CN108429250B - Equivalence method considering static frequency characteristics of external network - Google Patents
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Abstract
The invention discloses an equivalence method considering static frequency characteristics of an external network, which mainly comprises the following steps: 1) and establishing an original power network model. 2) Inputting basic parameters of the power network in the original power network model. 3) And establishing an equivalent power network model by using an equivalent method of consistency of the power flow and the sensitivity. 4) And calculating the static frequency characteristic of the equivalent load according to the equivalent power network model. 5) And calculating the static frequency characteristic of the equivalent generator according to the equivalent power network model. The method effectively keeps the consistency of the trend and the sensitivity, effectively keeps the static frequency characteristic of the external network, and more truly reflects the actual operation characteristic of the power system.
Description
Technical Field
The invention relates to the field of static equivalence methods of power systems, in particular to an equivalence method considering static frequency characteristics of an external network.
Background
Along with the continuous rising of new energy permeability, the system uncertainty is gradually enhanced, and the out-of-limit risks such as frequency, branch power, voltage and the like in the system tide are increasingly prominent. Therefore, to reflect the actual operating characteristics of the power system, the static frequency characteristics reflecting the load and generator frequency response should be accounted for in the power flow analysis. In addition, modern power systems have been developed into large and complex power grids which are layered, partitioned and tightly interconnected, and the overall scale is large, detailed data among subsystems are difficult to interact in real time, so that integrated power flow analysis is difficult to implement, and power flow analysis accuracy without considering external network influence is poor. Therefore, an equivalent model containing static frequency characteristics needs to be established to improve the feasibility and the calculation accuracy of the power flow analysis.
The existing equivalent models of the conventional static topological method, such as a PV equivalent model, a Thevenin equivalent model, a Ward equivalent model and the like, do not consider the static characteristic frequency characteristic of an external network in an equivalent network. In the existing equivalent model research considering the static frequency characteristics of the external network, the static frequency characteristics of the external network load and the generator are uniformly equivalent to boundary nodes by using a Ward equivalent method based on a direct current power flow model, and the obvious difference between the static frequency characteristics of the load and the generator is ignored. Meanwhile, the Ward equivalence method can only ensure the consistency of the tidal current before and after equivalence, and cannot keep the consistency of the sensitivity before and after equivalence. Therefore, it cannot truly reflect the actual operation characteristics of the power system, and may be difficult to adapt to power flow analysis in consideration of frequency variation.
Disclosure of Invention
The present invention is directed to solving the problems of the prior art.
The technical scheme adopted for achieving the purpose of the invention is that an equivalent method considering the static frequency characteristic of an external network mainly comprises the following steps:
1) and establishing an original power network model.
2) Inputting basic parameters of the power network in the original power network model.
Further, the basic parameters of the power network mainly include element parameters in the original network, the topology structure of the original network and the calculation result of the load flow at the moment of approach.
The element parameters in the original network mainly comprise the admittance to the ground of all nodes, the connection load power of all nodes, the impedance of all lines, the susceptance to the ground of all lines, the constraint condition of line transmission power, the impedance of a transformer, the admittance to the ground of the transformer, the transformation ratio of the transformer, the constraint condition of transformer transmission power, the output of a generator, the constraint condition of the output of the generator, the power frequency static characteristic coefficient of the generator and the power frequency static characteristic coefficient of the load.
The original network topology mainly comprises the connection relation of all nodes and the network partition condition.
The near moment power flow calculation result mainly comprises a node admittance matrix, a node voltage matrix and a node injection current matrix.
3) And establishing an equivalent power network model by using an equivalent method of consistency of the power flow and the sensitivity.
Further, the main steps of establishing the equivalent power network model are as follows:
and 3.1) calculating equivalent parameters in the equivalent power network model by using an equivalent method of load flow and sensitivity consistency. The equivalent parameters mainly comprise equivalent branch admittance yeqGij、yeqBiAnd yeqBijEquivalent ground branch admittance yeqBi0Node voltage amplitude U of sum-equivalent generatorGeqBi。
And 3.2) establishing an equivalent power network model according to the equivalent parameters and the original power network model.
4) And calculating the static frequency characteristic of the equivalent load according to the equivalent power network model.
Further, the main steps of calculating the static frequency characteristic of the equivalent load are as follows:
4.1) calculating the equivalent load current ILeq. Equivalent load current ILeqAs follows:
in the formula ILBThe load current of the original boundary network. I isLEThe load current of the original external network. Y isLLAnd the admittance submatrix is corresponding to the load node in the original external network. LB is the original boundary load node. LE is original outer net load node.For said admittance submatrix YLLThe inverse matrix of (c).
4.2) according to the equivalent load current ILeqCalculating the equivalent load power SLeq. Equivalent load power SLeqAs follows:
in the formula, SLBIs the original boundary load power. SLEIs the original outer net load power. U shapeLB_diagRepresenting main diagonal elements as boundary node voltages ULBThe diagonal matrix of (a). U shapeLE_diagRepresenting the main diagonal element as the external load node voltage ULEThe diagonal matrix of (a).For said admittance submatrixThe companion matrix of (a).For said admittance submatrix YLLThe companion matrix of (a). LB is the original boundary load node. LE is original outer net load node.
4.3) according to the equivalent load power SLeqCalculating the equivalent active load PLeqSum equivalent reactive load QLeq. The method mainly comprises the following steps:
4.3.1) setting an intermediate parameter H:
in the formula (I), the compound is shown in the specification,for said admittance submatrixThe companion matrix of (a).For said admittance submatrix YLLThe companion matrix of (a). LB is the original boundary load node. LE is original outer net load node. U shapeLE_diagRepresenting main diagonalElement is external load node voltage ULEThe diagonal matrix of (a).
4.3.2) equivalent active load PLeqAs follows:
in the formula, PLBThe active load for the original network boundary. PLEIs the original active load of the external network. U shapeLB_diag_realIs a diagonal matrix ULB_diagThe real parts of the elements form a matrix. U shapeLB_diag_imagIs a diagonal matrix ULB_diagThe imaginary part of the element constitutes a matrix. H is an intermediate parameter. QLEIs the original outer net reactive load. U shapeLB_diagRepresenting main diagonal elements as boundary node voltages ULBThe diagonal matrix of (a).
4.3.3) equivalent reactive load QLeqAs follows:
in the formula, QLBIs the original boundary reactive load. QLEIs the original outer net reactive load. U shapeLB_diag_realIs a diagonal matrix ULB_diagThe real parts of the elements form a matrix. U shapeLB_diag_imagIs a diagonal matrix ULB_diagThe imaginary part of the element constitutes a matrix. H is an intermediate parameter. U shapeLB_diagRepresenting main diagonal elements as boundary node voltages ULBThe diagonal matrix of (a). PLEIs the original active load of the external network.
4.4) setting a new energy station. And setting N as the new energy station node set. And setting L as the new energy station load node set. The new energy mainly comprises wind and light. And setting the new energy source to be a negative load, namely, transmitting the active load of the new energy source outwards.
Active load P of the new energyLAs follows:
PL=PLN+KLP(f-fN)。 (6)
in the formula, PLIs the active load P of the ith node under the frequency fLiThe constructed column vector. f is the frequency. f. ofNIs the nominal frequency. KLPThe coefficient K of the active load power frequency static characteristic of the ith nodeLPiThe constructed column vector. PLNRated active load P for the ith nodeLNiThe constructed column vector.
When in usei∈LWhen is, PLNiIs the rated active load of the ith node.
When i ∈ N, PLNi=Pprei+ΔPprei。 (7)
In the formula, PpreiAnd predicting active power of the ith node of the new energy station. Delta PpreiAnd predicting an active power error for the ith node of the new energy station. And i is any node of the new energy station. And N is a node set of the new energy station. And L is a set of load nodes for searching the new energy station.
Reactive load Q of the new energyLAs follows:
QL=QLN+KLQ(f-fN)。 (8)
in the formula, QLRespectively the reactive load Q of the ith node under the frequency fLiThe constructed column vector. QLNRated reactive load Q for the ith nodeLNiThe constructed column vector. KLQThe coefficient K of the power frequency static characteristic of the reactive load of the ith nodeLQiThe constructed column vector. f. ofNIs the nominal frequency. f is the frequency.
4.5) dividing the active load P according to the original internal network, the original external network and the original boundary network nodesLAnd reactive load QLThe following are respectively divided:
where LI represents the original internal network load node. KLPIs the active negative of the ith nodeStatic characteristic coefficient K of charge power frequencyLPiThe constructed column vector. PLNRated active load P for the ith nodeLNiThe constructed column vector. PLBThe active load for the original network boundary. PLEThe original external network is loaded with power. PLIThe original internal network is loaded with power.
Where LI represents the original internal network load node. QLNRated reactive load Q for the ith nodeLNiThe constructed column vector. KLQThe coefficient K of the power frequency static characteristic of the reactive load of the ith nodeLQiThe constructed column vector. QLBIs the original boundary network reactive load. QLEIs the original external network reactive load. QLIIs the original internal network reactive load.
4.6) substituting the original external network load with the static frequency characteristic in the formula 9 and the formula 10 into the equivalent load of the formula 5 and the formula 6, thereby obtaining the equivalent active load and the equivalent reactive load with the static frequency characteristic. The method mainly comprises the following steps:
4.6.1) setting the parameter A1Parameter A2Parameter A3And parameter A4And calculating the parameter A in turn1Parameter A2Parameter A3And parameter A4。
A1=H_realPLN_LE-H_imagQLN_LE。 (11)
In the formula, H_realIs the real part of the intermediate parameter H. PLN_LEThe equivalent rated active load of the external network. QLN_LEThe equivalent rated reactive load of the external network. H_imagIs the imaginary part of the intermediate parameter H.
A2=H_imagPLN_LE+H_realQLN_LE。 (12)
In the formula, H_imagIs the imaginary part of the intermediate parameter H. PLN_LEThe equivalent rated active load of the external network. QLN_LEThe equivalent rated reactive load of the external network. H_realIs the real part of the intermediate parameter H.
A3=H_realKLP_LE-H_imagKLQ_LE。 (13)
In the formula, H_realIs the real part of the intermediate parameter H. KLP_LEThe active load power frequency static characteristic coefficient K of the ith node in the external networkLPiThe constructed column vector. KLQ_LEThe coefficient K of the reactive load power frequency static characteristic of the ith node in the external networkLQiThe constructed column vector. H_imagIs the imaginary part of the intermediate parameter H.
A4=H_imagKLP_LE+H_realKLQ_LE。 (14)
In the formula, H_imagIs the imaginary part of the intermediate parameter H. KLP_LEThe active load power frequency static characteristic coefficient K of the ith node in the external networkLPiThe constructed column vector. KLQ_LEThe coefficient K of the reactive load power frequency static characteristic of the ith node in the external networkLQiThe constructed column vector. H_realIs the imaginary part of the intermediate parameter H.
4.6.2) according to parameter A3And parameter A4Calculating power frequency static characteristic coefficient K of equivalent active loadLeq_PPower frequency static characteristic coefficient K of sum equivalent reactive loadLeq_Q。
Equivalent active load power frequency static characteristic coefficient KLeq_PAs follows:
KLeq_p=KLP_LB-ULB_diag_realA3+ULB_diag_imagA4。 (15)
in the formula, KLP_LBActive load power frequency static characteristic coefficient K of ith node of boundary networkLPi_LBThe constructed column vector. U shapeLB_diag_realRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagThe real parts of the elements form a matrix. A. the3Is a set parameter. A. the4Is a set parameter. U shapeLB_diag_imagRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagThe imaginary part of the element constitutes a matrix.
Equivalent reactive load power frequency static characteristic coefficient KLeq_QAs follows:
KLeq_Q=KLQ_LB-ULB_diag_realA4-ULB_diag_imagA3。 (16)
in the formula, KLQ_LBThe coefficient K of the power frequency static characteristic of the reactive load of the ith node of the boundary networkLQi_LBThe constructed column vector. U shapeLB_diag_realRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagThe real parts of the elements form a matrix. A. the3Is a set parameter. A. the4Is a set parameter. U shapeLB_diag_imagRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagThe imaginary part of the element constitutes a matrix.
4.6.3) according to the parameter A1And parameter A2Calculating equivalent rated active load PLeq_LNRated reactive load Q of sum equivalentLeq_LN。
Equivalent rated active load PLeq_LNAs follows:
PLeq_LN=PLN_LB-ULB_diag_realA1+ULB_diag_imagA2。 (17)
in the formula, PLN_LBIs the equivalent rated active load of the boundary network. A. the1Is a set parameter. A. the2Is a set parameter. U shapeLB_diag_realRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagThe real parts of the elements form a matrix. U shapeLB_diag_imagRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagThe imaginary part of the element constitutes a matrix.
Equivalent rated reactive load QLeq_LNAs follows:
QLeq_LN=QLN_LB-ULB_diag_real A2-ULB_diag_imag A1。 (18)
in the formula, QLN_LBIs the equivalent rated reactive load of the boundary network. U shapeLB_diag_realRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagThe real parts of the elements form a matrix. U shapeLB_diag_imagRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagThe imaginary part of the element constitutes a matrix. A. the1Is a set parameter. A. the2Is a set parameter.
4.6.4) calculating the equivalent active load PLeqSum equivalent reactive load QLeq。
Equivalent active load PLeqAs follows:
PLeq=PLeq_LN+KLeq_P(f-fN)。 (19)
in the formula, PLeq_LNIs the equivalent rated active load. f is the frequency. f. ofNIs the nominal frequency. KLeq_PThe power frequency static characteristic coefficient is the equivalent power load.
Equivalent reactive load QLeqAs follows:
QLeq=QLeq_LN+KLeq_Q(f-fN)。 (20)
in the formula, QLeq_LNThe load is equivalent rated reactive load. f is the frequency. f. ofNIs the nominal frequency. QLeq_PThe power frequency static characteristic coefficient is equivalent reactive load.
5) And calculating the static frequency characteristic of the equivalent generator according to the equivalent power network model.
Further, the main steps of calculating the static frequency characteristic of the equivalent generator are as follows:
5.1) calculating the Current I of the equivalent Generator node GeqGeq. The method mainly comprises the following steps:
5.1.1) calculating the original network generator node injection current IG:
In the formula IGEIs the original external network generator node current. I isGIIs the original internal network generator node current.
UGEIs the original external network generator node voltage. U shapeGIIs the original external network generator voltage. U shapeLEIs the original external network voltage. U shapeLBIs the original boundary network voltage. U shapeLIIs the original internal network voltage.
YGG(GE)(GE)The admittance submatrix corresponding to the generator node in the original external network.
YGG(GI)(GI)The admittance submatrix corresponding to the generator node in the original internal network.
YGL(GE)(LE)And the admittance submatrices are corresponding to the generator nodes in the original external network and the nodes of the original external network.
YGL(GE)(LB)The method is characterized in that generator nodes are taken as corresponding rows and original boundary network nodes are taken as corresponding columns in an original external network, and therefore an admittance submatrix is generated.
GE is the original external network generator node. The GI is the original internal network generator node. GL is the original border network generator node. LI is the original internal network node. LB is the original border network node. The LE is the original external network node.
5.1.2) obtaining the original external network generator node voltage U according to the formula 21GE. The original external network generator node voltage UGEAs follows:
in the formula (I), the compound is shown in the specification,admittance submatrix Y corresponding to generator nodes in original external networkGG(GE)(GE)The inverse matrix of (c). I isGEIs the generator node current in the original external network. U shapeLEIs the original external network voltage. U shapeLBIs the original boundary network voltage. Y isGL(GE)(LE)In the original network, generator nodes of the original external network are taken as corresponding rows and original external network nodes are taken as corresponding columns, and therefore an admittance submatrix is generated. Y isGL(GE)(LB)In the original network, generator nodes of the original external network are taken as corresponding rows, and original boundary network nodes are taken as corresponding columns, so that an admittance submatrix is generated.
5.1.3) obtaining equivalent generator node voltage U according to a static equivalence method based on consistency of power flow and sensitivityGeq. The equivalent generator node voltage UGeqAs follows:
in the formula of UGEIs the original external network generator node voltage.In the equivalent network, an admittance submatrix Y 'is generated by taking equivalent load nodes as corresponding rows and equivalent generator nodes as corresponding columns'LGThe inverse matrix of (c). Y isLGThe load nodes are used as corresponding rows and the generator nodes are used as corresponding columns in the original network, and therefore the admittance submatrix is generated. Y isLLAnd the admittance submatrix is corresponding to the load node in the original external network.For said admittance submatrix YLLThe inverse matrix of (c). LB is the original boundary load node. LE is original outer net load node. GE is the original external network generator node. Gep is an equivalent generator node.
5.1.4) calculating the injection current I 'of the generator node in the equivalent network'G. Generator node injection current I 'in equivalent network'GAs follows:
of formula (II) to (III)'GG(Geq)(Geq)And obtaining the admittance submatrix corresponding to the generator node in the equivalent external network. Y isGG(GI)(GI)The admittance submatrix corresponding to the generator node in the original internal network. U shapeGIIs the original external network generator voltage. U shapeGeqIs the equivalent network generator node voltage. Y'GL(Geq)(LB)In the equivalent external network, equivalent generator nodes are taken as corresponding rows and equivalent boundary network nodes are taken as corresponding columns, so that an admittance submatrix is generated. Y'GL(GI)(LB)In the equivalent network, generator nodes of an equivalent internal network are taken as corresponding rows, and equivalent boundary network nodes are taken as corresponding columns, so that an admittance submatrix is generated. Y'GL(GI)(LI)In the equivalent network, generator nodes of the equivalent internal network are taken as corresponding rows and equivalent internal network nodes are taken as corresponding columns, so that the admittance submatrix is generated. U shapeLIIs the original internal network voltage. U shapeLBIs the original boundary network voltage.
5.1.5) from equation 24, the current I at the equivalent generator node Geq is obtainedGeq. Current I of the equivalent generator node GeqGeqAs follows:
of formula (II) to (III)'GG(Geq)(Geq)And obtaining the admittance submatrix corresponding to the generator node in the equivalent external network. Y isLGThe load nodes are used as corresponding rows and the generator nodes are used as corresponding columns in the original network, and therefore the admittance submatrix is generated. Y isLLAnd the admittance submatrix is corresponding to the load node in the original external network.For said admittance submatrix YLLThe inverse matrix of (c). LB is the original boundary load node. LE is original outer net load node. GE is the original external network generator node. U shapeLBIs the original boundary network voltage. EGEIs the original external network generator node voltage.
5.2) calculating to obtain the voltage U of the equivalent generator nodeGeq. The method mainly comprises the following steps:
5.2.1) setting a constant matrix C, a constant matrix F and a constant matrix D.
The constant matrix C is shown below:
in the formula, YLLAnd the admittance submatrix is corresponding to the load node in the original external network.For said admittance submatrix YLLThe inverse matrix of (c). LB is the original boundary load node. LE is original outer net load node. GE is the original external network generator node. Y isLGThe load nodes are used as corresponding rows and the generator nodes are used as corresponding columns in the original network, and therefore the admittance submatrix is generated.
The constant matrix F is shown below:
in the formula, YLLAnd the admittance submatrix is corresponding to the load node in the original external network.For said admittance submatrix YLLThe inverse matrix of (c). LB is the original boundary load node. LE is original outer net load node. GE is the original external network generator node. Y isLGThe load nodes are used as corresponding rows and the generator nodes are used as corresponding columns in the original network, and therefore the admittance submatrix is generated.
The constant matrix D is as follows:
in the formula, YLLAnd the admittance submatrix is corresponding to the load node in the original external network.For said admittance submatrix YLLThe inverse matrix of (c). LB is the original boundary load node. LE is original outer net load node. GE is the original external network generator node. Y isLGThe load nodes are used as corresponding rows and the generator nodes are used as corresponding columns in the original network, and therefore the admittance submatrix is generated.
5.2.2) voltage U of the equivalent generator node according to the constant matrix C, the constant matrix F and the constant matrix DGeqAs follows:
in the formula (I), the compound is shown in the specification,for outer net generator power matrix SGEThe companion matrix of (a). The matrix C, the matrix F and the matrix D are respectively set constant matrixes. U shapeLBIs the original boundary network voltage.
5.3) calculating the equivalent generator output SGeq. Equivalent generator output SGeqAs follows:
in the formula IGeq_diagIs composed ofGeqA diagonal matrix as a main diagonal element.For the diagonal matrix IGeq_diagThe companion matrix of (a). U shapeGEQIs the voltage at the equivalent generator node.
5.4) according to the equivalent generator output SGeqSum equivalent generator power SGETo obtain the equivalent generator output SGeqSum equivalent generator power SGEThe analytic relationship of (1):
in the formula, the matrix C, the matrix F, and the matrix D are respectively set constant matrices.For the diagonal matrix IGeq_diagThe companion matrix of (a). U shapeLBIs the original boundary network voltage.For outer net generator power matrix SGEThe companion matrix of (a).
5.5) according to the equivalent generator output SGeqSum equivalent generator power SGEThe equivalent generator active power P is obtained by analyzing the relationGeq. The method mainly comprises the following steps:
5.5.1) setting the intermediate parameter H1Intermediate parameter H2Intermediate parameter H21Intermediate parameter H22Intermediate parameter H23Intermediate parameter H24Intermediate parameter H25And an intermediate parameter H26。
The intermediate parameter H1As follows:
H1=IGeq_diag_realCreal+IGeq_diag_imagCimag。 (32)
in the formula IGeq_diag_realIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagThe real parts of the elements form a matrix. I isGeq_diag_imagIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagThe imaginary part of the element constitutes a matrix. CrealA matrix formed by the real parts of the elements of the constant matrix C. CimagBeing elements of a constant matrix CThe imaginary part constitutes a matrix.
The intermediate parameter H21As follows:
H21=-IGeq_diag_realCimag-IGeq_diag_imagCreal。 (33)
in the formula IGeq_diag_realIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagThe real parts of the elements form a matrix. I isGeq_diag_imagIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagThe imaginary part of the element constitutes a matrix. CrealA matrix formed by the real parts of the elements of the constant matrix C. CimagA matrix formed by the imaginary parts of the elements of the constant matrix C.
The intermediate parameter H22As follows:
in the formula, YGG(GE)(GE)_realA matrix formed by the real parts of the admittance submatrix elements corresponding to the generator nodes in the original external network. Y isGG(GE)(GE)_imagA matrix formed by the imaginary parts of the admittance submatrix elements corresponding to the generator nodes in the original external network. U shapeGE_imagFor the original external network generator node voltage UGEThe imaginary part of (c). U shapeGE_realFor the original external network generator node voltage UGEThe real part of (a). U shapeLE_realFor the original external network node voltage ULEThe real part of (a). U shapeLE_imagFor the original external network node voltage ULEThe imaginary part of (c). Y isGL(GE)(LE)_imagAs an admittance sub-matrix YGL(GE)(LE)The imaginary part of the element constitutes a matrix. Y isGL(GE)(LE)_realAs an admittance sub-matrix YGL(GE)(LE)The real parts of the elements form a matrix.
The intermediate parameter H23As follows:
in the formula, YGG(GE)(GE)_realAdmittance submatrix Y corresponding to generator nodes in original external networkGG(GE)(GE)The real parts of the elements form a matrix. Y isGG(GE)(GE)_imagAdmittance submatrix Y corresponding to generator nodes in original external networkGG(GE)(GE)The imaginary part of the element constitutes a matrix. U shapeGE_imagFor the original external network generator node voltage UGEThe imaginary part of (c). U shapeGE_realFor the original external network generator node voltage UGEThe real part of (a). U shapeLE_realFor the original external network node voltage ULEThe real part of (a). U shapeLE_imagFor the original external network node voltage ULEThe imaginary part of (c). Y isGL(GE)(LE)_imagAs an admittance sub-matrix YGL(GE)(LE)The imaginary part of the element constitutes a matrix. Y isGL(GE)(LE)_realAs an admittance sub-matrix YGL(GE)(LE)The real parts of the elements form a matrix.
The intermediate parameter H24As follows:
H24=-IGeq_diag_realFreal+IGeq_diag_imagFimag。 (36)
in the formula IGeq_diag_realIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagThe real parts of the elements form a matrix. I isGeq_diag_imagIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagThe imaginary part of the element constitutes a matrix. FrealA matrix formed by the real parts of the elements of the constant matrix F. FimagA matrix formed by the imaginary parts of the elements of the constant matrix F.
The intermediate parameter H25As follows:
H25=IGeq_diag_realFimag-IGeq_diag_imagFreal。 (37)
in the formula IGeq_diag_realIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagThe real parts of the elements form a matrix. I isGeq_diag_imagIs composed ofGeqDiagonal as a primary diagonal elementMatrix IGeq_diagThe imaginary part of the element constitutes a matrix. FrealA matrix formed by the real parts of the elements of the constant matrix F. FimagA matrix formed by the imaginary parts of the elements of the constant matrix F.
The intermediate parameter H26As follows:
H26=-IGeq_diag_realDreal-IGeq_diag_imagDimag。 (38)
in the formula IGeq_diag_realIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagThe real parts of the elements form a matrix. I isGeq_diag_imagIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagThe imaginary part of the element constitutes a matrix. DrealA matrix formed by the real parts of the elements of the constant matrix D. DimagA matrix formed by the imaginary parts of the elements of the constant matrix D.
In the formula, H21、H22、H23、H24、H25And H26Respectively, the set intermediate parameters. Y isGL(GE)(LB)_imagAs an admittance sub-matrix YGL(GE)(LB)The imaginary part of the element constitutes a matrix. Y isGL(GE)(LB)_realAs an admittance sub-matrix YGL(GE)(LB)The real parts of the elements form a matrix. U shapeGE_diag_realRepresenting main diagonal elements as external network generator node voltages UGEDiagonal matrix U ofGE_diagThe real parts of the elements form a matrix. U shapeGE_diag_imagRepresenting main diagonal elements as external network generator node voltages UGEDiagonal matrix U ofGE_diagThe imaginary part of the element constitutes a matrix. U shapeLB_imagFor the original border network node voltage ULBThe imaginary part of (c). U shapeLB_realFor the original border network node voltage ULBThe real part of (a).
5.5.2) according to the set intermediate parameter H1Intermediate parameter H2Intermediate parameter H21Intermediate parameter H22Intermediate parameter H23Intermediate parameter H24Intermediate parameter H25And an intermediate parameter H26To obtain the equivalent generator active power PGeq。
The equivalent generator active power PGeqAs follows:
PGeq=H1PGE+H2。 (40)
in the formula, H1And H2Respectively, the set intermediate parameters. PGEThe active power of the external network node is equivalent.
5.6) active Power P of the GeneratorGThe static frequency characteristic of (a) is as follows:
PG=PGmax-KG_diag(f-fGmax)。 (41)
in the formula, PGIs the active power output P of the generator from the ith node at the frequency fGiThe constructed column vector. PGmaxIs the maximum active power output P of the generator from the ith nodeGmaxiThe constructed column vector. KGFor the power frequency static characteristic coefficient K of the generator from the ith nodeGiThe constructed column vector. f. ofGmaxFor the frequency inflection point f when the generator of the ith node no longer has primary frequency modulation capabilityGmaxiThe constructed column vector. f is the frequency. KG_diagIs composed of a power frequency static characteristic coefficient KGAs a matrix of main diagonal elements.
5.7) dividing the active power P of the generator according to the internal network and the external networkGThe division is as follows:
in the formula, PGmax_GIMaximum active output P of generator at ith node of internal networkGmaxiThe constructed column vector. PGmax_GEThe maximum active output P of the generator of the ith node of the external networkGmaxiThe constructed column vector. KG_GIPower frequency of generator for ith node of internal networkCoefficient of static characteristics KGiThe constructed column vector. KG_GEPower frequency static characteristic coefficient K of generator for ith node of external networkGiThe constructed column vector. f. ofGmax_GIFrequency inflection point f when generator no longer has primary frequency modulation capability for ith node of internal networkGmaxiThe constructed column vector. f. ofGmax_GERepresenting a column vector consisting of the frequency inflection points when the external network generator no longer has primary modulation capability. f is the frequency. PGIThe equivalent internal network generator active power. PGEThe equivalent external network generator active power.
5.8) active Power P of the external network Generator to have static frequency characteristicsGESubstituting into the active power of the equivalent generator to obtain the active power output P of the equivalent generator with the static frequency characteristicGeq。
The equivalent generator active power output P with the static frequency characteristicGeqAs follows:
PGeq=PGmax_eq-KGeqf'。 (43)
wherein the column vector f' is an AND P composed of a state variable, i.e., a frequency fGeqThe column vectors of the same dimension. KGeqThe power frequency static characteristic coefficient of the equivalent network generator is obtained. PGmax_eqFor the original maximum active output information P of the external network generatorGmax_GEEquivalent information therein
Wherein, the original maximum active output information P of the external network generatorGmax_GEEquivalent information P thereinGmax_eqAs follows:
PGmax_eq=H1PGmax_GE+H2+KGeqfGmax_GE。 (44)
in the formula, H1And H2Respectively, the set intermediate parameters. f. ofGmax_GEIs a column vector consisting of the frequency inflection points when the external generator no longer has primary modulation capability. KGeqThe power frequency static characteristic coefficient of the equivalent network generator is obtained.
Equivalent network generator power frequency static characteristic coefficient KGeqAs follows:
KGeq=H1KG_GE。 (45)
in the formula, KG_GEPower frequency static characteristic coefficient K of generator for ith node of external networkGiThe constructed column vector. H1Is the set intermediate parameter. KG_GEThe power frequency static characteristic coefficient of the external grid generator is shown.
The technical effect of the present invention is undoubted. The invention provides an equivalence method considering the static frequency characteristics of an external network aiming at the deficiency of equivalence of the existing static topology method. The invention utilizes the equivalent method of the consistency of the tidal current and the sensitivity, improves the equivalence of the external network load and the external network generator, and introduces the equivalence of the static frequency characteristics of the external network load and the external network generator into the equivalence. The method effectively keeps the consistency of the trend and the sensitivity, effectively keeps the static frequency characteristic of the external network, and more truly reflects the actual operation characteristic of the power system.
Drawings
Fig. 1 is an equivalent network diagram.
Detailed Description
The present invention is further illustrated by the following examples, but it should not be construed that the scope of the above-described subject matter is limited to the following examples. Various substitutions and alterations can be made without departing from the technical idea of the invention and the scope of the invention is covered by the present invention according to the common technical knowledge and the conventional means in the field.
Example 1:
referring to fig. 1, an equivalent method considering the static frequency characteristics of an external network mainly includes the following steps:
1) and establishing an original power network model.
Further, the original power network model mainly includes an original external network E, an original network boundary, and an original internal network.
The original external network has E external network nodes.
There are B border nodes in the original network border.
The original internal network has I intranet nodes.The I intranet nodes comprise 1 balanced intranet node and I-1 unbalanced intranet nodes. The total number of elements in the original internal network is N. The number of available elements in the original internal network is Nf。
The basic parameters of the power network mainly comprise element parameters in an original network, an original network topology structure and a load flow calculation result at an approaching moment.
2) Inputting basic parameters of the power network in the original power network model.
Further, the basic parameters of the power network mainly include element parameters in the original network, the topology structure of the original network and the calculation result of the load flow at the moment of approach.
The element parameters in the original network mainly comprise the admittance to the ground of all nodes, the connection load power of all nodes, the impedance of all lines, the susceptance to the ground of all lines, the constraint condition of line transmission power, the impedance of a transformer, the admittance to the ground of the transformer, the transformation ratio of the transformer, the constraint condition of transformer transmission power, the output of a generator, the constraint condition of the output of the generator, the power frequency static characteristic coefficient of the generator and the power frequency static characteristic coefficient of the load.
The original network topology mainly comprises the connection relation of all nodes and the network partition condition.
The near moment power flow calculation result mainly comprises a node admittance matrix, a node voltage matrix and a node injection current matrix.
3) And establishing an equivalent power network model by using an equivalent method of consistency of the power flow and the sensitivity.
Further, the main steps of establishing the equivalent power network model are as follows:
and 3.1) calculating equivalent parameters in the equivalent power network model by using an equivalent method of load flow and sensitivity consistency. The equivalent parameters mainly comprise equivalent branch admittance yeqGij、yeqBiAnd yeqBijEquivalent ground branch admittance yeqBi0Node voltage amplitude U of sum-equivalent generatorGeqBi。
yeqGijRepresenting the original external network at the equivalentAnd (3) equal-value branch admittance among generator nodes.
yeqBijRepresenting the branch admittance between the original external network and the generator at the boundary nodes of the equivalence.
yeqBiRepresenting the isoleg admittance of the original external network between the boundary node and the isogenerator.
And after the equivalent parameters are calculated, drawing an equivalent network map according to the equivalent parameters.
And 3.2) establishing an equivalent power network model according to the equivalent parameters and the original power network model.
4) And calculating the static frequency characteristic of the equivalent load according to the equivalent power network model.
Further, the main steps of calculating the static frequency characteristic of the equivalent load are as follows:
4.1) calculating the equivalent load current ILeq. Equivalent load current ILeqAs follows:
in the formula ILBThe load current of the original boundary network. I isLEThe load current of the original external network. Y isLLAnd the admittance submatrix is corresponding to the load node in the original external network. LB is the original boundary load node. LE is original outer net load node.For said admittance submatrix YLLThe inverse matrix of (c).
4.2) according to the equivalent load current ILeqCalculating the equivalent load power SLeq. Equivalent load power SLeqAs follows:
in the formula, SLBIs the original boundary load power. SLEFor loading power to the original external network。ULB_diagRepresenting main diagonal elements as boundary node voltages ULBThe diagonal matrix of (a). U shapeLE_diagRepresenting the main diagonal element as the external load node voltage ULEThe diagonal matrix of (a).For said admittance submatrixThe companion matrix of (a).For said admittance submatrix YLLThe companion matrix of (a). LB is the original boundary load node. LE is original outer net load node.
4.3) according to the equivalent load power SLeqCalculating the equivalent active load PLeqSum equivalent reactive load QLeq. The method mainly comprises the following steps:
4.3.1) setting an intermediate parameter H:
in the formula (I), the compound is shown in the specification,for said admittance submatrixThe companion matrix of (a).For said admittance submatrix YLLThe companion matrix of (a). LB is the original boundary load node. LE is original outer net load node. U shapeLE_diagRepresenting the main diagonal element as the external load node voltage ULEThe diagonal matrix of (a).
4.3.2) equivalent active load PLeqAs follows:
in the formula, PLBThe active load for the original network boundary. PLEIs the original active load of the external network. U shapeLB_diag_realIs a diagonal matrix ULB_diagThe real parts of the elements form a matrix. U shapeLB_diag_imagIs a diagonal matrix ULB_diagThe imaginary part of the element constitutes a matrix. H is an intermediate parameter. QLEIs the original outer net reactive load. U shapeLB_diagRepresenting main diagonal elements as boundary node voltages ULBThe diagonal matrix of (a).
4.3.3) equivalent reactive load QLeqAs follows:
in the formula, QLBIs the original boundary reactive load. QLEIs the original outer net reactive load. U shapeLB_diag_realIs a diagonal matrix ULB_diagThe real parts of the elements form a matrix. U shapeLB_diag_imagIs a diagonal matrix ULB_diagThe imaginary part of the element constitutes a matrix. H is an intermediate parameter. U shapeLB_diagRepresenting main diagonal elements as boundary node voltages ULBThe diagonal matrix of (a). PLEIs the original active load of the external network.
4.4) setting a new energy station. And setting N as the new energy station node set. And setting L as the new energy station load node set. The new energy mainly comprises wind and light. And setting the new energy source to be a negative load, namely, transmitting the active load of the new energy source outwards.
Active load P of the new energyLAs follows:
PL=PLN+KLP(f-fN)。 (6)
in the formula, PLIs the active load P of the ith node under the frequency fLiThe constructed column vector. f is the frequency. f. ofNIs the nominal frequency. KLPIs composed ofActive load power frequency static characteristic coefficient K of ith nodeLPiThe constructed column vector. PLNRated active load P for the ith nodeLNiThe constructed column vector.
When i ∈ L, PLNiIs the rated active load of the ith node.
When i ∈ N, PLNi=Pprei+ΔPprei。 (7)
In the formula, PpreiAnd predicting active power of the ith node of the new energy station. Delta PpreiAnd predicting an active power error for the ith node of the new energy station. And i is any node of the new energy station. And N is a node set of the new energy station. And L is a set of load nodes for searching the new energy station.
Reactive load Q of the new energyLAs follows:
QL=QLN+KLQ(f-fN)。 (8)
in the formula, QLRespectively the reactive load Q of the ith node under the frequency fLiThe constructed column vector. QLNRated reactive load Q for the ith nodeLNiThe constructed column vector. KLQThe coefficient K of the power frequency static characteristic of the reactive load of the ith nodeLQiThe constructed column vector. f. ofNIs the nominal frequency. f is the frequency.
4.5) dividing the active load P according to the original internal network, the original external network and the original boundary network nodesLAnd reactive load QLThe following are respectively divided:
where LI represents the original internal network load node. KLPThe coefficient K of the active load power frequency static characteristic of the ith nodeLPiThe constructed column vector. PLNRated active load P for the ith nodeLNiThe constructed column vector. PLBThe active load for the original network boundary. PLEIs the original exteriorThe network active load. PLIThe original internal network is loaded with power.
Where LI represents the original internal network load node. QLNRated reactive load Q for the ith nodeLNiThe constructed column vector. KLQThe coefficient K of the power frequency static characteristic of the reactive load of the ith nodeLQiThe constructed column vector. QLBIs the original boundary network reactive load. QLEIs the original external network reactive load. QLIIs the original internal network reactive load.
4.6) substituting the original external network load with the static frequency characteristic in the formula 9 and the formula 10 into the equivalent load of the formula 5 and the formula 6, thereby obtaining the equivalent active load and the equivalent reactive load with the static frequency characteristic. The method mainly comprises the following steps:
4.6.1) calculating the parameter A1Parameter A2Parameter A3And parameter A4。
A1=H_realPLN_LE-H_imagQLN_LE。 (11)
In the formula, H_realIs the real part of the intermediate parameter H. PLN_LEThe equivalent rated active load of the external network. QLN_LEThe equivalent rated reactive load of the external network.
A2=H_imagPLN_LE+H_realQLN_LE。 (12)
In the formula, H_imagIs the imaginary part of the intermediate parameter H. PLN_LEThe equivalent rated active load of the external network. QLN_LEThe equivalent rated reactive load of the external network.
A3=H_realKLP_LE-H_imagKLQ_LE。 (13)
In the formula, H_realIs the real part of the intermediate parameter H. KLP_LEFor the ith section in the external networkActive load power frequency static characteristic coefficient K of pointLPiThe constructed column vector. KLQ_LEThe coefficient K of the reactive load power frequency static characteristic of the ith node in the external networkLQiThe constructed column vector. H_imagIs the imaginary part of the intermediate parameter H.
A4=H_imagKLP_LE+H_realKLQ_LE。 (14)
In the formula, H_imagIs the imaginary part of the intermediate parameter H. KLP_LEThe active load power frequency static characteristic coefficient K of the ith node in the external networkLPiThe constructed column vector. KLQ_LEThe coefficient K of the reactive load power frequency static characteristic of the ith node in the external networkLQiThe constructed column vector. H_realIs the imaginary part of the intermediate parameter H.
4.6.2) according to parameter A3And parameter A4Calculating power frequency static characteristic coefficient K of equivalent active loadLeq_PPower frequency static characteristic coefficient K of sum equivalent reactive loadLeq_Q。
Equivalent active load power frequency static characteristic coefficient KLeq_PAs follows:
KLeq_p=KLP_LB-ULB_diag_realA3+ULB_diag_imagA4。 (15)
in the formula, KLP_LBActive load power frequency static characteristic coefficient K of ith node of boundary networkLPi_LBThe constructed column vector. U shapeLB_diag_realRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagThe real parts of the elements form a matrix. A. the3Is a set parameter. A. the4Is a set parameter.
Equivalent reactive load power frequency static characteristic coefficient KLeq_QAs follows:
KLeq_Q=KLQ_LB-ULB_diag_realA4-ULB_diag_imagA3。 (16)
in the formula, KLQ_LBThe coefficient K of the power frequency static characteristic of the reactive load of the ith node of the boundary networkLQi_LBThe constructed column vector. U shapeLB_diag_realRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagThe real parts of the elements form a matrix. A. the3Is a set parameter. A. the4Is a set parameter.
4.6.3) according to the parameter A1And parameter A2Calculating equivalent rated active load PLeq_LNRated reactive load Q of sum equivalentLeq_LN。
Equivalent rated active load PLeq_LNAs follows:
PLeq_LN=PLN_LB-ULB_diag_realA1+ULB_diag_imagA2。 (17)
in the formula, PLN_LBIs the equivalent rated active load of the boundary network. A. the1Is a set parameter. A. the2Is a set parameter. U shapeLB_diag_realRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagThe real parts of the elements form a matrix. U shapeLB_diag_imagRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagThe imaginary part of the element constitutes a matrix.
Equivalent rated reactive load QLeq_LNAs follows:
QLeq_LN=QLN_LB-ULB_diag_real A2-ULB_diag_imag A1。 (18)
in the formula, QLN_LBIs the equivalent rated reactive load of the boundary network. U shapeLB_diag_realRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagThe real parts of the elements form a matrix. U shapeLB_diag_imagRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagThe imaginary part of the element constitutes a matrix. A. the1Is a set parameter. A. the2Is a set parameter.
4.6.4) calculating the equivalent active load PLeqSum equivalent reactive load QLeq。
Equivalence ofActive load PLeqAs follows:
PLeq=PLeq_LN+KLeq_P(f-fN)。 (19)
in the formula, PLeq_LNIs the equivalent rated active load. f is the frequency. f. ofNIs the nominal frequency. KLeq_PThe power frequency static characteristic coefficient is the equivalent power load.
Equivalent reactive load QLeqAs follows:
QLeq=QLeq_LN+KLeq_Q(f-fN)。 (20)
in the formula, QLeq_LNThe load is equivalent rated reactive load. f is the frequency. f. ofNIs the nominal frequency. QLeq_PThe power frequency static characteristic coefficient is equivalent reactive load.
5) And calculating the static frequency characteristic of the equivalent generator according to the equivalent power network model.
Further, the main steps of calculating the static frequency characteristic of the equivalent generator are as follows:
5.1) calculating the Current I of the equivalent Generator node GeqGeq. The method mainly comprises the following steps:
5.1.1) calculating the original network generator node injection current IG:
In the formula IGEIs the original external network generator node current. I isGIIs the original internal network generator node current.
UGEIs the original external network generator node voltage. U shapeGIIs the original external network generator voltage. U shapeLEIs the original external network voltage. U shapeLBIs the original boundary network voltage. U shapeLIIs the original internal network voltage.
YGG(GE)(GE)The admittance submatrix corresponding to the generator node in the original external network. Y isGG(GI)(GI)Admittance for generator node correspondence in original internal networkA sub-matrix. Y isGL(GE)(LE)And the admittance submatrices are corresponding to the generator nodes in the original external network and the nodes of the original external network. Y isGL(GE)(LB)The method is characterized in that generator nodes are taken as corresponding rows and original boundary network nodes are taken as corresponding columns in an original external network, and therefore an admittance submatrix is generated.
GE is the original external network generator node. The GI is the original internal network generator node. GL is the original border network generator node. LI is the original internal network node. LB is the original border network node. The LE is the original external network node.
5.1.2) obtaining the original external network generator node voltage U according to the formula 21GE. The original external network generator node voltage UGEAs follows:
in the formula (I), the compound is shown in the specification,admittance submatrix Y corresponding to generator nodes in original external networkGG(GE)(GE)The inverse matrix of (c). I isGEIs the generator node current in the original external network. U shapeLEIs the original external network voltage. U shapeLBIs the original boundary network voltage. Y isGL(GE)(LE)In the original network, generator nodes of the original external network are taken as corresponding rows and original external network nodes are taken as corresponding columns, and therefore an admittance submatrix is generated. Y isGL(GE)(LB)In the original network, generator nodes of the original external network are taken as corresponding rows, and original boundary network nodes are taken as corresponding columns, so that an admittance submatrix is generated.
5.1.3) obtaining equivalent generator node voltage U according to a static equivalence method based on consistency of power flow and sensitivityGeq. The equivalent generator node voltage UGeqAs follows:
in the formula of UGEIs the original external network generator node voltage.In the equivalent network, an admittance submatrix Y 'is generated by taking equivalent load nodes as corresponding rows and equivalent generator nodes as corresponding columns'LGThe inverse matrix of (c). Y isLGThe load nodes are used as corresponding rows and the generator nodes are used as corresponding columns in the original network, and therefore the admittance submatrix is generated. Y isLLAnd the admittance submatrix is corresponding to the load node in the original external network.For said admittance submatrix YLLThe inverse matrix of (c). LB is the original boundary load node. LE is original outer net load node. GE is the original external network generator node. Gep is an equivalent generator node.
5.1.4) calculating the injection current I 'of the generator node in the equivalent network'G. Generator node injection current I 'in equivalent network'GAs follows:
of formula (II) to (III)'GG(Geq)(Geq)And obtaining the admittance submatrix corresponding to the generator node in the equivalent external network. Y isGG(GI)(GI)The admittance submatrix corresponding to the generator node in the original internal network. U shapeGIIs the original external network generator voltage. U shapeGeqIs the equivalent network generator node voltage. Y'GL(Geq)(LB)In the equivalent external network, equivalent generator nodes are taken as corresponding rows and equivalent boundary network nodes are taken as corresponding columns, so that an admittance submatrix is generated. Y'GL(GI)(LB)In the equivalent network, generator nodes of an equivalent internal network are taken as corresponding rows, and equivalent boundary network nodes are taken as corresponding columns, so that an admittance submatrix is generated. Y'GL(GI)(LI)For an equivalent network, with an equivalent internal networkThe generator nodes are corresponding rows, the equivalent internal network nodes are corresponding columns, and therefore the admittance submatrix is generated. U shapeLIIs the original internal network voltage. U shapeLBIs the original boundary network voltage.
5.1.5) from equation 24, the current I at the equivalent generator node Geq is obtainedGeq. Current I of the equivalent generator node GeqGeqAs follows:
of formula (II) to (III)'GG(Geq)(Geq)And obtaining the admittance submatrix corresponding to the generator node in the equivalent external network. Y isLGThe load nodes are used as corresponding rows and the generator nodes are used as corresponding columns in the original network, and therefore the admittance submatrix is generated. Y isLLAnd the admittance submatrix is corresponding to the load node in the original external network.For said admittance submatrix YLLThe inverse matrix of (c). LB is the original boundary load node. LE is original outer net load node. GE is the original external network generator node. U shapeLBIs the original boundary network voltage. EGEIs the original external network generator node voltage.
5.2) calculating to obtain the voltage U of the equivalent generator nodeGeq. The method mainly comprises the following steps:
5.2.1) setting a constant matrix C, a constant matrix F and a constant matrix D.
The constant matrix C is shown below:
in the formula, YLLAnd the admittance submatrix is corresponding to the load node in the original external network.For said admittance submatrix YLLThe inverse matrix of (c). LB is the original boundary load node. LE is original outer net load node. GE is the original external network generator node. Y isLGThe load nodes are used as corresponding rows and the generator nodes are used as corresponding columns in the original network, and therefore the admittance submatrix is generated.
The constant matrix F is shown below:
in the formula, YLLAnd the admittance submatrix is corresponding to the load node in the original external network.For said admittance submatrix YLLThe inverse matrix of (c). LB is the original boundary load node. LE is original outer net load node. GE is the original external network generator node. Y isLGThe load nodes are used as corresponding rows and the generator nodes are used as corresponding columns in the original network, and therefore the admittance submatrix is generated.
The constant matrix D is as follows:
in the formula, YLLAnd the admittance submatrix is corresponding to the load node in the original external network.For said admittance submatrix YLLThe inverse matrix of (c). LB is the original boundary load node. LE is original outer net load node. GE is the original external network generator node. Y isLGThe load nodes are used as corresponding rows and the generator nodes are used as corresponding columns in the original network, and therefore the admittance submatrix is generated.
5.2.2) voltage U of the equivalent generator node according to the constant matrix C, the constant matrix F and the constant matrix DGeqAs follows:
in the formula (I), the compound is shown in the specification,for outer net generator power matrix SGEThe companion matrix of (a). The matrix C, the matrix F and the matrix D are respectively set constant matrixes. U shapeLBIs the original boundary network voltage.
5.3) calculating the equivalent generator output SGeq. Equivalent generator output SGeqAs follows:
in the formula IGeq_diagIs composed ofGeqA diagonal matrix as a main diagonal element.For the diagonal matrix IGeq_diagThe companion matrix of (a). U shapeGEQIs the voltage at the equivalent generator node.
5.4) according to the equivalent generator output SGeqSum equivalent generator power SGETo obtain the equivalent generator output SGeqSum equivalent generator power SGEThe analytic relationship of (1):
in the formula, the matrix C, the matrix F, and the matrix D are respectively set constant matrices.For the diagonal matrix IGeq_diagThe companion matrix of (a). U shapeLBIs the original boundary network voltage.Is outsideNetwork generator power matrix SGEThe companion matrix of (a).
5.5) according to the equivalent generator output SGeqSum equivalent generator power SGEThe equivalent generator active power P is obtained by analyzing the relationGeq. The method mainly comprises the following steps:
5.5.1) setting the intermediate parameter H1Intermediate parameter H2Intermediate parameter H21Intermediate parameter H22Intermediate parameter H23Intermediate parameter H24Intermediate parameter H25And an intermediate parameter H26。
The intermediate parameter H1As follows:
H1=IGeq_diag_realCreal+IGeq_diag_imagCimag。 (32)
in the formula IGeq_diag_realIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagThe real parts of the elements form a matrix. I isGeq_diag_imagIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagThe imaginary part of the element constitutes a matrix. CrealA matrix formed by the real parts of the elements of the constant matrix C. CimagA matrix formed by the imaginary parts of the elements of the constant matrix C.
The intermediate parameter H21As follows:
H21=-IGeq_diag_realCimag-IGeq_diag_imagCreal。 (33)
in the formula IGeq_diag_realIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagThe real parts of the elements form a matrix. I isGeq_diag_imagIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagThe imaginary part of the element constitutes a matrix. CrealA matrix formed by the real parts of the elements of the constant matrix C. CimagA matrix formed by the imaginary parts of the elements of the constant matrix C.
The intermediate parameter H22As follows:
in the formula, YGG(GE)(GE)_realA matrix formed by the real parts of the admittance submatrix elements corresponding to the generator nodes in the original external network. Y isGG(GE)(GE)_imagA matrix formed by the imaginary parts of the admittance submatrix elements corresponding to the generator nodes in the original external network. U shapeGE_imagFor the original external network generator node voltage UGEThe imaginary part of (c). U shapeGE_realFor the original external network generator node voltage UGEThe real part of (a). U shapeLE_realFor the original external network node voltage ULEThe real part of (a). U shapeLE_imagFor the original external network node voltage ULEThe imaginary part of (c). Y isGL(GE)(LE)_imagAs an admittance sub-matrix YGL(GE)(LE)The imaginary part of the element constitutes a matrix. Y isGL(GE)(LE)_realAs an admittance sub-matrix YGL(GE)(LE)The real parts of the elements form a matrix.
The intermediate parameter H23As follows:
in the formula, YGG(GE)(GE)_realAdmittance submatrix Y corresponding to generator nodes in original external networkGG(GE)(GE)The real parts of the elements form a matrix. Y isGG(GE)(GE)_imagAdmittance submatrix Y corresponding to generator nodes in original external networkGG(GE)(GE)The imaginary part of the element constitutes a matrix. U shapeGE_imagFor the original external network generator node voltage UGEThe imaginary part of (c). U shapeGE_realFor the original external network generator node voltage UGEThe real part of (a). U shapeLE_realFor the original external network node voltage ULEThe real part of (a). U shapeLE_imagFor the original external network node voltage ULEThe imaginary part of (c). Y isGL(GE)(LE)_imagAs an admittance sub-matrix YGL(GE)(LE)The imaginary part of the element constitutes a matrix. Y isGL(GE)(LE)_realAs an admittance sub-matrix YGL(GE)(LE)Element(s)The real part of (a).
The intermediate parameter H24As follows:
H24=-IGeq_diag_realFreal+IGeq_diag_imagFimag。 (36)
in the formula IGeq_diag_realIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagThe real parts of the elements form a matrix. I isGeq_diag_imagIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagThe imaginary part of the element constitutes a matrix. FrealA matrix formed by the real parts of the elements of the constant matrix F. FimagA matrix formed by the imaginary parts of the elements of the constant matrix F.
The intermediate parameter H25As follows:
H25=IGeq_diag_realFimag-IGeq_diag_imagFreal。 (37)
in the formula IGeq_diag_realIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagThe real parts of the elements form a matrix. I isGeq_diag_imagIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagThe imaginary part of the element constitutes a matrix. FrealA matrix formed by the real parts of the elements of the constant matrix F. FimagA matrix formed by the imaginary parts of the elements of the constant matrix F.
The intermediate parameter H26As follows:
H26=-IGeq_diag_realDreal-IGeq_diag_imagDimag。 (38)
in the formula IGeq_diag_realIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagThe real parts of the elements form a matrix. I isGeq_diag_imagIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagThe imaginary part of the element constitutes a matrix. DrealA matrix formed by the real parts of the elements of the constant matrix D. DimagBeing elements of a constant matrix DThe imaginary part constitutes a matrix.
In the formula, H21、H22、H23、H24、H25And H26Respectively, the set intermediate parameters. Y isGL(GE)(LB)_imagAs an admittance sub-matrix YGL(GE)(LB)The imaginary part of the element constitutes a matrix. Y isGL(GE)(LB)_realAs an admittance sub-matrix YGL(GE)(LB)The real parts of the elements form a matrix. U shapeGE_diag_realRepresenting main diagonal elements as external network generator node voltages UGEDiagonal matrix U ofGE_diagThe real parts of the elements form a matrix. U shapeGE_diag_imagRepresenting main diagonal elements as external network generator node voltages UGEDiagonal matrix U ofGE_diagThe imaginary part of the element constitutes a matrix. U shapeLB_imagFor the original border network node voltage ULBThe imaginary part of (c). U shapeLB_realFor the original border network node voltage ULBThe real part of (a).
5.5.2) according to the set intermediate parameter H1Intermediate parameter H2Intermediate parameter H21Intermediate parameter H22Intermediate parameter H23Intermediate parameter H24Intermediate parameter H25And an intermediate parameter H26To obtain the equivalent generator active power PGeq。
The equivalent generator active power PGeqAs follows:
PGeq=H1PGE+H2。 (40)
in the formula, H1And H2Respectively, the set intermediate parameters. PGEThe active power of the external network node is equivalent.
5.6) active Power P of the GeneratorGThe static frequency characteristic of (a) is as follows:
PG=PGmax-KG_diag(f-fGmax)。 (41)
in the formula (I), the compound is shown in the specification,PGis the active power output P of the generator from the ith node at the frequency fGiThe constructed column vector. PGmaxIs the maximum active power output P of the generator from the ith nodeGmaxiThe constructed column vector. KGFor the power frequency static characteristic coefficient K of the generator from the ith nodeGiThe constructed column vector. f. ofGmaxFor the frequency inflection point f when the generator of the ith node no longer has primary frequency modulation capabilityGmaxiThe constructed column vector. f is the frequency. KG_diagIs composed of a power frequency static characteristic coefficient KGAs a matrix of main diagonal elements.
5.7) dividing the active power P of the generator according to the internal network and the external networkGThe division is as follows:
in the formula, PGmax_GIMaximum active output P of generator at ith node of internal networkGmaxiThe constructed column vector. PGmax_GEThe maximum active output P of the generator of the ith node of the external networkGmaxiThe constructed column vector. KG_GIPower frequency static characteristic coefficient K of generator for ith node of internal networkGiThe constructed column vector. KG_GEPower frequency static characteristic coefficient K of generator for ith node of external networkGiThe constructed column vector. f. ofGmax_GIFrequency inflection point f when generator no longer has primary frequency modulation capability for ith node of internal networkGmaxiThe constructed column vector. f. ofGmax_GERepresenting a column vector consisting of the frequency inflection points when the external network generator no longer has primary modulation capability. f is the frequency. PGIThe equivalent internal network generator active power. PGEThe equivalent external network generator active power.
5.8) active Power P of the external network Generator to have static frequency characteristicsGESubstituting into the active power of the equivalent generator to obtain the active power output P of the equivalent generator with the static frequency characteristicGeq。
Said frequency has a static frequencyEquivalent generator active power output P of characteristicGeqAs follows:
PGeq=PGmax_eq-KGeqf'。 (43)
wherein the column vector f' is an AND P composed of a state variable, i.e., a frequency fGeqThe column vectors of the same dimension. KGeqThe power frequency static characteristic coefficient of the equivalent network generator is obtained. PGmax_eqFor the original maximum active output information P of the external network generatorGmax_GEEquivalent information within.
Wherein, the original maximum active output information P of the external network generatorGmax_GEEquivalent information P thereinGmax_eqAs follows:
PGmax_eq=H1PGmax_GE+H2+KGeqfGmax_GE。 (44)
in the formula, H1And H2Respectively, the set intermediate parameters. f. ofGmax_GEIs a column vector consisting of the frequency inflection points when the external generator no longer has primary modulation capability. KGeqThe power frequency static characteristic coefficient of the equivalent network generator is obtained.
Equivalent network generator power frequency static characteristic coefficient KGeqAs follows:
KGeq=H1KG_GE。 (45)
in the formula, KG_GEPower frequency static characteristic coefficient K of generator for ith node of external networkGiThe constructed column vector. H1Is the set intermediate parameter. KG_GEThe power frequency static characteristic coefficient of the external grid generator is shown.
Example 2:
an experiment for verifying an equivalent method considering static frequency characteristics of an external network mainly comprises the following steps:
1) and establishing a test system.
In the IEEE9 node system, the system is divided into an external network, a border node, and an internal network: an external node: node 2, node 3, node 6 and node 7. Boundary nodes: node 5 and node 9. Internal nodes: node 1 and node 4, where node 1 is a balanced node. In the IEEE118 node system, the system is also divided into an external network, a border node, and an internal network: an external node: node 80, node 83 to node 112. Boundary nodes: node 81 and node 82. Internal nodes: node 1 to node 79, node 113 to node 118, with node 69 being a balanced node.
In both test systems, the correlation coefficient between the outer net loads was taken to be 0.1. And the power frequency static characteristic coefficient per unit values of the conventional active load and the conventional reactive load are respectively 2 and-1.5. And the power frequency static characteristic coefficient per unit value of the generator at the unbalanced node and the balanced node is respectively 20 and 25. The rated frequency of the system is 50Hz, and the upper and lower limits of the frequency are 50.2Hz and 49.8Hz respectively.
2) Different comparison models
In order to verify the correctness and the effectiveness of the equivalent method considering the static frequency characteristics of the external network, the following 4 load flow calculation methods are adopted for carrying out static safety analysis and comparison:
m0: load flow calculation method based on original network (reference method).
M1: the invention provides an equivalent load flow calculation method.
M2: the equivalent method based on the consistency of the power flow and the sensitivity (namely 'StaticEvalintMethodPasedConponentParalyticationRepression and Sensiwitness Consistence') is an equivalent power flow calculation method only considering the sensitivity of an external network.
M3: and the load flow calculation method is based on a method of equating the external network to be a balance node, a PV node or a PQ node. Using an absolute error index e1And relative error index e2And measuring the error of the M1-M3 method and the M0 method.
3) Simulation verification of static frequency characteristic of equivalent method
The internal network load of the IEEE9 node system and the IEEE118 node system is increased by 12% and 8% in the same proportion respectively, and static security analysis is performed by utilizing M0-M3 respectively.
Table 1 lists the error analysis results of the system frequency and the maximum error branch active power.
As can be seen from Table 1, as the load on the intranet increases, the original network-based M0 method and the textThe proposed M1 method has no out-of-limit frequency, and the difference between the two is small, the maximum absolute error e1Only 0.03 HZ. However, the frequencies of the M2 and M3 models have been out of limit, with the maximum absolute error e1Respectively reaching 0.06Hz and 1.11 Hz. Meanwhile, the branch with the largest active power error is selected for comparison (the node 9 system is a 1-4 branch, and the node 118 system is a 77-82 branch). For the M1 model proposed by the invention, the maximum relative error e of the branch active power2Only 2.5%, while the maximum relative error e of the M2, M3 methods2Respectively up to 18.4% and 430.92%. Therefore, the method can effectively retain the static frequency characteristic information of the external network and improve the static security analysis precision. Value and e in Table 11The units of (b) correspond to the units of f, P, respectively, Hz, MW. e.g. of the type2The unit of (c) is%.
TABLE 1IEEE9 node system, IEEE118 node system frequency and error analysis results of maximum error branch active power
Therefore, the method effectively keeps the consistency of the trend and the sensitivity, effectively keeps the static frequency characteristic of the external network, and more truly reflects the actual operation characteristic of the power system.
Claims (2)
1. An equivalence method considering static frequency characteristics of an external network is characterized by comprising the following steps:
1) establishing an original power network model;
2) inputting basic parameters of the power network in the original power network model;
3) establishing an equivalent power network model by using an equivalent method of consistency of power flow and sensitivity;
the equivalent power network model is established by the following steps:
3.1) calculating equivalent parameters in the equivalent power network model by using an equivalent method of consistency of power flow and sensitivity; the equivalence parameter comprises an equivalence branch guideNano yeqGij、yeqBiAnd yeqBijEquivalent ground branch admittance yeqBi0Node voltage amplitude U of sum-equivalent generatorGeqBi;
yeqGijRepresenting the admittance of an equivalent branch between nodes of an equivalent generator of an original external network; y iseqBijRepresenting the branch admittance between the boundary nodes of the equivalence of the original external network and the generator; y iseqBiRepresenting the admittance of an equivalent branch between a boundary node and an equivalent generator of an original external network;
3.2) establishing an equivalent power network model according to the equivalent parameters and the original power network model;
4) calculating the static frequency characteristic of the equivalent load according to the equivalent power network model;
the steps of calculating the static frequency characteristic of the equivalent load are as follows:
4.1) calculating the equivalent load current ILeq(ii) a Equivalent load current ILeqAs follows:
in the formula ILBLoad current of the original boundary network; i isLEIs the load current of the original external network; y isLLAn admittance submatrix corresponding to a load node in an original external network; LB is an original boundary load node; LE is original outer net load node;for said admittance submatrix YLLThe inverse matrix of (d);
4.2) according to the equivalent load current ILeqCalculating the equivalent load power SLeq(ii) a Equivalent load power SLeqAs follows:
in the formula, SLBIs the original boundary load power; sLEIs the original outer net load power; u shapeLB_diagRepresenting main diagonal elements as boundary node voltages ULBA diagonal matrix of (a); u shapeLE_diagRepresenting the main diagonal element as the external load node voltage ULEA diagonal matrix of (a);for said admittance submatrixThe companion matrix of (a);for said admittance submatrix YLLThe companion matrix of (a); LB is an original boundary load node; LE is original outer net load node;
4.3) according to the equivalent load power SLeqCalculating the equivalent active load PLeqSum equivalent reactive load QLeq(ii) a The method comprises the following steps:
4.3.1) setting an intermediate parameter H:
in the formula (I), the compound is shown in the specification,for said admittance submatrixThe companion matrix of (a);for said admittance submatrix YLLThe companion matrix of (a); LB is an original boundary load node; LE is original outer net load node; u shapeLE_diagIndicating a major diagonal element as being externally negativeCharge node voltage ULEA diagonal matrix of (a);
4.3.2) equivalent active load PLeqAs follows:
in the formula, PLBActive load for original network boundary; pLEIs the original external network active load; u shapeLB_diag_realIs a diagonal matrix ULB_diagA matrix of real parts of the elements; u shapeLB_diag_imagIs a diagonal matrix ULB_diagA matrix of imaginary parts of the elements; h is an intermediate parameter; qLEIs the original outer net reactive load; u shapeLB_diagRepresenting main diagonal elements as boundary node voltages ULBA diagonal matrix of (a);
4.3.3) equivalent reactive load QLeqAs follows:
in the formula, QLBIs the original boundary reactive load; qLEIs the original outer net reactive load; u shapeLB_diag_realIs a diagonal matrix ULB_diagA matrix of real parts of the elements; u shapeLB_diag_imagIs a diagonal matrix ULB_diagA matrix of imaginary parts of the elements; h is an intermediate parameter; u shapeLB_diagRepresenting main diagonal elements as boundary node voltages ULBA diagonal matrix of (a); pLEIs the original external network active load;
4.4) setting a new energy station; setting N as the new energy station node set; setting L as the new energy station load node set; the new energy comprises wind and light; setting the new energy source to be a negative load, namely, the active load of the new energy source is transmitted outwards;
active load P of the new energyLAs follows:
PL=PLN+KLP(f-fN); (6)
in the formula, PLIs the active load P of the ith node under the frequency fLiA constructed column vector; f is the frequency; f. ofNIs a rated frequency; kLPThe coefficient K of the active load power frequency static characteristic of the ith nodeLPiA constructed column vector; pLNRated active load P for the ith nodeLNiA constructed column vector;
when i ∈ L, PLNiRated active load of the ith node;
when i ∈ N, PLNi=Pprei+ΔPprei; (7)
In the formula, PpreiPredicting active power for the ith node of the new energy station; delta PpreiPredicting an active power error for the ith node of the new energy station; i is any node of the new energy station; n is a node set of the new energy station; l is a set of load nodes for searching the new energy station;
reactive load Q of the new energyLAs follows:
QL=QLN+KLQ(f-fN); (8)
in the formula, QLRespectively the reactive load Q of the ith node under the frequency fLiA constructed column vector; qLNRated reactive load Q for the ith nodeLNiA constructed column vector; kLQThe coefficient K of the power frequency static characteristic of the reactive load of the ith nodeLQiA constructed column vector; f. ofNIs a rated frequency; f is the frequency;
4.5) dividing the active load P according to the original internal network, the original external network and the original boundary network nodesLAnd reactive load QLThe following are respectively divided:
wherein LI represents the original internal network load node; kLPIs active from the ith nodeCoefficient of static characteristics of load power frequency KLPiA constructed column vector; pLNRated active load P for the ith nodeLNiA constructed column vector; pLBActive load for original network boundary; pLEIs the original external network active load; pLIIs the original internal network active load; LB is an original boundary load node; LE is original outer net load node;
wherein LI represents the original internal network load node; qLNRated reactive load Q for the ith nodeLNiA constructed column vector; kLQThe coefficient K of the power frequency static characteristic of the reactive load of the ith nodeLQiA constructed column vector; qLBIs the original boundary network reactive load; qLEIs the original external network reactive load; qLIIs the original internal network reactive load;
4.6) substituting the original external network load with the static frequency characteristic in the formula (9) and the formula (10) into the equivalent load of the formula (5) and the formula (6) so as to obtain the equivalent active load and the equivalent reactive load with the static frequency characteristic; the method comprises the following steps:
4.6.1) setting the parameter A1Parameter A2Parameter A3And parameter A4And calculating A sequentially1Parameter A2Parameter A3And parameter A4;
A1=H_realPLN_LE-H_imagQLN_LE; (11)
In the formula, H_realIs the real part of the intermediate parameter H; pLN_LEThe equivalent rated active load of the external network; qLN_LEThe equivalent rated reactive load of the external network; h_imagIs the imaginary part of the intermediate parameter H;
A2=H_imagPLN_LE+H_realQLN_LE; (12)
in the formula, H_imagIs the imaginary part of the intermediate parameter H; pLN_LEThe equivalent rated active load of the external network; qLN_LEThe equivalent rated reactive load of the external network; h_realIs the real part of the intermediate parameter H;
A3=H_realKLP_LE-H_imagKLQ_LE; (13)
in the formula, H_realIs the real part of the intermediate parameter H; kLP_LEThe active load power frequency static characteristic coefficient K of the ith node in the external networkLPiA constructed column vector; kLQ_LEThe coefficient K of the reactive load power frequency static characteristic of the ith node in the external networkLQiA constructed column vector; h_imagIs the imaginary part of the intermediate parameter H;
A4=H_imagKLP_LE+H_realKLQ_LE; (14)
in the formula, H_imagIs the imaginary part of the intermediate parameter H; kLP_LEThe active load power frequency static characteristic coefficient K of the ith node in the external networkLPiA constructed column vector; kLQ_LEThe coefficient K of the reactive load power frequency static characteristic of the ith node in the external networkLQiA constructed column vector; h_realIs the imaginary part of the intermediate parameter H;
4.6.2) according to parameter A3And parameter A4Calculating power frequency static characteristic coefficient K of equivalent active loadLeq_PPower frequency static characteristic coefficient K of sum equivalent reactive loadLeq_Q;
Equivalent active load power frequency static characteristic coefficient KLeq_PAs follows:
KLeq_p=KLP_LB-ULB_diag_realA3+ULB_diag_imagA4; (15)
in the formula, KLP_LBActive load power frequency static characteristic coefficient K of ith node of boundary networkLPi_LBA constructed column vector; u shapeLB_diag_realRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagOf elementsA matrix of real parts; a. the3Is a set parameter; a. the4Is a set parameter; u shapeLB_diag_imagRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagA matrix of imaginary parts of the elements;
equivalent reactive load power frequency static characteristic coefficient KLeq_QAs follows:
KLeq_Q=KLQ_LB-ULB_diag_realA4-ULB_diag_imagA3; (16)
in the formula, KLQ_LBThe coefficient K of the power frequency static characteristic of the reactive load of the ith node of the boundary networkLQi_LBA constructed column vector; u shapeLB_diag_realRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagA matrix of real parts of the elements; a. the3Is a set parameter; a. the4Is a set parameter; u shapeLB_diag_imagRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagA matrix of imaginary parts of the elements;
4.6.3) according to the parameter A1And parameter A2Calculating equivalent rated active load PLeq_LNRated reactive load Q of sum equivalentLeq_LN;
Equivalent rated active load PLeq_LNAs follows:
PLeq_LN=PLN_LB-ULB_diag_realA1+ULB_diag_imagA2; (17)
in the formula, PLN_LBThe equivalent rated active load of the boundary network; a. the1Is a set parameter; a. the2Is a set parameter; u shapeLB_diag_realRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagA matrix of real parts of the elements; u shapeLB_diag_imagRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagA matrix of imaginary parts of the elements;
equivalent rated reactive load QLeq_LNAs follows:
QLeq_LN=QLN_LB-ULB_diag_realA2-ULB_diag_imagA1; (18)
in the formula, QLN_LBIs the equivalent rated reactive load of the boundary network; u shapeLB_diag_realRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagA matrix of real parts of the elements; u shapeLB_diag_imagRepresenting main diagonal elements as boundary node voltages ULBDiagonal matrix U ofLB_diagA matrix of imaginary parts of the elements; a. the1Is a set parameter; a. the2Is a set parameter;
4.6.4) calculating the equivalent active load PLeqSum equivalent reactive load QLeq;
Equivalent active load PLeqAs follows:
PLeq=PLeq_LN+KLeq_P(f-fN); (19)
in the formula, PLeq_LNIs the equivalent rated active load; f is the frequency; f. ofNIs a rated frequency; kLeq_PThe power frequency static characteristic coefficient is equivalent active load;
equivalent reactive load QLeqAs follows:
QLeq=QLeq_LN+KLeq_Q(f-fN); (20)
in the formula, QLeq_LNIs an equivalent rated reactive load; f is the frequency; f. ofNIs a rated frequency; qLeq_PThe power frequency static characteristic coefficient is equivalent reactive load;
5) calculating the static frequency characteristic of the equivalent generator according to the equivalent power network model;
the steps of calculating the static frequency characteristic of the equivalent generator are as follows:
5.1) calculating the Current I of the equivalent Generator node GeqGeq(ii) a The method comprises the following steps:
5.1.1) calculating the original network generator node injection current IG:
In the formula IGEIs the original external network generator node current; i isGIIs the original internal network generator node current;
UGEis the original external network generator node voltage; u shapeGIIs the original external network generator voltage; u shapeLEIs the original external network voltage; u shapeLBIs the original boundary network voltage; u shapeLIIs the original internal network voltage;
YGG(GE)(GE)the admittance submatrix corresponding to the generator node in the original external network;
YGG(GI)(GI)the admittance submatrix corresponding to the generator node in the original internal network;
YGL(GE)(LE)the admittance submatrixes corresponding to the generator nodes in the original external network and the original external network nodes;
YGL(GE)(LB)in an original external network, generator nodes are taken as corresponding rows and original boundary network nodes are taken as corresponding columns, so that an admittance submatrix is generated;
GE is an original external network generator node; GI is the original internal network generator node; GL is an original boundary network generator node; LI is an original internal network node; LB is an original boundary network node; LE is original external network node;
5.1.2) obtaining the original external network generator node voltage U according to the formula (21)GE(ii) a The original external network generator node voltage UGEAs follows:
in the formula (I), the compound is shown in the specification,admittance submatrix Y corresponding to generator nodes in original external networkGG(GE)(GE)The inverse matrix of (d); i isGEIs the generator node current in the original external network; u shapeLEIs the original external network voltage; u shapeLBIs the original boundary network voltage; y isGL(GE)(LE)In the original network, generator nodes of the original external network are taken as corresponding rows and original external network nodes are taken as corresponding columns, so that an admittance submatrix is generated; y isGL(GE)(LB)In the original network, generator nodes of the original external network are taken as corresponding rows and original boundary network nodes are taken as corresponding columns, so that an admittance submatrix is generated;
5.1.3) obtaining equivalent generator node voltage U according to a static equivalence method based on consistency of power flow and sensitivityGeq(ii) a The equivalent generator node voltage UGeqAs follows:
in the formula of UGEIs the original external network generator node voltage;in the equivalent network, an admittance submatrix Y 'is generated by taking equivalent load nodes as corresponding rows and equivalent generator nodes as corresponding columns'LGThe inverse matrix of (d); y isLGIn the original network, load nodes are used as corresponding rows, generator nodes are used as corresponding columns, and therefore an admittance submatrix is generated; y isLLAn admittance submatrix corresponding to a load node in an original external network;for said admittance submatrix YLLThe inverse matrix of (d); LB is an original boundary load node; LE is; GE is an original external network generator node; gep is an equivalent generator node;
5.1.4) calculating the injection current I 'of the generator node in the equivalent network'G(ii) a Generator node injection current I 'in equivalent network'GAs shown below:
Of formula (II) to (III)'GG(Geq)(Geq)The admittance submatrix corresponding to the generator node in the equivalent external network; y isGG(GI)(GI)The admittance submatrix corresponding to the generator node in the original internal network; u shapeGIIs the original external network generator voltage; u shapeGeqIs the equivalent network generator node voltage; y'GL(Geq)(LB)In an equivalent external network, equivalent generator nodes are taken as corresponding rows and equivalent boundary network nodes are taken as corresponding columns, so that an admittance submatrix is generated; y'GL(GI)(LB)In the equivalent network, generator nodes of an equivalent internal network are taken as corresponding rows, and equivalent boundary network nodes are taken as corresponding columns, so that an admittance submatrix is generated; y'GL(GI)(LI)In the equivalent network, generator nodes of the equivalent internal network are taken as corresponding rows and equivalent internal network nodes are taken as corresponding columns, so that an admittance submatrix is generated; u shapeLIIs the original internal network voltage; u shapeLBIs the original boundary network voltage;
5.1.5) obtaining the current I of the equivalent generator node Geq according to equation (24)Geq(ii) a Current I of the equivalent generator node GeqGeqAs follows:
of formula (II) to (III)'GG(Geq)(Geq)The admittance submatrix corresponding to the generator node in the equivalent external network; y isLGIn the original network, load nodes are used as corresponding rows, generator nodes are used as corresponding columns, and therefore an admittance submatrix is generated; y isLLAn admittance submatrix corresponding to a load node in an original external network;for said admittance submatrix YLLThe inverse matrix of (d); LB is an original boundary load node; LE is original outer net load node; GE is an original external network generator node; u shapeLBIs the original boundary network voltage; eGEIs the original external network generator node voltage;
5.2) calculating to obtain the voltage U of the equivalent generator nodeGeq(ii) a The method comprises the following steps:
5.2.1) setting a constant matrix C, a constant matrix F and a constant matrix D;
the constant matrix C is shown below:
in the formula, YLLAn admittance submatrix corresponding to a load node in an original external network;for said admittance submatrix YLLThe inverse matrix of (d); LB is an original boundary load node; LE is original outer net load node; GE is an original external network generator node; y isLGIn the original network, load nodes are used as corresponding rows, generator nodes are used as corresponding columns, and therefore an admittance submatrix is generated;
the constant matrix F is shown below:
in the formula, YLLAn admittance submatrix corresponding to a load node in an original external network;for said admittance submatrix YLLThe inverse matrix of (d); LB is an original boundary load node; LE is original outer net load node; GE is an original external network generator node; y isLGIn the original network, the load node is used as a corresponding row, and the generator node is used as a pairAnd (2) applying the obtained array to generate an admittance submatrix;admittance submatrix Y corresponding to generator nodes in original external networkGG(GE)(GE)The inverse matrix of (d); y isGL(GE)(LB)In the original network, generator nodes of the original external network are taken as corresponding rows and original boundary network nodes are taken as corresponding columns, so that an admittance submatrix is generated;
the constant matrix D is as follows:
in the formula, YLLAn admittance submatrix corresponding to a load node in an original external network;for said admittance submatrix YLLThe inverse matrix of (d); LB is an original boundary load node; LE is original outer net load node; GE is an original external network generator node; y isLGIn the original network, load nodes are used as corresponding rows, generator nodes are used as corresponding columns, and therefore an admittance submatrix is generated; y isGL(GE)(LE)In the original network, generator nodes of the original external network are taken as corresponding rows and original external network nodes are taken as corresponding columns, so that an admittance submatrix is generated;
5.2.2) voltage U of the equivalent generator node according to the constant matrix C, the constant matrix F and the constant matrix DGeqAs follows:
in the formula (I), the compound is shown in the specification,for outer net generator power matrix SGEThe companion matrix of (a); the matrix C, the matrix F and the matrix D are respectively set constant matrixes; u shapeLBIs the original boundary network voltage;
5.3) calculating the equivalent generator output SGeq(ii) a Equivalent generator output SGeqAs follows:
in the formula IGeq_diagIs composed ofGeqA diagonal matrix as a primary diagonal element;for the diagonal matrix IGeq_diagThe companion matrix of (a); u shapeGEQIs the voltage of the equivalent generator node;
5.4) according to the equivalent generator output SGeqSum equivalent generator power SGETo obtain the equivalent generator output SGeqSum equivalent generator power SGEThe analytic relationship of (1):
in the formula, a matrix C, a matrix F and a matrix D are respectively set constant matrixes;for the diagonal matrix IGeq_diagThe companion matrix of (a); u shapeLBIs the original boundary network voltage;for outer net generator power matrix SGEThe companion matrix of (a);
5.5) according to the equivalent generator output SGeqSum equivalent generator power SGEThe equivalent generator active power P is obtained by analyzing the relationGeq(ii) a The method comprises the following steps:
5.5.1) setting the intermediate parameter H1Intermediate parameter H2Intermediate parameter H21Intermediate parameter H22Intermediate parameter H23Intermediate parameter H24Intermediate parameter H25And an intermediate parameter H26;
The intermediate parameter H1As follows:
H1=IGeq_diag_realCreal+IGeq_diag_imagCimag; (32)
in the formula IGeq_diag_realIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagA matrix of real parts of the elements; i isGeq_diag_imagIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagA matrix of imaginary parts of the elements; crealA matrix formed by real parts of elements of a constant matrix C; cimagA matrix formed by imaginary parts of elements of a constant matrix C;
the intermediate parameter H21As follows:
H21=-IGeq_diag_realCimag-IGeq_diag_imagCreal; (33)
in the formula IGeq_diag_realIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagA matrix of real parts of the elements; i isGeq_diag_imagIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagA matrix of imaginary parts of the elements; crealA matrix formed by real parts of elements of a constant matrix C; cimagA matrix formed by imaginary parts of elements of a constant matrix C;
the intermediate parameter H22As follows:
in the formula, YGG(GE)(GE)_realFormation of real part of admittance submatrix elements corresponding to generator nodes in original external networkA matrix of (a); y isGG(GE)(GE)_imagA matrix formed by imaginary parts of admittance submatrix elements corresponding to generator nodes in an original external network; u shapeGE_imagFor the original external network generator node voltage UGEAn imaginary part of (d); u shapeGE_realFor the original external network generator node voltage UGEThe real part of (a); u shapeLE_realFor the original external network node voltage ULEThe real part of (a); u shapeLE_imagFor the original external network node voltage ULEAn imaginary part of (d); y isGL(GE)(LE)_imagAs an admittance sub-matrix YGL(GE)(LE)A matrix of imaginary parts of the elements; y isGL(GE)(LE)_realAs an admittance sub-matrix YGL(GE)(LE)A matrix of real parts of the elements;
the intermediate parameter H23As follows:
in the formula, YGG(GE)(GE)_realAdmittance submatrix Y corresponding to generator nodes in original external networkGG(GE)(GE)A matrix of real parts of the elements; y isGG(GE)(GE)_imagAdmittance submatrix Y corresponding to generator nodes in original external networkGG(GE)(GE)A matrix of imaginary parts of the elements; u shapeGE_imagFor the original external network generator node voltage UGEAn imaginary part of (d); u shapeGE_realFor the original external network generator node voltage UGEThe real part of (a); u shapeLE_realFor the original external network node voltage ULEThe real part of (a); u shapeLE_imagFor the original external network node voltage ULEAn imaginary part of (d); y isGL(GE)(LE)_imagAs an admittance sub-matrix YGL(GE)(LE)A matrix of imaginary parts of the elements; y isGL(GE)(LE)_realAs an admittance sub-matrix YGL(GE)(LE)A matrix of real parts of the elements;
the intermediate parameter H24As follows:
H24=-IGeq_diag_realFreal+IGeq_diag_imagFimag; (36)
in the formula IGeq_diag_realIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagA matrix of real parts of the elements; i isGeq_diag_imagIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagA matrix of imaginary parts of the elements; frealA matrix formed by real parts of elements of a constant matrix F; fimagA matrix formed by imaginary parts of elements of a constant matrix F;
the intermediate parameter H25As follows:
H25=IGeq_diag_realFimag-IGeq_diag_imagFreal; (37)
in the formula IGeq_diag_realIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagA matrix of real parts of the elements; i isGeq_diag_imagIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagA matrix of imaginary parts of the elements; frealA matrix formed by real parts of elements of a constant matrix F; fimagA matrix formed by imaginary parts of elements of a constant matrix F;
the intermediate parameter H26As follows:
H26=-IGeq_diag_realDreal-IGeq_diag_imagDimag; (38)
in the formula IGeq_diag_realIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagA matrix of real parts of the elements; i isGeq_diag_imagIs composed ofGeqDiagonal matrix I as main diagonal elementsGeq_diagA matrix of imaginary parts of the elements; drealA matrix formed by real parts of elements of a constant matrix D; dimagA matrix formed by imaginary parts of elements of a constant matrix D;
in the formula (I), the compound is shown in the specification,H21、H22、H23、H24、H25and H26Respectively set intermediate parameters; y isGL(GE)(LB)_imagAs an admittance sub-matrix YGL(GE)(LB)A matrix of imaginary parts of the elements; y isGL(GE)(LB)_realAs an admittance sub-matrix YGL(GE)(LB)A matrix of real parts of the elements; u shapeGE_diag_realRepresenting main diagonal elements as external network generator node voltages UGEDiagonal matrix U ofGE_diagA matrix of real parts of the elements; u shapeGE_diag_imagRepresenting main diagonal elements as external network generator node voltages UGEDiagonal matrix U ofGE_diagA matrix of imaginary parts of the elements; u shapeLB_imagFor the original border network node voltage ULBAn imaginary part of (d); u shapeLB_realFor the original border network node voltage ULBThe real part of (a);
5.5.2) according to the set intermediate parameter H1Intermediate parameter H2Intermediate parameter H21Intermediate parameter H22Intermediate parameter H23Intermediate parameter H24Intermediate parameter H25And an intermediate parameter H26To obtain the equivalent generator active power PGeq;
The equivalent generator active power PGeqAs follows:
PGeq=H1PGE+H2; (40)
in the formula, H1And H2Respectively set intermediate parameters; pGEThe active power of the equivalent external network node is obtained;
5.6) active Power P of the GeneratorGThe static frequency characteristic of (a) is as follows:
PG=PGmax-KG_diag(f-fGmax); (41)
in the formula, PGIs the active power output P of the generator from the ith node at the frequency fGiA constructed column vector; pGmaxIs the maximum active power output P of the generator from the ith nodeGmaxiA constructed column vector; kGFor the power-frequency-static characteristics of the generator from the ith nodeCoefficient KGiA constructed column vector; f. ofGmaxFor the frequency inflection point f when the generator of the ith node no longer has primary frequency modulation capabilityGmaxiA constructed column vector; f is the frequency; kG_diagIs composed of a power frequency static characteristic coefficient KGA matrix as a main diagonal element;
5.7) dividing the active power P of the generator according to the internal network and the external networkGThe division is as follows:
in the formula, PGmax_GIMaximum active output P of generator at ith node of internal networkGmaxiA constructed column vector; pGmax_GEThe maximum active output P of the generator of the ith node of the external networkGmaxiA constructed column vector; kG_GIPower frequency static characteristic coefficient K of generator for ith node of internal networkGiA constructed column vector; kG_GEPower frequency static characteristic coefficient K of generator for ith node of external networkGiA constructed column vector; f. ofGmax_GIFrequency inflection point f when generator no longer has primary frequency modulation capability for ith node of internal networkGmaxiA constructed column vector; f. ofGmax_GEA column vector representing a frequency inflection point when the external network generator no longer has primary frequency modulation capability; f is the frequency; pGIThe equivalent internal network generator active power; pGEThe equivalent external network generator active power;
5.8) active Power P of the external network Generator to have static frequency characteristicsGESubstituting into the active power of the equivalent generator to obtain the active power output P of the equivalent generator with the static frequency characteristicGeq;
The equivalent generator active power output P with the static frequency characteristicGeqAs follows:
PGeq=PGmax_eq-KGeqf'; (43)
wherein the column vector f' is a state variable, i.e. the frequency fOf structure and PGeqA column vector of the same dimension; kGeqThe power-frequency static characteristic coefficient of the equivalent network generator is obtained; pGmax_eqFor the original maximum active output information P of the external network generatorGmax_GEEquivalent information therein
Wherein, the original maximum active output information P of the external network generatorGmax_GEEquivalent information P thereinGmax_eqAs follows:
PGmax_eq=H1PGmax_GE+H2+KGeqfGmax_GE; (44)
in the formula, H1And H2Respectively set intermediate parameters; f. ofGmax_GEIs a column vector formed by frequency inflection points when the external generator no longer has primary frequency modulation capability; kGeqThe power-frequency static characteristic coefficient of the equivalent network generator is obtained;
equivalent network generator power frequency static characteristic coefficient KGeqAs follows:
KGeq=H1KG_GE; (45)
in the formula, KG_GEPower frequency static characteristic coefficient K of generator for ith node of external networkGiA constructed column vector; h1Is a set intermediate parameter; kG_GEThe power frequency static characteristic coefficient of the external grid generator is shown.
2. An equivalence method considering the static frequency characteristics of the external network according to claim 1, wherein: the basic parameters of the power network comprise element parameters in an original network, an original network topological structure and a load flow calculation result at an approaching moment;
the element parameters in the original network comprise the admittance to the ground of all nodes, the connection load power of all nodes, the impedance of all lines, the susceptance to the ground of all lines, the constraint condition of line transmission power, the impedance of a transformer, the admittance to the ground of the transformer, the transformation ratio of the transformer, the constraint condition of transformer transmission power, the output of a generator, the constraint condition of the output of the generator, the power-frequency static characteristic coefficient of the generator and the power-frequency static characteristic coefficient of the load;
the original network topology structure comprises the connection relation of all nodes and the network partition condition;
and the near moment power flow calculation result comprises a node admittance matrix, a node voltage matrix and a node injection current matrix.
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