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JP4239088B2 - Wind power generation equipment - Google Patents
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JP4239088B2 - Wind power generation equipment - Google Patents

Wind power generation equipment Download PDF

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JP4239088B2
JP4239088B2 JP2003422325A JP2003422325A JP4239088B2 JP 4239088 B2 JP4239088 B2 JP 4239088B2 JP 2003422325 A JP2003422325 A JP 2003422325A JP 2003422325 A JP2003422325 A JP 2003422325A JP 4239088 B2 JP4239088 B2 JP 4239088B2
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power generation
wind power
capacitor
generation facility
induction machine
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JP2005184990A (en
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親志 中沢
要祐 中西
敏之 太田
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Fuji Electric Co Ltd
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Fuji Electric Systems Co Ltd
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    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/70Wind energy
    • Y02E10/72Wind turbines with rotation axis in wind direction

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Description

本発明は、風車に連結された巻線形誘導機とその二次励磁を行うコンバータと高調波電流除去用のコンデンサとを備えた風力発電設備に関し、特に、前記コンデンサ及び連系系統のインダクタンスによる並列共振を抑制可能とした風力発電設備に関するものである。   The present invention relates to a wind power generation facility including a winding induction machine connected to a wind turbine, a converter for performing secondary excitation thereof, and a capacitor for removing harmonic current, and in particular, paralleling by the inductance of the capacitor and the interconnection system. The present invention relates to a wind power generation facility capable of suppressing resonance.

図3は、上位の電力系統に連系されるこの種の風力発電設備の従来技術を示している。なお、この構成は、後述する非特許文献1のFig.5に記載されているものである。
図3において、10は風車、20はギアボックス、30は巻線形誘導機、40は連系変圧器、50は二次励磁装置(周波数変換装置)としてのコンバータ、51は順変換部(コンバータ部)、52は逆変換部(インバータ部)、53は直流リンク部のコンデンサ、61はフィルタ用(高調波電流除去用)のコンデンサ、62はリアクトル、100は電力系統、101は引込ケーブルを示している。
FIG. 3 shows the prior art of this type of wind power generation facility interconnected to a higher power system. This configuration is described in FIG. 5 of Non-Patent Document 1 described later.
In FIG. 3, 10 is a windmill, 20 is a gear box, 30 is a winding induction machine, 40 is an interconnection transformer, 50 is a converter as a secondary excitation device (frequency conversion device), 51 is a forward conversion unit (converter unit) ), 52 is a reverse conversion unit (inverter unit), 53 is a DC link capacitor, 61 is a filter capacitor (for removing harmonic current), 62 is a reactor, 100 is a power system, and 101 is a lead-in cable. Yes.

上記構成において、誘導機30の一次巻線(固定子巻線)は引込ケーブル101及び連系変圧器40を介して電力系統100に接続され、また、誘導機30の二次巻線(回転子巻線)はコンバータ50の逆変換部52にスリップリングを介して接続されている。   In the above configuration, the primary winding (stator winding) of the induction machine 30 is connected to the power system 100 via the lead-in cable 101 and the interconnection transformer 40, and the secondary winding (rotor) of the induction machine 30. Winding) is connected to the reverse conversion part 52 of the converter 50 via a slip ring.

図4は、コンバータ50の制御回路の一例として非特許文献1のFig.9に記載されている制御ブロック図である。
図4において、電流検出器501、電圧検出器502により検出した誘導機30の一次側の電流I、電圧Vは電力演算器503に入力され、有効電力P及び無効電力Qが検出される。電力調節器504,505は各電力の指令値P,Qと検出値P,Qとのそれぞれの偏差がゼロになるように調節動作し、これらの出力が電流制御回路506に入力される。
4 is a control block diagram described in FIG. 9 of Non-Patent Document 1 as an example of the control circuit of the converter 50.
In FIG. 4, the current I N and voltage V S on the primary side of the induction machine 30 detected by the current detector 501 and the voltage detector 502 are input to the power calculator 503, and the active power P and the reactive power Q are detected. . The power regulators 504 and 505 perform an adjustment operation so that each deviation between the command values P * and Q * of each power and the detected values P and Q becomes zero, and these outputs are input to the current control circuit 506. .

電流検出器507により検出された誘導機30の二次巻線32の電流Iは、三相/二相変換器508によりd軸、q軸成分に分解され、これらの各成分IRd,IRqが電流制御回路506に入力される。同様に、電流検出器511により検出された誘導機30の一次巻線31の電流Iは三相/二相変換器509によりd軸成分,q軸成分に分解され、これらの各成分ISd,ISqも電流制御回路506に入力される。
電流制御回路506では、調節器504,505の出力と上記IRd,IRq,ISd,ISqとに基づいて、d軸電圧指令VRd及びq軸電圧指令VRqを演算し出力する。
Current I R of the current detector 507 induction machine 30 detected by the secondary winding 32, d-axis by a three-phase / two-phase converter 508, is broken down into q-axis component, each of these components I Rd, I Rq is input to the current control circuit 506. Similarly, d-axis component by the current I S is a three-phase / two-phase converter 509 of the primary winding 31 of the induction machine 30 detected by the current detector 511 is decomposed into q-axis component, each of these components I Sd , I Sq are also input to the current control circuit 506.
The current control circuit 506 calculates and outputs the d-axis voltage command V Rd and the q-axis voltage command V Rq based on the outputs of the regulators 504 and 505 and the above I Rd , I Rq , I Sd , and I Sq .

更に、誘導機30の一次巻線31の電圧Vは角度演算器510にも入力されており、この角度演算器510により演算された電圧ベクトルの角度φVSと、誘導機30の回転子の位置検出器512による検出角度φとの差(φVS−φ)が三相/二相変換器508、二相/三相変換器513に入力されている。なお、前記角度φVSは三相/二相変換器509にも入力されている。 Further, the voltage V S of the primary winding 31 of the induction machine 30 to the angle calculator 510 is inputted, the angle phi VS of the voltage vector calculated by the angle calculator 510, the induction machine 30 of the rotor A difference (φ VS −φ R ) from the detection angle φ R by the position detector 512 is input to the three-phase / two-phase converter 508 and the two-phase / three-phase converter 513. The angle φ VS is also input to the three-phase / two-phase converter 509.

二相/三相変換器513では、各軸の電圧指令VRd,VRq及び角度(φVS−φ)に基づいて、三相の電圧指令V を生成し、PWM回路514に出力する。PWM回路514では、電圧指令V をキャリアと比較することにより、逆変換部52に対するPWMパルスを生成し、IGBT等のスイッチング素子を駆動して誘導機30の二次巻線32に所定周波数及び大きさを持つ交流電圧を供給する。 The two-phase / three-phase converter 513 generates a three-phase voltage command V R * based on the voltage commands V Rd and V Rq and the angle (φ VS −φ R ) of each axis, and outputs it to the PWM circuit 514. To do. The PWM circuit 514 generates a PWM pulse for the inverse conversion unit 52 by comparing the voltage command V R * with the carrier, drives a switching element such as an IGBT, and supplies a predetermined frequency to the secondary winding 32 of the induction machine 30. And an alternating voltage having a magnitude is supplied.

また、電圧検出器516により検出したコンバータ50の直流リンク電圧VDCが、順変換部51側のPWM回路517に入力されている。更に、電流検出器515により検出された順変換部51の交流電流IGCが、前記電圧V,VDCと共にPWM回路517に入力されている。PWM回路517では、これらの電圧V,VDC及び電流IGCに基づいてPWMパルスを生成し、順変換部51のスイッチング素子を駆動して直流リンク電圧VDCを所定値に制御する。 Further, the DC link voltage VDC of the converter 50 detected by the voltage detector 516 is input to the PWM circuit 517 on the forward conversion unit 51 side. Further, the alternating current I GC of the forward conversion unit 51 detected by the current detector 515 is input to the PWM circuit 517 together with the voltages V S and V DC . The PWM circuit 517 generates a PWM pulse based on the voltages V S and V DC and the current I GC and drives the switching element of the forward conversion unit 51 to control the DC link voltage V DC to a predetermined value.

この風力発電設備では、周知の二次励磁制御により、風速、風向の変動等によって回転子の速度が変動し、誘導機30の出力が変動した場合でも、出力が常に指令値に一致するように誘導機30の二次電圧すなわち回転子速度を制御する動作が行われるため、回転子の速度変動を抑制して安定した運転を継続することができる。   In this wind power generation facility, the known secondary excitation control causes the rotor speed to fluctuate due to fluctuations in wind speed, wind direction, etc., so that the output always matches the command value even when the output of the induction machine 30 fluctuates. Since the operation of controlling the secondary voltage of the induction machine 30, that is, the rotor speed, is performed, the speed fluctuation of the rotor can be suppressed and the stable operation can be continued.

S.Muller, M.Deicke, Rik W. De Doncker,“Doubly fed induction generator systems for Wind turbines ”, Industry Applications Magazine, IEEE , Volume: 8 Issue: 3 , May-June 2002, p.26-p.32S. Muller, M. Deicke, Rik W. De Doncker, “Doubly fed induction generator systems for Wind turbines”, Industry Applications Magazine, IEEE, Volume: 8 Issue: 3, May-June 2002, p.26-p.32

さて、前記コンバータ50を構成する順変換部51及び逆変換部52をPWM(パルス幅変調)制御する場合、キャリア周波数に相当する高調波電流が発生することが知られており、図4の従来技術では、上記高調波電流を除去するためにフィルタ用のコンデンサ61が設けられている。
一方、この種の風力発電設備は、ノイズや電圧変動に比較的強い電源(配電線長が短い電源)に連系されることを仮定して構成されているため、上記フィルタの設計においてはコンバータ50からの高調波電流を除去することのみを考慮すればよい。
Now, it is known that when the forward conversion unit 51 and the reverse conversion unit 52 constituting the converter 50 are controlled by PWM (pulse width modulation), a harmonic current corresponding to the carrier frequency is generated. In the technology, a filter capacitor 61 is provided to remove the harmonic current.
On the other hand, this type of wind power generation equipment is configured on the assumption that it is connected to a power source that is relatively resistant to noise and voltage fluctuations (a power source having a short distribution line length). Only removing the harmonic current from 50 need be considered.

しかしながら、風力発電設備を比較的弱い電源(配電線長が長い電源)に連系する場合には、高調波電流除去用のコンデンサ61と系統インダクタンス(連系変圧器40の漏れインダクタンスを含む)とによる並列共振現象を考慮する必要があり、この共振周波数における系統電圧の振動が発生し易い条件に置かれることとなる。   However, when the wind power generation facility is connected to a relatively weak power source (a power source having a long distribution line length), the harmonic current removing capacitor 61 and the system inductance (including the leakage inductance of the interconnection transformer 40) It is necessary to consider the parallel resonance phenomenon due to the above, and the system voltage is likely to be oscillated at the resonance frequency.

ここで、図5は、従来の風力発電設備が比較的弱い電源に連系された場合の等価回路を示している。
図5において、Eは電圧源で表現した上位系統100(無限大母線)の電圧、r,L,Cは上位系統100の配電線の抵抗、インダクタンス、静電容量、r,L,Cは引込ケーブル101の抵抗、インダクタンス、静電容量、LTRは連系変圧器40の漏れインダクタンス、Cは高調波電流除去用コンデンサ61の静電容量、Gは電流源で表現した誘導機30を示す。
図5から明らかなように、コンデンサ61の静電容量Cは、インダクタンスL,L,LTRの直列回路と共に並列共振回路を構成している。
Here, FIG. 5 shows an equivalent circuit when the conventional wind power generation facility is linked to a relatively weak power source.
In FIG. 5, E is the voltage of the upper system 100 (infinite bus) expressed by a voltage source, r 1 , L 1 , C 1 are the resistance, inductance, capacitance, r 2 , L of the distribution line of the upper system 100. 2, C 2 is the resistance of the drop cable 101, inductance, capacitance, L TR is the leakage inductance of interconnection transformer 40, C h is the capacitance of the harmonic current eliminating capacitor 61, G is represented by a current source An induction machine 30 is shown.
As is apparent from FIG. 5, the capacitance C h of the capacitor 61 constitute a parallel resonance circuit with the series circuit of the inductance L 1, L 2, L TR .

いま、系統に接続されている負荷の変動、他の風力発電設備の停止・起動による外乱が発生すると、上記並列共振回路の共振周波数による電圧振動が励起される。
その結果、図6(a)に示すように、誘導機30から出力される基本波電圧に共振周波数の振動電圧が重畳されて運転が不安定になるおそれがあり、最悪の場合には周波数継電器等の保護機器が動作して風力発電設備の運転が停止してしまうという問題があった。なお、図6(a)において横軸は時間、縦軸は単位法表示した電圧の振幅である。
更に、上述した電圧の振動は、系統100に接続された機器に種々の悪影響を与えるという問題があった。
Now, when fluctuations in the load connected to the system and disturbance due to stop / start of other wind power generation facilities occur, voltage oscillation due to the resonance frequency of the parallel resonance circuit is excited.
As a result, as shown in FIG. 6 (a), there is a possibility that the oscillation voltage of the resonance frequency is superimposed on the fundamental wave voltage output from the induction machine 30, and the operation becomes unstable. In the worst case, the frequency relay There was a problem that the operation of the wind power generation equipment would be stopped due to the operation of the protective equipment. In FIG. 6A, the horizontal axis represents time, and the vertical axis represents voltage amplitude expressed in the unit method.
Furthermore, the above-described voltage oscillation has a problem in that various adverse effects are caused on the devices connected to the system 100.

ここで、図6(b)は風力発電設備の誘導機30から見たインピーダンスの大きさ(上段)及び位相角(下段)を示すもので、横軸は周波数である。この図から、約1.3[kHz]付近のインピーダンスが大きくなっており、前述した外乱によって並列共振が生じ、その共振周波数(約1.3[kHz])における電圧振動が励起されていることがわかる。   Here, FIG. 6B shows the magnitude (upper stage) and phase angle (lower stage) of the impedance viewed from the induction machine 30 of the wind power generation facility, and the horizontal axis is the frequency. From this figure, the impedance around 1.3 [kHz] is large, parallel resonance occurs due to the above-mentioned disturbance, and voltage oscillation at the resonance frequency (about 1.3 [kHz]) is excited. I understand.

そこで本発明は、高調波電流除去用のコンデンサに起因する並列共振現象による出力電圧の不安定性を抑制して、安定した運転を可能する風力発電設備を提供しようとするものである。   Therefore, the present invention aims to provide a wind power generation facility that can suppress the instability of the output voltage due to the parallel resonance phenomenon caused by the harmonic current removing capacitor and enables stable operation.

上記課題を解決するために、請求項1に記載した発明は、風車により駆動され、かつ発生電力を連系系統に供給する巻線形誘導機と、この巻線形誘導機を二次励磁するコンバータと、このコンバータの運転により発生する高調波電流を除去するためのコンデンサとを備えた風力発電設備において、
前記コンデンサ及び系統インダクタンスによる並列共振を抑制するために、以下の数式で与えられる値Rを持つ抵抗を、前記コンデンサに直列に接続したものである。
=2ζ√(X/Y
(ここで、Xは風力発電設備の出力電圧の基本波周波数における誘導機から見た系統リアクタンス[pu]、Yは同じく基本波周波数における前記コンデンサのサセプタンス[pu]、ζは減衰係数)
In order to solve the above-mentioned problem, the invention described in claim 1 is a winding induction machine that is driven by a windmill and supplies generated power to the interconnection system, and a converter that performs secondary excitation of the winding induction machine. In a wind power generation facility equipped with a capacitor for removing harmonic current generated by the operation of this converter,
In order to suppress parallel resonance by the capacitor and the system inductance, a resistor having a value R h given by the following equation, which are connected in series with said capacitor.
R h = 2ζ√ (X 0 / Y 0 )
(Where X 0 is the system reactance [pu] as seen from the induction machine at the fundamental wave frequency of the output voltage of the wind power generation facility, Y 0 is the susceptance [pu] of the capacitor at the fundamental wave frequency, and ζ is the attenuation coefficient)

請求項2に記載した発明は、請求項1に記載した風力発電設備において、前記減衰係数ζが約0.01〜約0.03であることを特徴とする。   The invention described in claim 2 is the wind power generation facility described in claim 1, wherein the attenuation coefficient ζ is about 0.01 to about 0.03.

本発明によれば、高調波電流吸収用のコンデンサに直列に接続した抵抗により、前記コンデンサと系統インダクタンスとによる並列共振が抑制され、風力発電設備の出力電圧に共振周波数成分が重畳されることはない。これにより、風力発電設備を停止させずに安定した運転を継続することができ、また、系統に接続された機器に対する悪影響を未然に防止することができる。   According to the present invention, the parallel resonance caused by the capacitor and the system inductance is suppressed by the resistor connected in series with the harmonic current absorbing capacitor, and the resonance frequency component is superimposed on the output voltage of the wind power generation facility. Absent. Thereby, stable operation can be continued without stopping the wind power generation facility, and adverse effects on the devices connected to the system can be prevented.

以下、図に沿って本発明の実施形態を説明する。
図1は、ノイズや電圧変動に比較的弱い電源に連系された本発明に係る風力発電設備の等価回路図である。なお、図5と同一の構成要素には同一の参照符号を付して説明を省略し、以下では異なる部分を中心に述べる。
Hereinafter, embodiments of the present invention will be described with reference to the drawings.
FIG. 1 is an equivalent circuit diagram of a wind power generation facility according to the present invention linked to a power source that is relatively weak against noise and voltage fluctuations. Note that the same components as those in FIG. 5 are denoted by the same reference numerals, description thereof is omitted, and different portions will be mainly described below.

図1と図5との比較から明らかなように、この実施形態では、高調波電流除去用コンデンサ61と直列に、抵抗R(その抵抗値もRにて表す)が接続されている。なお、風力発電設備の制御回路としては、例えば図4に示したような制御回路が使用される。 As is apparent from a comparison between FIG. 1 and FIG. 5, in this embodiment, a resistor R h (the resistance value is also represented by R h ) is connected in series with the harmonic current removing capacitor 61. For example, a control circuit as shown in FIG. 4 is used as the control circuit of the wind power generation facility.

図1のように抵抗Rを付加することにより、負荷変動や他の風力発電設備の停止・起動等の外乱が発生した場合でも、コンデンサ61の静電容量CとインダクタンスL,L,LTRの直列回路とによる並列共振現象が抑制され、誘導機30から出力される基本周波数の電圧に共振周波数の電圧が重畳されることはない。このため、周波数継電器等の保護機器が動作して風力発電設備の運転が停止するおそれはなく、安定した運転を継続することができる。 By adding the resistor R h as shown in FIG. 1, even when the disturbance of the stop-start such a load variation or other wind turbines occurs, inductance and capacitance C h of the capacitor 61 L 1, L 2 parallel resonance phenomenon due to a series circuit of L TR is suppressed, there is no possibility that the voltage of the resonance frequency to the voltage of the fundamental frequency output from the induction motor 30 is superimposed. For this reason, there is no possibility that the protection device such as the frequency relay operates and the operation of the wind power generation facility is stopped, and the stable operation can be continued.

図2(a)は、風力発電設備(誘導機30)の出力電圧波形であり、図6(a)と同様に横軸は時間、縦軸は単位法表示した電圧の振幅である。また、図2(b)は、図6(b)と同様に、誘導機30から見たインピーダンスの大きさ(上段)及び位相角(下段)を示しており、横軸は周波数である。
図2(a)から、抵抗Rを付加したことによって並列共振現象が抑制され、出力電圧波形はほぼ基本波成分のみになっていると共に、図2(b)から、共振周波数に相当する約1.3[kHz]におけるインピーダンスの変動も抑制されているのがわかる。
FIG. 2A shows an output voltage waveform of the wind power generation facility (induction machine 30). Like FIG. 6A, the horizontal axis represents time, and the vertical axis represents the voltage amplitude expressed in the unit method. FIG. 2B shows the magnitude (upper stage) and phase angle (lower stage) of the impedance viewed from the induction machine 30 as in FIG. 6B, and the horizontal axis is the frequency.
2 from (a), in parallel resonance phenomenon suppressed by the addition of resistor R h, with the output voltage waveform is substantially made only to the fundamental wave component, from FIG. 2 (b), about equivalent to the resonance frequency It can be seen that impedance fluctuations at 1.3 [kHz] are also suppressed.

ここで、高調波電流除去用コンデンサ61に直列に接続される抵抗Rは、以下の数式1で与えられる値Rであることが望ましい。
[数式1]
=2ζ√(X/Y
上記数式1において、Xは風力発電設備の出力電圧の基本波周波数における誘導機30から見た系統リアクタンス[pu]、Yは同じく基本波周波数における高調波電流除去用コンデンサ61のサセプタンス[pu]、ζは減衰係数(約0.01〜約0.03程度)である。
Here, the resistance R h connected in series to the harmonic current removing capacitor 61 is desirably a value R h given by the following Equation 1.
[Formula 1]
R h = 2ζ√ (X 0 / Y 0 )
In Formula 1, X 0 is the system reactance [pu] viewed from the induction machine 30 at the fundamental frequency of the output voltage of the wind power generation facility, and Y 0 is the susceptance [pu of the harmonic current removing capacitor 61 at the fundamental frequency. ] And ζ are damping coefficients (about 0.01 to about 0.03).

以下に、上述した数式1の導出方法を述べる。
図1における誘導機30の一次巻線電流をI、端子電圧をVとし、抵抗r,r及び静電容量C,Cを無視すると共に、インダクタンスL,L,LTRの合成値(誘導機30から見た系統のインダクタンス)をLとすると、数式2が成り立つ。
[数式2]
/I=(R+s/C)/[s+s(R/L)+(1/LC)]
なお、sはラプラス演算子である。
Hereinafter, a method for deriving Equation 1 will be described.
In FIG. 1, the primary winding current of the induction machine 30 is I G , the terminal voltage is V f , the resistors r 1 and r 2 and the capacitances C 1 and C 2 are ignored, and the inductances L 1 , L 2 , L When the combined value of TR (inductance of the system viewed from the induction machine 30) is L, Expression 2 is established.
[Formula 2]
V f / I G = (R h s 2 + s / C h) / [s 2 + s (R h / L) + (1 / LC h)]
Note that s is a Laplace operator.

ここで、二次振動系の特性方程式を考慮して、数式2におけるR/L=2ζω,1/LC=ω とおくと、数式3が得られ、X=ωL,Y=ωより、前記数式1が得られる。
[数式3]
=2ζ√(L/C )=2ζ√(ωL/ω
なお、ωは非減衰固有振動数(または単に固有振動数)であり、この固有振動数ω及び前記減衰係数ζは、二次振動系の過渡応答特性を決定するパラメータとして良く知られている。
Here, considering the characteristic equation of the secondary vibration system, when R h / L = 2ζω n and 1 / LC h = ω n 2 in Equation 2 , Equation 3 is obtained, and X 0 = ω 0 L , Y 0 = ω 0 Ch , the above formula 1 is obtained.
[Formula 3]
R h = 2ζ√ (L / C h) = 2ζ√ (ω 0 L / ω 0 C h)
Note that ω n is an undamped natural frequency (or simply natural frequency), and the natural frequency ω n and the damping coefficient ζ are well known as parameters for determining the transient response characteristics of the secondary vibration system. Yes.

以上のように、本発明は、特に長距離配電線の系統末端において連系された風力発電設備のごとく、系統インダクタンスと高調波電流除去用のコンデンサとによる並列共振が問題となる風力発電設備に適用することにより、その停止を回避して安定した運転を継続することが可能になる。   As described above, the present invention is particularly suitable for a wind power generation facility in which parallel resonance due to system inductance and a harmonic current removing capacitor is a problem, such as a wind power generation facility interconnected at the system end of a long-distance distribution line. By applying it, it is possible to avoid the stop and continue stable operation.

本発明の実施形態を示す等価回路図である。It is an equivalent circuit diagram showing an embodiment of the present invention. 本発明の実施形態の特性図である。It is a characteristic view of the embodiment of the present invention. 従来技術を示す構成図である。It is a block diagram which shows a prior art. 従来技術の制御ブロック図である。It is a control block diagram of a prior art. 従来技術の等価回路図である。It is an equivalent circuit diagram of a prior art. 従来技術の特性図である。It is a characteristic view of a prior art.

符号の説明Explanation of symbols

10:風車
20:ギアボックス
30:巻線形誘導機
40:連系変圧器
50:コンバータ
51:順変換部(コンバータ部)
52:逆変換部(インバータ部)
53:コンデンサ
61:コンデンサ
62:リアクトル
100:電力系統
101:引込ケーブル
:抵抗
:静電容量
10: Windmill 20: Gear box 30: Winding induction machine 40: Interconnection transformer 50: Converter 51: Forward conversion section (converter section)
52: Inverse conversion unit (inverter unit)
53: Capacitor 61: a capacitor 62: Reactor 100: Power line 101: drop cable R h: resistance C h: capacitance

Claims (2)

風車により駆動され、かつ発生電力を連系系統に供給する巻線形誘導機と、この巻線形誘導機を二次励磁するコンバータと、このコンバータの運転により発生する高調波電流を除去するためのコンデンサとを備えた風力発電設備において、
前記コンデンサ及び系統インダクタンスによる並列共振を抑制するために、以下の数式で与えられる値Rを持つ抵抗を、前記コンデンサに直列に接続したことを特徴とする風力発電設備。
=2ζ√(X/Y
(ここで、Xは風力発電設備の出力電圧の基本波周波数における誘導機から見た系統リアクタンス[pu]、Yは同じく基本波周波数における前記コンデンサのサセプタンス[pu]、ζは減衰係数)
Winding induction machine driven by a windmill and supplying generated power to the interconnection system, a converter for secondary excitation of this winding induction machine, and a capacitor for removing harmonic current generated by the operation of this converter In wind power generation equipment with
In order to suppress parallel resonance due to the capacitor and system inductance, a wind power generation facility characterized in that a resistor having a value R h given by the following equation is connected in series to the capacitor.
R h = 2ζ√ (X 0 / Y 0 )
(Where X 0 is the system reactance [pu] as seen from the induction machine at the fundamental wave frequency of the output voltage of the wind power generation facility, Y 0 is the susceptance [pu] of the capacitor at the fundamental wave frequency, and ζ is the attenuation coefficient)
請求項1に記載した風力発電設備において、
前記減衰係数ζが約0.01〜約0.03であることを特徴とする風力発電設備。
In the wind power generation facility according to claim 1,
The wind power generation facility, wherein the attenuation coefficient ζ is about 0.01 to about 0.03.
JP2003422325A 2003-12-19 2003-12-19 Wind power generation equipment Expired - Lifetime JP4239088B2 (en)

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Publication number Priority date Publication date Assignee Title
KR20230002059A (en) 2021-06-29 2023-01-05 주식회사 히타치하이테크 Inspection device and measurement device

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DE102008017715A1 (en) * 2008-04-02 2009-10-15 Nordex Energy Gmbh Method for operating a wind turbine with a double-fed asynchronous machine and wind turbine with a double-fed asynchronous machine
JP5721645B2 (en) 2012-02-06 2015-05-20 三菱重工業株式会社 Wind turbine generator control device, wind turbine generator, and wind turbine generator control method
CN103378783A (en) * 2012-04-16 2013-10-30 台达电子企业管理(上海)有限公司 Excitation control circuit, excitation control method, and electrical excitation wind power system of excitation control circuit
KR101379246B1 (en) * 2012-08-29 2014-03-28 삼성중공업 주식회사 Grid-connected filter and design method thereof

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20230002059A (en) 2021-06-29 2023-01-05 주식회사 히타치하이테크 Inspection device and measurement device
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