JPS6013263A - Active current detector - Google Patents
Active current detectorInfo
- Publication number
- JPS6013263A JPS6013263A JP12017883A JP12017883A JPS6013263A JP S6013263 A JPS6013263 A JP S6013263A JP 12017883 A JP12017883 A JP 12017883A JP 12017883 A JP12017883 A JP 12017883A JP S6013263 A JPS6013263 A JP S6013263A
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- Japan
- Prior art keywords
- current
- signal
- phase
- effective
- 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.)
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Abstract
Description
【発明の詳細な説明】
flE動機に流れる電流の有効電流を検出する有効電流
検出装置に門する。DETAILED DESCRIPTION OF THE INVENTION An effective current detection device for detecting an effective current flowing through a flE motor will now be described.
従来一般に、誘導電動機(以下、モータと称す)のトル
ク制御をVVVF装置を用いて行なうことは公知である
。いま七−夕の静間電圧実効値をv1相電流実効値を工
、力率をcos(θ)で表わすと、モータに入力される
バク−Pは下記(1)式で表わされる。2. Description of the Related Art Conventionally, it is generally known that torque control of an induction motor (hereinafter referred to as a motor) is performed using a VVVF device. Now, if Tanabata's static voltage effective value is expressed as v1 phase current effective value, and the power factor is expressed as cos(θ), then the power input to the motor is expressed by the following equation (1).
p=v’了v・P−CO8(θ) ・−・−・TI)さ
らにモータのトルクTは、回転数をNとすると概略下記
(2)式で表わされる。p=v'了v・P−CO8(θ)・−・−・TI) Further, the torque T of the motor is roughly expressed by the following equation (2), where N is the number of revolutions.
モータのトルク制御を行なう場合IこV/Nを一定値と
するようにVVVF装置の出力電圧を制御することは公
知の方法である。したがって、トルクTは電流実効値に
力率を乗じた値1cos(θ)(これを有効電流という
)に比例する。このことがらモータを所望のトルクもし
くは回転数で運転しようとする場合に、モータの有効J
WL流を検出し、これをフィードバソクイコー号とする
自動促j(1系をイ1り成することは4?文めて効果的
な手段となる。When controlling the torque of a motor, it is a known method to control the output voltage of a VVVF device so that I/V/N is kept at a constant value. Therefore, the torque T is proportional to the value 1cos(θ) (referred to as effective current) obtained by multiplying the effective current value by the power factor. This means that when trying to operate a motor at a desired torque or rotational speed, the motor's effective J
It is an effective means to detect the WL flow and use it as a feeder control signal.
モータの有効電流は次の方法で検出することがル
できる。モータの、(l冗得伯号を5in(ωt)で表
わすと、相電流はTpsln(ωを十θ)て衣わずこと
ができる。ただしil+は相電流の最大値、6は力率角
、(ωリ は電圧位相である。前i1シ相πXEiE信
号を便宜的に第1の電圧位相信号と称し、この相の電流
を第1の電す
流信号と称することにある。The effective current of the motor can be detected in the following way. If the motor is expressed as 5 inches (ωt), the phase current can be changed by Tpsln (ω is 10θ). However, il+ is the maximum value of the phase current, and 6 is the power factor angle. , (ω is the voltage phase. The previous i1 phase πXEiE signal is conveniently referred to as a first voltage phase signal, and the current of this phase is referred to as a first current signal.
次に第1のtχ電圧位相号に対して900の位相差を壱
する2ir、2の電圧位相信号をcoa(ωt)で表わ
し、第1の電流信号に対して900の位相差を有する第
2のifj vli;信号をIpcos(ωt+りで表
わ10以上、4 ;1Iijの1r1号を用いC第1の
電圧位相信号とm lのl’ffr tlflL IF
r号、また第2の電圧位相信号と第2の電流信りとをそ
れぞれ乗釣し、さらにお互を加えることで、下lie
(3)式で表わされるごとく電流最大値に力率を果した
値が得られる。Next, the voltage phase signal of 2ir, 2 which has a phase difference of 900 with respect to the first tχ voltage phase signal is expressed as coa (ωt), and the second voltage phase signal which has a phase difference of 900 with respect to the first current signal is expressed as coa(ωt). ifj vli; The signal is expressed as Ipcos (ωt + 10 or more, 4 ; Using 1r1 of 1Iij, C first voltage phase signal and m l'ffr tlflL IF
By multiplying the second voltage phase signal and the second current signal and adding them together, the lower lie
As expressed by equation (3), a value obtained by multiplying the maximum current value by the power factor is obtained.
5in(ωす(IF!’in(ωを十り月十cos(ω
す(iPcos(ωt−M1月= Ip cos (0
) ・・・・・・・・・・・・(3)また前述した電流
実効値工はI=IP/σ の間係があるため、上記(3
)式で得られる値は有効電流に比例する値である。した
がって以下ip Co5(θ)を有効電流と称する。5in(ωsu(IF!'in(ω)
(iP cos (ωt-M January = Ip cos (0
) ・・・・・・・・・・・・(3) Also, since the above-mentioned effective current value calculation has the relationship of I=IP/σ, the above-mentioned (3
) is a value proportional to the effective current. Therefore, ip Co5(θ) is hereinafter referred to as an effective current.
具体的に有効電流を検出する手段について、三相交流を
出力するvvvp i iを例にとり説明する。The means for specifically detecting the effective current will be explained by taking as an example vvvp i i which outputs three-phase alternating current.
第1図はVVVF装置に適用された従来の有効電流検出
装置を示すブロック図であり、図中、1はモータ、2は
インバータ装置、3は電流検出器、4は電圧指令発生器
、5は発振器である。6は有効電流検出装置を示し、7
はカウンタ、8.9は正弦波発生器、lOは2II!I
I変換器、 11.12は乗算器、13は加算器である
。93は相回転信号、94は相電流信号の切換スイッチ
、200は周波数指令を示す。FIG. 1 is a block diagram showing a conventional active current detection device applied to a VVVF device, in which 1 is a motor, 2 is an inverter device, 3 is a current detector, 4 is a voltage command generator, and 5 is a It is an oscillator. 6 indicates an effective current detection device; 7
is a counter, 8.9 is a sine wave generator, and lO is 2II! I
I converter, 11.12 is a multiplier, and 13 is an adder. Reference numeral 93 indicates a phase rotation signal, 94 a changeover switch for a phase current signal, and 200 a frequency command.
第1図において、周波数指令200により発振器5はv
vvp装置の出力周波数の整数倍の周波数のパルス列を
発生ずる。同時に周波数指令200は電圧指令発生器4
に入力されて周波数に比例する電圧をインバータ装置2
に指令する。発振器5の出力パルス列はカウンタ7に入
力される。カウンタ7に入力される。カウンタ7は入力
パルス列を計数し、VVVF装置の出力周波数の1周期
の長さに相当する値に達すると、計数値を零にするよう
動作する。よってインバータ装置2がこのカウンタ7の
動作に同期して重圧波形を出力することにより、このf
f+数値がVVVF装血の出力電圧の位相に対応する値
となることは容易に推察できるはずである。カウンタ7
は出力信号70に計数値を出力し、これを正弦波リレ生
器8および正弦波発生器9に与える。正弦波発生器8.
9は正弦波波形の波高値を0己憶しているjn211+
V ”、’r子で411成されており、入力されるカウ
ンタ7の計数値を位相イバ号と看做して、この谷位相に
対応する正弦波波形を出力する。たたし正弦波発生器9
は、正弦波発生器8に対し90゜の位相差を有する波形
を記憶させておくものとする。すなわち、正弦波発生器
8の出力である正弦波(71号80を5in(ωりで嵌
わすと、正弦波発生器9の出力である正弦波信号90は
coS(ωt)で表わされるものとづ−る。また5in
(ωt)を第1の電圧位相信号と称し、cos(ωt)
を第2の電圧位相信号と称することとする。In FIG. 1, the frequency command 200 causes the oscillator 5 to
A pulse train having a frequency that is an integral multiple of the output frequency of the vvp device is generated. At the same time, the frequency command 200 is generated by the voltage command generator 4.
The voltage proportional to the frequency is input to the inverter device 2.
command. The output pulse train of the oscillator 5 is input to the counter 7. It is input to counter 7. The counter 7 counts the input pulse train, and when it reaches a value corresponding to the length of one cycle of the output frequency of the VVVF device, it operates to make the count value zero. Therefore, by outputting a heavy pressure waveform in synchronization with the operation of this counter 7, the inverter device 2
It should be easy to infer that the f+ value corresponds to the phase of the output voltage of the VVVF blood supply. counter 7
outputs the count value as an output signal 70, which is applied to the sine wave relay generator 8 and the sine wave generator 9. Sine wave generator8.
9 is jn211+ which remembers the peak value of the sine wave waveform.
411 is formed by V'' and 'r, and the input count value of the counter 7 is regarded as a phase error signal, and a sine wave waveform corresponding to this valley phase is output. Vessel 9
Assume that the sine wave generator 8 stores a waveform having a phase difference of 90°. That is, when the sine wave (No. 71 80) which is the output of the sine wave generator 8 is fitted with 5 inches (ω), the sine wave signal 90 which is the output of the sine wave generator 9 is expressed as coS (ωt). Zuru.Mata 5in
(ωt) is called the first voltage phase signal, and cos(ωt)
will be referred to as the second voltage phase signal.
電流検出器3はモータ1の各相電流を検出するTπ十〇
で表わされるものである。電流信号31を基準にとり第
1の電流信号と呼ぶと、2軸変換器lOは他の2相の電
流信号32および33を用いて、第1の電流信号に対し
90’の位相差を有する!< 20)電流信号を作り出
す。具体的には下記(4)式のごとく電流信号33から
電流信号32を減nしl//T倍するO
鴫ll p aln (ωt+÷π+リーIp sin
(a+t−÷π→−θ))== Ip CO8(ωを
十〇) ・・・・・・・(4)2軸変換器lOの出力は
、第1の電流信号101と第2の電流信号102で表わ
す。The current detector 3 detects each phase current of the motor 1 and is expressed by Tπ10. Taking the current signal 31 as a reference and calling it the first current signal, the two-axis converter IO uses the other two-phase current signals 32 and 33 and has a phase difference of 90' with respect to the first current signal! <20) Create a current signal. Specifically, as shown in equation (4) below, the current signal 32 is subtracted from the current signal 33 by n and multiplied by l//T.
(a+t-÷π→-θ)) == Ip CO8 (ω is 10) (4) The output of the two-axis converter lO is the first current signal 101 and the second current It is represented by signal 102.
以上のごとくにして得られる4種のイハ号を用いて(3
)式で表わされる演算を実施すれば、モータlに流れる
有効電流が得られる。この演rf、は釆n器11.12
および加n器13で行なわれる。乗算器11でnXlの
電圧位相信号80すなわち5in(ωりと、第1の電流
信号101すなイ)ちlp sin (ωt+θ)が乗
算され、乗算器12で8112の電圧位相信号90すな
わちC05(ωりと、第2の電流信号102すなわちI
p Co5(ωを十〇)が乗3114されて、それぞれ
の演算結果110と120が加算器13で加算されると
有効電流結果130にIpcos(θ)が得られる。Using the four types of Iha obtained as described above, (3
), the effective current flowing through the motor l can be obtained. This performance rf is 11.12
and an adder 13. The multiplier 11 multiplies the voltage phase signal 80 of nXl, that is, 5in (ω and the first current signal 101), that is, lp sin (ωt+θ), and the multiplier 12 multiplies the voltage phase signal 90 of 8112, that is, C05 ( ω, the second current signal 102 or I
When p Co5 (ω is 10) is multiplied 3114 and the respective calculation results 110 and 120 are added by the adder 13, Ipcos(θ) is obtained as the effective current result 130.
いまモータlのhh方向を反転させるべく、相回転信号
93に信号を与えてVVVF’装置の出力する変流低圧
の相回転方向を変えると、電流信′@31を基準に考え
ると電流(8号31に対する電流信号32と33の関係
が反転する。このため2軸変換器lOの出力信号は、下
記(5)式で表わされるごとく極性が反転する。Now, in order to reverse the hh direction of the motor l, if a signal is given to the phase rotation signal 93 to change the phase rotation direction of the variable current low voltage output from the VVVF' device, the current (8 The relationship between current signals 32 and 33 with respect to No. 31 is reversed.Therefore, the polarity of the output signal of the two-axis converter IO is reversed as expressed by the following equation (5).
7(Ip ’I I n (0)l ” π十〇)−I
p sln (ωt+ 、 π+6 ) )= −Ip
Co5(ωを十〇) ・・・・・・・・・(5)この
まま有効1に流をめる演nを実施すると、演n K1’
j呆は−Ip cos (2ωt+りとなり正しい有効
電流の値がイ)1ら札ない。7(Ip 'I I n (0)l'' π10)-I
p sln (ωt+, π+6)) = −Ip
Co5 (ω is 10) ・・・・・・・・・(5) If we carry out the operation n that reduces the flow to effective 1, the operation n K1'
j is -Ip cos (2ωt+), so the correct effective current value is 1).
vvvi;’ i置の出力する交流電圧の相回転を反転
させても有効電流を正しく検出する手段きして従来考え
られていた方法は、vvvp装置が相回転を反転させる
と同時に電流信号32と電流信号33を切換スイッチ9
4により切換える方法である。しかし、現在の電子回路
技術では高い信頼性を有する切4チ)スイッチ94を装
置の大型化をせずに実現することは困難である。vvvi;' The conventionally considered method of correctly detecting the active current even if the phase rotation of the alternating current voltage output by the i position is reversed is to Switch 9 to change current signal 33
4. This is a method of switching. However, with current electronic circuit technology, it is difficult to realize a highly reliable on/off switch 94 without increasing the size of the device.
本発明は上述のような点に銑みなされたもので。The present invention has been made with the above points in mind.
切換スイッチを用いることなく、相回転を変更したとき
も有効電流を正しく検出する有効nLA検出装置を提供
するものである。以下、本発明を実施例図面にもとづい
て説明する。An object of the present invention is to provide an effective nLA detection device that correctly detects effective current even when changing phase rotation without using a changeover switch. Hereinafter, the present invention will be explained based on the drawings of the embodiments.
第2図は本発明による有効電流検出装置の一奥施例を示
すブロック図である。第2図においてへ31図と同一符
号で表わされるものは同一の1能を有するものである。FIG. 2 is a block diagram showing a further embodiment of the effective current detection device according to the present invention. Components in FIG. 2 denoted by the same reference numerals as those in FIG. 31 have the same functions.
本発明において正弦波発生器92は、相回転信号93に
応じて正弦波信号の極性を反転して出力が得られるよう
にしである。カウンタ7は従来例の第1図と同様にVV
VF装置の出力周波数の1周JpJを等間隔に分割して
計数するものである。いま仮に1周期を256分割する
ものとする。従来の区弦波発生器9ではカウンタ7の計
数値は0から255に対応してcos(ωt)を出力す
るように417成された。本発明による正弦波発生器9
2に力いCは、モータ1の正転方向に対し相回転信号9
3を“0°で受取り、このときの出力90は従来と同様
、カウンタ7のN1数値0から255に対しcos(ω
t)を得る。しかし、モータlの逆転方向に対し相回転
に(−@ 93を“loとrること4こより、正弦波i
生器92はカウンタ7のn1故値を例えは1000を加
算されたものとじてL″d取るようにする。そして正弦
波発生器92を1000から1255の計数値に対して
は−C05(ωりを出力するように11′1成すること
により、カウンタ7のfit数1直が0から255であ
っても相回転信号93が“loで逆転を表わす場合は、
第2の電圧位相信号90は−cos (ωt)が得られ
る◎したがって本発明は前記(5)式で表わされるごと
< V V V’ F 焦に:(の出力する相回転方向
を反転することにより生じる絹2の電流信号のM&性の
変化を、第2の電圧位相信号の極性を反転させることで
打消し、常に正しく有効電流が検出できる。In the present invention, the sine wave generator 92 is configured to invert the polarity of the sine wave signal according to the phase rotation signal 93 to obtain an output. The counter 7 is VV as in the conventional example shown in FIG.
One round JpJ of the output frequency of the VF device is divided into equal intervals and counted. Assume now that one cycle is divided into 256 parts. In the conventional square wave generator 9, the count value of the counter 7 is set to 417 so as to output cos(ωt) corresponding to values from 0 to 255. Sine wave generator 9 according to the invention
2, C is the phase rotation signal 9 for the forward rotation direction of the motor 1.
3 is received at “0°, and the output 90 at this time is cos(ω
t) is obtained. However, in the phase rotation with respect to the reverse direction of the motor l (-@ 93 is "lo" and r), the sine wave i
The generator 92 takes the value of n1 of the counter 7 as L″d, for example, by adding 1000.Then, the sine wave generator 92 takes −C05(ω By configuring 11'1 so as to output a value of
The second voltage phase signal 90 is -cos (ωt) ◎ Therefore, the present invention reverses the output phase rotation direction of < V V V' F as expressed by the above equation (5) By reversing the polarity of the second voltage phase signal, the change in the M& characteristic of the current signal of the silk 2 caused by this is canceled out, and the effective current can always be detected correctly.
このように本発明による有効電流の検出手段は、検出装
置に切換スイッチを用いてないため、枦めて信頼性の高
い有効電流検出装置を提供できるものである。As described above, since the effective current detection means according to the present invention does not use a changeover switch in the detection device, it is possible to provide a highly reliable effective current detection device.
さらに、本発明の方法はs Ipsln(θ)で表わさ
れる無効電流の検出についても応用可能であり、下記(
b)式で表わされる演算を実施ずれは無*’ @ mt
が得られる。Furthermore, the method of the present invention can also be applied to the detection of reactive current represented by s Ipsln (θ), and the following (
b) There is no deviation in performing the operation expressed by the formula *' @ mt
is obtained.
C08(ωt)(Ipain(ωを十〇))−sin(
ωt ) (1pcO8(ωを十θ月= Ip sin
(θ) −==−(6)そして相回転方向が反転した
場合は、M2の電圧信号と第2の電圧位相信号の極性を
反転さけるため、演n結果に一1psjnθが得られる
。よってこれをもう一度、極性を反転することにより正
しい無効電流を得ることができる。C08(ωt)(Ipain(ω is 10))−sin(
ωt ) (1pcO8(ω = Ip sin
(θ) −==−(6) When the phase rotation direction is reversed, in order to avoid reversing the polarity of the voltage signal of M2 and the second voltage phase signal, −1 psjnθ is obtained as the result of the operation n. Therefore, by reversing the polarity again, the correct reactive current can be obtained.
また%2軸変換器10についてもモータlの3相電流を
全て検出する必要はなく、例えば1o、流信弓31と電
流信号32の2相分でもよ<、′成流iFs号33は前
記2相から演算でめることも可能であることはdうまで
もない。Also, for the two-axis converter 10, it is not necessary to detect all the three-phase currents of the motor l; for example, it is also possible to detect two phases of the current signal 1o, the current signal 31, and the current signal 32. It goes without saying that it is also possible to calculate from two phases.
i1図はvvvi;’装置に適用された従来の有効電流
検出装置を示ずプ四ツク図 fjl、 2図は本発明に
よる有効rに流検出装置の一実施例を示すブロック図で
ある。
l・・・・・・誘導N、#機、2・・・・・インバータ
′装置、3・・・・・11C流検出器、4・・・・・・
11を圧指令発生器、5・・・・発振器、6・・・・有
効電流検出装置、7 カランタ、8,9.92・・・・
・・正弦波発生器、10・・・・・・2軸変換器、II
、12・・・・乗n器、 13−・・・加算器、93・
相@転信号、94・・・・相電流信号の切狼スイッチ
、200・・・・・・周波数指令。
特許出Aq人
東洋↑九機製造株式会社
代表者 土 井 厚
第 1図
第2 図Fig. 1 is a block diagram showing a conventional effective current detection device applied to a vvvi;'device; Fig. 2 is a block diagram showing an embodiment of an effective current detection device according to the present invention. l...Induction N, # machine, 2...Inverter' device, 3...11C flow detector, 4...
11 is a pressure command generator, 5... oscillator, 6... effective current detection device, 7 caranta, 8, 9.92...
...Sine wave generator, 10...Two-axis converter, II
, 12...N multiplier, 13-...Adder, 93...
Phase @ change signal, 94... Phase current signal cut-off switch, 200... Frequency command. Patent Author: Toyo↑Kyuki Seizo Co., Ltd. Representative Atsushi Doi Figure 1 Figure 2
Claims (1)
のうち基準とする第1の電流信号と、他相の′rIk流
6号を用いて合成されかつ前記第1の電流イi −g−
tこ対し90’の位相差を有する#!2の電流信号と、
前記第1の電流信号の流れる相の電圧位相を表わす第1
のηも圧1i号と、核部1の電圧位相に対して90’の
位相差を有する第2の電圧位相信号の4種の信号を用い
て前記誘導電動機に流れる電流の有効電流を検出する有
効電流検出装置において、前記多相父R電源装置の出力
相回転方向に応じて011記紹2の↑)を正位相信号の
極性を反転させて有効電流を演1゛1.せしめるように
構成したことを特徴とするイi効電流検出装置。The first current signal is synthesized using the reference first current signal among the phase currents of the induction motor connected to the multiphase or current rI device, and the 'rIk flow No. 6 of the other phase, and the first current i -g-
#! having a phase difference of 90' with respect to t! 2 current signal,
a first current signal representing a voltage phase of a phase through which the first current signal flows;
η also detects the effective current of the current flowing through the induction motor using four types of signals: pressure No. 1i and a second voltage phase signal having a phase difference of 90' with respect to the voltage phase of core section 1. In the effective current detection device, the active current is calculated by inverting the polarity of the positive phase signal (↑) of 011, Introduction 2, according to the output phase rotation direction of the multi-phase father R power supply device. An effective current detection device characterized in that it is configured to
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12017883A JPS6013263A (en) | 1983-07-04 | 1983-07-04 | Active current detector |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12017883A JPS6013263A (en) | 1983-07-04 | 1983-07-04 | Active current detector |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6013263A true JPS6013263A (en) | 1985-01-23 |
| JPH0145031B2 JPH0145031B2 (en) | 1989-10-02 |
Family
ID=14779848
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP12017883A Granted JPS6013263A (en) | 1983-07-04 | 1983-07-04 | Active current detector |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6013263A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0534580U (en) * | 1991-10-16 | 1993-05-07 | 日新電機株式会社 | Power system measuring device |
-
1983
- 1983-07-04 JP JP12017883A patent/JPS6013263A/en active Granted
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0534580U (en) * | 1991-10-16 | 1993-05-07 | 日新電機株式会社 | Power system measuring device |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0145031B2 (en) | 1989-10-02 |
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