-shaped cut core 18 of the second magnetic circuit. A leakage flux control winding 12 is wound around the second U-shaped cut core 11 of the first magnetic circuit, and a main flux control winding 17 is wound around the fourth U-shaped cut core 16 of the second magnetic circuit. .
【0028】図2は、図1に示した鎖交磁束制御形変圧
器装置の等価回路を示す回路構成を示したものであり、
×印部分は2個の磁心が90度回転させた状態で接触さ
れていることを示し、‖印部分は通常の変圧器磁心の配
列記号を示す。図3は、図1の変圧器を三相接続した鎖
交磁束制御形変圧器装置の回路構成の等価回路を表示し
たものである。FIG. 2 is a circuit diagram showing an equivalent circuit of the flux linkage control type transformer device shown in FIG.
A cross mark indicates that the two magnetic cores are in contact with each other while being rotated by 90 degrees, and a cross mark indicates the arrangement symbol of a normal transformer core. FIG. 3 shows an equivalent circuit of a circuit configuration of a flux linkage control type transformer device in which the transformers of FIG. 1 are connected in three phases.
【0029】図4は、三相用鎖交磁束制御形変圧器装置
の一実施例を説明するための斜視図で、第1の磁気回路
は第1のE形カットコア13と第1のU形カットコア1
1とで構成し、第2の磁気回路は第2のE形カットコア
18と第2のU形カットコア16で構成する。第1の磁
気回路の第1のE形カットコア13と第1のU形カット
コア11とを、そのカット面同志を互いに対向させ、か
つ、一方のカットコアに対して他方のカットコアを捩じ
れ方向に90度回転させて接触させた磁気回路で構成す
る。第2の磁気回路は第2のE形カットコア18と第2
のU形カットコア16とを、そのカット面同志を互いに
対向させ、かつ、一方のカットコアに対して他方のカッ
トコアを捩じれ方向に90度回転させて接触させた磁気
回路で構成する。一次巻線14と二次巻線19が三相で
ある点以外は図1と同様である。FIG. 4 is a perspective view for explaining an embodiment of a three-phase interlinkage flux control type transformer device. The first magnetic circuit is composed of a first E-shaped cut core 13 and a first U-shaped cut core. Shaped cut core 1
1, and the second magnetic circuit includes a second E-shaped cut core 18 and a second U-shaped cut core 16. The first E-shaped cut core 13 and the first U-shaped cut core 11 of the first magnetic circuit are arranged so that their cut surfaces face each other, and the other cut core is twisted with respect to one cut core. It is composed of a magnetic circuit rotated 90 degrees in the direction and brought into contact. The second magnetic circuit includes a second E-shaped cut core 18 and a second E-shaped cut core.
And the U-shaped cut core 16 is constituted by a magnetic circuit in which the cut surfaces are opposed to each other, and the other cut core is rotated by 90 degrees in the torsional direction and brought into contact with one cut core. It is the same as FIG. 1 except that the primary winding 14 and the secondary winding 19 are three-phase.
【0030】第1の磁気回路と第2の磁気回路の第1,
第2のE形カットコア13,18に共通の一次巻線14
を巻回し、第2の磁気回路の第2のE形カットコア18
に二次巻線19を巻回する。第1の磁気回路の第1のU
形カットコア11には漏洩磁束制御巻線12を、第2の
磁気回路の第2のU形カットコア16には主磁束制御巻
線17を巻回する。図5は、三相用鎖交磁束制御形変圧
器装置の等価回路を示す回路構成を示したものである。The first and second magnetic circuits,
Primary winding 14 common to second E-shaped cut cores 13 and 18
And the second E-shaped cut core 18 of the second magnetic circuit
Is wound around the secondary winding 19. The first U of the first magnetic circuit
A leakage flux control winding 12 is wound around the cut core 11, and a main flux control winding 17 is wound around the second U-shaped cut core 16 of the second magnetic circuit. FIG. 5 is a circuit diagram showing an equivalent circuit of a three-phase linkage magnetic flux control type transformer device.
【0031】図1の構成によれば、無負荷時の電圧調整
は、一次巻線14に電圧e1を印加することにより、第
1の磁気回路に磁束φ1−1、第2の磁気回路に磁束φ
1−2が発生する。一次巻線14には、第1の磁気回路
に磁束φ1−1、第2の磁気回路に磁束φ1−2が発生
するための励磁電流i1が流れる。第2の磁気回路に巻
回された二次巻線19に誘起する電圧は、第2の磁気回
路の磁束に応じた電圧e2が発生する。ここで、第2の
磁気回路の磁束は、第1の磁気回路の漏洩磁束制御巻線
12と第2の磁気回路の主磁束制御巻線17の励磁電流
ic1,ic2によって任意に調整できる。つまり、一
次巻線の電圧e1に対する磁束は第1の磁気回路と第2
の磁気回路の磁気抵抗に反比例して配分され、第1の磁
気回路と第2の磁気回路の磁気抵抗は漏洩磁束制御巻線
12と主磁束制御巻線17の励磁電流ic1,ic2に
よって調整できる。According to the configuration shown in FIG. 1, the voltage adjustment at the time of no load is performed by applying the voltage e1 to the primary winding 14 so that the magnetic flux φ1-1 is applied to the first magnetic circuit and the magnetic flux φ1-1 is applied to the second magnetic circuit. φ
1-2 occurs. In the primary winding 14, an exciting current i1 for generating a magnetic flux φ1-1 in the first magnetic circuit and a magnetic flux φ1-2 in the second magnetic circuit flows. As the voltage induced in the secondary winding 19 wound around the second magnetic circuit, a voltage e2 corresponding to the magnetic flux of the second magnetic circuit is generated. Here, the magnetic flux of the second magnetic circuit can be arbitrarily adjusted by the exciting currents ic1 and ic2 of the leakage magnetic flux control winding 12 of the first magnetic circuit and the main magnetic flux control winding 17 of the second magnetic circuit. That is, the magnetic flux for the voltage e1 of the primary winding is equal to the magnetic flux between the first magnetic circuit and the second magnetic circuit.
And the magnetic resistances of the first magnetic circuit and the second magnetic circuit can be adjusted by the exciting currents ic1 and ic2 of the leakage magnetic flux control winding 12 and the main magnetic flux control winding 17. .
【0032】負荷電流i2がある場合の電圧調整は、二
次巻線19に二次(負荷)電流i2が流れると第2の磁
気回路には一次巻線14の磁束φ1−2とは反対方向の
磁束φ2が発生し、これを打消すように一次巻線14に
負荷電流i1が流れるが第2の磁気回路の磁束φ1−2
は減少して二次電圧e2は低下する。このとき、第1の
磁気回路の磁束φ1−1は、一次巻線の印加電圧e1と
誘起電圧が平衡するため、第2の磁気回路の磁束φ1−
2の減少相当分増加する。ここで、第2のカットコアに
巻回された漏洩磁束制御巻線12に励磁電流ic1を流
すと、巻数と励磁電流を掛けた起磁力(アンペアター
ン)で生じる制御磁束φc1が、第1の磁気回路の第
1,第2のU形カットコア13,11の接触面15を通
る。The voltage adjustment in the presence of the load current i2 is performed in such a manner that when the secondary (load) current i2 flows through the secondary winding 19, the second magnetic circuit has a direction opposite to the magnetic flux φ1-2 of the primary winding 14. Is generated, and the load current i1 flows through the primary winding 14 so as to cancel the magnetic flux φ2, but the magnetic flux φ1-2 of the second magnetic circuit is generated.
Decreases, and the secondary voltage e2 decreases. At this time, the magnetic flux φ1-1 of the first magnetic circuit is equal to the magnetic flux φ1- of the second magnetic circuit because the applied voltage e1 of the primary winding and the induced voltage are balanced.
It increases by an amount corresponding to the decrease of 2. Here, when the exciting current ic1 flows through the leakage magnetic flux control winding 12 wound around the second cut core, the control magnetic flux φc1 generated by the magnetomotive force (ampere turn) multiplied by the number of windings and the exciting current becomes the first magnetic flux φc1. It passes through the contact surface 15 of the first and second U-shaped cut cores 13 and 11 of the magnetic circuit.
【0033】第1,第2のU形カットコアの接触面は磁
束φc1と磁束φ1−1の共通磁路になっており、この
共通磁路の磁気抵抗が増加し、一次巻線の印加電圧によ
る磁束φ1−1の通過が抑制され減少する。すると、一
次巻線14の印加電圧e1と誘起電圧が平衡するため、
第1の磁気回路の磁束φ1−1の減少相当分に対応して
第2の磁気回路の磁束φ1−2が増加して第2の磁気回
路上に巻回された一次巻線14と二次巻線19の鎖交磁
束が増加するので、二次電圧e2は増加する。The contact surfaces of the first and second U-shaped cut cores form a common magnetic path of the magnetic flux φc1 and the magnetic flux φ1-1. The magnetic resistance of the common magnetic path increases, and the applied voltage of the primary winding increases. And the passage of the magnetic flux φ1-1 is suppressed and reduced. Then, since the applied voltage e1 of the primary winding 14 and the induced voltage are balanced,
The magnetic flux φ1-2 of the second magnetic circuit increases correspondingly to the decrease of the magnetic flux φ1-1 of the first magnetic circuit, and the primary winding 14 wound on the second magnetic circuit and the secondary winding Since the interlinkage magnetic flux of the winding 19 increases, the secondary voltage e2 increases.
【0034】次に、二次巻線19の負荷が減少して二次
電流i2が減少すると、第2の磁気回路には一次巻線1
4の磁束φ1−2とは反対方向の磁束φ2が減少するの
で、磁束φ1−2が増加して一次巻線14と二次巻線1
9の鎖交磁束が増加し、二次電圧e2は上昇する。ここ
で、第1の磁気回路の第2のカットコアに巻回された漏
洩磁束制御巻線12の励磁電流ic1を減少させると、
巻数と励磁電流ic1を掛けた起磁力(アンペアター
ン)が減少して、第1の磁気回路の第1,第2のU形カ
ットコア13,11の接触面の前記共通磁路15の磁気
抵抗が減少し、一次巻線の印加電圧e1による磁束φ1
−1の通過が緩和され増加する。すると、一次巻線14
は印加電圧e1と誘起電圧が平衡するため磁束は一次巻
線の印加電圧e1に応じて一定であり、第1の磁気回路
の磁束φ1−1の増加相当分に対応して第2の磁気回路
の磁束φ1−2が減少して第2の磁気回路上に巻回され
た一次巻線14と二次巻線19の鎖交磁束が減少し、二
次電圧e2は低下する。Next, when the load on the secondary winding 19 decreases and the secondary current i2 decreases, the primary winding 1 is added to the second magnetic circuit.
4, the magnetic flux φ2 in the opposite direction to the magnetic flux φ1-2 decreases, the magnetic flux φ1-2 increases, and the primary winding 14 and the secondary winding 1
The interlinkage magnetic flux of No. 9 increases, and the secondary voltage e2 increases. Here, when the exciting current ic1 of the leakage magnetic flux control winding 12 wound around the second cut core of the first magnetic circuit is reduced,
The magnetomotive force (ampere turn) multiplied by the number of turns and the exciting current ic1 is reduced, and the magnetoresistance of the common magnetic path 15 at the contact surfaces of the first and second U-shaped cut cores 13 and 11 of the first magnetic circuit is reduced. Is reduced, and the magnetic flux φ1 due to the applied voltage e1 of the primary winding is reduced.
The passage of -1 is alleviated and increased. Then, the primary winding 14
Since the applied voltage e1 and the induced voltage are balanced, the magnetic flux is constant according to the applied voltage e1 of the primary winding, and the second magnetic circuit corresponds to the increase of the magnetic flux φ1-1 of the first magnetic circuit. Of the primary winding 14 and the secondary winding 19 wound on the second magnetic circuit decrease, and the secondary voltage e2 decreases.
【0035】二次(負荷)電流i2が有る場合はφ2に
よる第2の磁気回路のφ1−2の第1の磁気回路へのシ
フト量を漏洩磁束制御巻線の励磁電流ic1の制御によ
り調整し、二次巻線の鎖交磁束量を増減し、二次電圧e
2を調整できるが、無負荷で二次電流が無い場合は漏洩
磁束制御巻線を励磁してもφ1−2を増加する制御は可
能だが減少する制御はできない。そこで、第2の磁気回
路の第4のU形カットコア16に巻回された主磁束制御
巻線17に励磁電流を励磁すると励磁電流ic2に応じ
制御磁束φc2が、第2の磁気回路の第3,第4のU形
カットコア18,16の接続面を通る。第3,第4のU
形カットコアの接触面はφ1−2と磁束φc2の共通磁
路を形成しており、この共通磁路の磁気抵抗が増加し、
磁束φ1−2が減少する。したがって、無負荷時の場合
であっても漏洩磁束制御巻線の励磁電流と共に、主磁束
制御巻線に励磁電流を流し、両者の励磁電流を調整する
ことによりφ1−1とφ1−2の配分を制御することが
でき、例えば、φ1−2を減少することにより二次電圧
を低下させることもできる。進み負荷電流時の場合は、
一次巻線14の漏洩リアクタンス部分で進み電流成分に
よる電圧が上昇するため、漏洩磁束制御巻線12の励磁
電流ic1を増加して漏洩リアクタンスを減少させて電
圧上昇の抑制をはかりつつ、一次巻線14と二次巻線1
9の鎖交磁束を主磁束制御巻線17の励磁電流ic2に
よって調整する。主磁束制御巻線の励磁電流を増加する
と変圧器の主磁路を形成する第2の磁気回路の磁気抵抗
が大きくなって励磁リアクタンスが減少し、負荷に遅相
用のリアクトルが挿入されたのと等価になり一次側から
見た進み力率が改善され、電圧上昇は抑制される。If there is a secondary (load) current i2, the shift amount of φ1-2 of the second magnetic circuit to the first magnetic circuit by φ2 is adjusted by controlling the exciting current ic1 of the leakage flux control winding. , Increase or decrease the amount of interlinkage magnetic flux of the secondary winding,
2 can be adjusted, but when there is no secondary current with no load, even if the leakage flux control winding is excited, control to increase φ1-2 is possible, but control to decrease φ1-2 is not possible. Then, when an exciting current is excited in the main magnetic flux control winding 17 wound around the fourth U-shaped cut core 16 of the second magnetic circuit, the control magnetic flux φc2 according to the exciting current ic2, 3, passing through the connecting surface of the fourth U-shaped cut cores 18, 16; Third and fourth U
The contact surface of the shaped cut core forms a common magnetic path of φ1-2 and magnetic flux φc2, and the magnetic resistance of this common magnetic path increases,
The magnetic flux φ1-2 decreases. Therefore, even when no load is applied, the excitation current is supplied to the main magnetic flux control winding together with the excitation current of the leakage magnetic flux control winding, and the excitation currents of both are adjusted to distribute φ1-1 and φ1-2. Can be controlled, for example, the secondary voltage can be reduced by reducing φ1-2. In the case of advanced load current,
Since the voltage due to the leading current component rises in the leakage reactance portion of the primary winding 14, the exciting current ic1 of the leakage magnetic flux control winding 12 is increased to reduce the leakage reactance, thereby suppressing the voltage rise. 14 and secondary winding 1
9 are adjusted by the exciting current ic2 of the main magnetic flux control winding 17. When the exciting current of the main magnetic flux control winding is increased, the magnetic resistance of the second magnetic circuit forming the main magnetic path of the transformer is increased, the exciting reactance is reduced, and a reactor for lagging is inserted into the load. And the power factor as seen from the primary side is improved, and the voltage rise is suppressed.
【0036】図6は、図16に示したような従来の負荷
時タップ切換え電圧調整器を、図7に示すように、本発
明で構成した場合のベクトル図で、図中、Ioは主磁路
の励磁磁束に対応する励磁電流、E1は一次巻線の誘起
電圧、I1は負荷電流、IはIoとI1の和の一次電
流、IX1は一次巻線の漏洩リアクタンス電圧降下、V
1は一次巻線端子電圧、E2は二次巻線の誘起電圧、P
は一次巻線のタップ位置、V2は二次電圧である。FIG. 6 is a vector diagram when the conventional load tap switching voltage regulator as shown in FIG. 16 is constructed in accordance with the present invention as shown in FIG. 7, where Io is the main symbol . The exciting current corresponding to the exciting magnetic flux of the magnetic path, E1 is the induced voltage of the primary winding, I1 is the load current, I is the primary current of the sum of Io and I1, IX1 is the leakage reactance voltage drop of the primary winding, V
1 is the primary winding terminal voltage, E2 is the induced voltage of the secondary winding, P
Is the tap position of the primary winding, and V2 is the secondary voltage.
【0037】図6において、例えば、負荷電流I1の大
小等にかかわらず二次電圧V2を一定にするには、電圧
比(E2/E1)が一定であるから三角形OQRを一定
にすれば良く、漏洩リアクタンスXを調整してIX1を
一定にすると共に、励磁電流I0を調整してαを一定に
する。また、電圧条件を変える場合は、新たなバランス
条件となるように負荷電流の大きさと力率に応じて漏洩
リアクタンスX及び励磁電流I0を調整する。In FIG. 6, for example, to keep the secondary voltage V2 constant irrespective of the magnitude of the load current I1, the voltage ratio (E2 / E1) is constant, so that the triangle OQR may be fixed. while a constant IX1 by adjusting the leakage reactance X, is a constant α by adjusting the excitation current I 0. In the case of changing the voltage condition, to adjust the leakage reactance X and the exciting current I 0 in accordance with the magnitude and power factor of the load current so that a new balance condition.
【0038】図8は、第1の磁気回路の第1のU形カッ
トコアに補助巻線27を設けた一例を示したものであ
る。補助巻線を設けることにより漏洩磁束制御巻線の励
磁電源が得られると共に、二次電圧波形の高調波を低減
することができるが、本発明では、励磁電源として用い
るので、高調波低減については先願(特願平9−837
93号)に詳述しているので省略する。三相形について
も第1のE形カットコア13に三相補助巻線を巻回すれ
ば良いことは明らかである。FIG. 8 shows an example in which an auxiliary winding 27 is provided on the first U-shaped cut core of the first magnetic circuit. By providing the auxiliary winding, an excitation power supply for the leakage magnetic flux control winding can be obtained, and the harmonics of the secondary voltage waveform can be reduced. Prior application (Japanese Patent Application No. 9-837)
No. 93), and a description thereof will be omitted. It is clear that a three-phase auxiliary winding may be wound around the first E-shaped cut core 13 for the three-phase type.
【0039】図9は、漏洩磁束制御巻線の励磁電流ic
1の制御による二次電圧e2の制御特性を示したもので
あり、図10は主磁束制御巻線17の励磁電流ic2の
制御による二次電圧e2の制御特性を示したものであ
る。図より、漏洩磁束制御巻線と主磁束制御巻線の両励
磁電流ic1とic2の制御により二次電圧e2を広範
囲制御できることが理解できる。そこで漏洩磁束制御巻
線の励磁電流ic1を二次(負荷)電流値に基づいて制
御し、主磁束制御巻線の励磁電流ic2を二次電圧e2
に基づいて制御することにより二次巻線の電圧・電流特
性を所望の特性とする変圧器(電源)を得ることができ
る。FIG. 9 shows the exciting current ic of the leakage magnetic flux control winding.
10 shows the control characteristics of the secondary voltage e2 by the control of FIG. 1, and FIG. 10 shows the control characteristics of the secondary voltage e2 by the control of the exciting current ic2 of the main magnetic flux control winding 17. From the figure, it can be understood that the secondary voltage e2 can be controlled over a wide range by controlling both exciting currents ic1 and ic2 of the leakage magnetic flux control winding and the main magnetic flux control winding. Therefore, the exciting current ic1 of the leakage magnetic flux control winding is controlled based on the secondary (load) current value, and the exciting current ic2 of the main magnetic flux control winding is changed to the secondary voltage e2.
, It is possible to obtain a transformer (power supply) having desired voltage-current characteristics of the secondary winding.
【0040】また、図11は、二次巻線の負荷をパラメ
ータとした漏洩磁束制御巻線12の励磁電流ic1の制
御による二次電圧e2と補助巻線27の誘起電圧e3と
の相互関係を示したものである。図より、補助巻線の誘
起電圧e3は二次巻線の負荷の増加により上昇し、制御
電流ic1の増加により低下する。二次電圧e2は負荷
の増加により低下し、制御電流ic1の増加により上昇
する。この特性は、補助巻線の出力により漏洩磁束制御
巻線を励磁することにより負荷の増加による二次電圧の
低下を補償できることを示している。FIG. 11 shows the correlation between the secondary voltage e2 and the induced voltage e3 of the auxiliary winding 27 by controlling the exciting current ic1 of the leakage flux control winding 12 using the load of the secondary winding as a parameter. It is shown. As shown in the figure, the induced voltage e3 of the auxiliary winding increases with an increase in the load on the secondary winding, and decreases with an increase in the control current ic1. The secondary voltage e2 decreases as the load increases, and increases as the control current ic1 increases. This characteristic indicates that the excitation of the leakage flux control winding by the output of the auxiliary winding can compensate for the decrease in the secondary voltage due to the increase in load.
【0041】そこで、上記のように漏洩磁束制御巻線の
励磁電流をic1を二次(負荷)電流i2に略比例した
電流で制御すると共に、主磁束制御巻線の励磁電流ic
2を二次電圧が所定値を超えた場合に励磁することによ
り、両励磁電流ic1,ic2の制御により電力系統の
電圧変動にも拘わらず、二次(負荷)電流の変動に対し
二次電圧を自動的に一定値の幅に安定化することができ
る。図12は、この制御特性を示したものである。Therefore, as described above, the exciting current of the leakage flux control winding is controlled by the current ic1 which is substantially proportional to the secondary (load) current i2, and the exciting current ic of the main magnetic flux control winding is controlled.
2 is excited when the secondary voltage exceeds a predetermined value, so that the secondary excitation current ic1 and ic2 are controlled to control the secondary voltage with respect to the secondary (load) current variation despite the power system voltage variation. Can be automatically stabilized to a constant value range. FIG. 12 shows this control characteristic.
【0042】図13は、補助巻線27の誘起電圧e3に
より整流器22を介して漏洩磁束制御巻線12を励磁
し、また、二次巻線19に接続した変圧器25の二次巻
線により可飽和リアクトル26と整流器23を介して主
磁束制御巻線を励磁する三相形の二次電圧安定化鎖交磁
束制御形変圧器装置の等価回路を示す。可飽和リアクト
ルは二次電圧が所定の整定値になると飽和し、この値は
リアクトル及び/又は二次巻線に接続した変圧器のタッ
プを変えることにより変えることができる。この二次電
圧安定化鎖交磁束制御形変圧器装置により、二次電圧は
リアクトルの飽和設定値を超える電圧付近で安定化す
る。FIG. 13 shows that the leakage flux control winding 12 is excited via the rectifier 22 by the induced voltage e3 of the auxiliary winding 27, and the secondary winding of the transformer 25 connected to the secondary winding 19. 5 shows an equivalent circuit of a three-phase secondary voltage stabilized flux linkage control type transformer device that excites a main flux control winding via a saturable reactor 26 and a rectifier 23. The saturable reactor saturates when the secondary voltage reaches a predetermined set value, which can be changed by changing the tap of the transformer connected to the reactor and / or the secondary winding. By this secondary voltage stabilizing flux linkage control type transformer device, the secondary voltage is stabilized near a voltage exceeding the saturation set value of the reactor.
【0043】図14は、同じく三相形の二次電圧安定化
鎖交磁束制御形変圧器装置で、二次巻線19の回路に挿
入した変流器24の出力により整流器22を介して漏洩
磁束制御巻線12を励磁する例を示している。また、図
15は図16に示した従来のタップ切換変圧器を無タッ
プ化した電圧安定化鎖交磁束制御形変圧器装置の例を示
す。FIG. 14 shows a three-phase secondary voltage-stabilized interlinkage flux control type transformer device. The output of the current transformer 24 inserted in the circuit of the secondary winding 19 causes the leakage flux to flow through the rectifier 22. An example in which the control winding 12 is excited is shown. FIG. 15 shows an example of a voltage-stabilized flux linkage control type transformer device in which the conventional tap switching transformer shown in FIG. 16 is non-tapped.
【0044】[0044]
【発明の効果】以上のように、本発明により、漏洩磁束
制御巻線と主磁束制御巻線の両励磁電流を制御すること
により、二次電圧を連続的に調整することが可能な無タ
ップの変圧器を構成でき、また、両励磁電流の制御態様
により所望の電圧電流特性の電源を構成できると共に、
電力系統の電圧変動や、負荷変動による電圧変動を補償
する二次電圧安定化変圧器装置を構成できる。As described above, according to the present invention, by controlling both exciting currents of the leakage magnetic flux control winding and the main magnetic flux control winding, it is possible to continuously adjust the secondary voltage without tapping. And a power source having a desired voltage-current characteristic can be formed by controlling both exciting currents.
A secondary voltage stabilizing transformer device for compensating voltage fluctuations due to power system voltage fluctuations and load fluctuations can be configured.
【図1】 本発明による鎖交磁束制御形変圧器装置の一
実施例を示す斜視図である。FIG. 1 is a perspective view showing an embodiment of a flux linkage control type transformer device according to the present invention.
【図2】 鎖交磁束制御形変圧器装置の等価回路を示す
回路構成図である。FIG. 2 is a circuit diagram showing an equivalent circuit of a flux linkage control type transformer device.
【図3】 三相接続した鎖交磁束制御形変圧器装置の等
価回路を示す回路構成図である。FIG. 3 is a circuit diagram showing an equivalent circuit of a three-phase connected flux linkage control type transformer device.
【図4】 三相用鎖交磁束制御形変圧器装置の一実施例
を示す斜視図である。FIG. 4 is a perspective view showing an embodiment of a three-phase interlinkage flux control type transformer device.
【図5】 三相用鎖交磁束制御形変圧器装置の等価回路
を示す回路構成図である。FIG. 5 is a circuit configuration diagram showing an equivalent circuit of a three-phase linkage flux control type transformer device.
【図6】 図16に示すような従来の負荷時タップ切換
え電圧調整器を図7のように本発明で構成した場合のベ
クトル図である。6 is a vector diagram in a case where the conventional load tap switching voltage regulator as shown in FIG . 16 is configured according to the present invention as shown in FIG. 7;
【図7】 本発明で構成した電圧調整器の回路構成図で
ある。FIG. 7 is a circuit configuration diagram of a voltage regulator configured according to the present invention.
【図8】 図1の鎖交磁束制御形変圧器装置に補助巻線
を設けた場合の一実施例を示す斜視図である。8 is a perspective view showing an embodiment in which an auxiliary winding is provided in the flux linkage control type transformer device of FIG. 1;
【図9】 漏洩磁束制御巻線の励磁電流による二次電圧
の制御特性を示す図である。FIG. 9 is a diagram showing control characteristics of a secondary voltage by an exciting current of a leakage magnetic flux control winding.
【図10】 主磁束制御巻線の励磁電流による二次電圧
の制御特性を示す図である。FIG. 10 is a diagram showing control characteristics of a secondary voltage by an exciting current of a main magnetic flux control winding.
【図11】 二次巻線の負荷をパラメータとした漏洩磁
束制御巻線の励磁電流と補助巻線と二次巻線の電圧の関
係を示す図である。FIG. 11 is a diagram showing the relationship between the exciting current of the leakage flux control winding and the voltages of the auxiliary winding and the secondary winding, using the load of the secondary winding as a parameter.
【図12】 負荷変動に対する二次電圧の安定化特性を
示す図である。FIG. 12 is a diagram showing a stabilization characteristic of a secondary voltage with respect to a load change.
【図13】 二次電圧安定化鎖交磁束制御形変圧器装置
の一実施例を示す図である。FIG. 13 is a diagram showing an embodiment of a secondary voltage stabilized flux linkage controlling transformer device.
【図14】 二次電圧安定化鎖交磁束制御形変圧器装置
の他の実施例を示す図である。FIG. 14 is a diagram showing another embodiment of a secondary voltage stabilized flux linkage controlling transformer device.
【図15】 図16に示した従来のタップ切換変圧器を
本発明により二次電圧安定化変圧器装置として構成した
実施例を示す図である。FIG. 15 is a diagram showing an embodiment in which the conventional tap switching transformer shown in FIG. 16 is configured as a secondary voltage stabilizing transformer device according to the present invention.
【図16】 従来の負荷時タップ切換え電圧調整器であ
る。FIG. 16 shows a conventional on-load tap switching voltage regulator.
【図17】 本出願人が先に提案した従来の磁束制御形
可変変圧器の一例を示す斜視図である。FIG. 17 is a perspective view showing an example of a conventional flux control type variable transformer previously proposed by the present applicant.
11…第1の磁気回路の第2のU形カットコア,第1の
三相磁気回路の第1のU形カットコア、12…漏洩磁束
制御巻線、13…第1の磁気回路の第1のU形カットコ
ア,第1の三相磁気回路の第1のE形カットコア、14
…一次巻線、15…第1の磁気回路のカットコア面同志
の接触面、16…第2の磁気回路の第4のU形カットコ
ア,第2の三相磁気回路の第2のU形カットコア、17
…主磁束制御巻線、18…第2の磁気回路の第3のU形
カットコア,第2の三相磁気回路の第2のE形カットコ
ア、19…二次巻線、20…第2磁気回路のカットコア
面同志の接触面、21…変圧器用磁気回路、22,23
…整流器、24…変流器、26…可飽和リアクトル、2
7…補助巻線。11... The second U-shaped cut core of the first magnetic circuit, the first
A first U-shaped cut core of a three-phase magnetic circuit , 12: a leakage flux control winding, 13: a first U-shaped cut core of a first magnetic circuit
A, the first E-shaped cut core of the first three-phase magnetic circuit , 14
... primary winding, 15 ... contact surface of the cut core surface comrades of the first magnetic circuit, 16 ... fourth U-shaped second magnetic circuit Kattoko
A, the second U-shaped cut core of the second three-phase magnetic circuit , 17
... Main flux control winding, 18 ... Third U-shaped second magnetic circuit
Cut core, second E-shaped cut core of the second three-phase magnetic circuit
A , 19: secondary winding, 20: contact surface between cut core surfaces of the second magnetic circuit, 21: magnetic circuit for transformer, 22, 23
... Rectifier, 24 ... Current transformer, 26 ... Saturable reactor, 2
7 ... Auxiliary winding.
───────────────────────────────────────────────────── フロントページの続き (72)発明者 川上 峰夫 宮城県仙台市青葉区中山七丁目2番1号 東北電力株式会社研究開発センター内 (72)発明者 赤塚 重昭 宮城県仙台市青葉区中山七丁目2番1号 東北電力株式会社研究開発センター内 (72)発明者 八木 博美 宮城県多賀城市宮内2丁目2番1号 東 北電機製造株式会社内 (72)発明者 伊藤 高之 宮城県多賀城市宮内2丁目2番1号 東 北電機製造株式会社内 (56)参考文献 特開 平10−214732(JP,A) (58)調査した分野(Int.Cl.7,DB名) H01F 29/14 ──────────────────────────────────────────────────続 き Continued on the front page (72) Mineo Kawakami 2-1, Nakayama 7-chome, Aoba-ku, Sendai, Miyagi Prefecture Inside the R & D Center of Tohoku Electric Power Co., Inc. Chome 2-1 Tohoku Electric Power Co. R & D Center (72) Inventor Hiromi Yagi 2-2-1 Miyauchi Tagajo City, Miyagi Prefecture Tohoku Electric Manufacturing Co., Ltd. (72) Inventor Takayuki Ito Tagajo City, Miyagi Prefecture Miyauchi 2-2-1 Tohoku Electric Manufacturing Co., Ltd. (56) References JP-A-10-214732 (JP, A) (58) Fields investigated (Int. Cl. 7 , DB name) H01F 29/14
Claims (4)
し、第1の磁気回路は、第1のU形カットコアと第2の
U形カットコアとを、そのカット面同志を互いに対向さ
せ、かつ、一方のカットコアに対して他方のカットコア
を捩じれ方向に90度回転させて接触させた磁気回路で
構成し、第2の磁気回路は、第3のU形カットコアと第
4のU形カットコアとを、そのカット面同志を互いに対
向させ、かつ、一方のカットコアに対して他方のカット
コアを捩じれ方向に90度回転させて接触させた磁気回
路で構成し、第1の磁気回路の第1のU形カットコアと
第2の磁気回路の第3のU形カットコアに共通の一次巻
線を巻回し、第2の磁気回路の第3のU形カットコアに
は二次巻線を巻回し、第1の磁気回路の第2のU形カッ
トコアには漏洩磁束制御巻線を巻回し、第2の磁気回路
の第4のU形カットコアには主磁束制御巻線を巻回し、
前記主磁束制御巻線と前記漏洩磁束制御巻線の励磁電流
の値を変え、一次巻線の第1の磁気回路と第2の磁気回
路の磁気抵抗を変化させて、前記一次巻線と前記二次巻
線の鎖交磁束を制御し、二次巻線電圧を連続的に可変す
ることを特徴とする鎖交磁束制御形変圧器装置。The first magnetic circuit has a first U-shaped cut core and a second U-shaped cut core, and the first magnetic circuit has a cut surface between them. The second U-shaped cut core comprises a magnetic circuit in which one cut core is opposed to each other, and the other cut core is rotated by 90 degrees in a torsion direction and brought into contact with one cut core. The fourth U-shaped cut core is constituted by a magnetic circuit in which the cut surfaces are opposed to each other, and the other cut core is rotated by 90 degrees in the torsional direction with one cut core to make contact therewith, A primary winding is wound around a first U-shaped cut core of the first magnetic circuit and a third U-shaped cut core of the second magnetic circuit, and a third U-shaped cut core of the second magnetic circuit is formed. Is wound with a secondary winding, and the second U-shaped cut core of the first magnetic circuit is provided with a leakage magnetic flux control. A main magnetic flux control winding around a fourth U-shaped cut core of the second magnetic circuit;
By changing the value of the exciting current of the main magnetic flux control winding and the leakage magnetic flux control winding, and changing the magnetic resistance of the first magnetic circuit and the second magnetic circuit of the primary winding, the primary winding and the A flux linkage control type transformer device characterized in that the flux linkage of the secondary winding is controlled and the secondary winding voltage is continuously varied.
路を有し、第1の三相磁気回路は、第1のE形カットコ
アと第1のU形カットコアとを、そのカット面同志を互
いに対向させ、かつ、一方のカットコアに対して他方の
カットコアを捩じれ方向に90度回転させて接触させた
磁気回路で構成し、第2の三相磁気回路は、第2のE形
カットコアと第2のU形カットコアとを、そのカット面
同志を互いに対向させ、かつ、一方のカットコアに対し
て他方のカットコアを捩じれ方向に90度回転させて接
触させた磁気回路で構成し、第1の三相磁気回路の第1
のE形カットコアと第2の三相磁気回路の第2のE形カ
ットコアに共通の三相一次巻線を巻回し、第2の三相磁
気回路の第2のE形カットコアには三相二次巻線を巻回
し、第1の三相磁気回路の第1のU形カットコアには漏
洩磁束制御巻線を巻回し、第2の三相磁気回路の第2の
U形カットコアには主磁束制御巻線を巻回し、前記主磁
束制御巻線と前記漏洩磁束制御巻線の励磁電流の値を変
え、一次巻線の第1の三相磁気回路と第2の三相磁気回
路の磁気抵抗を変化させて、前記三相一次巻線と前記三
相二次巻線の鎖交磁束を一括制御し、三相二次巻線電圧
を連続的に可変することを特徴とする三相電圧の鎖交磁
束制御形変圧器装置。2. A first three-phase magnetic circuit having a first three-phase magnetic circuit and a second three-phase magnetic circuit, wherein the first three-phase magnetic circuit includes a first E-shaped cut core and a first U-shaped cut core. The cut surfaces are made to face each other, and one cut core is constituted by a magnetic circuit in which the other cut core is rotated by 90 degrees in a twisting direction and brought into contact with the other cut core, and the second three-phase magnetic circuit comprises: The second E-shaped cut core and the second U-shaped cut core are brought into contact with each other so that the cut surfaces thereof face each other, and the other cut core is rotated by 90 degrees in the twisting direction with respect to one cut core. And a first three-phase magnetic circuit.
A common three-phase primary winding is wound around the E-shaped cut core and the second E-shaped cut core of the second three-phase magnetic circuit, and the second E-shaped cut core of the second three-phase magnetic circuit has A three-phase secondary winding is wound, a leakage flux control winding is wound around a first U-shaped cut core of a first three-phase magnetic circuit, and a second U-shaped cut of a second three-phase magnetic circuit is formed. A main flux control winding is wound around the core, the value of the exciting current of the main flux control winding and the leakage flux control winding is changed, and a first three-phase magnetic circuit of a primary winding and a second three-phase magnetic circuit are formed. By changing the magnetic resistance of the magnetic circuit, collectively controlling the interlinkage magnetic flux of the three-phase primary winding and the three-phase secondary winding, continuously varying the three-phase secondary winding voltage. Three-phase voltage linkage flux control type transformer device.
おいて、第1の磁気回路の第2のU形カットコアに補助
巻線を巻回したことを特徴とする鎖交磁束制御形変圧器
装置。3. An interlinkage flux control type transformer device according to claim 1, wherein an auxiliary winding is wound around a second U-shaped cut core of the first magnetic circuit. Transformer equipment.
おいて、第1の三相磁気回路の第1のE字形カットコア
に補助巻線を巻回したことを特徴とする鎖交磁束制御形
変圧器装置。4. An interlinkage flux control transformer device according to claim 2, wherein an auxiliary winding is wound around a first E-shaped cut core of the first three-phase magnetic circuit. Controlled transformer device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP31462098A JP3343083B2 (en) | 1998-02-26 | 1998-11-05 | Linkage flux control type transformer device |
Applications Claiming Priority (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4544398 | 1998-02-26 | ||
| JP10-45443 | 1998-02-26 | ||
| JP31462098A JP3343083B2 (en) | 1998-02-26 | 1998-11-05 | Linkage flux control type transformer device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH11312613A JPH11312613A (en) | 1999-11-09 |
| JP3343083B2 true JP3343083B2 (en) | 2002-11-11 |
Family
ID=26385429
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP31462098A Expired - Fee Related JP3343083B2 (en) | 1998-02-26 | 1998-11-05 | Linkage flux control type transformer device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3343083B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP7427512B2 (en) * | 2020-04-10 | 2024-02-05 | 東北電力株式会社 | electromagnetic equipment |
-
1998
- 1998-11-05 JP JP31462098A patent/JP3343083B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH11312613A (en) | 1999-11-09 |
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| LAPS | Cancellation because of no payment of annual fees |