JPS60169114A - Phase adjustor - Google Patents
Phase adjustorInfo
- Publication number
- JPS60169114A JPS60169114A JP59022958A JP2295884A JPS60169114A JP S60169114 A JPS60169114 A JP S60169114A JP 59022958 A JP59022958 A JP 59022958A JP 2295884 A JP2295884 A JP 2295884A JP S60169114 A JPS60169114 A JP S60169114A
- Authority
- JP
- Japan
- Prior art keywords
- winding
- series
- current
- transformer
- 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.)
- Pending
Links
- 238000004804 winding Methods 0.000 claims abstract description 98
- 230000005284 excitation Effects 0.000 claims description 20
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical group [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 claims 1
- 230000004907 flux Effects 0.000 abstract description 23
- 238000010586 diagram Methods 0.000 description 12
- 238000013021 overheating Methods 0.000 description 5
- 239000000696 magnetic material Substances 0.000 description 3
- 238000000034 method Methods 0.000 description 3
- 230000009466 transformation Effects 0.000 description 3
- 239000007788 liquid Substances 0.000 description 2
- 230000001105 regulatory effect Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 230000000149 penetrating effect Effects 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F27/00—Details of transformers or inductances, in general
- H01F27/28—Coils; Windings; Conductive connections
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F27/00—Details of transformers or inductances, in general
- H01F27/34—Special means for preventing or reducing unwanted electric or magnetic effects, e.g. no-load losses, reactive currents, harmonics, oscillations, leakage fields
- H01F27/36—Electric or magnetic shields or screens
- H01F27/366—Electric or magnetic shields or screens made of ferromagnetic material
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F29/00—Variable transformers or inductances not covered by group H01F21/00
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Control Of Electrical Variables (AREA)
Abstract
Description
【発明の詳細な説明】
[発明の技術分野]
本発明は、電力用の位相調整器に係り、特に、1次側と
2次側の電圧比が常に同一となる様に位相調整を行うこ
とのできる位相調整器に関する。[Detailed Description of the Invention] [Technical Field of the Invention] The present invention relates to a power phase adjuster, and in particular, to a phase adjuster for adjusting the phase so that the voltage ratio between the primary side and the secondary side is always the same. This invention relates to a phase adjuster capable of
[発明の技術的背景]
位相調整器は、1次側と2次側の電圧位相を変化させて
、電力系統の潮流制御を行う装置であるが、位相調整方
式によっては、1次側と2次側の電圧比が位相角によっ
て変化してしまうことが起こり、系統運用上好ましくな
い場合がある。[Technical Background of the Invention] A phase adjuster is a device that controls power flow in a power system by changing the voltage phase between the primary and secondary sides. The voltage ratio on the next side may change depending on the phase angle, which may be unfavorable for system operation.
このため、1次側と2次側の電圧比を変化させないで、
位相角を調整する方式として、第1図に示す様な位相調
整方式が提案されている。Therefore, without changing the voltage ratio between the primary and secondary sides,
As a method for adjusting the phase angle, a phase adjustment method as shown in FIG. 1 has been proposed.
第1図は、調整変圧器1と直列変圧器2からなる位相調
整器である。調整変圧器1には各相の分路巻線3、タッ
プ巻線4、安定巻線5が巻装されており、安定巻線5は
三角結線されると共に、タップ巻線4、分路巻線3はそ
れぞれ星形結線されている。FIG. 1 shows a phase adjuster consisting of a regulating transformer 1 and a series transformer 2. In FIG. The regulating transformer 1 is wound with a shunt winding 3, a tap winding 4, and a stable winding 5 for each phase. The wires 3 are each connected in a star shape.
一方、直列変圧器2には、各相の励磁巻線6及び直列巻
線7が巻装されており、励磁巻線6は三角結線された後
、タップ切換器(図示せず)を介してタップ巻線4に接
続され、タップ位置に応じた電圧で直列巻線7を励磁す
る。また、直列巻線7は、その中央(中間電位点)から
端子を引出して、自相と直角成分の電圧を有する分路巻
線3の線路端側に接続すると共に、両端はそれぞれ1次
、2次端子に接続する。On the other hand, the series transformer 2 is wound with excitation windings 6 and series windings 7 for each phase, and the excitation windings 6 are triangularly connected and then connected through a tap changer (not shown). It is connected to the tap winding 4 and excites the series winding 7 with a voltage according to the tap position. Further, the series winding 7 has a terminal drawn out from its center (intermediate potential point) and connected to the line end side of the shunt winding 3 having a voltage of a component at right angles to its own phase, and both ends are connected to the primary, Connect to secondary terminal.
以上の構成とすると、第2図のベクトル図に示す如く、
1次端子電圧81及び2次端子電圧91は、分路巻線電
圧31にこれと直角成分の直列巻線調気電圧71の1/
2をベクトル的に加減した電圧となるため、電圧絶対値
は互いに等しく、位相差は概略直列巻線調気電圧に比例
づる。従って、タップ切換器を操作して直列巻線調気電
圧を変化させることにより、電圧絶対値を等しくしたま
ま、1次電圧、2次電圧間の位相差を変化させることが
できる。With the above configuration, as shown in the vector diagram in Figure 2,
The primary terminal voltage 81 and the secondary terminal voltage 91 are equal to orthogonal to the shunt winding voltage 31 and 1/1 of the series winding regulation voltage 71.
Since the voltages are obtained by adding or subtracting 2 vectorwise, the voltage absolute values are equal to each other, and the phase difference is approximately proportional to the series winding control voltage. Therefore, by operating the tap changer to change the series winding control voltage, it is possible to change the phase difference between the primary voltage and the secondary voltage while keeping the absolute voltage values the same.
以上説明した回路構成とした場合の具体的な直列変圧器
の巻線構成としては、一般に第3図が考えられる。即ち
、鉄心脚9に内側から励磁巻線6、直列巻線7の順に巻
装し、直列巻線は上下に2分割して(巻き方向は上下同
一方向)その中央(中間電圧点)より端子Xを引出して
対応する相の分路巻線(図示せず)に接続すると共に、
上下端はそれぞれ1機端子U、2広端子Uに接続する構
成である。FIG. 3 can generally be considered as a specific winding configuration of a series transformer in the case of the circuit configuration described above. That is, the excitation winding 6 and the series winding 7 are wound around the core leg 9 from the inside in this order, and the series winding is divided into two halves (winding direction is the same direction above and below), and the terminal is connected from the center (intermediate voltage point). X and connect it to the shunt winding (not shown) of the corresponding phase, and
The upper and lower ends are connected to one terminal U and two wide terminals U, respectively.
[背景技術の問題点]
ところで、各巻線に流れる電流及びこの電流によって生
ずるもれ磁束について考えて見る。[Problems with Background Art] Now, let's consider the current flowing through each winding and the leakage magnetic flux caused by this current.
各巻線に流れる電流は、第4図のベクトル図に示す様に
、直列巻線の上部には1次線路電流■1が流れ、直列巻
線下部には1次線路電流と調整角αだけ位相が異なり大
きさは等しい電流■2が流れる。また、励磁巻線には、
上記電流によるアンペアターンをキャンセルするための
電流が流れる。As shown in the vector diagram in Figure 4, the current flowing through each winding is such that the primary line current ■1 flows in the upper part of the series winding, and the phase of the primary line current is equal to the adjustment angle α in the lower part of the series winding. A current (2) with different magnitudes and the same magnitude flows. In addition, in the excitation winding,
A current flows to cancel the ampere turn caused by the above current.
ここで、励磁巻線電流と同位相成分の電流及び、直角位
相成分の電流に分離して各々の電流によるもれ磁束分布
を考えると、同位相成分の電流によるもれ磁束は、第5
図の様に通常の変圧器と同一の分布となり、タンク壁上
下でキャンセルするが、直角位相成分の電流ににるもれ
磁束は、直列巻線の上下でアンペアターンがキャンセル
される形となるため、第6図の様にタンク上下でキャン
セルせず、タンク壁10−タンク底11−鉄心9又はタ
ンク壁10−タンクカバー12−鉄心9の経路で循環す
る形となる。Here, if we consider the leakage flux distribution due to the current of the same phase component as the excitation winding current and the current of the quadrature component and the current of the quadrature component, the leakage flux due to the current of the same phase component is the fifth
As shown in the figure, the distribution is the same as that of a normal transformer, and it is canceled at the top and bottom of the tank wall, but the leakage magnetic flux in the quadrature component current is in the form of ampere turns canceled at the top and bottom of the series winding. Therefore, as shown in FIG. 6, the liquid does not cancel at the top and bottom of the tank, but instead circulates along the tank wall 10 - tank bottom 11 - iron core 9 or tank wall 10 - tank cover 12 - iron core 9 path.
第5図の同位相成分のもれ磁束に対しては、タンク側面
に磁気シールド13を取付けて、上下の磁束のバスを作
りタンク壁への磁束の浸入を防止して、タンク壁の過熱
を容易に防ぐことができるが、第6図のタンク上下でキ
ャンセルしないもれ磁束に対しては、それがタンク底1
1或いはタンクカバー12に侵入することを防止づるの
は極めて困難であることから、タンクを非磁性材で製作
する等のタンク過熱防止策を取る必要がある。To deal with the leakage magnetic flux of the same phase component shown in Fig. 5, a magnetic shield 13 is installed on the side of the tank to create an upper and lower magnetic flux bus to prevent the magnetic flux from penetrating into the tank wall and prevent overheating of the tank wall. Although it can be easily prevented, leakage magnetic flux that is not canceled at the top and bottom of the tank in Figure 6 is caused by
Since it is extremely difficult to prevent the liquid from entering the tank cover 12 or the tank cover 12, it is necessary to take measures to prevent the tank from overheating, such as making the tank from a non-magnetic material.
しかしながら、タンクを非磁性材で製作することは、機
器のコストが極端に高くなり、必ずしも現実的ではない
。また、タンク底やタンクカバーの内側にタンク壁10
と同様な磁気シールドを設番プることも、タンクの構造
の複雑化を招き望ましい手段とはいえない。However, manufacturing the tank from a non-magnetic material increases the cost of the equipment extremely and is not necessarily practical. In addition, the tank wall 10 is installed on the tank bottom or inside the tank cover.
Installing a similar magnetic shield is also not a desirable method because it complicates the structure of the tank.
し発明の目的]
本発明は、上記の様な従来技術の問題点を解消づるため
に提案されたもので、その目的は、直列変圧器の巻線か
らのもれ磁束によるタンク壁の過熱を、簡単な構造で且
つ効果的に防止できる位相調整器を提供することにある
。OBJECT OF THE INVENTION The present invention was proposed in order to solve the problems of the prior art as described above, and its purpose is to prevent overheating of the tank wall due to leakage magnetic flux from the windings of the series transformer. The object of the present invention is to provide a phase adjuster that has a simple structure and can effectively prevent the problem.
[発明の概要]
本発明の位相調整器は、励磁巻線と、2個の直列巻線単
位に等分割された直列巻線とを巻装して成る直列変圧器
を備え、且つ前記2個の直列巻線単位の巻線の巻き方向
を逆にすると共に、2個の直列巻線単位を同心円筒状に
配置することにより、励磁巻線電流と同位相成分及び直
角位相成分のいずれの電流によるもれ磁束も、タンク壁
の上下でキャンセルされる様にしたものである。[Summary of the Invention] The phase adjuster of the present invention includes a series transformer wound with an excitation winding and a series winding equally divided into two series winding units, and By reversing the winding direction of the series winding units and arranging the two series winding units in a concentric cylindrical shape, it is possible to control the excitation winding current and both the in-phase component and the quadrature phase component. The magnetic flux leakage caused by this is also canceled at the top and bottom of the tank wall.
[発明の実施例]
以下、本発明の位相調整器の一例を第7図により具体的
に説明する。[Embodiments of the Invention] Hereinafter, an example of the phase adjuster of the present invention will be specifically explained with reference to FIG.
第7図において、鉄心脚9には、その内側から励磁巻線
6.1機端子Uに接続される直列巻線単位72.2広端
子Uに接続される直列巻線単位73の順に、各巻線が同
心円筒状に巻装されている。In FIG. 7, from the inside of the core leg 9, the excitation winding 6.1 series winding unit 72 connected to the machine terminal U, 2 the series winding unit 73 connected to the wide terminal U are arranged in the following order: The wires are wound into concentric cylinders.
各直列巻線単位72.73は、それぞれ巻回数は同−で
、巻き方向は互いに逆方向となっており、直列巻線単位
72.73の下部同士を一括した後、X端子を引出して
調整変圧器の対応する相の分路巻線に接続させると共に
、各直列巻線単位72゜73の上部はそれぞれ1次U端
子、2次(」端子に接続させたものである。Each series winding unit 72, 73 has the same number of windings, and the winding direction is opposite to each other. After the lower parts of the series winding unit 72, 73 are tied together, the X terminal is pulled out and adjusted. It is connected to the shunt winding of the corresponding phase of the transformer, and the upper part of each series winding unit 72, 73 is connected to the primary U terminal and the secondary ('') terminal, respectively.
この様な構成とした場合、各巻線に流れる電流は、第8
図に示す様に、1次端子に接続された直列巻線単位72
には1次線路電流11が流れ、2次端子Uに接続された
直列巻線単位73には1次線路電流と調整器αだけ位相
が異なり大きさは等しい電流12が流れる。また、励磁
巻線には、上記電流によるアンペアターンをキャンセル
覆るための電流Ig が流れる。In such a configuration, the current flowing through each winding is
As shown in the figure, a series winding unit 72 connected to the primary terminal
A primary line current 11 flows through the series winding unit 73 connected to the secondary terminal U, and a current 12 which has a phase difference from the primary line current by the regulator α but is equal in magnitude flows through the series winding unit 73 connected to the secondary terminal U. Further, a current Ig flows through the excitation winding to cancel and cover the ampere turn caused by the current.
励磁巻線電流と同位相成分の電流及び、直角位相成分の
電流に分離して各々の電流によるもれ磁束分布を考える
と、励磁巻線電流と同位相成分のもれ磁束分布は第9図
の様になり、これは通常の変圧器と同一の分布となり、
タンクの上下でキャンセルされることになる。また、励
磁巻線電流と直角位相成分の電流によるもれ磁束分布は
、第10図の如くとなり、これもまた通常変圧器と同様
タンク壁の上下でキャンセルされることになる。If we consider the leakage flux distribution due to each current by separating it into a current with the same phase component as the excitation winding current and a current with a quadrature component, the leakage flux distribution of the same phase component with the excitation winding current is shown in Figure 9. This is the same distribution as a normal transformer,
It will be canceled by the top and bottom of the tank. Further, the leakage magnetic flux distribution due to the excitation winding current and the quadrature phase component current is as shown in FIG. 10, and this is also canceled at the top and bottom of the tank wall as in a normal transformer.
従って、本実施例によれば、励磁巻線電流と同位相成分
の電流によるもれ磁束及びその直角成分の電流によるも
れ磁束の両者に対して、タンク壁面に磁気シールド13
を取付けて磁束のパスを作り、タンク底或いはタンクカ
バーへの磁束の侵入を防止して、タンク壁の過熱を容易
に防止することができる。Therefore, according to this embodiment, the magnetic shield 13 is installed on the tank wall to prevent both the leakage magnetic flux due to the current having the same phase component as the excitation winding current and the leakage magnetic flux due to the current having the perpendicular component to the excitation winding current.
can be installed to create a magnetic flux path, prevent magnetic flux from entering the tank bottom or tank cover, and easily prevent overheating of the tank wall.
なお、本発明は、直列巻線を構成する2個の巻線単位を
同心円筒状に配置することを特徴とするものであり、他
の点は前記実施例に限定されるものではない。例えば、
2個の直列巻線単位を鉄心脚側に、励磁巻線を外側に配
置りることも可能である。Note that the present invention is characterized in that two winding units constituting a series winding are arranged in a concentric cylindrical shape, and other points are not limited to the above embodiments. for example,
It is also possible to arrange two series winding units on the core leg side and the excitation winding on the outside.
[発明の効果]
以上の様に本発明によれば、直列巻線を構成する各巻線
単位の配置形状に配慮を施すという極めて簡単な手段に
J二り、タンクを非磁性材で構成する等の高価な対策を
とることなく、直列変圧器の巻線のちれ磁束によるタン
クの過熱を防止した位相調整器を提供することが可能と
なる。[Effects of the Invention] As described above, according to the present invention, there are extremely simple measures such as taking into account the arrangement shape of each winding unit that constitutes the series winding, and constructing the tank from a non-magnetic material. Therefore, it is possible to provide a phase adjuster that prevents overheating of a tank due to magnetic flux torn from windings of a series transformer without taking expensive measures.
第1図は変圧比一定の位相調整器の結線図、第2図は変
圧比一定の位相調整器の原理を示す電圧ベクトル図、第
3図は変圧比一定の位相調整器の直列変圧器の巻線構成
図、第4図は第3図で示した直列変圧器の各巻線に流れ
る電流を示づベクトル図、第5図、第6図はそれぞれ第
3図で示した直列変圧器の励磁巻線電流と同位相成分電
流によるもれ磁束分布及び直角位相成分電流によるもれ
磁束分布を示す説明図、第7図は本発明による直列変圧
器の巻線構成図、第8図は第7図の巻線構成とした時の
各巻線に流れる電流を示すベクトル図、第9図は第7図
の巻線構成とした時の励磁巻線電流と同位相成分電流に
よるもれ磁束分布を示す説明図、第10図は第7図の巻
線構成とした時の励11巻IJIN流と直角位相成分電
流によるもれ磁束分布を示す説明図である。
1・・・調整変圧器、2・・・直列変圧器、3・・・分
路巻線、4・・・タップ巻線、5・・・安定巻線、6・
・・励磁巻線、7・・・直列巻線、31・・・分路巻線
電圧、71・・・直列巻線電圧、81・・・1次端子電
圧、91・・・2次端子電圧、10・・・タンク壁、1
1・・・タンク底、12・・・タンクカバー13・・・
磁気シールド、72.73・・・直列巻線単位。
第1図
第2図
第3図
第5図
第6図
第7図
第81!1
第9図
第10図Figure 1 is a wiring diagram of a phase regulator with a constant transformation ratio, Figure 2 is a voltage vector diagram showing the principle of a phase regulator with a constant transformation ratio, and Figure 3 is a series transformer diagram of a phase regulator with a constant transformation ratio. A winding configuration diagram, Figure 4 shows the current flowing through each winding of the series transformer shown in Figure 3, a vector diagram, Figures 5 and 6 show the excitation of the series transformer shown in Figure 3, respectively. An explanatory diagram showing the leakage flux distribution due to the winding current and the in-phase component current and the leakage flux distribution due to the quadrature phase component current, FIG. 7 is a winding configuration diagram of the series transformer according to the present invention, and FIG. A vector diagram showing the current flowing through each winding when the winding configuration is as shown in the figure. Figure 9 shows the leakage flux distribution due to the excitation winding current and the same phase component current when the winding configuration is as shown in Figure 7. The explanatory diagram, FIG. 10, is an explanatory diagram showing the leakage magnetic flux distribution due to the 11-turn excitation IJIN current and quadrature phase component current when the winding configuration shown in FIG. 7 is used. DESCRIPTION OF SYMBOLS 1... Adjustment transformer, 2... Series transformer, 3... Shunt winding, 4... Tap winding, 5... Stable winding, 6...
... Excitation winding, 7... Series winding, 31... Shunt winding voltage, 71... Series winding voltage, 81... Primary terminal voltage, 91... Secondary terminal voltage , 10...tank wall, 1
1... Tank bottom, 12... Tank cover 13...
Magnetic shield, 72.73...Series winding unit. Figure 1 Figure 2 Figure 3 Figure 5 Figure 6 Figure 7 Figure 81!1 Figure 9 Figure 10
Claims (1)
相調整器において、 励磁巻線と、2個の直列巻線単位に等分割された直列巻
線とを鉄心脚に巻装して直列変圧器を構成し、且つ前記
2個の直列巻線単位の巻線の巻き方向を逆にすると共に
、2個の直列巻線単位を同心円筒状に配置し、各直列巻
線単位の一端を一括接続して対応する相の分路巻線に接
続し、各直列巻線単位の他端をそれぞれ1次又は2次の
線路端子に接続したことを特徴とする位相調整器。[Claims] In a constant transformer ratio phase adjuster comprising an adjustment transformer and a series transformer, an excitation winding and a series winding equally divided into two series windings are connected to an iron core. The coils are wound around the legs to constitute a series transformer, and the winding directions of the two series winding units are reversed, and the two series winding units are arranged in a concentric cylindrical shape, and each A phase characterized in that one end of each series winding unit is connected together and connected to the shunt winding of the corresponding phase, and the other end of each series winding unit is connected to a primary or secondary line terminal, respectively. regulator.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59022958A JPS60169114A (en) | 1984-02-13 | 1984-02-13 | Phase adjustor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59022958A JPS60169114A (en) | 1984-02-13 | 1984-02-13 | Phase adjustor |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS60169114A true JPS60169114A (en) | 1985-09-02 |
Family
ID=12097108
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP59022958A Pending JPS60169114A (en) | 1984-02-13 | 1984-02-13 | Phase adjustor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS60169114A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5557248A (en) * | 1994-02-24 | 1996-09-17 | Synektron Corporation | Magnetizer for magnets with shaped magnetic waveform |
-
1984
- 1984-02-13 JP JP59022958A patent/JPS60169114A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5557248A (en) * | 1994-02-24 | 1996-09-17 | Synektron Corporation | Magnetizer for magnets with shaped magnetic waveform |
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