JPS586377B2 - AC synchronous machine field current measuring device - Google Patents
AC synchronous machine field current measuring deviceInfo
- Publication number
- JPS586377B2 JPS586377B2 JP51037494A JP3749476A JPS586377B2 JP S586377 B2 JPS586377 B2 JP S586377B2 JP 51037494 A JP51037494 A JP 51037494A JP 3749476 A JP3749476 A JP 3749476A JP S586377 B2 JPS586377 B2 JP S586377B2
- Authority
- JP
- Japan
- Prior art keywords
- voltage
- current
- field current
- synchronous machine
- field
- 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
Links
Landscapes
- Tests Of Circuit Breakers, Generators, And Electric Motors (AREA)
- Control Of Eletrric Generators (AREA)
- Synchronous Machinery (AREA)
Description
【発明の詳細な説明】
この発明は主としてブラシレス同期機の界磁電流測定装
置に適するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention is mainly suitable for a field current measuring device for a brushless synchronous machine.
従来この種回転機の界磁電流の測定方法として一般に知
られているものの一例を第1図に示す。An example of a conventionally known method for measuring the field current of this type of rotating machine is shown in FIG.
図において、1ぱ同期発電機の固定子、2はその回転部
分で、2aは交流励磁機の回転電機子巻線、2bは交流
励磁機の電機子巻線2aの出力を整流するための回転整
流器、2Cは同期発電機の界磁巻線、3は交流励磁機の
界磁巻線、4は交流励磁機の界磁巻線回路に挿入した分
流器、5は交流励磁機の界磁電流計である。In the figure, 1 is the stator of the synchronous generator, 2 is its rotating part, 2a is the rotating armature winding of the AC exciter, and 2b is the rotation for rectifying the output of the armature winding 2a of the AC exciter. rectifier, 2C is the field winding of the synchronous generator, 3 is the field winding of the AC exciter, 4 is the shunt inserted in the field winding circuit of the AC exciter, 5 is the field current of the AC exciter It is a total.
次にこの装置について説明する。Next, this device will be explained.
同期発電機の界磁巻線2cは、回転整流器2b、交流励
磁機の電機子巻線2aと共に、運転中は常時回転してお
り直接界磁電流を計測することができない。The field winding 2c of the synchronous generator, together with the rotating rectifier 2b and the armature winding 2a of the AC exciter, is constantly rotating during operation, and the field current cannot be directly measured.
そのため同期発電機界磁電流の代わりに、ほぼ相対的な
関係にある交流励磁機の界磁電流計5で交流励磁機の界
磁電流を計測し、同期発電機の界磁電流を推定している
。Therefore, instead of measuring the synchronous generator field current, the field current of the AC exciter is measured using the field ammeter 5 of the AC exciter, which has an almost relative relationship, and the field current of the synchronous generator is estimated. There is.
従来の同期発電機の界磁電流はこのような方法で推定す
るために、交流励磁機の磁気回路の飽和による誤差、同
期発電機の界磁巻線2Cや交流励磁機の電機子巻線2a
の温度変化による誤差が大きく、実用上は単に目安とし
ての利用価値しかないという欠点があった。In order to estimate the field current of a conventional synchronous generator using this method, errors due to saturation of the magnetic circuit of the AC exciter, field winding 2C of the synchronous generator, and armature winding 2a of the AC exciter are
The problem is that the error due to temperature changes is large, and in practical terms it is only useful as a guide.
さらに同期発電機の界磁電流を直読することができず、
また電流値推定の手間がかかるという欠点もあった。Furthermore, it is not possible to directly read the field current of the synchronous generator,
Another drawback is that it takes time and effort to estimate the current value.
この発明は上述のような従来の装置の欠点を解消するこ
とを目的としてなされたもので、同期機の内部誘起電圧
を検出することにより、内部誘起電圧と比例関係にある
同期機の界磁電流を直読することができる精度の良いブ
ラシレス同期機の界磁電流検出に適する界磁電流測定装
置を提供するものである。This invention was made with the aim of eliminating the drawbacks of the conventional devices as described above. By detecting the internal induced voltage of the synchronous machine, the field current of the synchronous machine, which is proportional to the internal induced voltage, can be detected. The object of the present invention is to provide a field current measuring device suitable for detecting the field current of a brushless synchronous machine with high precision and capable of directly reading the field current.
次にこの発明の一実施例を図に基づいて説明する。Next, one embodiment of the present invention will be described based on the drawings.
第2図において、7は交流発電機1の出力電流を検出す
るための変流器、8は同期発電機の端子電圧によって付
勢される関数変換器で、発電機の界磁巻線に流れる界磁
電流と発電機1に発生する発電機電圧の、いわゆる第4
図に示すような無負荷飽和特性曲線と同様の、第5図に
示すような入出力関係を有するものである。In Fig. 2, 7 is a current transformer for detecting the output current of the alternator 1, and 8 is a function converter energized by the terminal voltage of the synchronous generator, which flows into the field winding of the generator. The so-called 4th generation of the field current and the generator voltage generated in the generator 1
It has an input/output relationship as shown in FIG. 5, which is similar to the no-load saturation characteristic curve shown in the figure.
9は同期発電機1の内部誘起電圧に比例した電圧を作る
電圧検出回路、10はこの電圧検出回路の内部誘起電圧
を界磁電流として変換し、表示する変換表示装置である
。9 is a voltage detection circuit that generates a voltage proportional to the internal induced voltage of the synchronous generator 1, and 10 is a conversion display device that converts the internal induced voltage of this voltage detection circuit as a field current and displays it.
なお、その他の構成は第1図に示す従来の装置と同様で
あるから説明を省略する。Note that the other configurations are the same as the conventional device shown in FIG. 1, so the explanation will be omitted.
この発明は上述のように交流発電機1に発生する内部誘
起電圧を検出し、界磁電流として表示するようにしたも
ので、界磁電流と内部誘起電圧との関係は界磁巻線の温
度変化による低抗変化にかかわらず常に一定の相対関係
を有することを利用したものである。As described above, this invention detects the internal induced voltage generated in the alternator 1 and displays it as a field current.The relationship between the field current and the internal induced voltage is determined by the temperature of the field winding. This takes advantage of the fact that there is always a constant relative relationship regardless of the low resistance change due to change.
第3図は電圧検出回路9の一実施例、第6図、第7図は
第3図に示す装置の説明のためのベクトル図である。FIG. 3 is an embodiment of the voltage detection circuit 9, and FIGS. 6 and 7 are vector diagrams for explaining the device shown in FIG. 3.
第3図において、7は交流発電機1の出力電流を検出す
るための変流器、8は交流発電機1の端子電圧を検出し
、交流発電機1の磁気飽和特性を補正するための関数変
換器、11は関数変換器8の出力電圧と、変流器7によ
って検出した交流発電機1の出力電流に比例する電圧を
ベクトル合成するための変圧器、12は変流器7の二次
電流を分流する低抗、E1は変圧器11の二次電圧、E
2は抵抗120両端電圧、E3は電圧検出回路9の出力
電圧で交流発電機の界磁巻線電流に比例する。In FIG. 3, 7 is a current transformer for detecting the output current of the alternator 1, and 8 is a function for detecting the terminal voltage of the alternator 1 and correcting the magnetic saturation characteristics of the alternator 1. Converter 11 is a transformer for vector synthesis of the output voltage of the function converter 8 and a voltage proportional to the output current of the alternator 1 detected by the current transformer 7; 12 is a secondary of the current transformer 7; A low resistor that shunts the current, E1 is the secondary voltage of the transformer 11, E
2 is the voltage across the resistor 120, and E3 is the output voltage of the voltage detection circuit 9, which is proportional to the field winding current of the alternator.
第6図においてEu,Ev,Ewは交流発電機1の相電
圧、IvはV相電流、θは力率角とする。In FIG. 6, Eu, Ev, and Ew are the phase voltages of the alternator 1, Iv is the V-phase current, and θ is the power factor angle.
第7図においてEtおよび■は交流発電機1の端子電圧
および出力電流、■・xdは交流発電機1の同期インピ
ーダンスxdによる電圧降下、Eoは交流発電機1の内
部誘起電圧である。In FIG. 7, Et and ■ are the terminal voltage and output current of the alternator 1, ■·xd is the voltage drop due to the synchronous impedance xd of the alternator 1, and Eo is the internal induced voltage of the alternator 1.
第3図において関数変換器をU,W相間に、変流器7を
V相に接続するとEl,E2tE3のベクトルは第6図
に示すようになる。In FIG. 3, when the function converter is connected between the U and W phases and the current transformer 7 is connected to the V phase, the vectors of El and E2tE3 become as shown in FIG. 6.
即ち、E1はEu,Ewの合成ベクトルEwuに基づき
該Ewuと同位相になり、またE2はV相電流Ivに基
づき該Ivと同位相になる。That is, E1 has the same phase as Ewu based on the composite vector Ewu of Eu and Ew, and E2 has the same phase as Iv based on the V-phase current Iv.
ここでE1はEtに比例した値であり、E2は■に比例
した値であるから関数変換器8と抵抗12と変圧器11
を適当に選定すれば第6図のE,,E2,E3でできる
三角形と第7図に示すEt,I・xd,Eoで形成され
る三角形は負荷の大きさ、力率のいかんにかかわらず相
似形となる。Here, E1 is a value proportional to Et, and E2 is a value proportional to ■, so the function converter 8, resistor 12, and transformer 11
If , is selected appropriately, the triangle formed by E, , E2, and E3 in Figure 6 and the triangle formed by Et, I xd, and Eo shown in Figure 7 can be obtained regardless of the load size or power factor. They become similar shapes.
したがって、電圧E3は交流発電機1の内部誘起電圧E
oに比例することになり、さらに界磁電流と一定の比例
関係を保つことになる。Therefore, the voltage E3 is the internal induced voltage E of the alternator 1.
o, and maintains a constant proportional relationship with the field current.
この実施例では交流同期発電機について説明したが、交
流同期電動機についても同様にして界磁電流を検出測定
することができる。In this embodiment, an AC synchronous generator has been described, but the field current can be similarly detected and measured for an AC synchronous motor.
このようにこの発明によれば交流同期機の内部誘起電圧
を検出することにより、交流同期機の界磁電流を検出で
きるように構成したため、ブラシレス同期機の界磁電流
を直読することができ、界磁巻線の抵抗変化による誤差
、磁気飽和による誤差の少ない界磁電流を検出すること
ができる。As described above, according to the present invention, the field current of the AC synchronous machine can be detected by detecting the internal induced voltage of the AC synchronous machine, so the field current of the brushless synchronous machine can be directly read. It is possible to detect field current with less error due to resistance change in the field winding and less error due to magnetic saturation.
さらに回転部分は従来のままの構造で良く、交流同期機
製作完了後でも容易に取り付け可能な、精度の良い界磁
電流検出、測定装置を得ることができる。Furthermore, the rotating part may have the same structure as before, and a highly accurate field current detection and measurement device that can be easily installed even after the AC synchronous machine is manufactured can be obtained.
第1図は従来の同期機の界磁電流を推定する装置を説明
するためのブラシレス同期機の結線図、第2図はこの発
明の一実施例による界磁電流検出、測定装置を示す結線
図、第3図は第2図に示す装置の説明のための電圧検出
回路の一実施例を示す結線図、第4図は交流同期機の無
負荷飽和特性曲線、第5図はこの発明になる関数変換器
の入力、出力関係を示す特性曲線、第6図、第7図は第
3図に示す電圧検出回路の説明のためのベクトル図であ
る。
図中1は交流発電機、2は回転部分、3は交流励磁機の
界磁巻線、4は分流器、5は交流励磁機界磁電流計、7
は変流器、8は関数変換器、9は電圧検出回路、10は
界磁電流表示装置、11は変圧器、12は抵抗である。
なお各図中、同一符号は同一又は相当部分を示す.Fig. 1 is a wiring diagram of a brushless synchronous machine to explain a conventional device for estimating field current of a synchronous machine, and Fig. 2 is a wiring diagram showing a field current detection and measurement device according to an embodiment of the present invention. , Fig. 3 is a wiring diagram showing an embodiment of the voltage detection circuit for explaining the device shown in Fig. 2, Fig. 4 is a no-load saturation characteristic curve of an AC synchronous machine, and Fig. 5 is the present invention. Characteristic curves showing the input and output relationships of the function converter, FIGS. 6 and 7 are vector diagrams for explaining the voltage detection circuit shown in FIG. 3. In the figure, 1 is the AC generator, 2 is the rotating part, 3 is the field winding of the AC exciter, 4 is the shunt, 5 is the AC exciter field ammeter, 7
8 is a current transformer, 8 is a function converter, 9 is a voltage detection circuit, 10 is a field current display device, 11 is a transformer, and 12 is a resistor. In each figure, the same symbols indicate the same or equivalent parts.
Claims (1)
電圧によって付勢され、上記同期機の界磁電流と内部誘
起電圧の無負荷飽和特性曲線と同様の入出力関係を有す
る関数変換器と、上記同期機の第2相の相電流に比例す
る出力電圧を得るための変流器および変圧装置と、上記
関数変換器の出力電圧と上記変流器および変圧装置の出
力電圧との合成電圧に応動する装置とを備えたことを特
徴とする交流同期機の界磁電流計測装置。1 It is energized by the voltage between the first and third phase terminals on the AC side of a three-phase AC synchronous machine, and has an input/output relationship similar to the no-load saturation characteristic curve of the field current and internal induced voltage of the above synchronous machine. a current transformer and a voltage transformer for obtaining an output voltage proportional to the phase current of the second phase of the synchronous machine; an output voltage of the function converter and an output of the current transformer and the voltage transformer; 1. A field current measuring device for an AC synchronous machine, comprising a device that responds to a composite voltage.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP51037494A JPS586377B2 (en) | 1976-04-02 | 1976-04-02 | AC synchronous machine field current measuring device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP51037494A JPS586377B2 (en) | 1976-04-02 | 1976-04-02 | AC synchronous machine field current measuring device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS52120311A JPS52120311A (en) | 1977-10-08 |
| JPS586377B2 true JPS586377B2 (en) | 1983-02-04 |
Family
ID=12499065
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP51037494A Expired JPS586377B2 (en) | 1976-04-02 | 1976-04-02 | AC synchronous machine field current measuring device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS586377B2 (en) |
-
1976
- 1976-04-02 JP JP51037494A patent/JPS586377B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS52120311A (en) | 1977-10-08 |
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