WO2022042158A1 - Mmc small-signal impedance modeling method based on fourier decomposition - Google Patents

Mmc small-signal impedance modeling method based on fourier decomposition Download PDF

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WO2022042158A1
WO2022042158A1 PCT/CN2021/108181 CN2021108181W WO2022042158A1 WO 2022042158 A1 WO2022042158 A1 WO 2022042158A1 CN 2021108181 W CN2021108181 W CN 2021108181W WO 2022042158 A1 WO2022042158 A1 WO 2022042158A1
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mmc
frequency
state
domain
model
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李清
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中国南方电网有限责任公司超高压输电公司检修试验中心
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    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02JCIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
    • H02J3/00Circuit arrangements for ac mains or ac distribution networks
    • H02J3/36Arrangements for transfer of electric power between ac networks via a high-tension dc link
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F17/00Digital computing or data processing equipment or methods, specially adapted for specific functions
    • G06F17/10Complex mathematical operations
    • G06F17/14Fourier, Walsh or analogous domain transformations, e.g. Laplace, Hilbert, Karhunen-Loeve, transforms
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F17/00Digital computing or data processing equipment or methods, specially adapted for specific functions
    • G06F17/10Complex mathematical operations
    • G06F17/16Matrix or vector computation, e.g. matrix-matrix or matrix-vector multiplication, matrix factorization
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F30/00Computer-aided design [CAD]
    • G06F30/20Design optimisation, verification or simulation
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02JCIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
    • H02J3/00Circuit arrangements for ac mains or ac distribution networks
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02JCIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
    • H02J3/00Circuit arrangements for ac mains or ac distribution networks
    • H02J3/01Arrangements for reducing harmonics or ripples
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02JCIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
    • H02J3/00Circuit arrangements for ac mains or ac distribution networks
    • H02J3/24Arrangements for preventing or reducing oscillations of power in networks
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02JCIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
    • H02J3/00Circuit arrangements for ac mains or ac distribution networks
    • H02J3/36Arrangements for transfer of electric power between ac networks via a high-tension dc link
    • H02J2003/365Reducing harmonics or oscillations in HVDC
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02JCIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
    • H02J2203/00Indexing scheme relating to details of circuit arrangements for AC mains or AC distribution networks
    • H02J2203/20Simulating, e g planning, reliability check, modelling or computer assisted design [CAD]
    • 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
    • Y02E40/00Technologies for an efficient electrical power generation, transmission or distribution
    • Y02E40/40Arrangements for reducing harmonics
    • 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
    • Y02E60/00Enabling technologies; Technologies with a potential or indirect contribution to GHG emissions mitigation
    • Y02E60/60Arrangements for transfer of electric power between AC networks or generators via a high voltage DC link [HVCD]

Definitions

  • the invention relates to the technical field of power transmission and distribution of power systems, in particular to an MMC small-signal impedance modeling method based on Fourier decomposition.
  • the modular multilevel converter has the advantages of modular structure, high efficiency, small size, high output waveform quality, easy installation and maintenance, etc., in the high voltage direct current transmission (High Voltage Direct Current, HVDC) ) and asynchronous grid interconnection systems have been widely used.
  • HVDC High Voltage Direct Current
  • MMC-based photovoltaic, wind power and DC transmission systems have also experienced subsynchronous oscillations with a frequency of 20 to 30 Hz. , which seriously affects the safe operation of the system.
  • the structure of MMC is more complex, resulting in a more complex control system than traditional converters.
  • the multi-time scale dynamic control characteristics of MMC and its relationship with the power grid The interaction between them is the main factor leading to the frequent occurrence of system oscillation accidents. Therefore, the stability analysis of the MMC-HVDC system is particularly important.
  • the MMC small-signal model is an important tool for analyzing the stability of MMC-HVDC systems. Because MMC has multiple frequency harmonic components in the bridge arm current and capacitor voltage during steady-state operation, and has typical time-varying nonlinear multi-frequency response characteristics, the modeling methods and linear system analysis methods of traditional power electronic converters are all different. Difficult to apply directly to MMC.
  • the small signal modeling methods for MMC can be roughly divided into two categories: time domain and frequency domain.
  • the time-domain modeling method analyzes the small-signal stability of the system based on eigenvalues and root locus by obtaining the parameter matrix of the system. Although the time-domain modeling method can describe the internal dynamic characteristics of MMC, the modeling process is complex, and it is difficult to explain the complex harmonic coupling problem within the MMC, which has great limitations when applied to the stability analysis of AC and DC systems.
  • the frequency domain analysis method establishes the system frequency domain impedance model, and then uses frequency domain analysis tools such as impedance stability criterion and Bode diagram to study the small-signal stability of the AC and DC systems.
  • the measurement verification is more applicable in the stability analysis of the actual MMC-HVDC system.
  • the methods of frequency domain modeling for MMC mainly include harmonic linearization and Fourier decomposition.
  • the basic idea of multi-harmonic linearization is to inject a small perturbation signal at a specific frequency into the excitation of the system, and deduce the response corresponding to the perturbation frequency in the state variable, so as to obtain a linear model considering the small perturbation component;
  • the small-signal impedance of the system can be obtained by dividing the voltage and current in the system, thereby realizing the analysis of system stability.
  • the harmonic linearization method to model MMC, the process is complicated, which is not conducive to computer programming.
  • the above shortcomings can be overcome when the MMC is modeled by the Fourier decomposition method.
  • the Fourier decomposition method can obtain the small-signal impedance model of MMC by converting the time domain model to the frequency domain, and then performing small disturbance analysis at the steady-state operating point.
  • the modeling process is relatively simple, and it is easy to program and solve, and the model accuracy is higher.
  • the traditional Fourier decomposition method adopts the derivation method for modeling, and does not consider the internal harmonic coupling of the MMC, and the model accuracy still needs to be improved.
  • the present invention provides an MMC small-signal impedance modeling method based on Fourier decomposition, aiming to solve the technical problem that the existing MMC small-signal impedance modeling method is inaccurate, and can make the model It is applied to analyze the stability of the MMC-based HVDC transmission system, and then improve the operational reliability of the MMC-based HVDC transmission system.
  • the technical scheme of the present invention is as follows:
  • the MMC includes three-phase bridge arms corresponding to three-phase alternating current one-to-one, and the three-phase bridge arms are connected in parallel; each phase bridge arm includes an upper bridge arm connected in series and the lower bridge arm, and the upper bridge arm contains N sub-modules connected in series, and the lower bridge arm contains N sub-modules connected in series, including the following steps:
  • Step 1 transform the single-phase branch of the MMC into an average value equivalent circuit, write the basic circuit equation of the MMC, and obtain the mathematical model of the MMC; represent the mathematical model of the MMC in the form of a state space , get the MMC time-domain state-space model
  • A(t), B(t) are the matrices representing the parameters of the MMC circuit
  • x(t) is the selected state variable
  • i c (t) is the phase circulating current
  • i g (t) is the AC side current
  • u(t) is the selected output variable
  • u(t) [U dc ,0,0,u g (t)] T
  • U dc is the DC side voltage
  • ug (t) is the AC side voltage
  • elements X, U, A, B correspond to x(t), u(t), A(t), B(t) in the MMC time-domain state space model, respectively, and Q represents the diagonal of the frequency information matrix;
  • step 3 the steady-state operating point of the MMC is solved on the MMC frequency-domain steady-state model.
  • the complex variable s in the MMC frequency-domain steady-state model tends to zero.
  • Step 4 the small perturbation analysis method is applied to the MMC time domain state space model to obtain the time domain state equation:
  • the symbol " ⁇ " represents a small disturbance signal
  • the disturbance term ⁇ B(t) 0
  • the linearized time-domain state equation is obtained after ignoring the quadratic term in the formula:
  • ⁇ X -(A- ⁇ Q) -1 ( ⁇ AX+B ⁇ U);
  • Step 5 inject a voltage disturbance ⁇ up with a frequency of ⁇ p into the MMC, and calculate the corresponding current response ⁇ ip at the frequency of ⁇ p by using the established MMC small signal model;
  • Step 6 by calculating the ratio of the disturbance voltage generated at the disturbance frequency ⁇ p to the corresponding disturbance current, obtain the AC side small-signal impedance of the MMC at the disturbance frequency ⁇ p , which is defined as:
  • Step 7 Change the magnitude of the disturbance frequency within a preset range according to requirements, and repeat steps 5 and 6 to obtain an impedance curve of the MMC within the preset range.
  • the present invention has the following beneficial effects:
  • the Fourier decomposition method is adopted to consider the harmonic coupling problem inside the converter, so that the impedance model of the MMC is more accurate.
  • the MMC impedance curve obtained by modeling is almost consistent with the actual MMC impedance curve, and the modeling accuracy is high.
  • the model can be applied to analyze the stability of the MMC-based HVDC transmission system, thereby improving the operational reliability of the MMC-based HVDC transmission system.
  • Fig. 1 is the topological structure schematic diagram of MMC
  • Fig. 2 is the flow chart of the MMC small-signal impedance modeling method based on Fourier decomposition in the present embodiment
  • Fig. 3 is the schematic diagram of the average value equivalent circuit of the MMC single-phase branch
  • FIG. 4 is a schematic diagram of the comparison between the existing MMC small-signal impedance modeling method and the actual MMC impedance
  • FIG. 5 is a schematic diagram of a comparison between the MMC small-signal impedance modeling method based on Fourier decomposition and the actual MMC impedance using this specific embodiment.
  • FIG. 1 A MMC small-signal impedance modeling method based on Fourier decomposition, the adopted MMC topology structure is shown in FIG. 1 , the MMC includes three-phase bridge arms corresponding to three-phase alternating current one-to-one, and the three-phase bridge arms are connected in parallel;
  • Each phase bridge arm includes an upper bridge arm and a lower bridge arm in series, and the upper bridge arm includes N sub-modules connected in series, and the lower bridge arm includes N sub-modules connected in series, including the following steps, and the process is shown in Figure 2:
  • Step 1 transform the single-phase branch of the MMC into an average value equivalent circuit, the equivalent circuit refers to the schematic diagram of FIG. 3, write the basic circuit equation of the MMC, and obtain the mathematical model of the MMC;
  • the mathematical model of is expressed in the form of state space, and the MMC time domain state space model is obtained.
  • A(t), B(t) are the matrices representing the parameters of the MMC circuit
  • x(t) is the selected state variable
  • i c (t) is the phase circulating current
  • i g (t) is the AC side current
  • u(t) is the selected output variable
  • u(t) [U dc ,0,0,u g (t)] T
  • U dc is the DC side voltage
  • ug (t) is the AC side voltage
  • Step 2 based on Fourier series decomposition, transform the MMC time domain state space model into a frequency domain equation through Fourier decomposition, that is, transform the MMC time domain model into the frequency domain through Fourier decomposition, and obtain the MMC frequency domain.
  • Steady-state model sX (AQ)X+BU;
  • elements X, U, A, B correspond to x(t), u(t), A(t), B(t) in the MMC time-domain state space model, respectively, and Q represents the diagonal of the frequency information matrix;
  • step 3 the steady-state operating point of the MMC is solved on the MMC frequency-domain steady-state model.
  • the complex variable s in the MMC frequency-domain steady-state model tends to zero.
  • Step 4 the small perturbation analysis method is applied to the MMC time domain state space model to obtain the time domain state equation:
  • the symbol " ⁇ " represents a small disturbance signal.
  • B(t) is a constant coefficient matrix in MMC
  • the disturbance term is 0
  • the disturbance term ⁇ B(t) 0
  • the linearity is obtained after ignoring the quadratic term in the formula
  • the time-domain state equation is:
  • ⁇ X -(A- ⁇ Q) -1 ( ⁇ AX+B ⁇ U);
  • Step 5 inject a voltage disturbance ⁇ up with a frequency of ⁇ p into the MMC, and calculate the corresponding current response ⁇ ip at the frequency of ⁇ p by using the established MMC small signal model;
  • Step 6 by calculating the ratio of the disturbance voltage generated at the disturbance frequency ⁇ p to the corresponding disturbance current, obtain the AC side small-signal impedance of the MMC at the disturbance frequency ⁇ p , which is defined as:
  • Step 7 Change the magnitude of the disturbance frequency within a preset range according to requirements, repeat steps 5 and 6, and obtain an impedance curve of the MMC within the preset range.
  • the matrices A(t) and B(t) in the step 1 are respectively expressed as:
  • R is the MMC bridge arm resistance
  • C is the capacitance value of the half-bridge sub-module in parallel
  • N is the number of bridge arm sub-modules
  • L is the MMC bridge arm inductance
  • s u (t) , s l (t) are the switching functions of the upper and lower arms of the MMC, respectively, expressed as:
  • m 1 and ⁇ 1 are the modulation ratio and phase of the fundamental frequency modulation voltage generated by the controller
  • m 2 and ⁇ 2 are the modulation ratio and phase of the double frequency modulation voltage generated by the second harmonic circulating current controller
  • ⁇ 1 2 ⁇ f
  • f is the fundamental frequency of 50Hz.
  • X [...,X -3 ,X -2 ,X -1 ,X 0 ,X 1 ,X 2 ,X 3 ,...];
  • I is an identity matrix with the same order as the state variables
  • O is a zero matrix with the same order as the state variables
  • the subscripts of the elements represent the harmonic orders considered.
  • the Fourier coefficients of the h-th harmonic of x(t), u(t), A(t), and B(t) in the MMC time-domain state space model correspond to the elements X h , U h , A h , B h ,
  • M1 m 1 /2
  • M 2 m 2 /2
  • m 1 is the modulation ratio of the fundamental frequency modulation voltage generated by the controller
  • m 2 is the double frequency modulation voltage generated by the second harmonic circulating current controller.
  • modulation ratio C arm is the capacitance value connected in parallel with the half-bridge sub-module
  • I c and I g are the upper arm of the phase circulating current, the sum of the capacitor voltage, the sum of the capacitor voltage of the lower arm, and the frequency domain state variable corresponding to the AC side current
  • the subscript h is the considered harmonic order
  • U dc is the direct current side voltage value
  • U g is the AC side voltage amplitude
  • T represents the transposed matrix.
  • ⁇ A(t), ⁇ x(t), and ⁇ u(t) in the time-domain state equation are matrices formed by disturbance signals, which are respectively expressed as:
  • ⁇ X [..., X p-3 , X p-2 , X p-1 , X p , X p+1 , X p+2 , X p+3 ,...] T ;
  • ⁇ U [..., U p-3 , U p-2 , U p-1 , U p , U p+1 , U p+2 , U p+3 ,...] T ;
  • a p ⁇ h represents the complex Fourier coefficient of the conjugate corresponding to the matrix A at the frequency of ⁇ p ⁇ h ⁇ 1 ;
  • X p ⁇ h represents the complex Fourier of the conjugate corresponding to the matrix X at the frequency of ⁇ p ⁇ h ⁇ 1 Coefficient;
  • U p ⁇ h represents the complex Fourier coefficient of the conjugate corresponding to the U matrix at the frequency of ⁇ p ⁇ h ⁇ 1 .
  • the MMC converter in the process of small-signal impedance modeling for MMC, the MMC converter is treated as a two-level VSC converter, and the harmonic coupling problem inside the converter is not considered, so that the obtained The accuracy of the MMC impedance model is greatly reduced.
  • the corresponding MMC AC impedance is compared with the actual MMC impedance, as shown in Figure 4. It can be seen from the figure that the MMC impedance curve modeled by the traditional method is different from the actual MMC impedance curve. larger.
  • the small signal impedance model of the present invention takes into account the internal harmonic coupling of the MMC, as shown in FIG. 5 , the MMC impedance curve and the actual MMC impedance curve are almost identical, and the model accuracy is higher.

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Abstract

Disclosed in the present invention is an MMC small-signal impedance modeling method based on Fourier decomposition, comprising the following steps: step 1, establishing an MMC time-domain state-space model; step 2, converting the MMC time-domain state-space model into a frequency domain by means of Fourier decomposition to obtain an MMC frequency-domain steady-state model; step 3, solving a steady-state working point of the MMC on the MMC frequency-domain steady-state model; step 4, performing perturbation linearization on the MMC at the steady-state working point to obtain a small-signal model of the MMC; step 5, injecting a voltage disturbance Δup having a frequency of ωp into the MMC, and calculating a corresponding current response Δip at the frequency ωp by means of the established small-signal model; step 6, dividing the disturbance voltage by the corresponding disturbance current to obtain the impedance of the MMC at the disturbance frequency; and step 7, changing the disturbance frequency, and repeating steps 5 and 6 to obtain an impedance curve of the MMC within a certain range. The present invention solves the problem that existing models cannot take harmonic coupling in an MMC into consideration, making the established model more accurate.

Description

基于傅里叶分解的MMC小信号阻抗建模方法MMC Small Signal Impedance Modeling Method Based on Fourier Decomposition 技术领域technical field
本发明涉及电力系统输配电技术领域,尤其涉及一种基于傅里叶分解的MMC小信号阻抗建模方法。The invention relates to the technical field of power transmission and distribution of power systems, in particular to an MMC small-signal impedance modeling method based on Fourier decomposition.
背景技术Background technique
由于模块化多电平换流器(Modular Multilevel Converter,MMC)具有模块化结构,效率高,体积小,输出波形质量高,易于安装、维护等优点,在高压直流输电(High Voltage Direct Current,HVDC)和异步电网互联系统中得到了广泛应用。但近年来国内外多个柔性直流工程在调试或运行过程中出现了高频谐波谐振现象,基于MMC的光伏、风电及直流输电系统也多次出现了频率为20~30Hz的次同步振荡现象,严重影响着系统的安全运行。由于MMC结构相比于传统的两电平、三电平换流器要复杂,导致它的控制系统要比传统的换流器更为复杂,MMC的多时间尺度动态控制特性及其与电网之间的相互作用是导致系统振荡事故频发主要因素。因此,针对MMC-HVDC系统的稳定性分析就显得尤为重要。Because the modular multilevel converter (MMC) has the advantages of modular structure, high efficiency, small size, high output waveform quality, easy installation and maintenance, etc., in the high voltage direct current transmission (High Voltage Direct Current, HVDC) ) and asynchronous grid interconnection systems have been widely used. However, in recent years, many flexible DC projects at home and abroad have experienced high-frequency harmonic resonance during commissioning or operation, and MMC-based photovoltaic, wind power and DC transmission systems have also experienced subsynchronous oscillations with a frequency of 20 to 30 Hz. , which seriously affects the safe operation of the system. Compared with traditional two-level and three-level converters, the structure of MMC is more complex, resulting in a more complex control system than traditional converters. The multi-time scale dynamic control characteristics of MMC and its relationship with the power grid The interaction between them is the main factor leading to the frequent occurrence of system oscillation accidents. Therefore, the stability analysis of the MMC-HVDC system is particularly important.
MMC小信号模型是分析MMC-HVDC系统的稳定性的重要工具。由于MMC在稳态运行时桥臂电流和电容电压中具有多种频次谐波分量,具有典型的时变非线性多频率响应特征,导致传统电力电子变换器的建模方法和线性系统分析方法均难以直接应用于MMC。目前对于MMC的小信号建模方法大致可以分为时域和频域两类。时域建模法通过获得系统的参数矩阵进而基于特征值和根轨迹分析系统的小信号稳定性。时域建模方法虽然可以描述MMC的内部动态特性,但建模过程复杂,且难以解释MMC内部复杂的谐波耦合问题,应用于交直流系统稳定性分析时有较大局限性。The MMC small-signal model is an important tool for analyzing the stability of MMC-HVDC systems. Because MMC has multiple frequency harmonic components in the bridge arm current and capacitor voltage during steady-state operation, and has typical time-varying nonlinear multi-frequency response characteristics, the modeling methods and linear system analysis methods of traditional power electronic converters are all different. Difficult to apply directly to MMC. At present, the small signal modeling methods for MMC can be roughly divided into two categories: time domain and frequency domain. The time-domain modeling method analyzes the small-signal stability of the system based on eigenvalues and root locus by obtaining the parameter matrix of the system. Although the time-domain modeling method can describe the internal dynamic characteristics of MMC, the modeling process is complex, and it is difficult to explain the complex harmonic coupling problem within the MMC, which has great limitations when applied to the stability analysis of AC and DC systems.
频域分析法通过建立系统频域阻抗模型,进而利用阻抗稳定判据和Bode图等频域分析工具研究交直流系统小信号稳定性,并可通过信号测试法对MMC及交流系统频域阻抗进行测量验证,在实际MMC-HVDC系统稳定性分析中更为适用。目前针对MMC进行频域建模的方法主要包括谐波线性化和傅里叶分解法。多谐波线性化的基本思路是在系统的激励中注入特定频率下的小扰动信号,分别推导状态变量中扰动频率所对应的响应,从而获得考虑小扰动分量的线性模型;随后再将线性模型中的电压与电流相除即可获得系统的小信号阻抗,进而实现系统稳定性的分析。但使用谐波线性化方法对MMC进行建模时,其过程复杂,不利于计算机编程实现。采用傅里叶分解法对MMC进行建模时可以克服上述缺点。傅里叶分解法通过将时域模型转化至频域,然后在稳态工作点进行小扰动分析即可得到MMC的小信号阻抗模型,建模过程较为简单,并且易于编程求解,模型精度更高。但传统的傅里叶分解法采用推导的方式进行建模,且没有考虑MMC内部谐波耦合,模型精度仍然有待提高。The frequency domain analysis method establishes the system frequency domain impedance model, and then uses frequency domain analysis tools such as impedance stability criterion and Bode diagram to study the small-signal stability of the AC and DC systems. The measurement verification is more applicable in the stability analysis of the actual MMC-HVDC system. At present, the methods of frequency domain modeling for MMC mainly include harmonic linearization and Fourier decomposition. The basic idea of multi-harmonic linearization is to inject a small perturbation signal at a specific frequency into the excitation of the system, and deduce the response corresponding to the perturbation frequency in the state variable, so as to obtain a linear model considering the small perturbation component; The small-signal impedance of the system can be obtained by dividing the voltage and current in the system, thereby realizing the analysis of system stability. However, when using the harmonic linearization method to model MMC, the process is complicated, which is not conducive to computer programming. The above shortcomings can be overcome when the MMC is modeled by the Fourier decomposition method. The Fourier decomposition method can obtain the small-signal impedance model of MMC by converting the time domain model to the frequency domain, and then performing small disturbance analysis at the steady-state operating point. The modeling process is relatively simple, and it is easy to program and solve, and the model accuracy is higher. . However, the traditional Fourier decomposition method adopts the derivation method for modeling, and does not consider the internal harmonic coupling of the MMC, and the model accuracy still needs to be improved.
发明内容SUMMARY OF THE INVENTION
针对上述现有技术的不足,本发明提供一种基于傅里叶分解的MMC小信号阻抗建模方法,旨在解决现有MMC小信号阻抗建模方法不精确的技术问题,并且能够将该模型应用于分析基于MMC的高压直流输电系统的稳定性,进而提高基于MMC的高压直流输电系统运行 可靠性。In view of the above-mentioned deficiencies of the prior art, the present invention provides an MMC small-signal impedance modeling method based on Fourier decomposition, aiming to solve the technical problem that the existing MMC small-signal impedance modeling method is inaccurate, and can make the model It is applied to analyze the stability of the MMC-based HVDC transmission system, and then improve the operational reliability of the MMC-based HVDC transmission system.
为解决上述技术问题,本发明的技术方案如下:For solving the above-mentioned technical problems, the technical scheme of the present invention is as follows:
一种基于傅里叶分解的MMC小信号阻抗建模方法,所述MMC包括与三相交流电一一对应的三相桥臂,三相桥臂并联;每相桥臂均包含串联的上桥臂与下桥臂,并且上桥臂包含串联的N个子模块,下桥臂包含串联的N个子模块,包括以下步骤:An MMC small-signal impedance modeling method based on Fourier decomposition, the MMC includes three-phase bridge arms corresponding to three-phase alternating current one-to-one, and the three-phase bridge arms are connected in parallel; each phase bridge arm includes an upper bridge arm connected in series and the lower bridge arm, and the upper bridge arm contains N sub-modules connected in series, and the lower bridge arm contains N sub-modules connected in series, including the following steps:
步骤1,将所述MMC的单相支路变换为平均值等效电路,列写MMC的基本电路方程,得到所述MMC的数学模型;将所述MMC的数学模型以状态空间的形式进行表示,得到MMC时域状态空间模型
Figure PCTCN2021108181-appb-000001
Step 1, transform the single-phase branch of the MMC into an average value equivalent circuit, write the basic circuit equation of the MMC, and obtain the mathematical model of the MMC; represent the mathematical model of the MMC in the form of a state space , get the MMC time-domain state-space model
Figure PCTCN2021108181-appb-000001
其中,A(t),B(t)是表征MMC电路参数的矩阵,x(t)为所选取的状态变量,
Figure PCTCN2021108181-appb-000002
i c(t)为相环流,
Figure PCTCN2021108181-appb-000003
为上桥臂电容电压之和,
Figure PCTCN2021108181-appb-000004
为下桥臂电容电压之和,i g(t)为交流侧电流,u(t)为所选取的输出变量,u(t)=[U dc,0,0,u g(t)] T,U dc为直流侧电压,u g(t)为交流侧电压;
Among them, A(t), B(t) are the matrices representing the parameters of the MMC circuit, x(t) is the selected state variable,
Figure PCTCN2021108181-appb-000002
i c (t) is the phase circulating current,
Figure PCTCN2021108181-appb-000003
is the sum of the capacitor voltages of the upper bridge arm,
Figure PCTCN2021108181-appb-000004
is the sum of the capacitor voltages of the lower bridge arm, i g (t) is the AC side current, u(t) is the selected output variable, u(t)=[U dc ,0,0,u g (t)] T , U dc is the DC side voltage, ug (t) is the AC side voltage;
步骤2,基于Fourier级数分解,通过傅里叶分解将所述MMC时域状态空间模型转化为频域方程,得到MMC频域定常模型sX=(A-Q)X+BU; Step 2, based on Fourier series decomposition, transform the MMC time-domain state space model into a frequency-domain equation through Fourier decomposition, and obtain the MMC frequency-domain steady-state model sX=(A-Q)X+BU;
其中,元素X,U,A,B分别对应于所述MMC时域状态空间模型中的x(t),u(t),A(t),B(t),Q表示频率信息的对角矩阵;Wherein, elements X, U, A, B correspond to x(t), u(t), A(t), B(t) in the MMC time-domain state space model, respectively, and Q represents the diagonal of the frequency information matrix;
步骤3,在所述MMC频域定常模型上对MMC的稳态工作点进行求解,MMC在稳态运行时,所述MMC频域定常模型中的复变量s趋近于零,对所述MMC频域定常模型sX=(A-Q)X+BU求逆,得到系统的稳态工作点X ss=-(A-Q) -1(BU); In step 3, the steady-state operating point of the MMC is solved on the MMC frequency-domain steady-state model. When the MMC is in steady-state operation, the complex variable s in the MMC frequency-domain steady-state model tends to zero. The frequency domain steady model sX=(AQ)X+BU is inverted to obtain the steady-state operating point of the system X ss =-(AQ) -1 (BU);
步骤4,将小扰动分析法应用于所述MMC时域状态空间模型,得到时域状态方程:Step 4, the small perturbation analysis method is applied to the MMC time domain state space model to obtain the time domain state equation:
Figure PCTCN2021108181-appb-000005
Figure PCTCN2021108181-appb-000005
其中,符号“Δ”表示小扰动信号,扰动项ΔB(t)=0,忽略式中的2次项后得到线性化时域状态方程:Among them, the symbol "Δ" represents a small disturbance signal, the disturbance term ΔB(t)=0, and the linearized time-domain state equation is obtained after ignoring the quadratic term in the formula:
Figure PCTCN2021108181-appb-000006
Figure PCTCN2021108181-appb-000006
将所述线性化时域状态方程转化到频域,当系统稳态运行时,复变量s趋于0,将所述稳态工作点和所述线性化时域状态方程整理为矩阵形式后得到MMC小信号模型:Transform the linearized time-domain state equation into the frequency domain. When the system is running in a steady state, the complex variable s tends to 0. After arranging the steady-state operating point and the linearized time-domain state equation into a matrix form, we get MMC small signal model:
ΔAX+(A-ΔQ)ΔX+BΔU=0;ΔAX+(A-ΔQ)ΔX+BΔU=0;
将所述稳态工作点代入所述MMC小信号模型后,对于一个给定的输入信号扰动ΔU,解出状态变量的扰动响应:After substituting the steady-state operating point into the MMC small-signal model, for a given input signal perturbation ΔU, the perturbation response of the state variable is solved:
ΔX=-(A-ΔQ) -1(ΔAX+BΔU); ΔX=-(A-ΔQ) -1 (ΔAX+BΔU);
步骤5,向MMC注入频率为ω p的电压扰动Δu p,通过建立的所述MMC小信号模型计算在ω p频率下对应的电流响应Δi pStep 5, inject a voltage disturbance Δup with a frequency of ω p into the MMC, and calculate the corresponding current response Δip at the frequency of ω p by using the established MMC small signal model;
步骤6,通过计算在扰动频率ω p下产生的扰动电压和对应的扰动电流之比,得到MMC在所述扰动频率ω p下的交流侧小信号阻抗,其定义为: Step 6, by calculating the ratio of the disturbance voltage generated at the disturbance frequency ωp to the corresponding disturbance current, obtain the AC side small-signal impedance of the MMC at the disturbance frequency ωp , which is defined as:
Figure PCTCN2021108181-appb-000007
Figure PCTCN2021108181-appb-000007
步骤7,根据需求在预设的范围内改变扰动频率的大小,重复步骤5和步骤6,得到 MMC在所述预设的范围内的阻抗曲线。Step 7: Change the magnitude of the disturbance frequency within a preset range according to requirements, and repeat steps 5 and 6 to obtain an impedance curve of the MMC within the preset range.
与现有技术相比,本发明具有以下有益效果:Compared with the prior art, the present invention has the following beneficial effects:
1、对MMC进行小信号阻抗建模的过程中,采用傅里叶分解法的建模方法,能够考虑换流器内部的谐波耦合问题,从而使得到的MMC的阻抗模型的较为精确,通过建模所得到的MMC阻抗曲线和实际MMC阻抗曲线几乎吻合,建模精度高。1. In the process of modeling the small-signal impedance of MMC, the Fourier decomposition method is adopted to consider the harmonic coupling problem inside the converter, so that the impedance model of the MMC is more accurate. The MMC impedance curve obtained by modeling is almost consistent with the actual MMC impedance curve, and the modeling accuracy is high.
2、由于本发明所建立的模型精度高,因此能够将该模型应用于分析基于MMC的高压直流输电系统的稳定性,进而提高基于MMC的高压直流输电系统运行可靠性。2. Due to the high accuracy of the model established by the present invention, the model can be applied to analyze the stability of the MMC-based HVDC transmission system, thereby improving the operational reliability of the MMC-based HVDC transmission system.
附图说明Description of drawings
图1是MMC的拓扑结构示意图;Fig. 1 is the topological structure schematic diagram of MMC;
图2是本具体实施方式中基于傅里叶分解的MMC小信号阻抗建模方法的流程图;Fig. 2 is the flow chart of the MMC small-signal impedance modeling method based on Fourier decomposition in the present embodiment;
图3是MMC单相支路的平均值等效电路示意图;Fig. 3 is the schematic diagram of the average value equivalent circuit of the MMC single-phase branch;
图4是采用现有MMC小信号阻抗建模方法与实际MMC阻抗的对比示意图;FIG. 4 is a schematic diagram of the comparison between the existing MMC small-signal impedance modeling method and the actual MMC impedance;
图5是采用本具体实施方式的基于傅里叶分解的MMC小信号阻抗建模方法与实际MMC阻抗的对比示意图。FIG. 5 is a schematic diagram of a comparison between the MMC small-signal impedance modeling method based on Fourier decomposition and the actual MMC impedance using this specific embodiment.
具体实施方式detailed description
为使本发明的目的、技术方案及优点更加清楚、明确,下面结合附图和具体实施方式对本发明的内容做进一步详细说明。可以理解的是,此处所描述的具体实施例仅仅用于解释本发明,而非对本发明的限定。另外还需要说明的是,为了便于描述,附图中仅示出了与本发明相关的部分而非全部内容。In order to make the objectives, technical solutions and advantages of the present invention clearer and clearer, the content of the present invention will be further described in detail below with reference to the accompanying drawings and specific embodiments. It should be understood that the specific embodiments described herein are only used to explain the present invention, but not to limit the present invention. In addition, it should be noted that, for the convenience of description, the drawings only show some but not all of the contents related to the present invention.
一种基于傅里叶分解的MMC小信号阻抗建模方法,采用的MMC拓扑结构参考图1所示,所述MMC包括与三相交流电一一对应的三相桥臂,三相桥臂并联;每相桥臂均包含串联的上桥臂与下桥臂,并且上桥臂包含串联的N个子模块,下桥臂包含串联的N个子模块,包括以下步骤,流程如图2所示:A MMC small-signal impedance modeling method based on Fourier decomposition, the adopted MMC topology structure is shown in FIG. 1 , the MMC includes three-phase bridge arms corresponding to three-phase alternating current one-to-one, and the three-phase bridge arms are connected in parallel; Each phase bridge arm includes an upper bridge arm and a lower bridge arm in series, and the upper bridge arm includes N sub-modules connected in series, and the lower bridge arm includes N sub-modules connected in series, including the following steps, and the process is shown in Figure 2:
步骤1,将所述MMC的单相支路变换为平均值等效电路,该等效电路参阅图3的示意图,列写MMC的基本电路方程,得到所述MMC的数学模型;将所述MMC的数学模型以状态空间的形式进行表示,得到MMC时域状态空间模型
Figure PCTCN2021108181-appb-000008
Step 1, transform the single-phase branch of the MMC into an average value equivalent circuit, the equivalent circuit refers to the schematic diagram of FIG. 3, write the basic circuit equation of the MMC, and obtain the mathematical model of the MMC; The mathematical model of is expressed in the form of state space, and the MMC time domain state space model is obtained.
Figure PCTCN2021108181-appb-000008
其中,A(t),B(t)是表征MMC电路参数的矩阵,x(t)为所选取的状态变量,
Figure PCTCN2021108181-appb-000009
i c(t)为相环流,
Figure PCTCN2021108181-appb-000010
为上桥臂电容电压之和,
Figure PCTCN2021108181-appb-000011
为下桥臂电容电压之和,i g(t)为交流侧电流,u(t)为所选取的输出变量,u(t)=[U dc,0,0,u g(t)] T,U dc为直流侧电压,u g(t)为交流侧电压;
Among them, A(t), B(t) are the matrices representing the parameters of the MMC circuit, x(t) is the selected state variable,
Figure PCTCN2021108181-appb-000009
i c (t) is the phase circulating current,
Figure PCTCN2021108181-appb-000010
is the sum of the capacitor voltages of the upper bridge arm,
Figure PCTCN2021108181-appb-000011
is the sum of the capacitor voltages of the lower bridge arm, i g (t) is the AC side current, u(t) is the selected output variable, u(t)=[U dc ,0,0,u g (t)] T , U dc is the DC side voltage, ug (t) is the AC side voltage;
步骤2,基于Fourier级数分解,通过傅里叶分解将所述MMC时域状态空间模型转化为频域方程,即通过傅里叶分解将MMC的时域模型转换至频域,得到MMC频域定常模型sX=(A-Q)X+BU;Step 2, based on Fourier series decomposition, transform the MMC time domain state space model into a frequency domain equation through Fourier decomposition, that is, transform the MMC time domain model into the frequency domain through Fourier decomposition, and obtain the MMC frequency domain. Steady-state model sX=(AQ)X+BU;
其中,元素X,U,A,B分别对应于所述MMC时域状态空间模型中的x(t),u(t),A(t),B(t),Q表示频率信息的对角矩阵;Wherein, elements X, U, A, B correspond to x(t), u(t), A(t), B(t) in the MMC time-domain state space model, respectively, and Q represents the diagonal of the frequency information matrix;
步骤3,在所述MMC频域定常模型上对MMC的稳态工作点进行求解,MMC在稳态运行 时,所述MMC频域定常模型中的复变量s趋近于零,对所述MMC频域定常模型sX=(A-Q)X+BU求逆,得到系统的稳态工作点X ss=-(A-Q) -1(BU); In step 3, the steady-state operating point of the MMC is solved on the MMC frequency-domain steady-state model. When the MMC is in steady-state operation, the complex variable s in the MMC frequency-domain steady-state model tends to zero. The frequency domain steady model sX=(AQ)X+BU is inverted to obtain the steady-state operating point of the system X ss =-(AQ) -1 (BU);
步骤4,将小扰动分析法应用于所述MMC时域状态空间模型,得到时域状态方程:Step 4, the small perturbation analysis method is applied to the MMC time domain state space model to obtain the time domain state equation:
Figure PCTCN2021108181-appb-000012
Figure PCTCN2021108181-appb-000012
其中,符号“Δ”表示小扰动信号,考虑到B(t)在MMC中是常系数矩阵,因此扰动项为0,扰动项ΔB(t)=0,忽略式中的2次项后得到线性化时域状态方程:Among them, the symbol "Δ" represents a small disturbance signal. Considering that B(t) is a constant coefficient matrix in MMC, the disturbance term is 0, the disturbance term ΔB(t)=0, and the linearity is obtained after ignoring the quadratic term in the formula The time-domain state equation is:
Figure PCTCN2021108181-appb-000013
Figure PCTCN2021108181-appb-000013
将所述线性化时域状态方程转化到频域,当系统稳态运行时,复变量s趋于0,将所述稳态工作点和所述线性化时域状态方程整理为矩阵形式后得到MMC小信号模型:Transform the linearized time-domain state equation into the frequency domain. When the system is running in a steady state, the complex variable s tends to 0. After arranging the steady-state operating point and the linearized time-domain state equation into a matrix form, we get MMC small signal model:
ΔAX+(A-ΔQ)ΔX+BΔU=0;ΔAX+(A-ΔQ)ΔX+BΔU=0;
将所述稳态工作点代入所述MMC小信号模型后,对于一个给定的输入信号扰动ΔU,解出状态变量的扰动响应:After substituting the steady-state operating point into the MMC small-signal model, for a given input signal perturbation ΔU, the perturbation response of the state variable is solved:
ΔX=-(A-ΔQ) -1(ΔAX+BΔU); ΔX=-(A-ΔQ) -1 (ΔAX+BΔU);
步骤5,向MMC注入频率为ω p的电压扰动Δu p,通过建立的所述MMC小信号模型计算在ω p频率下对应的电流响应Δi pStep 5, inject a voltage disturbance Δup with a frequency of ω p into the MMC, and calculate the corresponding current response Δip at the frequency of ω p by using the established MMC small signal model;
步骤6,通过计算在扰动频率ω p下产生的扰动电压和对应的扰动电流之比,得到MMC在所述扰动频率ω p下的交流侧小信号阻抗,其定义为: Step 6, by calculating the ratio of the disturbance voltage generated at the disturbance frequency ωp to the corresponding disturbance current, obtain the AC side small-signal impedance of the MMC at the disturbance frequency ωp , which is defined as:
Figure PCTCN2021108181-appb-000014
Figure PCTCN2021108181-appb-000014
步骤7,根据需求在预设的范围内改变扰动频率的大小,重复步骤5和步骤6,得到MMC在所述预设的范围内的阻抗曲线。Step 7: Change the magnitude of the disturbance frequency within a preset range according to requirements, repeat steps 5 and 6, and obtain an impedance curve of the MMC within the preset range.
进一步的,所述步骤1中的矩阵A(t),B(t)分别表示为:Further, the matrices A(t) and B(t) in the step 1 are respectively expressed as:
Figure PCTCN2021108181-appb-000015
Figure PCTCN2021108181-appb-000015
Figure PCTCN2021108181-appb-000016
Figure PCTCN2021108181-appb-000016
其中,R为MMC桥臂电阻,C=C arm/N,C arm为半桥子模块所并联的电容值,N为桥臂子模块个数,L为MMC桥臂电感;s u(t),s l(t)分别为MMC上下桥臂的开关函数,表示为: Among them, R is the MMC bridge arm resistance, C=C arm /N, C arm is the capacitance value of the half-bridge sub-module in parallel, N is the number of bridge arm sub-modules, and L is the MMC bridge arm inductance; s u (t) , s l (t) are the switching functions of the upper and lower arms of the MMC, respectively, expressed as:
Figure PCTCN2021108181-appb-000017
Figure PCTCN2021108181-appb-000017
其中,m 1和θ 1是控制器产生的基频调制电压的调制比和相位,m 2和θ 2是二次谐波环 流控制器产生的二倍频调制电压的调制比和相位,ω 1=2πf,f为50Hz的基波频率。 where m 1 and θ 1 are the modulation ratio and phase of the fundamental frequency modulation voltage generated by the controller, m 2 and θ 2 are the modulation ratio and phase of the double frequency modulation voltage generated by the second harmonic circulating current controller, and ω 1 =2πf, f is the fundamental frequency of 50Hz.
进一步的,所述步骤2中的元素X,U,A,B分别表示为:Further, the elements X, U, A, B in the step 2 are respectively expressed as:
X=[…,X -3,X -2,X -1,X 0,X 1,X 2,X 3,…]; X=[…,X -3 ,X -2 ,X -1 ,X 0 ,X 1 ,X 2 ,X 3 ,…];
U=[…,U -3,U -2,U -1,U 0,U 1,U 2,U 3,…]; U=[…,U -3 ,U - 2 ,U - 1 , U0 ,U1,U2, U3 ,…];
Figure PCTCN2021108181-appb-000018
Figure PCTCN2021108181-appb-000018
Figure PCTCN2021108181-appb-000019
Figure PCTCN2021108181-appb-000019
Q=diag[…,-j3ω 1I,-j2ω 1I,-jω 1I,O,jω 1I,j2ω 1I,j3ω 1I,…]; Q=diag[…,-j3ω 1 I,-j2ω 1 I,-jω 1 I,O,jω 1 I,j2ω 1 I,j3ω 1 I,…];
其中,I是具有和状态变量相同阶数的的单位矩阵,O是具有和状态变量相同阶数的零矩阵,元素的下标表示考虑的谐波次数。where I is an identity matrix with the same order as the state variables, O is a zero matrix with the same order as the state variables, and the subscripts of the elements represent the harmonic orders considered.
进一步的,所述MMC时域状态空间模型中的x(t),u(t),A(t),B(t)的第h次谐波的傅里叶系数分别对应于元素X h,U h,A h,B hFurther, the Fourier coefficients of the h-th harmonic of x(t), u(t), A(t), and B(t) in the MMC time-domain state space model correspond to the elements X h , U h , A h , B h ,
其中,in,
Figure PCTCN2021108181-appb-000020
Figure PCTCN2021108181-appb-000020
U 0=[U dc,0,0,0],U 1=[0,0,0,0.5U g],U ±h=[0](h≥2); U 0 =[U dc ,0,0,0],U 1 =[0,0,0,0.5U g ],U ±h =[0](h≥2);
Figure PCTCN2021108181-appb-000021
Figure PCTCN2021108181-appb-000021
Figure PCTCN2021108181-appb-000022
Figure PCTCN2021108181-appb-000022
Figure PCTCN2021108181-appb-000023
Figure PCTCN2021108181-appb-000023
Figure PCTCN2021108181-appb-000024
Figure PCTCN2021108181-appb-000024
Figure PCTCN2021108181-appb-000025
B ±h=[0 0 0 0] T(h≥1);
Figure PCTCN2021108181-appb-000025
B ±h = [0 0 0 0] T (h≥1);
其中,M1=m 1/2,M 2=m 2/2,m 1是控制器产生的基频调制电压的调制比,m 2是二次谐波环流控制器产生的二倍频调制电压的调制比,C arm为半桥子模块所并联的电容值,I c
Figure PCTCN2021108181-appb-000026
和I g分别为相环流上桥臂、电容电压之和、下桥臂电容电压之和,以及交流侧电流所对应的频域状态变量;下标h为考虑的谐波次数,U dc为直流侧电压值,U g为交流侧电压幅值,上标T代表转置矩阵。
Among them, M1=m 1 /2, M 2 =m 2 /2, m 1 is the modulation ratio of the fundamental frequency modulation voltage generated by the controller, and m 2 is the double frequency modulation voltage generated by the second harmonic circulating current controller. modulation ratio, C arm is the capacitance value connected in parallel with the half-bridge sub-module, I c ,
Figure PCTCN2021108181-appb-000026
and I g are the upper arm of the phase circulating current, the sum of the capacitor voltage, the sum of the capacitor voltage of the lower arm, and the frequency domain state variable corresponding to the AC side current; the subscript h is the considered harmonic order, and U dc is the direct current side voltage value, U g is the AC side voltage amplitude, and the superscript T represents the transposed matrix.
进一步的,所述时域状态方程中的ΔA(t)、Δx(t)、Δu(t)为扰动信号构成的矩阵,分别表示为:Further, ΔA(t), Δx(t), and Δu(t) in the time-domain state equation are matrices formed by disturbance signals, which are respectively expressed as:
Figure PCTCN2021108181-appb-000027
Figure PCTCN2021108181-appb-000027
ΔX=[…,X p-3,X p-2,X p-1,X p,X p+1,X p+2,X p+3,…] TΔX=[..., X p-3 , X p-2 , X p-1 , X p , X p+1 , X p+2 , X p+3 ,...] T ;
ΔU=[…,U p-3,U p-2,U p-1,U p,U p+1,U p+2,U p+3,…] TΔU=[..., U p-3 , U p-2 , U p-1 , U p , U p+1 , U p+2 , U p+3 ,...] T ;
其中,A p±h表示A矩阵在ωp±hω 1频率下所对应共轭的复傅里叶系数;X p±h表示X矩阵在ωp±hω 1频率下所对应共轭的复傅里叶系数;U p±h表示U矩阵在ωp±hω 1频率下所对应共轭的复傅里叶系数。 Among them, A p±h represents the complex Fourier coefficient of the conjugate corresponding to the matrix A at the frequency of ωp±hω 1 ; X p±h represents the complex Fourier of the conjugate corresponding to the matrix X at the frequency of ωp±hω 1 Coefficient; U p±h represents the complex Fourier coefficient of the conjugate corresponding to the U matrix at the frequency of ωp±hω 1 .
现有技术中在对MMC进行小信号阻抗建模的过程中,将MMC换流器视为两电平VSC换流器进行处理,不考虑换流器内部的谐波耦合问题,从而使得到的MMC的阻抗模型的精度大打折扣,对应的MMC交流阻抗与实际MMC阻抗对比,如参考图4所示,从图中可以看出,采用传统方法建模得到的MMC阻抗曲线和实际MMC阻抗曲线相差较大。而采用本发明的小信号阻抗模型由于考虑了MMC内部谐波耦合,如图5所示,MMC阻抗曲线和实际MMC阻抗曲线几乎吻合,模型精度更高。In the prior art, in the process of small-signal impedance modeling for MMC, the MMC converter is treated as a two-level VSC converter, and the harmonic coupling problem inside the converter is not considered, so that the obtained The accuracy of the MMC impedance model is greatly reduced. The corresponding MMC AC impedance is compared with the actual MMC impedance, as shown in Figure 4. It can be seen from the figure that the MMC impedance curve modeled by the traditional method is different from the actual MMC impedance curve. larger. However, since the small signal impedance model of the present invention takes into account the internal harmonic coupling of the MMC, as shown in FIG. 5 , the MMC impedance curve and the actual MMC impedance curve are almost identical, and the model accuracy is higher.
上述实施例只是为了说明本发明的技术构思及特点,其目的是在于让本领域内的普通技术人员能够了解本发明的内容并据以实施,并不能以此限制本发明的保护范围。凡是根据本发明内容的实质所做出的等效的变化或修饰,都应涵盖在本发明的保护范围内。The above-mentioned embodiments are only for illustrating the technical concept and characteristics of the present invention, and the purpose thereof is to enable those of ordinary skill in the art to understand the content of the present invention and implement them accordingly, and not to limit the protection scope of the present invention. All equivalent changes or modifications made according to the essence of the present invention shall be included within the protection scope of the present invention.

Claims (5)

  1. 一种基于傅里叶分解的MMC小信号阻抗建模方法,所述MMC包括与三相交流电一一对应的三相桥臂,三相桥臂并联;每相桥臂均包含串联的上桥臂与下桥臂,并且上桥臂包含串联的N个子模块,下桥臂包含串联的N个子模块,其特征在于,包括以下步骤:An MMC small-signal impedance modeling method based on Fourier decomposition, the MMC includes three-phase bridge arms corresponding to three-phase alternating current one-to-one, and the three-phase bridge arms are connected in parallel; each phase bridge arm includes an upper bridge arm connected in series With the lower bridge arm, and the upper bridge arm includes N sub-modules connected in series, and the lower bridge arm includes N sub-modules connected in series, it is characterized in that, comprising the following steps:
    步骤1,将所述MMC的单相支路变换为平均值等效电路,列写MMC的基本电路方程,得到所述MMC的数学模型;将所述MMC的数学模型以状态空间的形式进行表示,得到MMC时域状态空间模型
    Figure PCTCN2021108181-appb-100001
    Step 1, transform the single-phase branch of the MMC into an average value equivalent circuit, write the basic circuit equation of the MMC, and obtain the mathematical model of the MMC; represent the mathematical model of the MMC in the form of a state space , get the MMC time-domain state-space model
    Figure PCTCN2021108181-appb-100001
    其中,A(t),B(t)是表征MMC电路参数的矩阵,x(t)为所选取的状态变量,
    Figure PCTCN2021108181-appb-100002
    i c(t)为相环流,
    Figure PCTCN2021108181-appb-100003
    为上桥臂电容电压之和,
    Figure PCTCN2021108181-appb-100004
    为下桥臂电容电压之和,i g(t)为交流侧电流,u(t)为所选取的输出变量,u(t)=[U dc,0,0,u g(t)] T,U dc为直流侧电压,u g(t)为交流侧电压;
    Among them, A(t), B(t) are the matrices representing the parameters of the MMC circuit, x(t) is the selected state variable,
    Figure PCTCN2021108181-appb-100002
    i c (t) is the phase circulating current,
    Figure PCTCN2021108181-appb-100003
    is the sum of the capacitor voltages of the upper bridge arm,
    Figure PCTCN2021108181-appb-100004
    is the sum of the capacitor voltage of the lower bridge arm, i g (t) is the AC side current, u(t) is the selected output variable, u(t)=[U dc ,0,0,u g (t)] T , U dc is the DC side voltage, ug (t) is the AC side voltage;
    步骤2,基于Fourier级数分解,通过傅里叶分解将所述MMC时域状态空间模型转化为频域方程,得到MMC频域定常模型sX=(A-Q)X+BU;Step 2, based on Fourier series decomposition, transform the MMC time-domain state space model into a frequency-domain equation through Fourier decomposition, and obtain the MMC frequency-domain steady-state model sX=(A-Q)X+BU;
    其中,元素X,U,A,B分别对应于所述MMC时域状态空间模型中的x(t),u(t),A(t),B(t),Q表示频率信息的对角矩阵;Wherein, elements X, U, A, B correspond to x(t), u(t), A(t), B(t) in the MMC time-domain state space model, respectively, and Q represents the diagonal of the frequency information matrix;
    步骤3,在所述MMC频域定常模型上对MMC的稳态工作点进行求解,MMC在稳态运行时,所述MMC频域定常模型中的复变量s趋近于零,对所述MMC频域定常模型sX=(A-Q)X+BU求逆,得到系统的稳态工作点X ss=-(A-Q) -1(BU); In step 3, the steady-state operating point of the MMC is solved on the MMC frequency-domain steady-state model. When the MMC is in steady-state operation, the complex variable s in the MMC frequency-domain steady-state model tends to zero. The frequency domain steady model sX=(AQ)X+BU is inverted to obtain the steady-state operating point of the system X ss =-(AQ) -1 (BU);
    步骤4,将小扰动分析法应用于所述MMC时域状态空间模型,得到时域状态方程:Step 4, the small perturbation analysis method is applied to the MMC time domain state space model to obtain the time domain state equation:
    Figure PCTCN2021108181-appb-100005
    Figure PCTCN2021108181-appb-100005
    其中,符号“Δ”表示小扰动信号,扰动项ΔB(t)=0,忽略式中的2次项后得到线性化时域状态方程:Among them, the symbol "Δ" represents a small disturbance signal, the disturbance term ΔB(t)=0, and the linearized time-domain state equation is obtained after ignoring the quadratic term in the formula:
    Figure PCTCN2021108181-appb-100006
    Figure PCTCN2021108181-appb-100006
    将所述线性化时域状态方程转化到频域,当系统稳态运行时,复变量s趋于0,将所述稳态工作点和所述线性化时域状态方程整理为矩阵形式后得到MMC小信号模型:Transform the linearized time-domain state equation into the frequency domain. When the system is running in a steady state, the complex variable s tends to 0. After arranging the steady-state operating point and the linearized time-domain state equation into a matrix form, we get MMC small signal model:
    ΔAX+(A-ΔQ)ΔX+BΔU=0;ΔAX+(A-ΔQ)ΔX+BΔU=0;
    将所述稳态工作点代入所述MMC小信号模型后,对于一个给定的输入信号扰动ΔU,解出状态变量的扰动响应:After substituting the steady-state operating point into the MMC small-signal model, for a given input signal perturbation ΔU, the perturbation response of the state variable is solved:
    ΔX=-(A-ΔQ) -1(ΔAX+BΔU); ΔX=-(A-ΔQ) -1 (ΔAX+BΔU);
    步骤5,向MMC注入频率为ω p的电压扰动Δu p,通过建立的所述MMC小信号模型计算在ω p频率下对应的电流响应Δi pStep 5, inject a voltage disturbance Δup with a frequency of ω p into the MMC, and calculate the corresponding current response Δip at the frequency of ω p by using the established MMC small signal model;
    步骤6,通过计算在扰动频率ω p下产生的扰动电压和对应的扰动电流之比,得到MMC在所述扰动频率ω p下的交流侧小信号阻抗,其定义为: Step 6, by calculating the ratio of the disturbance voltage generated at the disturbance frequency ωp to the corresponding disturbance current, obtain the AC side small-signal impedance of the MMC at the disturbance frequency ωp , which is defined as:
    Figure PCTCN2021108181-appb-100007
    Figure PCTCN2021108181-appb-100007
    步骤7,根据需求在预设的范围内改变扰动频率的大小,重复步骤5和步骤6,得到MMC在所述预设的范围内的阻抗曲线。Step 7: Change the magnitude of the disturbance frequency within a preset range according to requirements, repeat steps 5 and 6, and obtain an impedance curve of the MMC within the preset range.
  2. 如权利要求1所述的基于傅里叶分解的MMC小信号阻抗建模方法,其特征在于,所述 步骤1中的矩阵A(t),B(t)分别表示为:The MMC small-signal impedance modeling method based on Fourier decomposition as claimed in claim 1, is characterized in that, the matrix A (t) in described step 1, B (t) are respectively expressed as:
    Figure PCTCN2021108181-appb-100008
    Figure PCTCN2021108181-appb-100008
    Figure PCTCN2021108181-appb-100009
    Figure PCTCN2021108181-appb-100009
    其中,R为MMC桥臂电阻,C=C arm/N,,C arm为半桥子模块所并联的电容值,N为桥臂子模块个数,L为MMC桥臂电感;s u(t),s l(t)分别为MMC上下桥臂的开关函数,表示为: Among them, R is the MMC bridge arm resistance, C=C arm /N, and C arm is the capacitance value of the half-bridge sub-modules connected in parallel, N is the number of bridge arm sub-modules, and L is the MMC bridge arm inductance; s u (t ), s l (t) are the switching functions of the upper and lower arms of the MMC, respectively, expressed as:
    Figure PCTCN2021108181-appb-100010
    Figure PCTCN2021108181-appb-100010
    其中,m 1和θ 1是控制器产生的基频调制电压的调制比和相位,m 2和θ 2是二次谐波环流控制器产生的二倍频调制电压的调制比和相位,ω 1=2πf,f为50Hz的基波频率。 where m 1 and θ 1 are the modulation ratio and phase of the fundamental frequency modulation voltage generated by the controller, m 2 and θ 2 are the modulation ratio and phase of the double frequency modulation voltage generated by the second harmonic circulating current controller, and ω 1 =2πf, f is the fundamental frequency of 50Hz.
  3. 如权利要求1所述的基于傅里叶分解的MMC小信号阻抗建模方法,其特征在于,所述步骤2中的元素X,U,A,B分别表示为:The MMC small-signal impedance modeling method based on Fourier decomposition according to claim 1, wherein the elements X, U, A, B in the step 2 are respectively expressed as:
    X=[…,X -3,X -2,X -1,X 0,X 1,X 2,X 3,…]; X=[…,X -3 ,X -2 ,X -1 ,X 0 ,X 1 ,X 2 ,X 3 ,…];
    U=[…,U -3,U -2,U -1,U 0,U 1,U 2,U 3,…]; U=[…,U -3 ,U - 2 ,U - 1 , U0 ,U1,U2, U3 ,…];
    Figure PCTCN2021108181-appb-100011
    Figure PCTCN2021108181-appb-100011
    Figure PCTCN2021108181-appb-100012
    Figure PCTCN2021108181-appb-100012
    Q=diag[…,-j3ω 1I,-j2ω 1I,-jω 1I,O,jω 1I,j2ω 1I,j3ω 1I,…]; Q=diag[…,-j3ω 1 I,-j2ω 1 I,-jω 1 I,O,jω 1 I,j2ω 1 I,j3ω 1 I,…];
    其中,I是具有和状态变量相同阶数的的单位矩阵,O是具有和状态变量相同阶数的零 矩阵,元素的下标表示考虑的谐波次数。where I is an identity matrix with the same order as the state variables, O is a zero matrix with the same order as the state variables, and the subscripts of the elements represent the harmonic orders considered.
  4. 如权利要求1所述的基于傅里叶分解的MMC小信号阻抗建模方法,其特征在于,所述MMC时域状态空间模型中的x(t),u(t),A(t),B(t)的第h次谐波的傅里叶系数分别对应于元素X h,U h,A h,B hThe MMC small-signal impedance modeling method based on Fourier decomposition according to claim 1, wherein x(t), u(t), A(t) in the MMC time-domain state space model, The Fourier coefficients of the h-th harmonic of B(t) correspond to the elements X h , U h , A h , B h , respectively,
    其中,in,
    Figure PCTCN2021108181-appb-100013
    Figure PCTCN2021108181-appb-100013
    U 0=[U dc,0,0,0],U 1=[0,0,0,0.5U g],U ±h=[0](h≥2); U 0 =[U dc ,0,0,0],U 1 =[0,0,0,0.5U g ],U ±h =[0](h≥2);
    Figure PCTCN2021108181-appb-100014
    Figure PCTCN2021108181-appb-100014
    Figure PCTCN2021108181-appb-100015
    Figure PCTCN2021108181-appb-100015
    Figure PCTCN2021108181-appb-100016
    Figure PCTCN2021108181-appb-100016
    Figure PCTCN2021108181-appb-100017
    Figure PCTCN2021108181-appb-100017
    Figure PCTCN2021108181-appb-100018
    Figure PCTCN2021108181-appb-100018
    其中,M1=m 1/2,M 2=m 2/2,m 1是控制器产生的基频调制电压的调制比,m 2是二次谐波环 流控制器产生的二倍频调制电压的调制比,C arm为半桥子模块所并联的电容值,I c
    Figure PCTCN2021108181-appb-100019
    和I g分别为相环流上桥臂、电容电压之和、下桥臂电容电压之和,以及交流侧电流所对应的频域状态变量;下标h为考虑的谐波次数,U dc为直流侧电压值,U g为交流侧电压幅值,上标T代表转置矩阵。
    Among them, M1=m 1 /2, M 2 =m 2 /2, m 1 is the modulation ratio of the fundamental frequency modulation voltage generated by the controller, and m 2 is the double frequency modulation voltage generated by the second harmonic circulating current controller. modulation ratio, C arm is the capacitance value connected in parallel with the half-bridge sub-module, I c ,
    Figure PCTCN2021108181-appb-100019
    and I g are the upper arm of the phase circulating current, the sum of the capacitor voltage, the sum of the capacitor voltage of the lower arm, and the frequency domain state variable corresponding to the AC side current; the subscript h is the considered harmonic order, and U dc is the direct current side voltage value, U g is the AC side voltage amplitude, and the superscript T represents the transposed matrix.
  5. 如权利要求1所述的基于傅里叶分解的MMC小信号阻抗建模方法,其特征在于,所述时域状态方程中的ΔA(t)、Δx(t)、Δu(t)为扰动信号构成的矩阵,分别表示为:The MMC small-signal impedance modeling method based on Fourier decomposition according to claim 1, wherein ΔA(t), Δx(t) and Δu(t) in the time-domain state equation are disturbance signals The formed matrices are represented as:
    Figure PCTCN2021108181-appb-100020
    Figure PCTCN2021108181-appb-100020
    ΔX=[…,X p-3,X p-2,X p-1,X p,X p+1,X p+2,X p+3,…] TΔX=[..., X p-3 , X p-2 , X p-1 , X p , X p+1 , X p+2 , X p+3 ,...] T ;
    ΔU=[…,U p-3,U p-2,U p-1,U p,U p+1,U p+2,U p+3,…] TΔU=[..., U p-3 , U p-2 , U p-1 , U p , U p+1 , U p+2 , U p+3 ,...] T ;
    其中,A p±h表示A矩阵在ωp±hω 1频率下所对应共轭的复傅里叶系数;X p±h表示X矩阵在ωp±hω 1频率下所对应共轭的复傅里叶系数;U p±h表示U矩阵在ωp±hω 1频率下所对应共轭的复傅里叶系数。 Among them, A p±h represents the complex Fourier coefficient of the conjugate corresponding to the matrix A at the frequency of ωp±hω 1 ; X p±h represents the complex Fourier of the conjugate corresponding to the matrix X at the frequency of ωp±hω 1 Coefficient; U p±h represents the complex Fourier coefficient of the conjugate corresponding to the U matrix at the frequency of ωp±hω 1 .
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