CN116345463A - Main and distribution network integrated system random power flow calculation method - Google Patents

Main and distribution network integrated system random power flow calculation method Download PDF

Info

Publication number
CN116345463A
CN116345463A CN202310199205.6A CN202310199205A CN116345463A CN 116345463 A CN116345463 A CN 116345463A CN 202310199205 A CN202310199205 A CN 202310199205A CN 116345463 A CN116345463 A CN 116345463A
Authority
CN
China
Prior art keywords
power
power flow
distribution network
load
main
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
CN202310199205.6A
Other languages
Chinese (zh)
Inventor
王京景
王吉文
戴长春
张炜
李端超
谢大为
吴旭
王磊
丁超
麦立
许斌
王海港
徐军
郑学磊
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Anhui Mingsheng Hengzhuo Technology Co ltd
State Grid Anhui Electric Power Co Ltd
Original Assignee
Anhui Mingsheng Hengzhuo Technology Co ltd
Anhui Zhiling Power Technology Co ltd
State Grid Anhui Electric Power Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Anhui Mingsheng Hengzhuo Technology Co ltd, Anhui Zhiling Power Technology Co ltd, State Grid Anhui Electric Power Co Ltd filed Critical Anhui Mingsheng Hengzhuo Technology Co ltd
Priority to CN202310199205.6A priority Critical patent/CN116345463A/en
Publication of CN116345463A publication Critical patent/CN116345463A/en
Pending legal-status Critical Current

Links

Images

Classifications

    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02JCIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
    • H02J3/00Circuit arrangements for ac mains or ac distribution networks
    • H02J3/04Circuit arrangements for ac mains or ac distribution networks for connecting networks of the same frequency but supplied from different sources
    • H02J3/06Controlling transfer of power between connected networks; Controlling sharing of load between connected networks
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F17/00Digital computing or data processing equipment or methods, specially adapted for specific functions
    • G06F17/10Complex mathematical operations
    • G06F17/18Complex mathematical operations for evaluating statistical data, e.g. average values, frequency distributions, probability functions, regression analysis
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02JCIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
    • H02J3/00Circuit arrangements for ac mains or ac distribution networks
    • H02J3/38Arrangements for parallely feeding a single network by two or more generators, converters or transformers
    • H02J3/381Dispersed generators
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02JCIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
    • H02J3/00Circuit arrangements for ac mains or ac distribution networks
    • H02J3/38Arrangements for parallely feeding a single network by two or more generators, converters or transformers
    • H02J3/46Controlling of the sharing of output between the generators, converters, or transformers
    • H02J3/466Scheduling the operation of the generators, e.g. connecting or disconnecting generators to meet a given demand
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02JCIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
    • H02J2203/00Indexing scheme relating to details of circuit arrangements for AC mains or AC distribution networks
    • H02J2203/20Simulating, e g planning, reliability check, modelling or computer assisted design [CAD]
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02JCIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
    • H02J2300/00Systems for supplying or distributing electric power characterised by decentralized, dispersed, or local generation
    • H02J2300/20The dispersed energy generation being of renewable origin
    • H02J2300/22The renewable source being solar energy
    • H02J2300/24The renewable source being solar energy of photovoltaic origin
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02JCIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
    • H02J2300/00Systems for supplying or distributing electric power characterised by decentralized, dispersed, or local generation
    • H02J2300/20The dispersed energy generation being of renewable origin
    • H02J2300/28The renewable source being wind energy
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02JCIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
    • H02J2300/00Systems for supplying or distributing electric power characterised by decentralized, dispersed, or local generation
    • H02J2300/40Systems for supplying or distributing electric power characterised by decentralized, dispersed, or local generation wherein a plurality of decentralised, dispersed or local energy generation technologies are operated simultaneously

Landscapes

  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Power Engineering (AREA)
  • Data Mining & Analysis (AREA)
  • General Physics & Mathematics (AREA)
  • Mathematical Optimization (AREA)
  • Theoretical Computer Science (AREA)
  • Mathematical Physics (AREA)
  • Computational Mathematics (AREA)
  • Pure & Applied Mathematics (AREA)
  • Mathematical Analysis (AREA)
  • Bioinformatics & Computational Biology (AREA)
  • Operations Research (AREA)
  • Probability & Statistics with Applications (AREA)
  • Evolutionary Biology (AREA)
  • Algebra (AREA)
  • Bioinformatics & Cheminformatics (AREA)
  • Databases & Information Systems (AREA)
  • Software Systems (AREA)
  • General Engineering & Computer Science (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Supply And Distribution Of Alternating Current (AREA)

Abstract

The invention discloses a random power flow calculation method of a main distribution network integrated system, which comprises the following steps of; step 1: collecting network parameters of a main distribution network; step 2: dividing a main distribution network according to line voltage levels, network topology structures and the like, and determining boundary nodes; step 3: establishing wind power, photovoltaic output power and load probability density functions according to the wind speed, illumination intensity, load and other data; step 4: taking wind power, photovoltaic and load randomness into consideration, and carrying out random power flow calculation on the distribution network by utilizing a point estimation method; step 5: obtaining boundary node voltage amplitude expectation and phase angle expectation according to the tide result in the step 4; step 6: calculating the sum of absolute values of corresponding voltage amplitude differences of n boundary nodes of two adjacent iterations; step 7: and (5) solving a probability density function of the output load flow variable by using Gram-Charlier series expansion. According to the invention, the load randomness and the main-distribution integrated power grid load flow probability distribution after a large amount of new energy sources such as wind power, photovoltaic and the like are accessed are accurately estimated and considered, and the static safety analysis is more effectively carried out.

Description

Main and distribution network integrated system random power flow calculation method
Technical Field
The invention belongs to the field of steady-state analysis of power systems, and relates to a random power flow calculation method of a main distribution network integrated system.
Background
The traditional trend calculation is to calculate the network topology structure, line impedance parameters, transformer transformation ratio, active and reactive power output of generator nodes, active and reactive power of load nodes and other parameters as known quantities, and is generally called deterministic trend calculation. In recent years, however, clean energy sources such as wind power and photovoltaic and the like are largely connected into a power grid, the trend distribution of the system is changed, the output of the wind power and the photovoltaic is easily influenced by wind speed, illumination intensity, weather and other environmental factors, and the randomness and uncertainty of the wind power and the photovoltaic are caused to lead the output of the wind power and the photovoltaic to be not constant any more, but are random variables obeying a certain probability distribution. In addition, in the actual running of the power grid, the load demand is also changed at moment, and the deterministic power flow calculation cannot accurately reflect the power flow distribution of the power grid in real time. The random power flow energy effectively considers various uncertainty factors in the system, obtains probability characteristics of the power flow of the system, and reflects the power flow distribution of the power grid more truly.
For the current calculation of the traditional power grid, a unified model is generally established, and a certain method is used for obtaining a current calculation result, for example, a Newton-Lapherson method, a PQ decomposition method and the like can be used for a main network; the power distribution network can adopt forward-push back generation, Z-Bus method and the like, and the result meeting the convergence accuracy can be obtained. However, as the power grid in China adopts a layered and partitioned management system, each level of dispatching mechanism models the power grid in the jurisdiction range in detail, the distributed management causes the information island phenomenon, and only limited information can be exchanged between systems in different levels, so that the problem that a unified model is difficult to build to perform load flow calculation on the main distribution network is fundamentally caused. Even if sufficient information can be obtained, the main-distribution integrated model is built at the expense of precision, the huge node and branch number of the whole system can cause the abnormal huge calculation scale, massive calculation resources are required to be occupied, and the requirement of on-line calculation is difficult to meet. The data of the main distribution network have obvious difference, for example, the reactance-resistance ratio in the main network is far greater than that of the distribution network; the network parameter values of the main distribution network and the branch power have the order-of-magnitude level difference and the like, so that the problems of poor convergence of a nonlinear equation set of power flow calculation, easy singular jacobian matrix and the like are caused, and the difficulty of power flow solving is greatly increased. The master-slave split method is used as the most common master-slave integrated power flow calculation method, the master-slave network is respectively modeled and calculated, the problems are fundamentally solved, the power distribution network is equivalent to a constant power load when the power flow of the master network is calculated, the master network is equivalent to a constant voltage source when the power flow of the power distribution network is calculated, the master power distribution network is connected through boundary nodes, and convergence is finally achieved through alternate iterative operation, so that the master-slave split method is widely applied. However, with the large amount of access of new energy sources such as wind power, photovoltaic and the like and considering the randomness of loads, the main network and the distribution network are more tightly coupled, and bidirectional energy flow possibly occurs, and the main network and the distribution network are continuously and simply equivalent to a constant voltage source and a constant power load, so that the calculation result and the actual value error are increased, and the traditional master-slave split method also has corresponding problems in calculating the random tide of the main-distribution integrated system.
Disclosure of Invention
The invention provides a random power flow calculation method of a main distribution network integrated system, which aims to overcome the defects in the prior art. Based on the principle of a master-slave splitting method, carrying out random power flow calculation on a main power distribution network respectively, firstly giving boundary node voltage, and calculating the random power flow of the power distribution network by considering wind power, photovoltaic output and load randomness to obtain boundary node voltage amplitude
Figure BDA0004108452270000021
And the expected value of phase angle->
Figure BDA0004108452270000022
Then, calculating the random power flow of the main network by taking the boundary node as a relation to obtain the expected +.>
Figure BDA0004108452270000023
And the expected variance of phase angle>
Figure BDA0004108452270000024
And calculating whether the sum of absolute values of corresponding voltage amplitude differences and the sum of absolute values of corresponding phase differences of n boundary nodes of adjacent iterations meet convergence accuracy. If all of them meet, then the global random is reachedConverging tide; otherwise, the steps 4 to 6 are alternately iterated until convergence; after the convergence of the power flow is judged, the moment of each step of the current main and distribution network power flow variable is considered as the moment of each step of the main and distribution network integrated system power flow variable, and the probability density function of the output power flow variable is obtained by utilizing Gram-Charlier series expansion, so that the probability distribution of the main and distribution integrated system power flow can be finally obtained, and the method can be used for static security analysis of the main and distribution network integrated system.
The invention adopts the following technical scheme for solving the technical problems:
the random power flow calculation method of the main and distribution network integrated system comprises the following steps:
step 1: collecting network parameters of a main distribution network, including parameters such as network topology, line parameters, active power and reactive power of generator nodes and the like; historical data such as wind speed, illumination intensity, load and the like;
step 2: dividing a main distribution network according to line voltage levels, network topological structures and the like, determining boundary nodes, forming a set B by the boundary nodes, setting boundary node voltage amplitude convergence criteria epsilon 1 and phase angle convergence criteria epsilon, wherein the number of the nodes is n 2
Step 3: establishing wind power, photovoltaic output power and load probability density functions according to data such as wind speed, illumination intensity and load, and obtaining digital characteristics such as expected and variance;
step 4: taking wind power, photovoltaic and load randomness into consideration, carrying out random power flow calculation on the distribution network by using a point estimation method to obtain each moment of a power flow variable of the distribution network;
step 5: obtaining the expected voltage amplitude of the boundary node from the tide result in the step 4
Figure BDA0004108452270000031
And phase angle expectation
Figure BDA0004108452270000032
Calculating the random power flow of the main network by taking the boundary nodes as relations to obtain the amplitude expectation of the boundary node voltage
Figure BDA0004108452270000033
Is about to phase angle expectation>
Figure BDA0004108452270000034
Step 6: calculating whether the sum of absolute values of corresponding voltage amplitude differences and the sum of absolute values of corresponding phase differences of n boundary nodes of two adjacent iterations meet convergence precision or not, and reaching convergence after the sum of absolute values meets the precision, otherwise, alternately iterating the steps 4 to 6 until convergence;
step 7: after the convergence of the power flow is judged, the moment of each step of the current main power flow variable and the moment of each step of the current power flow variable of the distribution network are the moment of each step of the power flow variable of the main power flow and distribution network integrated system, and the probability density function of the output power flow variable is obtained by means of Gram-Charlier series expansion;
a random power flow calculation method of a main distribution network integrated system is characterized in that the step 3 is carried out according to the following steps:
for wind power generation, the wind speed is considered to be compliant with Weibull distribution, and when the wind speed changes, the relation between the output power of the wind power generator and the wind power generation active power and the probability density function are as follows:
Figure BDA0004108452270000041
Figure BDA0004108452270000042
k in 1 =P r /(v r -v ci ),k 2 =-k 1 v ci Is a constant coefficient; v is wind speed; v ci Is the cut-in wind speed; v co Cutting out wind speed; v r Is the rated wind speed; k. c is the shape parameter and the scale parameter of Weibull distribution respectively; the method can be obtained by the average value and standard deviation of the collected historical wind speed data; p (P) r The rated output power of the wind driven generator is obtained.
For photovoltaic power generation, the illumination intensity is considered to approximately follow the Beta distribution, and the probability density function of the output power of the photovoltaic array is as follows:
Figure BDA0004108452270000043
wherein: p (P) m And P m,max Respectively outputting an actual value and a maximum value of active power; a and b are shape parameters of Beta distribution, and are determined by the average value and standard deviation of collected historical illumination intensity data; f is a gamma function. In the distribution simulation of the actual historical data of the load, the load is considered to be approximately subjected to normal distribution, and then the load active power P load
Reactive power Q load The probability density function of (2) is:
Figure BDA0004108452270000044
in the middle, mu P 、μ Q The method is characterized by respectively absorbing the expectations of active power and reactive power for the load; sigma (sigma) P 、σ Q The variances of the active power and the reactive power are absorbed by the load respectively.
A random power flow calculation method of a main distribution network integrated system is characterized in that the point estimation method of the step 4 is carried out according to the following steps:
the expected mu is obtained by wind power, photovoltaic output and load probability density functions k Variance sigma k Equal digital characteristic, calculating position coefficient xi of each input variable k,i Probability coefficient p k,i
Figure BDA0004108452270000051
Figure BDA0004108452270000052
Determining three value points x according to the mean value and variance of the random variable k,i ,i=1,2,3
x k,i =μ kk,i σ k ,i=1,2,3 (7)
Each value point value of the random variable isx k,i And taking the average value of the rest random variables, and carrying out deterministic power flow calculation by utilizing a Newton-Laporton method to obtain power flow distribution X (i, k) of the main-distribution integrated system.
For each random variable, three values are needed, and 3 deterministic power flow calculations are needed until the calculation is completed for all random variables. And calculating each moment of the distribution network power flow X by using the following formula.
Figure BDA0004108452270000053
A random power flow calculation method of a main distribution network integrated system is characterized in that the step 6 is carried out according to the following steps:
the random power flow calculation is carried out on the distribution network and the main network respectively in the steps 4 and 5 to obtain the expectation of calculating the voltage amplitude and the phase angle of the boundary node in two adjacent iterations
Figure BDA0004108452270000054
And->
Figure BDA0004108452270000055
Figure BDA0004108452270000056
Wherein i=1, 2, …, n, n is the number of boundary nodes; calculating whether the sum of absolute values of corresponding voltage amplitude differences and the sum of absolute values of corresponding phase differences of n boundary nodes of two adjacent iterations meet convergence precision, and reaching convergence after the convergence precision is met, otherwise, alternately iterating the steps 4 to 6 until convergence, wherein the convergence criterion is as follows:
Figure BDA0004108452270000061
further, an apparatus, comprising:
one or more processors;
a memory for storing one or more programs;
when one or more of the programs are executed by one or more of the processors, the one or more of the processors implement a method for calculating random power flow of a main-distribution network integrated system as described above.
Further, a storage medium containing computer executable instructions, which when executed by a computer processor, are for performing a method of random power flow calculation for a primary distribution network integrated system as described above.
The beneficial effects of the invention are as follows:
the invention provides a random power flow calculation method of a main and distribution network integrated system based on a principle of a master-slave splitting method and a point estimation random power flow algorithm, which is used for calculating random power flow of a power distribution network and a main power network respectively by taking boundary nodes as relations to obtain the voltage amplitude and phase angle expectations of the boundary nodes of two adjacent iterations.
Drawings
FIG. 1 is a schematic flow chart of the present invention;
Detailed Description
The following description of the technical solutions in the embodiments of the present disclosure will be made clearly and completely with reference to the accompanying drawings in the embodiments of the present disclosure, and it is apparent that the described embodiments are only some embodiments of the present disclosure, not all embodiments. All other embodiments, which can be made by one of ordinary skill in the art based on the embodiments in this disclosure without inventive faculty, are intended to fall within the scope of this disclosure.
The invention will be described in further detail below with reference to the accompanying drawings.
As shown in fig. 1, a method for calculating random power flow of a main-distribution network integrated system specifically includes the following steps:
step 1: collecting network parameters of a main distribution network, including network topology, line parameters, active power, reactive power and other deterministic parameters of generators and load nodes; historical data such as wind speed, illumination intensity, load and the like;
step 2: dividing a main distribution network according to line voltage levels, line topological structures and the like, and determining boundary nodes, wherein the number of the boundary nodes is n;
as a bridge for the connection of the main distribution network, the boundary nodes can be understood as load nodes in the main network as well as generator nodes of the distribution network. And establishing a boundary node set B, removing residual nodes of the boundary nodes by the main network node to form a set T, and forming a set D by the residual distribution network nodes.
Step 3: establishing wind power, photovoltaic output power and load probability density functions according to data such as wind speed, illumination intensity and load, and obtaining digital characteristics such as expected and variance;
for wind power generation, the wind speed is considered to be compliant with Weibull distribution, and when the wind speed changes, the relation between the output power of the wind power generator and the wind power generation active power and the probability density function are as follows:
Figure BDA0004108452270000071
Figure BDA0004108452270000072
k in 1 =P r /(v r -v ci ),k 2 =-k 1 v ci Is a constant coefficient; v is wind speed; v ci Is the cut-in wind speed; v co Cutting out wind speed; v r Is the rated wind speed; k. c is the shape parameter and the scale parameter of Weibull distribution respectively; the method can be obtained by the average value and standard deviation of the collected historical wind speed data; p (P) r The rated output power of the wind driven generator is obtained.
For photovoltaic power generation, the illumination intensity is considered to approximately follow the Beta distribution, and the probability density function of the output power of the photovoltaic array is as follows:
Figure BDA0004108452270000081
wherein: p (P) m And P m,max Respectively outputting an actual value and a maximum value of active power; a and b are shape parameters of Beta distribution, and are determined by the average value and standard deviation of collected historical illumination intensity data; f is a gamma function.
In the distribution simulation of the actual history data of the load, the load is considered to be approximately compliant with normal distribution, and the load absorbs the active power P load Reactive power Q load Can be described as:
Figure BDA0004108452270000082
wherein mu P 、σ P 、μ Q 、σ Q The expected and variance of the collected historical load active power and reactive power, respectively.
Step 4: giving boundary node voltage amplitude and phase angle, taking wind power, photovoltaic and load randomness into consideration, and carrying out random power flow calculation on the distribution network by using a point estimation method to obtain each moment of a power flow variable of the distribution network;
the distribution network tide equation is as follows: s is S D -S DB -S DD =0
Wherein: s is S D Injecting complex power vectors for nodes in the set D, S DT Vector formed by branch complex power flowing into node set T for node in node set D, S DD And (3) a branch complex power vector flowing into the node set for the node in the node set D. Because of randomness of wind power, photovoltaic output and load, the number of random variables contained in power flow calculation of a power distribution network is set as m, and three value points x are determined for one random variable according to expectations and variances of the random variable k,i ,i=1,2,3,k=1,2,…m。
x k,i =μ kk,i σ k ,i=1,2,3 (5)
Wherein:
Figure BDA0004108452270000091
for each value point, the residual variable is averaged, and a deterministic power flow calculation is performed to obtain a deterministic power flow result f (x) k,i ). 3 deterministic power flow calculations are performed on a random variable. Repeating the calculation process until all random variables are calculated to obtain each moment E (X) of distribution network power flow distribution j ):
Figure BDA0004108452270000092
Figure BDA0004108452270000093
The expected voltage amplitude of n boundary nodes can be obtained through each moment of power flow distribution of the power distribution network
Figure BDA0004108452270000094
Is about to phase angle expectation>
Figure BDA0004108452270000095
Where i=1, 2, …, n. n is the number of boundary nodes. k is the distinction between adjacent iterations of the distribution network and the main network. B represents a set of border nodes.
Step 5: calculating the random power flow of the main network by taking the boundary nodes as the relations to obtain the expectation of the voltage amplitude of the boundary nodes
Figure BDA0004108452270000096
And phase angle->
Figure BDA0004108452270000097
The specific process is as follows: the main network tide equation is:
Figure BDA0004108452270000098
wherein S is T 、S B Complex power vectors respectively injected for nodes of the corresponding node set; s is S XY Is the complex power vector of each node on the node set X flowing into the node set Y; s is S XX The complex power vector of the own branch flows into the nodes of the node set X.
The calculation of the main network random power flow still adopts a point estimation method, and the process is consistent as described in the step 4, and is not repeated here. Wherein the boundary nodes correspond to load nodes and are treated as random variables. Obtaining each moment of the main network tide variable after the calculation is completed, namely obtaining the expected voltage amplitude of the boundary node
Figure BDA0004108452270000101
And the expected variance of phase angle>
Figure BDA0004108452270000102
Where i=1, 2, …, n. n is the number of boundary nodes. k+1 is the distinction between adjacent iterations of the distribution network and the main network. B represents a set of border nodes.
Step 6: and calculating whether the sum of absolute values of corresponding voltage amplitude differences and the sum of absolute values of corresponding phase differences of n boundary nodes of adjacent iterations meet convergence accuracy. If both the power flows are satisfied, the convergence of the global random power flow is achieved; otherwise, the steps 4 to 6 are alternately iterated until convergence, and the convergence criterion is as follows:
Figure BDA0004108452270000103
i.e. if at the same time satisfy
Figure BDA0004108452270000104
And->
Figure BDA0004108452270000105
Considering that the overall random power flow convergence is achieved, exiting the loop, and performing step 7; otherwise, returning to the step 4, the step 4 and the step 6 are alternately iterated until convergence.
Step 7: after the convergence of the power flow is judged, the moment of each step of the current main power flow variable and the moment of each step of the current power flow variable of the distribution network are regarded as the moment of each step of the power flow variable of the main power flow and distribution network integrated system, and the probability density function of the output power flow variable is obtained by utilizing Gram-Charlier series expansion, and the specific process is as follows:
firstly, the main and distribution network integrated power flow X is standardized:
Figure BDA0004108452270000106
where μ and σ are the expectation and variance of X, respectively. Then->
Figure BDA00041084522700001011
The probability density function of (2) is:
Figure BDA0004108452270000107
wherein the method comprises the steps of
Figure BDA0004108452270000108
Figure BDA0004108452270000109
Is a probability density function that obeys a standard normal distribution.
The probability density function of the main distribution network integrated power flow X is:
Figure BDA00041084522700001010
based on the same inventive concept, the present invention also provides a computer apparatus comprising: one or more processors, and memory for storing one or more computer programs; the program includes program instructions and the processor is configured to execute the program instructions stored in the memory. The processor may be a central processing unit (Central Processing Unit, CPU), but may also be other general purpose processors, digital signal processors (Digital Signal Processor, DSP), application specific integrated circuits (Application SpecificIntegrated Circuit, ASIC), field-Programmable gate arrays (FPGAs) or other Programmable logic devices, discrete gate or transistor logic devices, discrete hardware components, etc., which are the computational core and control core of the terminal for implementing one or more instructions, in particular for loading and executing one or more instructions within a computer storage medium to implement the methods described above.
It should be further noted that, based on the same inventive concept, the present invention also provides a computer storage medium having a computer program stored thereon, which when executed by a processor performs the above method. The storage media may take the form of any combination of one or more computer-readable media. The computer readable medium may be a computer readable signal medium or a computer readable storage medium. The computer readable storage medium can be, for example, but not limited to, an electronic, magnetic, optical, electrical, magnetic, infrared, or semiconductor system, apparatus, or device, or a combination of any of the foregoing. More specific examples (a non-exhaustive list) of the computer-readable storage medium would include the following: an electrical connection having one or more wires, a portable computer diskette, a hard disk, a Random Access Memory (RAM), a read-only memory (ROM), an erasable programmable read-only memory (EPROM or flash memory), an optical fiber, a portable compact disc read-only memory (CD-ROM), an optical storage device, a magnetic storage device, or any suitable combination of the foregoing. In the context of this document, a computer readable storage medium may be any tangible medium that can contain, or store a program for use by or in connection with an instruction execution system, apparatus, or device.
In the description of the present specification, the descriptions of the terms "one embodiment," "example," "specific example," and the like, mean that a particular feature, structure, material, or characteristic described in connection with the embodiment or example is included in at least one embodiment or example of the present disclosure. In this specification, schematic representations of the above terms do not necessarily refer to the same embodiments or examples. Furthermore, the particular features, structures, materials, or characteristics described may be combined in any suitable manner in any one or more embodiments or examples.
The foregoing has shown and described the basic principles, principal features, and advantages of the present disclosure. It will be understood by those skilled in the art that the present disclosure is not limited to the embodiments described above, which have been described in the foregoing and description merely illustrates the principles of the disclosure, and that various changes and modifications may be made therein without departing from the spirit and scope of the disclosure, which is defined in the appended claims.

Claims (6)

1. A random power flow calculation method of a main distribution network integrated system comprises the following steps:
step 1: collecting network parameters of a main distribution network, including network topology, line parameters and active and reactive power parameters of generator nodes; wind speed, illumination intensity and load history data;
step 2: dividing a main distribution network according to line voltage levels and a network topological structure, determining boundary nodes, wherein the boundary nodes form a set B, the number of the boundary nodes is n, and setting boundary node voltage amplitude convergence criteria epsilon 1 and phase angle convergence criteria epsilon 2
Step 3: building wind power, photovoltaic output power and load probability density functions according to wind speed, illumination intensity and load data to obtain expected variance digital characteristics;
step 4: taking wind power, photovoltaic and load randomness into consideration, carrying out random power flow calculation on the distribution network by using a point estimation method to obtain each moment of a power flow variable of the distribution network;
step 5: obtaining the expected voltage amplitude of the boundary node from the tide result in the step 4
Figure FDA0004108452260000011
And phase angle expectation
Figure FDA0004108452260000012
Calculating the random power flow of the main network by taking the boundary nodes as relations to obtain the amplitude expectation of the boundary node voltage
Figure FDA0004108452260000013
Is about to phase angle expectation>
Figure FDA0004108452260000014
Step 6: calculating whether the sum of absolute values of corresponding voltage amplitude differences and the sum of absolute values of corresponding phase differences of n boundary nodes of two adjacent iterations meet convergence precision or not, and reaching convergence after the sum of absolute values meets the precision, otherwise, alternately iterating the steps 4 to 6 until convergence;
step 7: after the convergence of the power flow is judged, the moment of each step of the current main power flow variable and the moment of each step of the current power flow variable of the distribution network are the moment of each step of the power flow variable of the main power flow and distribution network integrated system, and the probability density function of the output power flow variable is obtained by means of Gram-Charlier series expansion.
2. The method for calculating the random power flow of the integrated system of the main distribution network according to claim 1, wherein the step 3 comprises:
for wind power generation, the wind speed is considered to follow Weibull distribution, and when the wind speed changes, the relation between the output power of the wind power generator and the wind speed and the probability density function of the active power of wind power generation are as follows:
Figure FDA0004108452260000021
Figure FDA0004108452260000022
k in 1 =P r /(v r -v ci ),k 2 =-k 1 v ci Is a constant coefficient; v is wind speed; v ci Is the cut-in wind speed; v co Cutting out wind speed; v r Is the rated wind speed; k. c is the shape parameter and the scale parameter of Weibull distribution respectively; the method can be obtained by the average value and standard deviation of the collected historical wind speed data; p (P) r Rated output power of the wind driven generator;
for photovoltaic power generation, the illumination intensity is considered to obey beta distribution, and the probability density function of the output power of the photovoltaic array is as follows:
Figure FDA0004108452260000023
wherein: p (P) m And P m,max Respectively outputting an actual value and a maximum value of active power; a and b are shape parameters of Beta distribution, and are determined by the average value and standard deviation of collected historical illumination intensity data; f is a gamma function; in the distribution simulation of the actual historical data of the load, the load is considered to be approximately subjected to normal distribution, and then the load active power P load Reactive power Q load The probability density function of (2) is:
Figure FDA0004108452260000024
in the middle, mu P 、μ Q The method is characterized by respectively absorbing the expectations of active power and reactive power for the load; sigma (sigma) P 、σ Q The variances of the active power and the reactive power are absorbed by the load respectively.
3. The method for calculating the random power flow of the integrated system of the main distribution network according to claim 1, wherein the point estimation method of the step 4 is performed according to the following steps:
the expected mu is obtained by wind power, photovoltaic output and load probability density functions k Variance sigma k Equal digital characteristic, calculating position coefficient xi of each input variable k,i Probability coefficient p k,i
Figure FDA0004108452260000031
Figure FDA0004108452260000032
Determining three value points x according to the mean value and variance of the random variable k,i ,i=1,2,3
x k,i =μ kk,i σ k ,i=1,2,3 (7)
Each value point value of the random variable is x k,i Taking the average value of the rest random variables, and carrying out deterministic power flow calculation by utilizing a Newton-Lapherson method to obtain power flow distribution X (i, k) of the main-distribution integrated system;
three values are needed for each random variable, and 3 deterministic power flow calculations are needed until calculation is completed for all random variables; calculating each moment of the distribution network power flow X by using the following formula;
Figure FDA0004108452260000033
4. the method for calculating the random power flow of the integrated system of the main distribution network according to claim 1, wherein the step 6 is performed as follows:
the random power flow calculation is carried out on the distribution network and the main network respectively in the step 4 and the step 5 to obtain the expectation of calculating the voltage amplitude and the phase angle of the boundary node in two adjacent iterations
Figure FDA0004108452260000034
And->
Figure FDA0004108452260000035
Figure FDA0004108452260000036
Wherein i=1, 2, …, n, n is the number of boundary nodes; calculating whether the sum of absolute values of corresponding voltage amplitude differences and the sum of absolute values of corresponding phase differences of n boundary nodes of two adjacent iterations meet convergence precision, and reaching convergence after the convergence precision is met, otherwise, alternately iterating the steps 4 to 6 until convergence, wherein the convergence criterion is as follows:
Figure FDA0004108452260000037
5. an apparatus, the apparatus comprising:
one or more processors;
a memory for storing one or more programs,
the one or more programs, when executed by the one or more processors, cause the one or more processors to perform a method of stochastic load flow calculation of a primary distribution network integration system according to any of claims 1-4.
6. A computer readable storage medium storing a computer program, wherein the program when executed by a processor implements a method for calculating a random power flow of a main distribution network integrated system according to any one of claims 1 to 4.
CN202310199205.6A 2023-03-03 2023-03-03 Main and distribution network integrated system random power flow calculation method Pending CN116345463A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202310199205.6A CN116345463A (en) 2023-03-03 2023-03-03 Main and distribution network integrated system random power flow calculation method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202310199205.6A CN116345463A (en) 2023-03-03 2023-03-03 Main and distribution network integrated system random power flow calculation method

Publications (1)

Publication Number Publication Date
CN116345463A true CN116345463A (en) 2023-06-27

Family

ID=86881507

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202310199205.6A Pending CN116345463A (en) 2023-03-03 2023-03-03 Main and distribution network integrated system random power flow calculation method

Country Status (1)

Country Link
CN (1) CN116345463A (en)

Similar Documents

Publication Publication Date Title
Williams et al. Probabilistic load flow modeling comparing maximum entropy and Gram-Charlier probability density function reconstructions
CN109088407B (en) Power distribution network state estimation method based on deep belief network pseudo-measurement modeling
Ahmed et al. Probabilistic distribution load flow with different wind turbine models
CN112800683B (en) System short-circuit current level evaluation method and system based on convolutional neural network
CN103236691A (en) Method of three-phase unbalance load flow calculation based on complex affine mathematical theory
Samet et al. Analytic time series load flow
CN110518591B (en) Load flow calculation method for uncertain power system
CN107274028A (en) A kind of many wind fields based on mixing Copula functions are exerted oneself Forecasting Methodology
CN112508279A (en) Regional distributed photovoltaic prediction method and system based on spatial correlation
CN113328467B (en) Probability voltage stability evaluation method, system, terminal device and medium
Zhuo et al. Rsm-based approximate dynamic programming for stochastic energy management of power systems
CN116345463A (en) Main and distribution network integrated system random power flow calculation method
CN116452005A (en) Risk assessment method, device, equipment and storage medium for electric power system
CN103714212A (en) Transient simulation-oriented power distribution system model simplification error control method
CN112217215B (en) PSD-BPA-based large-scale power system random load flow calculation method
CN111682552B (en) Data-driven reactive voltage control method, device, equipment and storage medium
Hayes et al. Viable computation of the largest Lyapunov characteristic exponent for power systems
CN109494747B (en) Power grid probability load flow calculation method based on alternating gradient algorithm
Ji et al. Probabilistic optimal power flow considering the dependence of multiple wind farms using pair diffusive kernel copula
CN112751334A (en) Power grid online modeling method and system based on memory computing architecture
CN114256865A (en) Wind power installed capacity calculation method considering load increase direction randomness
Cai et al. Study on Wind Power Prediction Based on EEMD-LSTM
Eidiani et al. A Detailed Study on Prevailing ATC Methods for Optimal Solution Development
CN113809772B (en) Method and device for improving safety of wind power uncertainty of secondary time scale
Fournel et al. On the use of yearly load scenarios to estimate the volume of curtailed generation

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
TA01 Transfer of patent application right
TA01 Transfer of patent application right

Effective date of registration: 20240716

Address after: 230022 No. 9 Huangshan Road, Baohe District, Hefei City, Anhui Province

Applicant after: State Grid Anhui Electric Power Company

Country or region after: China

Applicant after: Anhui Mingsheng HENGZHUO Technology Co.,Ltd.

Address before: 230022 No. 9 Huangshan Road, Baohe District, Hefei City, Anhui Province

Applicant before: State Grid Anhui Electric Power Company

Country or region before: China

Applicant before: Anhui Mingsheng HENGZHUO Technology Co.,Ltd.

Applicant before: Anhui Zhiling Power Technology Co.,Ltd.