CN110968958B - Wind power plant equivalence modeling method based on single-machine equivalence and selection modal analysis - Google Patents

Wind power plant equivalence modeling method based on single-machine equivalence and selection modal analysis Download PDF

Info

Publication number
CN110968958B
CN110968958B CN201911267197.4A CN201911267197A CN110968958B CN 110968958 B CN110968958 B CN 110968958B CN 201911267197 A CN201911267197 A CN 201911267197A CN 110968958 B CN110968958 B CN 110968958B
Authority
CN
China
Prior art keywords
equivalent
model
wind
rotor
state
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
CN201911267197.4A
Other languages
Chinese (zh)
Other versions
CN110968958A (en
Inventor
古庭赟
林呈辉
徐长宝
吕黔苏
高吉普
伍华伟
马覃峰
赵轩
肖小兵
范强
徐梅梅
顾威
祝健杨
李博文
陈相吉
张历
龙秋风
刘明顺
牛唯
张俊玮
苏立
汪明媚
孟令雯
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.)
Guizhou Power Grid Co Ltd
Original Assignee
Guizhou Power Grid 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 Guizhou Power Grid Co Ltd filed Critical Guizhou Power Grid Co Ltd
Priority to CN201911267197.4A priority Critical patent/CN110968958B/en
Publication of CN110968958A publication Critical patent/CN110968958A/en
Application granted granted Critical
Publication of CN110968958B publication Critical patent/CN110968958B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Control Of Eletrric Generators (AREA)
  • Wind Motors (AREA)

Abstract

The invention discloses a wind power plant equivalence modeling method based on single machine equivalence and selection modal analysis, which is characterized in that more than one double-fed fan in a wind power plant is subjected to single machine equivalent polymerization to form one double-fed fan; modeling a dynamic mathematical model of a doubly-fed fan of a wind power plant to obtain a full-order mathematical model; equating the full-order mathematical model to be an aggregation model; then, reducing the equivalent doubly-fed wind turbine by selecting a modal analysis order reduction method; the method solves the problems that the dynamic equivalence method for the wind power plant in the prior art has some limitations on the stability research of a fan grid-connected system, and the physical meaning of a variable cannot be guaranteed not to change; the technical problems that the calculation efficiency is low and the like are caused by the fact that the system order is possibly too high only by using the single equivalent polymerization method.

Description

Wind power plant equivalence modeling method based on single-machine equivalence and selection modal analysis
Technical Field
The invention belongs to the technical field of power systems, and particularly relates to a wind power plant equivalence modeling method based on single-machine equivalence and selection modal analysis.
Background
Due to the fact that the problem of energy shortage and the problem of environmental pollution are increasingly serious due to the steady increase of global energy consumption in recent decades, new energy power generation, particularly wind power generation, is more and more emphasized, and plays an increasingly important role in a power system. Due to the randomness of wind energy and the uncertainty of accessing the power grid, the research on the stability of the wind turbine accessing the power grid gradually becomes a focus. The method has important significance for reasonably modeling the wind power plant for researching the dynamic characteristics of the grid connection of the wind power plant. The dynamic equivalence method of the wind power plant is mainly divided into two types according to whether a single machine structure is reserved: one is a polymerization process and the other is a reduction process. The stability research on the fan grid-connected system has some limitations, and the physical meaning of the variable cannot be guaranteed not to change; the technical problems that the calculation efficiency is low and the like are caused by the fact that the system order is possibly too high only by using the single equivalent polymerization method.
Disclosure of Invention
The technical problem to be solved by the invention is as follows: the wind power plant equivalence modeling method based on single-machine equivalence and selection modal analysis is provided to solve the problem that a dynamic equivalence method of a wind power plant has some limitations for stability research of a fan grid-connected system, and the physical meaning of variables cannot be guaranteed not to change; the technical problems that the calculation efficiency is low and the like are caused by the fact that the system order is possibly too high only by using the single equivalent polymerization method.
The technical scheme of the invention is as follows:
the method comprises the steps that more than one double-fed fan in the wind power plant is subjected to single-machine equivalent polymerization to form one double-fed fan; modeling a dynamic mathematical model of a doubly-fed fan of a wind power plant to obtain a full-order mathematical model; equating the full-order mathematical model to be an aggregation model; and then reducing the equivalent doubly-fed wind turbine by selecting a modal analysis order reduction method.
The modeling of the dynamic mathematical model of the doubly-fed wind turbine of the wind power plant comprises a transmission system model, a generator model, a current converter model and an external network model;
the model of the wind turbine is the transmission relation between wind energy and mechanical energy:
Figure BDA0002313185130000011
in the formula, PtMechanical power output by the wind turbine is kW; λ is tip speed ratio, θ is pitch angle; v. ofwindIs the wind speed, in m/s; cpIs a dimensionless wind energy utilization coefficient; a. thewtIs the area swept by the blade in m2(ii) a ρ is the air density in kg/m3
The transmission system is slowed down into a single mass model, and the dynamic equation of the single mass model is
Figure BDA0002313185130000021
In the formula: omegas、ωrThe synchronous rotation speed of the generator and the rotation speed of the rotor are respectively. HDIs the wind turbine inertia time constant, TmFor mechanical torque, TeIs generator electrical torque, E'qDAnd E'dDTransient rotor voltages, I, of the q-axis and d-axis, respectivelyqsAnd IdsQ-axis current and d-axis current of the generator stator side, respectively;
the generator adopts a two-axis model, adopts a dq coordinate system with q axis leading d axis by 90 degrees, and defines the following variables under the coordinate system:
Figure BDA0002313185130000022
in formula (II)'0Is the transient open-circuit time constant; rrIs the rotor resistance; x'sIs a transient reactance; xmIs the mutual impedance between the stator and the rotor; xsIs a stator reactance; xrIs the rotor reactance; psidrIs a rotor d-axis flux linkage; psiqrA rotor q-axis flux linkage; omegasIs the synchronous speed.
Neglecting the change process of the stator flux linkage, the simplified model of the doubly-fed induction fan is as follows:
Figure BDA0002313185130000023
in the formula: rsIs a stator resistor; i isdrIs the rotor d-axis current; i isqrIs the rotor q-axis current;
VDto be fixedA sub terminal voltage; vdrAnd VqrRotor d-axis and q-axis voltages, respectively; pgenAnd QgenRespectively active power and reactive power to the grid side.
The rotor side control design of the converter is based on active output and reactive output decoupling; voltage V on the stator side when the d-axis is oriented for stator flux linkageqs=VDV ds0 and the control system uses the most common proportional-integral (P-I) control, the model is:
Figure BDA0002313185130000031
wherein x1Is the active outer loop control integral state quantity, KI1Is the active outer loop control integral coefficient, KP1Is the active outer loop control proportionality coefficient, x2Is the current inner loop controlling the integral state quantity, KI2Is the current inner loop control integral coefficient, KP2Is the current inner loop control proportionality coefficient, x3Is a reactive outer loop control integral state quantity, KI3Is the reactive outer loop control integral coefficient, KP3Is the reactive outer loop control proportionality coefficient, x4Is the current inner loop controlling the integral state quantity, KI4Is the current inner loop control integral coefficient, KP4Is the current inner loop control proportionality coefficient; prefAs active power reference value, QrefIs an active power reference value;
network equation between generator side and grid: the generator side is also connected with a load through impedance; the network side balance equation of the system is expressed as
Figure BDA0002313185130000032
In the formula R1And X1Respectively a resistor and a reactor of a transmission line connected with an infinite bus; r2And X2Respectively a resistance and a reactance of a transmission line connected with the load end; v is the voltage of the infinite bus, VDAnd thetaDAre respectively generator machinesVoltage and phase angle of the terminal; vLAnd thetaLRespectively a load end voltage and a phase angle; pLAnd QLLoad active power and reactive power respectively; i isaAnd IbThe current of an infinite bus is injected into the lower machine end of the synchronous coordinate system; i ispAnd IqIs the current injected into the network at the lower end of the synchronous coordinate system and is expressed as follows
Figure BDA0002313185130000041
In the formula IGFor current at the injector side of the grid-connected converter, PrThe active power at the injector end of the grid-connected converter is obtained.
The method for equating the full order mathematical model to the aggregation model comprises the following steps:
in a wind farm, the total mechanical power is
Figure BDA0002313185130000042
Wherein ng is the number of wind generating sets in the wind power plant,
Figure BDA0002313185130000043
for the mechanical power of each fan it is necessary,
Figure BDA0002313185130000044
is the total equivalent mechanical power.
In a steady state, the wind energy utilization factor of each fan is the largest regardless of the wind speed, and therefore,
Figure BDA0002313185130000045
while assuming theta i0; by using the definition of the wind energy utilization factor,
Figure BDA0002313185130000046
the mechanical power is then
Figure BDA0002313185130000047
Considering that the blade length of an equivalent wind turbine is the same as that of a single wind turbine; meanwhile, it is assumed that there is an equivalent active controller, so that the equivalent active controller is in a steady state
Figure BDA0002313185130000048
When the equivalent wind energy is
Figure BDA0002313185130000049
Defining a new equivalent wind speed
Figure BDA00023131851300000410
Is composed of
Figure BDA00023131851300000411
Figure BDA00023131851300000412
Taking into account the equivalent angular velocity
Figure BDA00023131851300000413
Having the same speed range as the angular speed of the individual wind turbine units, the torque equation can be expressed as
Figure BDA0002313185130000051
In the formula: b ise=ng×B;
Obtaining the mechanical power and the torque of the polymerization model by using the equivalent wind speed; treating the equivalent power as the sum of the powers of the single fans; then keeping equivalent variables and parameters; the active and reactive power references correspond to the sum of all wind turbine reference values, expressed as
Figure BDA0002313185130000052
Figure BDA0002313185130000053
Wherein: ceNg × C, an equivalent coefficient of a prescribed equivalent power reference value;
in the equation of motion of the rotor
Figure BDA00023131851300000513
And
Figure BDA00023131851300000514
is shown as
Figure BDA0002313185130000054
Figure BDA0002313185130000055
Equivalent stator current of
Figure BDA0002313185130000056
In the equivalent model, the equivalent voltage has the same order of magnitude as the voltage in each individual wind turbine, and the current is ng times; the total power injected into the rotor circuit is
Figure BDA0002313185130000057
Equivalent rotor current of
Figure BDA0002313185130000058
Model relating to equivalent controllers
Figure BDA0002313185130000059
Figure BDA00023131851300000510
Figure BDA00023131851300000511
Figure BDA00023131851300000512
By the polymerization of the monomer(s) in the presence of a catalyst,
Figure BDA0002313185130000061
are all amplified by ng times;
therefore, the temperature of the molten metal is controlled,
Figure BDA0002313185130000062
Figure BDA0002313185130000063
at the time of the steady-state,
Figure BDA0002313185130000064
the polymerization model has the same order of magnitude as a single fan;
all fans are connected in parallel and equivalent resistance and equivalent reactance parameters are calculated; obtaining equivalent impedance Z of wind power plant at PCC point when wind turbine is short-circuitedequiv(ii) a The equivalent fan model is connected with an external network through an equivalent circuit; series impedance of equivalent circuit equal to Zequiv
The method for reducing the equivalent doubly-fed wind turbine by selecting the order reduction method of modal analysis comprises the following steps:
selecting dominant mode
The first step is to select a dominant mode, namely a dominant pole or a dominant characteristic value, and select a mode which is closest to an imaginary axis in the left half plane of the complex plane as the dominant mode;
② determining the relevant status
The participation matrix P is used to reflect the relationship between modalities and state variables, which is defined as follows:
Figure BDA0002313185130000065
element P in the participation matrix Pki=ukivkiAs an engagement factor, it can be used to measure the degree of mutual engagement between the ith modality and the kth state variable;
structure order reducing system
Let R be equal to Rr×1In order to be a function of the relevant state variable,
Figure BDA0002313185130000066
in order to be an irrelevant state variable,
thus linearizing the system
Figure BDA0002313185130000067
Can be expressed as
Figure BDA0002313185130000068
The irrelevant state subsystem can be expressed as
Figure BDA0002313185130000069
Wherein y iszAn output of the subsystem for an unrelated state; the relevant state subsystem is represented as
Figure BDA00023131851300000610
The states and inputs of the uncorrelated state subsystems are z and r, respectively; for t ≧ t0The analytical solution for z is:
Figure BDA0002313185130000071
the correlation state r can be represented as:
Figure BDA0002313185130000072
wherein λ isiIs the ith dominant mode, viIs its corresponding feature vector; liIs a constant; then there are:
Figure BDA0002313185130000073
output y of uncorrelated state subsystemszThe analytic solution of (c) is:
Figure BDA0002313185130000074
wherein, H (lambda)i)=A12iI-A22)-1A21Is the transfer function of the uncorrelated state subsystems;
the dynamic response of the uncorrelated state subsystems to the correlated state r is represented as:
yz=M0r
M0a sufficient condition exists that rank (V)h) H; if and only if rank (V)h) When h is r, M0There is a unique solution; finally, the following reduced order system is obtained:
Figure BDA0002313185130000075
in the formula, Ar=A11+M0
For an input-output system, the following division is made
Figure BDA0002313185130000076
Obtaining a reduced order model (A)r,Br,Cr,Dr)。
Figure BDA0002313185130000081
The invention has the beneficial effects that:
the invention establishes a full-order model of the wind turbine, the drive train, the generator, the inverter and their external network. Firstly, a polymerization model differential-algebraic equation set is established according to a full-order mathematical model of the whole system. The aggregation model is based on the idea of wind power plant single machine equivalence. Then, further performing order reduction analysis on the polymerization model by using a method of selecting modal analysis, and enabling the order reduction analysis to be equivalent to a first-order model, wherein the method not only retains the physical meaning of the original variable, but also has strong applicability and flexibility; and finally, on the premise of not losing precision, by carrying out aggregation and order reduction analysis on the wind power plant, the method can greatly reduce the model order of the system and improve the calculation efficiency.
The invention has the advantages that: the method has the advantages that the wind power plant is subjected to single-machine equivalence and equivalent single-machine reduction, the physical meaning of the original variable is reserved, and the method has strong applicability and flexibility. Compared with a full-order model, the order of the model is greatly reduced, and the calculation efficiency is improved. And the aggregation model can restore the dynamic characteristics of the wind power plant with certain precision.
The method solves the problems that the dynamic equivalence method for the wind power plant in the prior art has some limitations on the stability research of a fan grid-connected system, and the physical meaning of a variable cannot be guaranteed not to change; the technical problems that the calculation efficiency is low and the like are caused by the fact that the system order is possibly too high only by using the single equivalent polymerization method.
Drawings
FIG. 1 is a graph of wind speed and equivalent speed for each fan in an embodiment;
FIG. 2 is a graph illustrating the output power of each fan in an exemplary embodiment;
FIG. 3 is a sum of active power of an equivalent fan and actual 10 fan outputs in an embodiment;
FIG. 4 is a diagram illustrating a comparison of model orders in an embodiment;
FIG. 5 illustrates exemplary system feature values in accordance with certain embodiments.
Detailed Description
A wind power plant equivalence modeling method based on single machine equivalence and selection modal analysis is characterized in that a plurality of double-fed fans in a wind power plant are subjected to single machine equivalent aggregation to form one double-fed fan, and then the equivalence double-fed fan is subjected to order reduction through an order reduction method of the selection modal analysis.
A double-fed-fan wind power plant-based aggregation reduced-order analysis method is characterized by comprising the following steps:
(A) the dynamic mathematical model modeling of the doubly-fed wind turbine of the wind power plant comprises a transmission system model, a generator model, a current converter model and an external network model.
The model of the wind turbine is the transmission relationship between wind energy and mechanical energy, and the transmission relationship comprises the following steps:
Figure BDA0002313185130000091
in the formula, PtIs the mechanical power output by the wind turbine in kW. λ is tip speed ratio, θ is pitch angle; v. ofwindIs the wind speed in m/s. CpIs a dimensionless wind energy utilization coefficient. A. thewtIs the area swept by the blade in m2. ρ is the air density in kg/m3
② the driveline is typically slowed down to a single mass model. The dynamic equation of the single mass model is
Figure BDA0002313185130000092
In the formula: omegas、ωrThe synchronous rotation speed of the generator and the rotation speed of the rotor are respectively. HDIs the wind turbine inertia time constant, TmFor mechanical torque, TeIs generator electrical torque, E'qDAnd E'dDTransient rotor voltages, I, of the q-axis and d-axis, respectivelyqsAnd IdsQ-axis current and d-axis current of the generator stator side, respectively;
thirdly, the generator adopts a two-axis model, adopts a dq coordinate system with q axis leading d axis by 90 degrees, and defines the following variables under the coordinate system:
Figure BDA0002313185130000093
in formula (II)'0Is the transient open-circuit time constant; rrIs the rotor resistance; x'sIs a transient reactance; xmIs the mutual impedance between the stator and the rotor; xsIs a stator reactance; xrIs the rotor reactance; psidrIs a rotor d-axis flux linkage; psiqrA rotor q-axis flux linkage; omegasIs the synchronous speed.
Neglecting the change process of the stator flux linkage, the simplified model of the doubly-fed induction fan is as follows:
Figure BDA0002313185130000101
in the formula: rsIs a stator resistor; i isdrIs the rotor d-axis current; i isqrIs the rotor q-axis current; vDIs the stator terminal voltage; vdrAnd VqrRotor d-axis and q-axis voltages, respectively; pgenAnd QgenRespectively active power and reactive power to the grid side.
And fourthly, decoupling based on active output and reactive output in the control design of the rotor side of the converter. When the d axis isStator side voltage V when stator flux linkage is orientedqs=VDV ds0 and the control system uses the most common proportional-integral (P-I) control, which is modeled as:
Figure BDA0002313185130000102
wherein x1Is the active outer loop control integral state quantity, KI1Is the active outer loop control integral coefficient, KP1Is the active outer loop control proportionality coefficient, x2Is the current inner loop controlling the integral state quantity, KI2Is the current inner loop control integral coefficient, KP2Is the current inner loop control proportionality coefficient, x3Is a reactive outer loop control integral state quantity, KI3Is the reactive outer loop control integral coefficient, KP3Is the reactive outer loop control proportionality coefficient, x4Is the current inner loop controlling the integral state quantity, KI4Is the current inner loop control integral coefficient, KP4Is the current inner loop control proportionality coefficient; prefAs active power reference value, QrefIs an active power reference value.
A network equation between the generator side and the power grid: the generator side is also connected to a load via an impedance. The network side balance equation of the system can be expressed as
Figure BDA0002313185130000111
In the formula R1And X1Respectively a resistor and a reactor of a transmission line connected with an infinite bus; r2And X2Respectively a resistance and a reactance of a transmission line connected with the load end; v is the voltage of the infinite bus, VDAnd thetaDThe voltage and the phase angle of the generator terminal are respectively; vLAnd thetaLRespectively a load end voltage and a phase angle; pLAnd QLLoad active power and reactive power respectively; i isaAnd IbThe current of an infinite bus is injected into the lower machine end of the synchronous coordinate system; i ispAnd IqIs the current injected into the network at the lower end of the synchronous coordinate system and is expressed as follows
Figure BDA0002313185130000112
In the formula IGCurrent at the injector end of the grid-connected converter; prThe active power at the injector end of the grid-connected converter is obtained.
(B) The full-order mathematical model is equivalent to the aggregate model. In a wind farm, the total mechanical power is
Figure BDA0002313185130000113
Wherein ng is the number of wind generating sets in the wind power plant,
Figure BDA0002313185130000114
for the mechanical power of each fan it is necessary,
Figure BDA0002313185130000115
is the total equivalent mechanical power.
To obtain an equivalent or aggregate model, this total power is defined as the mechanical power applied to the shaft of the equivalent generator or to the equivalent generator. Generally, the aggregate model technique is based on the idea of increasing the power of a single wind turbine.
All wind power plants are considered to have the same parameters and they do not necessarily operate at the same wind speed. Since the speed control maximizes the penetration of wind energy, the wind energy utilization coefficient is also maximized. In a steady state, the wind energy utilization factor of each wind turbine is the largest regardless of the wind speed. Therefore, the temperature of the molten metal is controlled,
Figure BDA0002313185130000116
while assuming thetai0 (wind speed remains within its limits, no tilt angle control is needed). By using the definition of the wind energy utilization factor,
Figure BDA0002313185130000117
the mechanical power is then
Figure BDA0002313185130000118
Consider that the blade length of an equivalent wind turbine is the same as a single wind turbine. Meanwhile, it is assumed that there is an equivalent active controller, so that the equivalent active controller is in a steady state
Figure BDA0002313185130000121
When the equivalent wind energy is
Figure BDA0002313185130000122
Defining a new equivalent wind speed
Figure BDA0002313185130000123
Is composed of
Figure BDA0002313185130000124
Therefore, the temperature of the molten metal is controlled,
Figure BDA0002313185130000125
furthermore, the equivalent angular velocity is taken into account
Figure BDA0002313185130000126
Having the same speed range as the angular speed of the individual wind turbine units, e.g.
Figure BDA0002313185130000127
The torque equation can be expressed as
Figure BDA0002313185130000128
Wherein: b ise=ng×B。
Currently, with equivalent wind speed, the mechanical power and torque of the aggregate model have been derived. To determine all the parameters of the aggregate model, the equivalent power is considered as the sum of the powers of the individual fans in the same way as before. Then, equivalent variables and parameters are kept equal. The polymerization process chosen is similar to that used for the mixed speed fan. The active and reactive power references correspond to the sum of all wind turbine reference values, expressed as
Figure BDA0002313185130000129
Figure BDA00023131851300001210
Wherein: ceNg × C is an equivalent coefficient of a prescribed equivalent power reference value.
Then in the equation of motion of the rotor
Figure BDA00023131851300001211
And
Figure BDA00023131851300001212
can be expressed as
Figure BDA00023131851300001213
Figure BDA00023131851300001214
Wherein the equivalent stator current is
Figure BDA00023131851300001215
In the equivalent model, the equivalent voltage is of the same order of magnitude as the voltage in each individual wind turbine, and the current is approximately ng times. Total power injected into the rotor circuit is
Figure BDA00023131851300001216
Wherein the equivalent rotor current is
Figure BDA0002313185130000131
A model associated with an equivalent controller is studied.
Figure BDA0002313185130000132
Figure BDA0002313185130000133
Figure BDA0002313185130000134
Figure BDA0002313185130000135
In the formula: by the polymerization of the monomer(s) in the presence of a catalyst,
Figure BDA0002313185130000136
are all amplified by ng times. Therefore, the temperature of the molten metal is controlled,
Figure BDA0002313185130000137
Figure BDA0002313185130000138
it is worth noting that, at steady state,
Figure BDA0002313185130000139
the polymerization model is of the same order of magnitude as a single fan.
Finally, by observing an algebraic equation, all fans need to be connected in parallel and the equivalent resistance and equivalent reactance parameters need to be calculated. Considering an external network connected with wind power, and obtaining equivalent impedance Z of the wind power plant at a PCC point when a fan is in short circuitequiv. And then, the equivalent fan model is connected with an external network through an equivalent line. Series impedance of equivalent circuit equal to Zequiv
In summary, the following parameters need to be scaled:
Figure BDA00023131851300001310
all other parameters are equal to a single fan parameter.
(C) And carrying out SMA (shape memory alloy) order reduction treatment on the wind power plant aggregation model.
SMA is a set of comprehensive algorithms for modeling, analyzing and controlling a linear dynamics system. In this context, SMA is used to reduce the order of the aggregated fan stand-alone model, and its core idea is to select the state variables most relevant to the system dominant mode, and intercept these as the reserved state variables, thereby reducing the order of the system. This is briefly described below.
Selecting dominant mode
The first step of SMA is to select the so-called dominant mode, i.e. the dominant pole or dominant eigenvalue, here the mode in the left half-plane of the complex plane closest to the imaginary axis is selected as the dominant mode.
② determining the relevant status
The participation matrix P is used to reflect the relationship between modalities and state variables, which is defined as follows:
Figure BDA0002313185130000141
element P in the participation matrix Pki=ukivkiCan be used to measure the participation factorThe degree of mutual engagement between the ith modality and the kth state variable.
Structure order reducing system
Let R be equal to Rr×1In order to be a function of the relevant state variable,
Figure BDA0002313185130000142
in order to be an irrelevant state variable,
thus linearizing the system
Figure BDA0002313185130000143
Can be expressed as
Figure BDA0002313185130000144
The irrelevant state subsystem can be expressed as
Figure BDA0002313185130000145
Wherein y iszIs the output of the uncorrelated state subsystems. The associated state subsystem may be represented as
Figure BDA0002313185130000146
The states and inputs of the uncorrelated state subsystems are z and r, respectively. For t ≧ t0The analytical solution for z is:
Figure BDA0002313185130000147
the correlation state r can be represented as:
Figure BDA0002313185130000148
wherein λ isiIs the ith dominant mode, viIs it corresponds toThe feature vector of (2). Note that viOnly this part of the relevant state is considered. liIs a constant. Substituting equation 72 into equation 71, there are:
Figure BDA0002313185130000151
output y of uncorrelated state subsystemszThe analytic solution of (c) is:
Figure BDA0002313185130000152
wherein, H (lambda)i)=A12iI-A22)-1A21Is the transfer function of the uncorrelated state subsystems.
The above constructively demonstrates that the dynamic response of an irrelevant state subsystem to a relevant state r can be expressed as:
yz=M0r (38)
here, M0A sufficient condition exists that rank (V)h) H; if and only if rank (V)h) When h is r, M0There is a unique solution. The following reduced order system is finally obtained:
Figure BDA0002313185130000153
in the formula, Ar=A11+M0
The above results in a reduced order model of the autonomous system, for which the following divisions can be made.
Figure BDA0002313185130000154
Similar to A in autonomous systemrBy the method of construction of (A), a reduced order model (A) can be obtainedr,Br,Cr,Dr). Wherein,
Figure BDA0002313185130000155
the working principle of the invention is as follows: a full-order model of the wind turbine, the drive train, the generator, the converter and its external network is considered. Firstly, a polymerization model differential-algebraic equation set is established according to a full-order mathematical model of the whole system. The aggregation model is based on the idea of wind power plant single machine equivalence. And then, further carrying out reduced order analysis on the polymerization model by using a method of selecting modal analysis, and enabling the polymerization model to be equivalent to a first-order model. . And finally, on the premise of not losing precision, by carrying out aggregation and order reduction analysis on the wind power plant, the method can greatly reduce the model order of the system and improve the calculation efficiency.
Firstly, equating the parameters of the fans, and equating 10 fans of the wind power plant to be a single fan, wherein the wind speed accepted by the 10 fans is as follows
Figure BDA0002313185130000161
As shown, the dotted line is equivalent wind speed, and the output active power of each fan is as shown.
After the wind power plant is subjected to equivalence single-machine analysis, the order reduction analysis is carried out on the single-machine model by adopting the selected mode analysis method, the equivalent wind speed is used as an input variable of the system, the emitted active power is used as an output variable of the system, and the following linearized model can be obtained by using a Jacobian matrix J of the system at a balance point:
Figure BDA0002313185130000162
Figure BDA0002313185130000163
the system is subjected to small interference stability analysis at a given specific working point, and the solution of the characteristic value is shown in figure 5
By analyzing 7 characteristic values, the lambda can be obviously seen5The absolute value is the smallest compared to the other 6 eigenvalues, which are closer to the imaginary axis, for which purpose λ is chosen when the order reduction is performed5As the dominant mode.
For lambda5Is analyzed to obtain the state variable omega most relevant to the factorrThus, the characteristic value of the correlation is λ5And the associated state variable is ωrConstructing a reduced order system by rearranging the state variables, wherein the reserved state variables are arranged to the top
Figure BDA0002313185130000164
Figure BDA0002313185130000171
Wherein Z ═ E'qD,E′dD,Δx1,Δx2,Δx3,Δx4]TAre uncorrelated state variables. Consider z (t) ═ λ5I-A22)-1A21ΔωrReducing the model
Figure BDA0002313185130000172
ΔPgen=αPΔωr (47)
Wherein
Figure BDA0002313185130000173
Figure BDA0002313185130000174
Further obtain
Figure BDA0002313185130000175
Wherein
Figure BDA0002313185130000176
Figure BDA0002313185130000177
Figure BDA0002313185130000178
At steady state, the output success can be expressed as
Figure BDA0002313185130000179
When the input wind speed of the system is as shown in fig. 1, fig. 3 shows the active power output by the system by adopting a full-order model, an aggregation model and a reduced-order model of a wind farm, and it can be seen that the aggregation model and the reduced-order model basically restore the dynamic behavior of the original system with a certain precision.
Fig. 4 is a comparison graph of orders of three models, in this example, a full-order model of a wind farm composed of 10 fans is 70 orders, after an aggregation equivalence is a single-machine model, the model order is reduced to 7 orders, and then the order reduction is performed by a method of selecting modal analysis, and the model order after the order reduction is 1 order, so that the model order is greatly reduced and the complexity of analysis problems is simplified while the steady-state and transient-state behaviors of the system are reduced with a certain precision.

Claims (2)

1. A wind power plant equivalence modeling method based on single-machine equivalence and selection modal analysis is characterized by comprising the following steps: the method comprises the steps that more than one double-fed fan in the wind power plant is subjected to single-machine equivalent polymerization to form one double-fed fan; modeling a dynamic mathematical model of a doubly-fed fan of a wind power plant to obtain a full-order mathematical model; equating the full-order mathematical model to be an aggregation model; then, reducing the equivalent doubly-fed wind turbine by selecting a modal analysis order reduction method;
the modeling of the dynamic mathematical model of the doubly-fed wind turbine of the wind power plant comprises a transmission system model, a generator model, a current converter model and an external network model;
the model of the wind turbine is the transmission relation between wind energy and mechanical energy:
Figure FDA0002696977340000011
in the formula, PtMechanical power output by the wind turbine is kW; λ is tip speed ratio, θ is pitch angle; v. ofwindIs the wind speed, in m/s; cpIs a dimensionless wind energy utilization coefficient; a. thewtIs the area swept by the blade in m2(ii) a ρ is the air density in kg/m3(ii) a The transmission system is slowed down into a single mass model, and the dynamic equation of the single mass model is
Figure FDA0002696977340000012
In the formula: omegas、ωrThe synchronous rotating speed of the generator and the rotating speed of the rotor are respectively set; hDIs the wind turbine inertia time constant, TmFor mechanical torque, TeIs generator electrical torque, E'qDAnd E'dDTransient rotor voltages, I, of the q-axis and d-axis, respectivelyqsAnd IdsQ-axis current and d-axis current of the generator stator side, respectively;
the generator adopts a two-axis model, adopts a dq coordinate system with q axis leading d axis by 90 degrees, and defines the following variables under the coordinate system:
Figure FDA0002696977340000013
in formula (II)'0Is the transient open-circuit time constant; rrIs the rotor resistance; x'sIs a transient reactance; xmIs the mutual impedance between the stator and the rotor; xsIs a stator reactance; xrIs the rotor reactance; psidrIs a rotor d-axis flux linkage; psiqrA rotor q-axis flux linkage; omegasThe synchronous rotating speed is adopted;
neglecting the change process of the stator flux linkage, the simplified model of the doubly-fed induction fan is as follows:
Figure FDA0002696977340000021
in the formula: rsIs a stator resistor; i isdrIs the rotor d-axis current; i isqrIs the rotor q-axis current; vDIs the stator terminal voltage; vdrAnd VqrRotor d-axis and q-axis voltages, respectively; pgenAnd QgenRespectively the active power and the reactive power transmitted to the power grid side;
the rotor side control design of the converter is based on active output and reactive output decoupling; voltage V on the stator side when the d-axis is oriented for stator flux linkageqs=VD,Vds0 and the control system uses the most common proportional-integral (P-I) control, the model is:
Figure FDA0002696977340000031
wherein x1Is the active outer loop control integral state quantity, KI1Is the active outer loop control integral coefficient, KP1Is the active outer loop control proportionality coefficient, x2Is the current inner loop controlling the integral state quantity, KI2Is the current inner loop control integral coefficient, KP2Is the current inner loop control proportionality coefficient, x3Is a reactive outer loop controlIntegrating the state quantity, KI3Is the reactive outer loop control integral coefficient, KP3Is the reactive outer loop control proportionality coefficient, x4Is the current inner loop controlling the integral state quantity, KI4Is the current inner loop control integral coefficient, KP4Is the current inner loop control proportionality coefficient; prefAs active power reference value, QrefAs active power reference value
Network equation between generator side and grid: the generator side is also connected with a load through impedance; the network side balance equation of the system is expressed as
Figure FDA0002696977340000032
In the formula R1And X1Respectively a resistor and a reactor of a transmission line connected with an infinite bus; r2And X2Respectively a resistance and a reactance of a transmission line connected with the load end; v is the voltage of the infinite bus, VDAnd thetaDThe voltage and the phase angle of the generator terminal are respectively; vLAnd thetaLRespectively a load end voltage and a phase angle; pLAnd QLLoad active power and reactive power respectively; i isaAnd IbThe current of an infinite bus is injected into the lower machine end of the synchronous coordinate system; i ispAnd IqIs the current injected into the network at the lower end of the synchronous coordinate system and is expressed as follows
Figure FDA0002696977340000041
In the formula IGFor current at the injector side of the grid-connected converter, PrActive power at the injector end of the grid-connected converter;
the method for equating the full order mathematical model to the aggregation model comprises the following steps:
in a wind farm, the total mechanical power is
Figure FDA0002696977340000042
Wherein ng is the number of wind generating sets in the wind power plant,
Figure FDA0002696977340000043
for the mechanical power of each fan it is necessary,
Figure FDA0002696977340000044
is the total equivalent mechanical power;
in a steady state, the wind energy utilization factor of each fan is the largest regardless of the wind speed, and therefore,
Figure FDA0002696977340000045
while assuming thetai0; by using the definition of the wind energy utilization factor,
Figure FDA0002696977340000046
the mechanical power is then
Figure FDA0002696977340000047
Considering that the blade length of an equivalent wind turbine is the same as that of a single wind turbine; meanwhile, it is assumed that there is an equivalent active controller, so that the equivalent active controller is in a steady state
Figure FDA0002696977340000048
When the equivalent wind energy is
Figure FDA0002696977340000051
Defining a new equivalent wind speed
Figure FDA0002696977340000052
Is composed of
Figure FDA0002696977340000053
Figure FDA0002696977340000054
Taking into account the equivalent angular velocity
Figure FDA0002696977340000055
Having the same speed range as the angular speed of the individual wind turbine units, the torque equation can be expressed as
Figure FDA0002696977340000056
In the formula: b ise=ng×B;
Obtaining the mechanical power and the torque of the polymerization model by using the equivalent wind speed; treating the equivalent power as the sum of the powers of the single fans; then keeping equivalent variables and parameters; the active and reactive power references correspond to the sum of all wind turbine reference values, expressed as
Figure FDA0002696977340000057
Figure FDA0002696977340000058
Wherein: ceNg × C, an equivalent coefficient of a prescribed equivalent power reference value;
in the equation of motion of the rotor
Figure FDA0002696977340000059
And
Figure FDA00026969773400000510
is shown as
Figure FDA00026969773400000511
Figure FDA0002696977340000061
Equivalent stator current of
Figure FDA0002696977340000062
In the equivalent model, the equivalent voltage has the same order of magnitude as the voltage in each individual wind turbine, and the current is ng times; the total power injected into the rotor circuit is
Figure FDA0002696977340000063
Equivalent rotor current of
Figure FDA0002696977340000064
Model relating to equivalent controllers
Figure FDA0002696977340000065
Figure FDA0002696977340000066
Figure FDA0002696977340000067
Figure FDA0002696977340000068
By the polymerization of the monomer(s) in the presence of a catalyst,
Figure FDA0002696977340000069
are all amplified by ng times;
therefore, the temperature of the molten metal is controlled,
Figure FDA00026969773400000610
Figure FDA00026969773400000611
at the time of the steady-state,
Figure FDA00026969773400000612
the polymerization model has the same order of magnitude as a single fan;
all fans are connected in parallel and equivalent resistance and equivalent reactance parameters are calculated; obtaining equivalent impedance Z of wind power plant at PCC point when wind turbine is short-circuitedequiv(ii) a The equivalent fan model is connected with an external network through an equivalent circuit; series impedance of equivalent circuit equal to Zequiv
2. The wind power plant equivalence modeling method based on stand-alone equivalence and selection modal analysis according to claim 1, characterized in that: the method for reducing the equivalent doubly-fed wind turbine by selecting the order reduction method of modal analysis comprises the following steps:
selecting dominant mode
The first step is to select a dominant mode, namely a dominant pole or a dominant characteristic value, and select a mode which is closest to an imaginary axis in the left half plane of the complex plane as the dominant mode;
② determining the relevant status
The participation matrix P is used to reflect the relationship between modalities and state variables, which is defined as follows:
Figure FDA0002696977340000071
element P in the participation matrix Pki=ukivkiAs an engagement factor, it can be used to measure the degree of mutual engagement between the ith modality and the kth state variable;
structure order reducing system
Let R be equal to Rr×1For the relevant state variable, z ∈ R(n-r)×1Are uncorrelated state variables, thus linearizing the system
Figure FDA0002696977340000072
Can be expressed as
Figure FDA0002696977340000073
The irrelevant state subsystem can be expressed as
Figure FDA0002696977340000074
Wherein y iszAn output of the subsystem for an unrelated state; the relevant state subsystem is represented as
Figure FDA0002696977340000081
The states and inputs of the uncorrelated state subsystems are z and r, respectively; for t ≧ t0The analytical solution for z is:
Figure FDA0002696977340000082
the correlation state r can be represented as:
Figure FDA0002696977340000083
wherein λ isiIs the ith dominant mode, viIs its corresponding feature vector; liIs a constant; then there are:
Figure FDA0002696977340000084
output y of uncorrelated state subsystemszThe analytic solution of (c) is:
Figure FDA0002696977340000085
wherein, H (lambda)i)=A12iI-A22)-1A21Is the transfer function of the uncorrelated state subsystems;
the dynamic response of the uncorrelated state subsystems to the correlated state r is represented as:
yz=M0r
M0a sufficient condition exists that rank (V)h) H; if and only if rank (V)h) When h is r, M0There is a unique solution; finally, the following reduced order system is obtained:
Figure FDA0002696977340000091
in the formula, Ar=A11+M0
For an input-output system, the following division is made
Figure FDA0002696977340000092
Obtaining a reduced order model (A)r,Br,Cr,Dr)
Figure FDA0002696977340000093
CN201911267197.4A 2019-12-11 2019-12-11 Wind power plant equivalence modeling method based on single-machine equivalence and selection modal analysis Active CN110968958B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201911267197.4A CN110968958B (en) 2019-12-11 2019-12-11 Wind power plant equivalence modeling method based on single-machine equivalence and selection modal analysis

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201911267197.4A CN110968958B (en) 2019-12-11 2019-12-11 Wind power plant equivalence modeling method based on single-machine equivalence and selection modal analysis

Publications (2)

Publication Number Publication Date
CN110968958A CN110968958A (en) 2020-04-07
CN110968958B true CN110968958B (en) 2020-12-01

Family

ID=70033829

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201911267197.4A Active CN110968958B (en) 2019-12-11 2019-12-11 Wind power plant equivalence modeling method based on single-machine equivalence and selection modal analysis

Country Status (1)

Country Link
CN (1) CN110968958B (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111884259B (en) * 2020-08-04 2022-08-23 浙江大学 Station-level wind turbine generator equivalence method considering system small interference stability characteristics
CN114357787B (en) * 2022-01-10 2024-05-28 华北电力大学 Offshore wind farm equivalent modeling method and system
CN115758672B (en) * 2022-10-26 2023-07-28 广东工业大学 Method for constructing power electronic new energy power system reduced order small signal model

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102012956A (en) * 2010-11-30 2011-04-13 山东科技大学 Wind farm equivalent method based on wind farm input wind speed and wind direction chance fluctuation
US20150318697A1 (en) * 2013-03-29 2015-11-05 Gansu Electric Power Corporation Wind Power Technology Center A method for improving small disturbance stability after double-fed unit gets access to the system
CN109217365A (en) * 2018-09-11 2019-01-15 石河子大学 A kind of brushless dual-feed motor virtual synchronous control method
CN110543701A (en) * 2019-08-15 2019-12-06 南方电网科学研究院有限责任公司 Wind speed-based direct-drive wind turbine generator sequence impedance modeling method and device

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108011364B (en) * 2017-11-28 2019-02-22 郑州轻工业学院 A method of analysis DFIG kinetic characteristics and Electrical Power System Dynamic reciprocal effect
CN110263377B (en) * 2019-05-21 2020-11-13 上海交通大学 Wind power plant single-machine equivalent aggregation modeling method based on frequency domain mapping

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102012956A (en) * 2010-11-30 2011-04-13 山东科技大学 Wind farm equivalent method based on wind farm input wind speed and wind direction chance fluctuation
US20150318697A1 (en) * 2013-03-29 2015-11-05 Gansu Electric Power Corporation Wind Power Technology Center A method for improving small disturbance stability after double-fed unit gets access to the system
CN109217365A (en) * 2018-09-11 2019-01-15 石河子大学 A kind of brushless dual-feed motor virtual synchronous control method
CN110543701A (en) * 2019-08-15 2019-12-06 南方电网科学研究院有限责任公司 Wind speed-based direct-drive wind turbine generator sequence impedance modeling method and device

Also Published As

Publication number Publication date
CN110968958A (en) 2020-04-07

Similar Documents

Publication Publication Date Title
CN110968958B (en) Wind power plant equivalence modeling method based on single-machine equivalence and selection modal analysis
CN105179164B (en) Wind-energy changing system sliding-mode control and device based on T-S fuzzy models
CN107294116A (en) A kind of multiple domain power system load control method for frequency
CN107947228B (en) Stochastic stability analysis method for power system containing wind power based on Markov theory
CN108488035A (en) The stall of permanent magnet direct-driving aerogenerator group and variable pitch mixing control method
CN106059422A (en) Fuzzy control method for double-fed electric field subsynchronous oscillation inhibition
CN109713661A (en) The analysis method that wind power plant access influences the multi-computer system fault extreme mute time
CN110970925A (en) Double-fed fan based damping and modeling method for improving system through fast active power modulation
Eberhart et al. Open source library for the simulation of wind power plants
Liao et al. Hybrid control of DFIGs for short‐term and long‐term frequency regulation support in power systems
CN111049178A (en) Method for analyzing stability control of direct-drive permanent magnet wind turbine generator through VSC-HVDC grid connection
Liang et al. The modeling and numerical simulations of wind turbine generation system with free vortex method and simulink
CN118040717A (en) System critical inertia demand quantitative evaluation method considering source load inertia supporting capacity
Yao et al. RBF neural network based self-tuning PID pitch control strategy for wind power generation system
Yao et al. Variable speed wind turbine maximum power extraction based on fuzzy logic control
CN110417047B (en) Method for analyzing SSCI damping characteristics of doubly-fed fan based on complex torque coefficient
Moumani et al. Modeling and backstepping control of DFIG used in wind enegry conversion system
Dong et al. Surrogate-assisted cooperation control of network-connected doubly fed induction generator wind farm with maximized reactive power capacity
CN116111610A (en) Frequency dynamic characteristic analysis method and related device for wind power variable pitch control
CN110912180A (en) Doubly-fed wind turbine model order reduction method based on selected mode analysis
Wang et al. Sliding mode control for maximum wind energy capture of DFIG-based wind turbine
Qian et al. A new pitch control strategy for variable-speed wind generator
Hui et al. Load frequency control of power systems with wind turbine through flywheels
Ran et al. Robust Adaptive MPPT Control of Wind Turbine Based on Prescribed Performance
Meng et al. Multi-degree of freedom optimization control for large inertia wind energy conversion system using model predictive approach

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