CN114564821B - Grid-connected inverter impedance modeling method based on single-phase disturbance injection - Google Patents

Grid-connected inverter impedance modeling method based on single-phase disturbance injection Download PDF

Info

Publication number
CN114564821B
CN114564821B CN202210091536.3A CN202210091536A CN114564821B CN 114564821 B CN114564821 B CN 114564821B CN 202210091536 A CN202210091536 A CN 202210091536A CN 114564821 B CN114564821 B CN 114564821B
Authority
CN
China
Prior art keywords
frequency
omega
phase
grid
disturbance
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.)
Active
Application number
CN202210091536.3A
Other languages
Chinese (zh)
Other versions
CN114564821A (en
Inventor
赵静波
马俊鹏
王顺亮
刘天琪
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Sichuan University
Electric Power Research Institute of State Grid Jiangsu Electric Power Co Ltd
Original Assignee
Sichuan University
Electric Power Research Institute of State Grid Jiangsu Electric Power Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Sichuan University, Electric Power Research Institute of State Grid Jiangsu Electric Power Co Ltd filed Critical Sichuan University
Priority to CN202210091536.3A priority Critical patent/CN114564821B/en
Publication of CN114564821A publication Critical patent/CN114564821A/en
Application granted granted Critical
Publication of CN114564821B publication Critical patent/CN114564821B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • 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
    • H02J3/38Arrangements for parallely feeding a single network by two or more generators, converters or transformers
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02MAPPARATUS FOR CONVERSION BETWEEN AC AND AC, BETWEEN AC AND DC, OR BETWEEN DC AND DC, AND FOR USE WITH MAINS OR SIMILAR POWER SUPPLY SYSTEMS; CONVERSION OF DC OR AC INPUT POWER INTO SURGE OUTPUT POWER; CONTROL OR REGULATION THEREOF
    • H02M7/00Conversion of ac power input into dc power output; Conversion of dc power input into ac power output
    • H02M7/42Conversion of dc power input into ac power output without possibility of reversal
    • H02M7/44Conversion of dc power input into ac power output without possibility of reversal by static converters
    • H02M7/48Conversion of dc power input into ac power output without possibility of reversal by static converters using discharge tubes with control electrode or semiconductor devices with control electrode
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02MAPPARATUS FOR CONVERSION BETWEEN AC AND AC, BETWEEN AC AND DC, OR BETWEEN DC AND DC, AND FOR USE WITH MAINS OR SIMILAR POWER SUPPLY SYSTEMS; CONVERSION OF DC OR AC INPUT POWER INTO SURGE OUTPUT POWER; CONTROL OR REGULATION THEREOF
    • H02M7/00Conversion of ac power input into dc power output; Conversion of dc power input into ac power output
    • H02M7/42Conversion of dc power input into ac power output without possibility of reversal
    • H02M7/44Conversion of dc power input into ac power output without possibility of reversal by static converters
    • H02M7/48Conversion of dc power input into ac power output without possibility of reversal by static converters using discharge tubes with control electrode or semiconductor devices with control electrode
    • H02M7/493Conversion of dc power input into ac power output without possibility of reversal by static converters using discharge tubes with control electrode or semiconductor devices with control electrode the static converters being arranged for operation in parallel
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F2113/00Details relating to the application field
    • G06F2113/04Power grid 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
    • H02J2203/00Indexing scheme relating to details of circuit arrangements for AC mains or AC distribution networks
    • H02J2203/10Power transmission or distribution systems management focussing at grid-level, e.g. load flow analysis, node profile computation, meshed network optimisation, active network management or spinning reserve management
    • 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

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Physics & Mathematics (AREA)
  • Theoretical Computer Science (AREA)
  • Computer Hardware Design (AREA)
  • Evolutionary Computation (AREA)
  • Geometry (AREA)
  • General Engineering & Computer Science (AREA)
  • General Physics & Mathematics (AREA)
  • Measurement Of Resistance Or Impedance (AREA)

Abstract

The invention discloses a grid-connected inverter impedance modeling method based on single-phase disturbance injection, which specifically comprises the following steps: analyzing harmonic response frequency generated after single-phase disturbance is injected into an alternating current power grid by considering phase-locked loop frequency coupling response; representing positive and negative order harmonic responses at the PCC using a fast Fourier transform and an alpha beta coordinate system; and optimizing the frequency point selection value and the number of the single-phase disturbance injection according to different coupling harmonic conditions. The invention provides the impedance modeling method based on single-phase disturbance injection, which reduces the complexity and the required capacity of impedance measurement equipment, reduces the volume of the equipment and improves the accuracy of impedance modeling.

Description

Grid-connected inverter impedance modeling method based on single-phase disturbance injection
Technical Field
The invention belongs to the field of converter modeling, and particularly relates to a grid-connected inverter impedance modeling method based on single-phase disturbance injection.
Background
Impedance modeling has become an important tool for stability analysis of converter-grid interconnection systems. The impedance model is built by measuring the impedance values of the grid-connected inverter under different frequencies through a mathematical method, however, the traditional three-phase impedance measurement method requires that the impedance measurement transpose has large capacity and volume, which brings about higher cost and energy consumption. The single-phase disturbance injection method only needs to carry out one-time frequency sweep, frequency sweep times are reduced, and the single-phase disturbance injection method only needs to inject harmonic waves through the single-phase inverter, so that the complexity of the harmonic generation device is reduced, single-time energy consumption is reduced, and the economical efficiency and the practicability are improved. The existing impedance calculation method considering frequency coupling needs to change the impedance of a power grid, and the operation is likely to change the operating point of the system, and is complex in operation and unfavorable for practical use.
Disclosure of Invention
In order to reduce the volume and energy consumption of the grid-connected inverter impedance measurement device and ensure the accuracy of measurement results, the invention provides a grid-connected inverter impedance modeling method based on single-phase disturbance injection.
The invention discloses a grid-connected inverter impedance modeling method based on single-phase disturbance injection, which comprises the following steps of:
step 1: and calculating the harmonic frequency generated by three phases after disturbance is injected into the alternating-current side single phase of the grid-connected inverter.
After the A-phase injection voltage disturbance at the alternating current side of the grid-connected inverter, the three-phase alternating current voltage signal is expressed as:
Wherein, V 1 is the power grid voltage amplitude, V p is the disturbance voltage amplitude, omega 0 is the power grid voltage angular frequency, omega p is the disturbance voltage angular frequency, and theta p is the disturbance voltage initial phase.
The three-phase alternating voltage signal is converted into dq:
wherein θ s is the phase of the phase locked loop output.
The formula (2) is expressed as a complex variable form:
Form e jx =cos x+ jsin x is euler transformation, the small disturbance voltage signal is subjected to dq transformation, only q-axis component causes the disturbance quantity of delta theta generated by the output phase theta s of the phase-locked loop, and the transfer function of the phase-locked loop is as follows:
Wherein k pp is a phase-locked loop proportional coefficient, k pi is a phase-locked loop integral coefficient, and after phase angle disturbance is introduced due to the influence of phase-locked loop and Park conversion:
θ=ω0t+Δθ (5)
substituting the formula (5) into the formula (3) and performing linearization to obtain the following components:
Equation (6) is converted into:
wherein, The imaginary part of (a) is-jV 1 Deltaθ, complex variable/>Combining equation (4) and equation (5) yields:
obtained according to formulas (6), (7) and (8):
As can be seen from equation (9), due to the effect of the phase-locked loop, a single-phase voltage disturbance with frequency ω p is input, four frequency responses (ω p0)、(ω0p)、(ω0p) and (- ω 0p) are generated in the dq coordinate system, and converted into three-phase coordinate systems, and the four frequencies become ω p、(2ω0p)、(2ω0p) and- ω p, which are the single-input multiple-output phenomenon generated by frequency coupling caused by the phase-locked loop.
Step 2: and injecting voltage (or current) disturbance with different frequencies into any one phase of the alternating current side of the grid-connected inverter, extracting voltage and current at a common point (point of common coupling, PCC), and obtaining three-phase positive and negative sequence subharmonic amplitude values by adopting fast Fourier transform (fast fourier transform, FFT).
After single-phase injection voltage disturbance, extracting three-phase voltage and current signals at PCC, obtaining voltage and current signals v α、vβ,iα、iβ under an alpha beta coordinate system through Clark conversion, and obtaining positive and negative sequence harmonic waves of the voltage and the current through FFT analysis:
Wherein v p、ip is positive sequence voltage and current harmonic, v n、in is negative sequence voltage and current harmonic, Representing the component with angular frequency ω after fourier transformation.
Step 3: according to the obtained amplitude of each subharmonic, obtaining self-impedance and transimpedance which consider frequency coupling;
the self-impedance expression of the grid-connected inverter is as follows:
Wherein Z s is the self-impedance of the grid-connected inverter, Z a is the mutual impedance of the grid-connected inverter, Y s is the self-admittance of the grid-connected inverter, and Y a is the mutual admittance of the grid-connected inverter.
Y s and Y a are calculated from formula (12):
Wherein Y sp) represents the self-admittance of the grid-connected inverter at the frequency of the injection disturbance frequency omega p, Y ac) represents the mutual admittance of the grid-connected inverter at the coupling frequency omega c at the frequency of the injection disturbance frequency, Y ap)* represents the conjugation of the mutual admittance of the grid-connected inverter at the frequency of the injection disturbance frequency omega p, Y sc)* represents the self-admittance of the grid-connected inverter at the coupling frequency omega c at the frequency of the injection disturbance frequency, Component of response current at omega p of grid-connected inverter port after single-phase disturbance representing injection frequency omega p,/>Component of response current at omega p of grid-connected inverter port after single-phase disturbance representing coupling frequency with injection frequency of omega p,/>Conjugation of coupling frequency omega c component of response current of grid-connected inverter port after single-phase disturbance representing injection frequency omega p at omega p,/>Component of response current at omega c of grid-connected inverter port after single-phase disturbance representing coupling frequency with injection frequency of omega p,/>Component of response voltage of grid-connected inverter port at omega p after single-phase disturbance representing injection frequency omega p,/>Component of response voltage of grid-connected inverter port at omega p after single-phase disturbance representing coupling frequency with injection frequency of omega p,/>Conjugation of coupling frequency omega c component of response voltage of grid-connected inverter port after single-phase disturbance representing injection frequency omega p at omega p,/>A component of the response voltage at ω c of the grid-tie inverter port after single-phase disturbance representing the coupling frequency at ω p is injected.
When the injection disturbance frequency ω p is less than 2ω 0, the coupling frequency harmonic should be 2ω 0p component of the positive sequence component; when the injection disturbance frequency ω p is greater than 2ω 0, the coupling frequency harmonic should be a 2ω 0p component of the negative sequence component;
in impedance scanning, small disturbance signals with the frequency omega p and the coupling frequency |2ω 0p | are required to be respectively injected, and harmonic components with the frequency omega p and the corresponding coupling frequency are extracted from the obtained voltage and current at the PCC.
The specific classification is as follows:
when the preset frequency is omega p less than 2 omega 0:
(1) Injecting a small disturbance signal with the frequency of omega p into any one phase of the alternating current side of the grid-connected inverter;
(2) Extracting positive sequence voltage and current harmonic components with frequencies of omega p and 2 omega 0p at PCC;
(3) Injecting a small disturbance signal with the frequency of 2ω 0p into any one phase of the alternating current side of the grid-connected inverter;
(4) Positive sequence voltage and current harmonic components at PCC frequency omega p and 2 omega 0p are extracted.
When the preset frequency is omega p greater than 2 omega 0:
(1) Injecting a small disturbance signal with the frequency of omega p into any one phase of the alternating current side of the grid-connected inverter;
(2) Extracting positive sequence voltage and current harmonic components with the frequency of omega p and negative sequence voltage and current harmonic components with the frequency of omega p-2ω0 at the PCC;
(3) Injecting a small disturbance signal with the frequency of omega p-2ω0 into any one phase of the alternating current side of the grid-connected inverter;
(4) Positive sequence voltage and current harmonic components with the frequency omega p and negative sequence voltage and current harmonic components with the frequency omega p-2ω0 at the PCC are extracted.
The beneficial technical effects of the invention are as follows:
According to the invention, under the condition of considering frequency coupling of the phase-locked loop, the modeling method capable of reducing the volume of the impedance measuring device and not changing the impedance of the power grid is provided, response harmonic conditions generated by single-phase injection disturbance in a three-phase system are analyzed, the harmonic component extraction method when injection disturbance frequencies are different is illustrated, disturbance injection times are reduced, energy consumption during impedance measurement is reduced, and modeling precision is improved.
Drawings
FIG. 1 is a block diagram of a grid-connected inverter impedance measurement system according to the present invention;
FIG. 2 is a graph comparing the modeling results of the self-impedance and the transadmittance of the grid-connected inverter with the sweep frequency results.
Detailed Description
The invention will be described in further detail with reference to the drawings and the detailed description.
In the figure 1, an impedance and an ideal three-phase power supply are used for simulating an alternating current power grid, a direct current side is equivalent to a direct current voltage source, three-phase voltage and current responses are extracted from a PCC, three-phase voltage and current information of harmonic components with required frequency is obtained through a data preprocessing module, and a grid-connected inverter impedance model is obtained through a data computing module.
The invention discloses a grid-connected inverter impedance modeling method based on single-phase disturbance injection, which comprises the following steps of:
step 1: and calculating the harmonic frequency generated by three phases after disturbance is injected into the alternating-current side single phase of the grid-connected inverter.
After the A-phase injection voltage disturbance at the alternating current side of the grid-connected inverter, the three-phase alternating current voltage signal is expressed as:
Wherein, V 1 is the power grid voltage amplitude, V p is the disturbance voltage amplitude, omega 0 is the power grid voltage angular frequency, omega p is the disturbance voltage angular frequency, and theta p is the disturbance voltage initial phase.
The three-phase alternating voltage signal is converted into dq:
wherein θ s is the phase of the phase locked loop output.
The formula (2) is expressed as a complex variable form:
The form e jx =cos x+ jsin x is euler transformation, the small disturbance voltage signal is subjected to dq transformation, only q-axis component causes the output phase θ s of the phase-locked loop to generate the disturbance quantity of Δθ, and the transfer function of the phase-locked loop is as follows:
Wherein k pp is a phase-locked loop proportional coefficient, k pi is a phase-locked loop integral coefficient, and after phase angle disturbance is introduced due to the influence of phase-locked loop and Park conversion:
θ=ω0t+Δθ (5)
substituting the formula (5) into the formula (3) and performing linearization to obtain the following components:
Equation (6) is converted into:
wherein, The imaginary part of (a) is-jV 1 Deltaθ, complex variable/>Combining equation (4) and equation (5) yields:
obtained according to formulas (6), (7) and (8):
As can be seen from equation (9), due to the effect of the phase-locked loop, a single-phase voltage disturbance with frequency ω p is input, four frequency responses (ω p0)、(ω0p)、(ω0p) and (- ω 0p) are generated in the dq coordinate system, and converted into three-phase coordinate systems, and the four frequencies become ω p、(2ω0p)、(2ω0p) and- ω p, which are the single-input multiple-output phenomenon generated by frequency coupling caused by the phase-locked loop.
Step 2: and injecting voltage (or current) disturbance with different frequencies into any one phase of the alternating current side of the grid-connected inverter, extracting voltage and current at a common point (point of common coupling, PCC), and obtaining three-phase positive and negative sequence subharmonic amplitude values by adopting fast Fourier transform (fast fourier transform, FFT).
After single-phase injection voltage disturbance, extracting three-phase voltage and current signals at PCC, obtaining voltage and current signals v α、vβ,iα、iβ under an alpha beta coordinate system through Clark conversion, and obtaining positive and negative sequence harmonic waves of the voltage and the current through FFT analysis:
Wherein v p、ip is positive sequence voltage and current harmonic, and v n、in is negative sequence voltage and current harmonic.
Step 3: according to the obtained amplitude of each subharmonic, obtaining self-impedance and transimpedance which consider frequency coupling;
the self-impedance expression of the grid-connected inverter is as follows:
Wherein Z s is the self-impedance of the grid-connected inverter, Z a is the mutual impedance of the grid-connected inverter, Y s is the self-admittance of the grid-connected inverter, and Y a is the mutual admittance of the grid-connected inverter.
Y s and Y a are calculated from formula (12):
Wherein Y sp) represents the self-admittance of the grid-connected inverter at the frequency of the injection disturbance frequency omega p, Y ac) represents the mutual admittance of the grid-connected inverter at the coupling frequency omega c at the frequency of the injection disturbance frequency, Y ap)* represents the conjugation of the mutual admittance of the grid-connected inverter at the frequency of the injection disturbance frequency omega p, Y sc)* represents the self-admittance of the grid-connected inverter at the coupling frequency omega c at the frequency of the injection disturbance frequency, Component of response current at omega p of grid-connected inverter port after single-phase disturbance representing injection frequency omega p,/>Component of response current at omega p of grid-connected inverter port after single-phase disturbance representing coupling frequency with injection frequency of omega p,/>Conjugation of coupling frequency omega c component of response current of grid-connected inverter port after single-phase disturbance representing injection frequency omega p at omega p,/>Component of response current at omega c of grid-connected inverter port after single-phase disturbance representing coupling frequency with injection frequency of omega p,/>Component of response voltage of grid-connected inverter port at omega p after single-phase disturbance representing injection frequency omega p,/>Component of response voltage of grid-connected inverter port at omega p after single-phase disturbance representing coupling frequency with injection frequency of omega p,/>Conjugation of coupling frequency omega c component of response voltage of grid-connected inverter port after single-phase disturbance representing injection frequency omega p at omega p,/>A component of the response voltage at ω c of the grid-tie inverter port after single-phase disturbance representing the coupling frequency at ω p is injected.
When the injection disturbance frequency ω p is less than 2ω 0, the coupling frequency harmonic should be 2ω 0p component of the positive sequence component; when the injection disturbance frequency ω p is greater than 2ω 0, the coupling frequency harmonic should be a 2ω 0p component of the negative sequence component;
in impedance scanning, small disturbance signals with the frequency omega p and the coupling frequency |2ω 0p | are required to be respectively injected, and harmonic components with the frequency omega p and the corresponding coupling frequency are extracted from the obtained voltage and current at the PCC.
The specific classification is as follows:
when the preset frequency is omega p less than 2 omega 0:
(1) Injecting a small disturbance signal with the frequency of omega p into any one phase of the alternating current side of the grid-connected inverter;
(2) Extracting positive sequence voltage and current harmonic components with frequencies of omega p and 2 omega 0p at PCC;
(3) Injecting a small disturbance signal with the frequency of 2ω 0p into any one phase of the alternating current side of the grid-connected inverter;
(4) Positive sequence voltage and current harmonic components at PCC frequency omega p and 2 omega 0p are extracted.
When the preset frequency is omega p greater than 2 omega 0:
(1) Injecting a small disturbance signal with the frequency of omega p into any one phase of the alternating current side of the grid-connected inverter;
(2) Extracting positive sequence voltage and current harmonic components with the frequency of omega p and negative sequence voltage and current harmonic components with the frequency of omega p-2ω0 at the PCC;
(3) Injecting a small disturbance signal with the frequency of omega p-2ω0 into any one phase of the alternating current side of the grid-connected inverter;
(4) Positive sequence voltage and current harmonic components with the frequency omega p and negative sequence voltage and current harmonic components with the frequency omega p-2ω0 at the PCC are extracted.
Fig. 2 is a graph of comparing calculated values and measured values of the amplitude and the phase of the self-admittance and the mutual admittance of the grid-connected inverter, the graph (a) and the graph (d) are graphs of the amplitude and the phase of the self-admittance, the graph (b) and the graph (c) are graphs of the amplitude and the phase of the mutual admittance, the solid line is a theoretical value admittance curve calculated according to an admittance expression, the scattered point is an admittance value corresponding to each frequency obtained through actual measurement, and it can be seen that the measured values and the calculated values of the admittance of the grid-connected inverter are consistent, and the accuracy of the method is higher.

Claims (2)

1. A grid-connected inverter impedance modeling method based on single-phase disturbance injection is characterized by comprising the following steps:
step 1: calculating harmonic frequency generated by three phases after disturbance is injected into a single phase at an alternating current side of the grid-connected inverter;
After the A-phase injection voltage disturbance at the alternating current side of the grid-connected inverter, the three-phase alternating current voltage signal is expressed as:
Wherein, V 1 is the power grid voltage amplitude, V p is the disturbance voltage amplitude, omega 0 is the power grid voltage angular frequency, omega p is the disturbance voltage angular frequency, theta p is the disturbance voltage initial phase, and t is time;
the three-phase alternating voltage signal is converted into dq:
Wherein θ s is the phase of the phase locked loop output;
The formula (2) is expressed as a complex variable form:
The form e jx = cosx + jsinx is euler transformation, the small disturbance voltage signal is subjected to dq transformation, only q-axis component causes the output phase θ s of the phase-locked loop to generate the disturbance quantity of Δθ, and the transfer function of the phase-locked loop is as follows:
Wherein k pp is a phase-locked loop proportional coefficient, k pi is a phase-locked loop integral coefficient, and after phase angle disturbance is introduced due to the influence of phase-locked loop and Park conversion:
θ=ω0t+Δθ (5)
substituting the formula (5) into the formula (3) and performing linearization to obtain the following components:
Equation (6) is converted into:
wherein, The imaginary part of (a) is-jV 1 Deltaθ, complex variable/>Combining equation (4) and equation (5) yields:
obtained according to formulas (6), (7) and (8):
As can be seen from equation (9), due to the effect of the phase-locked loop, a single-phase voltage disturbance with frequency ω p is input, four frequency responses (ω p0)、(ω0p)、(ω0p) and (- ω 0p) are generated in the dq coordinate system, and converted into three-phase coordinate systems, and the four frequencies become ω p、(2ω0p)、(2ω0p) and- ω p;
Step 2: injecting voltage disturbance with different frequencies into any one phase of the alternating current side of the grid-connected inverter, extracting voltage and current at a common point PCC, and obtaining the amplitude of each subharmonic of the positive and negative sequences of the three phases by adopting fast Fourier transformation;
After single-phase injection voltage disturbance, extracting three-phase voltage and current signals at PCC, obtaining voltage and current signals v α、vβ,iα、iβ under an alpha beta coordinate system through Clark conversion, and obtaining positive and negative sequence harmonic waves of the voltage and the current through FFT analysis:
Wherein v p、ip is positive sequence voltage and current harmonic, v n、in is negative sequence voltage and current harmonic, A component representing angular frequency ω after fourier transform;
Step 3: according to the obtained amplitude of each subharmonic, obtaining self-impedance and transimpedance which consider frequency coupling;
the self-impedance expression of the grid-connected inverter is as follows:
Wherein Z s is the self-impedance of the grid-connected inverter, Z a is the mutual impedance of the grid-connected inverter, Y s is the self-admittance of the grid-connected inverter, and Y a is the mutual admittance of the grid-connected inverter;
Y s and Y a are calculated from formula (12):
Wherein Y sp) represents the self-admittance of the grid-connected inverter at the frequency of the injection disturbance frequency omega p, Y ac) represents the mutual admittance of the grid-connected inverter at the coupling frequency omega c at the frequency of the injection disturbance frequency, Y ap)* represents the conjugation of the mutual admittance of the grid-connected inverter at the frequency of the injection disturbance frequency omega p, Y sc)* represents the self-admittance of the grid-connected inverter at the coupling frequency omega c at the frequency of the injection disturbance frequency, Component of response current at omega p of grid-connected inverter port after single-phase disturbance representing injection frequency omega p,/>Component of response current at omega p of grid-connected inverter port after single-phase disturbance representing coupling frequency with injection frequency of omega p,/>Conjugation of coupling frequency omega c component of response current of grid-connected inverter port after single-phase disturbance representing injection frequency omega p at omega p,/>Component of response current at omega c of grid-connected inverter port after single-phase disturbance representing coupling frequency with injection frequency of omega p,/>Component of response voltage of grid-connected inverter port at omega p after single-phase disturbance representing injection frequency omega p,/>Component of response voltage of grid-connected inverter port at omega p after single-phase disturbance representing coupling frequency with injection frequency of omega p,/>Conjugation of coupling frequency omega c component of response voltage of grid-connected inverter port after single-phase disturbance representing injection frequency omega p at omega p,/>A component representing the response voltage of the grid-connected inverter port at omega c after single-phase disturbance of the coupling frequency with the injection frequency of omega p;
When the injection disturbance frequency ω p is less than 2ω 0, the coupling frequency harmonic should be 2ω 0p component of the positive sequence component; when the injection disturbance frequency ω p is greater than 2ω 0, the coupling frequency harmonic should be a 2ω 0p component of the negative sequence component;
in impedance scanning, small disturbance signals with the frequency omega p and the coupling frequency |2ω 0p | are required to be respectively injected, and harmonic components with the frequency omega p and the corresponding coupling frequency are extracted from the obtained voltage and current at the PCC.
2. The method for modeling impedance of a grid-connected inverter based on single-phase disturbance injection according to claim 1, wherein different signals are required to be injected and extracted according to the magnitude relation between 2 ω 0 and ω p, and the method is classified as follows:
when the preset frequency is omega p less than 2 omega 0:
(1) Injecting a small disturbance signal with the frequency of omega p into any one phase of the alternating current side of the grid-connected inverter;
(2) Extracting positive sequence voltage and current harmonic components with frequencies of omega p and 2 omega 0p at PCC;
(3) Injecting a small disturbance signal with the frequency of 2ω 0p into any one phase of the alternating current side of the grid-connected inverter;
(4) Extracting positive sequence voltage and current harmonic components with frequencies of omega p and 2 omega 0p at PCC;
when the preset frequency is omega p greater than 2 omega 0:
(1) Injecting a small disturbance signal with the frequency of omega p into any one phase of the alternating current side of the grid-connected inverter;
(2) Extracting positive sequence voltage and current harmonic components with the frequency of omega p and negative sequence voltage and current harmonic components with the frequency of omega p-2ω0 at the PCC;
(3) Injecting a small disturbance signal with the frequency of omega p-2ω0 into any one phase of the alternating current side of the grid-connected inverter;
(4) Positive sequence voltage and current harmonic components with the frequency omega p and negative sequence voltage and current harmonic components with the frequency omega p-2ω0 at the PCC are extracted.
CN202210091536.3A 2022-01-26 2022-01-26 Grid-connected inverter impedance modeling method based on single-phase disturbance injection Active CN114564821B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202210091536.3A CN114564821B (en) 2022-01-26 2022-01-26 Grid-connected inverter impedance modeling method based on single-phase disturbance injection

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202210091536.3A CN114564821B (en) 2022-01-26 2022-01-26 Grid-connected inverter impedance modeling method based on single-phase disturbance injection

Publications (2)

Publication Number Publication Date
CN114564821A CN114564821A (en) 2022-05-31
CN114564821B true CN114564821B (en) 2024-05-31

Family

ID=81714152

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202210091536.3A Active CN114564821B (en) 2022-01-26 2022-01-26 Grid-connected inverter impedance modeling method based on single-phase disturbance injection

Country Status (1)

Country Link
CN (1) CN114564821B (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN114935692B (en) * 2022-07-25 2022-11-08 国网浙江省电力有限公司经济技术研究院 Method and device for measuring impedance of converter
CN116735971B (en) * 2023-05-12 2024-07-09 武汉大学 Multi-node impedance measurement device and method for power distribution network
CN116418049B (en) * 2023-06-08 2023-08-11 四川大学 Accurate admittance modeling method for sagging-controlled three-phase grid-connected inverter
CN116699248B (en) * 2023-08-01 2023-12-15 中国电力科学研究院有限公司 Broadband impedance measurement method and system for new energy power generation unit

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108964118A (en) * 2018-06-19 2018-12-07 湖南大学 Phase-locked loop-considered small-signal impedance modeling method for single-phase grid-connected inverter
CN113890096A (en) * 2021-10-20 2022-01-04 东南大学 Converter sequence impedance modeling method in rectification inversion mode

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108964118A (en) * 2018-06-19 2018-12-07 湖南大学 Phase-locked loop-considered small-signal impedance modeling method for single-phase grid-connected inverter
CN113890096A (en) * 2021-10-20 2022-01-04 东南大学 Converter sequence impedance modeling method in rectification inversion mode

Non-Patent Citations (4)

* Cited by examiner, † Cited by third party
Title
Impedance Modeling and Stability Analysis of a Three-phase Three-level NPC Inverter Connected to the Grid;Bo Zhang;CSEE JOURNAL OF POWER AND ENERGY SYSTEMS;20200630;第6卷(第2期);全文 *
Impedance-Phased Dynamic Control Method for Grid-Connected Inverters in a Weak Grid;Xin Chen 等;IEEE TRANSACTIONS ON POWER ELECTRONICS;20170131;第32卷(第1期);全文 *
新能源并网逆变器序阻抗建模及其阻抗测量研究;黄耀;中国优秀硕士学位论文全文数据库工程科技Ⅱ辑;20210215;全文 *
考虑采样过程的换流器混杂宽频导纳模型;冯麟 等;中国电机工程学报;20210929;全文 *

Also Published As

Publication number Publication date
CN114564821A (en) 2022-05-31

Similar Documents

Publication Publication Date Title
CN114564821B (en) Grid-connected inverter impedance modeling method based on single-phase disturbance injection
Asiminoaei et al. A new method of on-line grid impedance estimation for PV inverter
CN107121609A (en) A kind of electric network impedance on-line identification method and device that injection is disturbed based on PRBS
CN101533053B (en) Load simulation and detection device of static reactive power compensation testing platform
CN101627312A (en) AC electric quantity measuring device
CN110598253A (en) Multi-input multi-output frequency domain impedance modeling method for modular multilevel converter
Ortega et al. Reference current computation methods for active power filters: Accuracy assessment in the frequency domain
CN103630748A (en) Device and method for harmonic impedance measurement of micro-grid
CN110108946B (en) Self-impedance and mutual impedance measuring system and method of three-phase grid-connected converter
CN107064744A (en) A kind of harmonic source location method
CN105510719A (en) Three-phase power grid harmonic impedance measurement method
Zhang et al. A non-intrusive identification method of harmonic source loads for industrial users
CN113702706B (en) Power grid impedance measurement method based on power electronic converter
CN207472983U (en) A kind of electric network impedance on-line identification device based on PRBS disturbance injections
CN103513133B (en) The measurement apparatus of MCR type SVC device dynamic response time and method
CN116735971B (en) Multi-node impedance measurement device and method for power distribution network
CN110098610B (en) Real-time identification method and system for oscillation leading mode of power system under fault disturbance
CN102749488A (en) Power grid harmonic wave real-time on-line monitor and method for detecting harmonic wave using same
Pigazo et al. Accurate and computationally efficient implementation of the IEEE 1459-2000 standard in three-phase three-wire power systems
CN115343535A (en) System harmonic impedance estimation method based on Kalman filtering
Chirindo et al. Non-Intrusive Efficiency Estimation of Inverter-Fed Induction Motors
CN204855583U (en) Transient state of accurate heavy current rises and flows generating device
CN111106618A (en) Harmonic analysis method and device for new energy power generation equipment to access power system
CN109212311A (en) A kind of real-time fractional harmonic wave detection method of novel comb filtering
CN110531299A (en) The compressed sensing indirect measurement method of electric energy meter dynamic measuring signal electric energy magnitude

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant