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JPS6142520B2 - - Google Patents
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JPS6142520B2 - - Google Patents

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Publication number
JPS6142520B2
JPS6142520B2 JP53092187A JP9218778A JPS6142520B2 JP S6142520 B2 JPS6142520 B2 JP S6142520B2 JP 53092187 A JP53092187 A JP 53092187A JP 9218778 A JP9218778 A JP 9218778A JP S6142520 B2 JPS6142520 B2 JP S6142520B2
Authority
JP
Japan
Prior art keywords
generator
input terminal
connection point
voltage
output voltage
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
Application number
JP53092187A
Other languages
Japanese (ja)
Other versions
JPS5518885A (en
Inventor
Toshiharu Chiba
Ichihiro Hibino
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.)
Shinko Electric Co Ltd
Original Assignee
Shinko Electric Co Ltd
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 Shinko Electric Co Ltd filed Critical Shinko Electric Co Ltd
Priority to JP9218778A priority Critical patent/JPS5518885A/en
Publication of JPS5518885A publication Critical patent/JPS5518885A/en
Publication of JPS6142520B2 publication Critical patent/JPS6142520B2/ja
Granted legal-status Critical Current

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  • Control Of Eletrric Generators (AREA)

Description

【発明の詳細な説明】 本発明は回転数の低下時の界磁巻線の焼損を防
止するようにしたブラシレス同期発電機の励磁制
御装置を提供することを目的とする。
DETAILED DESCRIPTION OF THE INVENTION An object of the present invention is to provide an excitation control device for a brushless synchronous generator that prevents burnout of the field winding when the rotational speed decreases.

以下、図示する実施例により本発明の構成およ
び作用を詳細に説明する。
Hereinafter, the structure and operation of the present invention will be explained in detail with reference to illustrated embodiments.

第1図は出力電圧一定の場合の回転数−界磁電
流特性である。この図から明らかなように同期発
電機を自動電圧調整器によつて定電圧制御する場
合、回転数が低下すると、界磁電流が増大する。
したがつて、この状態で長時間運転すると、界磁
巻線を焼損する。そしてこの危険性はブラシ付の
場合よりもブラシレスの場合が大きい。この特性
を一般式で表わすと次のようになる。
FIG. 1 shows the rotation speed-field current characteristic when the output voltage is constant. As is clear from this figure, when the synchronous generator is controlled at constant voltage by an automatic voltage regulator, as the rotational speed decreases, the field current increases.
Therefore, if the device is operated for a long time in this state, the field winding will burn out. And this risk is greater with brushless than with brush. This characteristic can be expressed as a general formula as follows.

If=KV/N ……(1) こゝで、Ifは界磁電流、V0は発電機出力電圧、
Nは回転数、Kは定数である。この式から、Ifを
一定にするには、V/Nを一定に保つ必要がある。
If=KV 0 /N 2 ...(1) Here, If is the field current, V 0 is the generator output voltage,
N is the number of rotations, and K is a constant. From this equation, in order to keep If constant, it is necessary to keep V 0 /N 2 constant.

したがつて、次のように表わされる。Therefore, it can be expressed as follows.

V0N2 ……(2) これを図で示したのが第2図である。この第2
図から明らかなように、回転数Nが低下しても、
界磁電流Ifを一定に保つためには発電機出力電圧
V0を2乗カーブで低減させる必要がある。しか
し、一方、発電機の通常の運転状態では、定格回
転数附近で回転数が変動しても、発電機出力電圧
は一定電圧に保つ必要がある。第3図は、この両
方の条件を満たすような回転数−出力電圧特性図
である。すなわち、定格回転数Nrより一定値だ
け小さな回転数N1より大きな部分では定格電圧
Vorで運転し、N1より小さな部分では出力電圧V0
を回転数の2乗カーブで低減させるようにする。
しかし、V0∝N2特性で制御すると、回路が複雑
となる。又、エンジンで発電機を駆動する場合、
一般には定常で±5%、瞬時で±10%程度の回転
数変動率であるので第3図のN1を定格回転数Nr
の90%程度に設定すれば、N1以下では界磁電流If
が増大しないように出力電圧V0を低減すれば必
ずしも2乗カーブで低減させなくても実用上支障
はなく、むしろ点線で示したb直線で低減させれ
ば界磁巻線の加熱も少くなり、回路も簡単とな
る。このときの界磁電流Ifは曲線cのように減少
する。第4図は、第3図のb直線、c曲線の特性
で励磁制御するようにした励磁制御装置の接続図
例である。図中、Gは同期発電機の電機子、
ACEXは交流励磁機、F1,F2は界磁巻線、V0
発電機出力電圧、Trは変圧器、PTは計器用変圧
器、SCRはサイリスター、SDはサイリスタード
ライバー、OPは演算増巾器、ZDはチエナーダイ
オード、D1〜D3はダイオード、PGは回転数Nに
比例した出力Vを発生する関数発生器、R1〜R5
は抵抗器、VRは可変抵抗器である。又、O端子
は発電機出力線中の共通線でOボルト線であり、
端子BとOとの間に発電機電圧の帰還電圧Vgが
帰還される。このような構成で、第3図の回転数
がN1以上のときは、函数発生器PGの出力電圧V
はツエナーダイオードZDの電圧VZDより高くな
るため、ダイオードD1でカツトされ、この点で
切り離されたのと全く同じ状態となる。したがつ
て、ツエナーダイオードZDの電圧VZDを基準電
圧としてVg=−VZDとなるように、すなわち、
発電帰出力電圧が定電圧Vorになるように制御さ
れる。次に回転数がN1以下に下ると、函数発生
器PGの出力電圧Vがツエナー電圧VZDより低く
なる。このため、ツエナーダイオードZD側より
PGへ差電圧(VZD−V)によつて電流が流れ
る。
V 0 = K N 2 ...(2) This is illustrated in Figure 2. This second
As is clear from the figure, even if the rotational speed N decreases,
In order to keep the field current If constant, the generator output voltage
It is necessary to reduce V 0 with a square curve. However, on the other hand, under normal operating conditions of the generator, the generator output voltage needs to be maintained at a constant voltage even if the rotational speed fluctuates around the rated rotational speed. FIG. 3 is a rotation speed-output voltage characteristic diagram that satisfies both of these conditions. In other words, the rated voltage is higher than the rotation speed N 1 , which is smaller than the rated rotation speed Nr by a certain value.
Operating at Vor, output voltage V 0 in parts smaller than N 1
is reduced according to the square curve of the rotational speed.
However, controlling using the V 0 ∝N 2 characteristic makes the circuit complicated. Also, when driving a generator with an engine,
In general, the rotation speed fluctuation rate is about ±5% in steady state and ±10% instantaneously, so N 1 in Fig. 3 is the rated rotation speed Nr.
If the field current is set to about 90% of N 1 or less, the field current If
As long as the output voltage V 0 is reduced so as not to increase, there is no practical problem even if the output voltage V 0 is not necessarily reduced according to the squared curve.In fact, if it is reduced according to the straight line b shown by the dotted line, the heating of the field winding will be reduced. , the circuit becomes simpler. At this time, the field current If decreases as shown by curve c. FIG. 4 is an example of a connection diagram of an excitation control device that performs excitation control using the characteristics of the b straight line and c curve in FIG. 3. In the figure, G is the armature of the synchronous generator,
ACEX is AC exciter, F 1 and F 2 are field windings, V 0 is generator output voltage, Tr is transformer, PT is potential transformer, SCR is thyristor, SD is thyristor driver, OP is operation Amplifier, ZD is a Chener diode, D 1 to D 3 are diodes, PG is a function generator that generates an output V proportional to the rotation speed N, R 1 to R 5
is a resistor and VR is a variable resistor. Also, the O terminal is a common line among the generator output lines and is an O volt line.
A feedback voltage Vg of the generator voltage is fed back between terminals B and O. With such a configuration, when the rotation speed in Fig. 3 is N 1 or more, the output voltage V of the function generator PG
Since it becomes higher than the voltage V ZD of the Zener diode ZD, it is cut by the diode D1 , and the state is exactly the same as being cut off at this point. Therefore, with the voltage V ZD of the Zener diode ZD as the reference voltage, Vg = -V ZD , that is,
The power generation return output voltage is controlled to be a constant voltage Vor. Next, when the rotational speed falls below N1 , the output voltage V of the function generator PG becomes lower than the Zener voltage V ZD . For this reason, from the Zener diode ZD side
Current flows to PG due to the differential voltage (V ZD -V).

この結果、基準点がJ点からH点に移り、函数
発生器PGの電圧Vを基準電圧として制御される
こととなる。何故ならば、H点と演算増巾器OP
の反転入力端子間にツエナーダイオードZDと抵
抗R2に加え抵抗R4の電圧降下分(VZD−V)が
挿入されるため、基準電圧はVZD−(VZD−V)=
Vとなり、H,B間の電圧がVとなるように制御
されることになるからである。一方、H,B間に
印加される電圧は、Vg+(VZD−V)となる。し
たがつて、帰還電圧Vgは Vg+(VZD−V)=Vより Vg=2V−VZD となり、第3図のようにb直線状に変化すること
となる。この結果、界磁電流Ifが第3図c曲線状
の特性で変化するため、発電機の回転数が、N1
より低下してもN1時の界磁電流値より大きくな
ることはなくなる。尚、第5図中、点線で示した
自励式の場合、電圧が低下し、自動電圧調整器の
動作が不能になる領域であるため、実際上は出力
電圧Vo=O、界磁電流If=Oになることを示した
ものである。
As a result, the reference point moves from point J to point H, and control is performed using the voltage V of the function generator PG as the reference voltage. The reason is that the H point and the operational amplifier OP
In addition to the Zener diode ZD and the resistor R 2 , the voltage drop of the resistor R 4 (V ZD - V) is inserted between the inverting input terminal of the
This is because the voltage between H and B is controlled to be V. On the other hand, the voltage applied between H and B is Vg+(V ZD -V). Therefore, since Vg+(V ZD -V)=V, the feedback voltage Vg becomes Vg=2V-V ZD , and changes linearly b as shown in FIG. As a result, the field current If changes according to the curve-like characteristics shown in Figure 3c, so the rotational speed of the generator changes to N 1
Even if the field current decreases further, it will never become larger than the field current value at N1 . In the case of the self-excited type shown by the dotted line in Figure 5, the voltage drops and the automatic voltage regulator becomes inoperable, so in reality, the output voltage Vo = O and the field current If = This shows that it becomes O.

以上の説明から容易に理解されるように本発明
により(1)回転数の低下時、界磁電流の増大を防止
できる。(2)定格回転数附近では函数発生器がダイ
オードで切離された状態となるため、定電圧制御
精度が函数発生器の影響で低下するのを防止でき
る。(3)回路構成が簡単、安価、小形化でき、信頼
性の向上につながる等の優れた効果がもたらされ
る。
As can be easily understood from the above explanation, the present invention can (1) prevent an increase in field current when the rotational speed decreases; (2) Since the function generator is disconnected by a diode near the rated rotation speed, it is possible to prevent constant voltage control accuracy from decreasing due to the influence of the function generator. (3) The circuit configuration is simple, inexpensive, and compact, and provides excellent effects such as improved reliability.

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

第1図は発電機出力電圧一定の場合の回転数一
界磁電流特性図、第2図は界磁電流一定の場合の
回転数−発電機出力電圧特性図、第3図は定格回
転数附近で一定発電機出力電圧、低回転数で発電
機出力電圧が回転数の2乗に比例するようにした
回転数−発電機電圧特性図、第4図は本発明によ
る励磁制御装置の接続図例、第5図は本発明の励
磁制御装置による回転数−発電機電圧、界磁電流
特性例図である。 V0……発電機出力電圧、Nr……定格回転数、
ZD……チエナーダイオード、PG……函数発生
器。
Figure 1 is a rotation speed vs. field current characteristic diagram when the generator output voltage is constant, Figure 2 is a rotation speed vs. generator output voltage characteristic diagram when the field current is constant, and Figure 3 is around the rated rotation speed. Figure 4 is an example of a connection diagram of the excitation control device according to the present invention. , FIG. 5 is an example diagram of the rotation speed-generator voltage and field current characteristics by the excitation control device of the present invention. V 0 ... Generator output voltage, Nr... Rated rotation speed,
ZD...Cheener diode, PG...Function generator.

Claims (1)

【特許請求の範囲】[Claims] 1 発電機出力電圧を帰還して励磁し、自動電圧
調整を行うブラシレス同期発電装置において、演
算増巾器OP,R5の反転入力端子に入力抵抗R1
介した第1の入力端子B;上記演算増巾器OP,
R5の非反転入力端子に第1の入力抵抗R3を介し
た第1の接続点H;上記第1の接続点Hに更に第
2の入力抵抗R4を介した第2の入力端子J;上
記演算増巾器OP,R5の反転入力端子に更に他の
抵抗R2を介した第2の接続点A;を設け、上記
第2の入力端子Jと上記第2の接続点Aとの間に
第2の入力端子J側がアノード側となるようにツ
エナーダイオードZDを接続し、又、上記第1の
接続点HからダイオードD1を順方向に介して、
発電機の回転数に比例した出力電圧を発生する函
数発生器PGを第1の接続点Hがプラス側となる
ように、上記第2の接続点Aに接続し、更に上記
第1の入力端子Bと上記第2の入力端子Jとの間
に発電機出力電圧の帰還電圧Vgを入力して、上
記演算増巾器OP,R5の出力端子から、発電機の
界磁電流指令信号を出力するようにして、低回転
時の界磁電流の増加を防止するようにしたことを
特徴とするブラシレス同期発電機の励磁制御装
置。
1. In a brushless synchronous power generator that excites by feeding back the generator output voltage and performs automatic voltage adjustment, the first input terminal B is connected to the inverting input terminal of the operational amplifier OP, R5 via the input resistor R1 ; The above operational amplifier OP,
A first connection point H via a first input resistor R 3 to the non-inverting input terminal of R 5 ; a second input terminal J via a second input resistor R 4 to the first connection point H; A second connection point A is further provided at the inverting input terminal of the operational amplifier OP, R5 via another resistor R2 , and the second input terminal J and the second connection point A are connected to each other. In between, a Zener diode ZD is connected so that the second input terminal J side becomes the anode side, and a diode D1 is connected in the forward direction from the first connection point H,
A function generator PG that generates an output voltage proportional to the rotation speed of the generator is connected to the second connection point A so that the first connection point H is on the positive side, and further connected to the first input terminal. A feedback voltage Vg of the generator output voltage is input between B and the second input terminal J, and a field current command signal of the generator is output from the output terminal of the operational amplifier OP, R5 . An excitation control device for a brushless synchronous generator, characterized in that an increase in field current during low rotation is prevented in this way.
JP9218778A 1978-07-27 1978-07-27 Excitation control unit of brushless synchronous motor Granted JPS5518885A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9218778A JPS5518885A (en) 1978-07-27 1978-07-27 Excitation control unit of brushless synchronous motor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9218778A JPS5518885A (en) 1978-07-27 1978-07-27 Excitation control unit of brushless synchronous motor

Publications (2)

Publication Number Publication Date
JPS5518885A JPS5518885A (en) 1980-02-09
JPS6142520B2 true JPS6142520B2 (en) 1986-09-22

Family

ID=14047430

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9218778A Granted JPS5518885A (en) 1978-07-27 1978-07-27 Excitation control unit of brushless synchronous motor

Country Status (1)

Country Link
JP (1) JPS5518885A (en)

Also Published As

Publication number Publication date
JPS5518885A (en) 1980-02-09

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