Disclosure of Invention
The invention provides a method and a system for calculating a black start partitioning scheme of a power supply network.
In order to achieve the above purpose, the method for calculating the black start partitioning scheme of the power supply network comprises the following steps:
constructing a minimum topological relation matrix of the load nodes and the black start power supply nodes, wherein elements in the relation matrix are minimum topological distances between each load node and the black start power supply nodes;
establishing a load node relation matrix table according to the incidence relation among the load nodes, wherein elements in the load node relation matrix table are used for representing the connection state between every two load nodes;
introducing variables for representing whether the load nodes are of a type of load and variables for representing whether the load nodes are adjustable loads;
constructing a partition range table, wherein elements in the partition range table are partition subordinate relation values of each black-start power supply node and each load node;
constructing an energy function by using elements in the minimum topological relation matrix of the constructed load nodes and black-start power supply nodes, elements in a load node relation matrix table, and introduced variables for representing whether the load nodes are a type of load and variables for representing whether the load nodes are adjustable loads;
and solving the established energy function to obtain each unit element value in the partition range table, and dividing the power supply partition according to each unit element value in the partition range table, wherein the load power supply node and the black start power supply node corresponding to the unit with the element value of 1 are divided into the same partition.
Further, the minimum topological relation matrix of the load nodes and the black-start power supply nodes is as follows:
|
w1 |
w2 |
…
|
wj |
…
|
wN |
B1 |
d11 |
d12 |
…
|
d1j |
…
|
d1N |
B2 |
d21 |
d22 |
…
|
d2j |
…
|
d2N |
…
|
…
|
…
|
…
|
…
|
…
|
…
|
Bi |
di1 |
di2 |
…
|
dij |
…
|
diN |
…
|
…
|
…
|
…
|
…
|
…
|
…
|
BM |
dM1 |
dM2 |
…
|
dMj |
…
|
dMN |
wherein, w1~wNRepresenting the load node, B, in the system1~BMRepresenting M black-start power supply nodes, dijThe minimum topological distance between each load node and the black start power supply node is shown, N is the number of the load nodes, M is the number of the black start power supply nodes, i is the serial number of the black start power supply node, i is more than or equal to 1 and less than or equal to M, j is the serial number of the load nodes, and j is more than or equal to 1 and less than or equal to N.
Further, element E in the load node relationship matrix tablejkThe values are as follows:
further, the variable vip is used for representing whether the load node is a class load or notjAnd a variable con for characterizing whether the load node is an adjustable loadjThe value is taken according to the following formula:
further, the partition range table is:
|
w1 |
w2 |
…
|
wj
|
…
|
wN |
B1 |
v11 |
v12 |
…
|
…
|
…
|
v1N |
B2 |
v21 |
v22 |
…
|
…
|
…
|
v2N |
…
|
…
|
…
|
…
|
…
|
…
|
…
|
Bi |
vi1 |
vi2 |
…
|
vij |
…
|
viN |
…
|
…
|
…
|
…
|
…
|
…
|
…
|
BM |
vM1 |
…
|
…
|
vMj |
…
|
vMN |
wherein v isijPartition dependency values, v, for black start power node i and load node jijIs 0 or 1; each column in the partition range table has only one element of 1, and the others are 0; v. ofij When 1, it indicates the load node wjRow-in black start power node BiV. power supply section ofijWhen 0 denotes the load node wjNon-intrusive black start power node BiThe power supply partition of (1).
Further, the energy function is expressed as follows:
wherein E is an energy function value, E1-E5 are coefficients greater than 0, v
ijPartition dependency values, v, for black start power node i and load node j
mnThe partition dependency values of a black start power source node M and a load node N are obtained, M is the serial number of the black start power source node, M is more than or equal to 1 and less than or equal to M, M is not less than i, N is the serial number of the load node, N is more than or equal to 1 and less than or equal to N, and N is not equal to j; e
jnRepresenting the connection state of a load node j and a load node n; gamma ray
iIs an intermediate variable, τ
iIs the intermediate variable(s) of the variable,
w
jis the capacity of node j, s
iIs B
iΔ is a scale factor;
α
ipower supply node B for black start
iThe minimum force coefficient of (c).
A power supply network black start partition scheme computing system comprises a memory and a processor, wherein the memory is stored with a computer program capable of running on the processor, and the processor executes the computer program to realize the computing method.
Compared with the prior art, the invention has at least the following beneficial technical effects:
the invention provides a brand new energy function to achieve the aim of minimum inter-partition junctor, and describes the constraint conditions of minimum junctor, balance between adjustable load and black start power supply, quick power restoration of one class of load and the like by using a uniform analytic expression for the first time. Because the optimal partition scheme and the constraint conditions are simultaneously expressed by a uniform analytic expression, the partition scheme can be directly solved by solving a differential equation system. The process of solving the system of differential equations is itself a process of gradually reducing the energy function to a minimum value in the direction of the gradient. The energy function can be reduced to the lowest value by solving the differential equation, and the obtained solution is the analytic solution of the optimal partition scheme.
The design of the energy function is characterized in that the analytic expressions corresponding to all constraint terms in the energy function can be 0 only when the obtained solution is reasonable and feasible. The number of links is minimal, and the energy function is only guaranteed to be minimal when the obtained solution is reasonable and feasible. Therefore, the rationality of the solution can be guaranteed by the solution when the energy function obtained by solving the differential equation is the lowest, the connecting line can be minimized, and the decision can be conveniently and quickly made. The method is suitable for program implementation and is actually verified, the power grid and the most common IEEE-39 node system provided by the embodiment are actually calculated and verified, the iterative computation times reach the minimum value of the energy function within 200 times, at the moment, the constraint terms of the energy function are all 0, and the obtained solution is reasonable and the number of connecting lines is minimum. The invention provides a brand new thought and method for the calculation of the black start partitioning scheme.
The invention uniformly considers the constraint conditions of balancing between the adjustable load and the black start power supply, ensuring the quick recovery of power supply of the load and the like in the energy function. In order to rapidly solve the partition scheme, an analytic solution of the optimal partition scheme is directly solved by a method for solving a differential equation system, instead of providing manual selection of various schemes. The proposed method provides a new approach for the determination of black start partitioning schemes without the aid of other linear programming tools.
Furthermore, the first term of the energy function is 0 only under one condition, namely the sum of the numerical values of each column in the partition range table is 1, namely only one unit in each column of the partition range table is 1, and the rest are 0, so that each load node is ensured to be powered by a black start power supply; in the second term constraint of the energy function, the capacity of the black-start power supply node i is greater than the total amount of a class of loads in the power supply area
If the value is 0, otherwise, the value is 1, and the power supply power balance of the power supply area is ensured;
it can be found that the capacity of the black-start power supply node i is less than the total amount of adjustable load in its supply area
Is 0, otherwise is 1; the third item can restrict the adjustable load capacity of each subarea to be larger than the output force of the black start power supply; the fourth item restricts the loss caused by power supply of each load node as small as possible; the fifth item ensures that the nodes of each zone are wired to the black start power supply node of that zone.
Detailed Description
In order to make the objects and technical solutions of the present invention clearer and easier to understand. The present invention will be described in further detail with reference to the following drawings and examples, wherein the specific examples are provided for illustrative purposes only and are not intended to limit the present invention.
In the description of the present invention, the terms "first" and "second" are used for descriptive purposes only and are not to be construed as indicating or implying relative importance or implying any number of technical features indicated. Thus, a feature defined as "first" or "second" may explicitly or implicitly include one or more of that feature. In the description of the present invention, "a plurality" means two or more unless otherwise specified. In the description of the present invention, it should be noted that, unless otherwise explicitly specified or limited, the terms "mounted," "connected," and "connected" are to be construed broadly, e.g., as meaning either a fixed connection, a removable connection, or an integral connection; can be mechanically or electrically connected; they may be connected directly or indirectly through intervening media, or they may be interconnected between two elements. The specific meanings of the above terms in the present invention can be understood in specific cases to those skilled in the art.
Referring to fig. 1, a power supply network black start partition scheme calculation method includes the following steps:
the method comprises the following steps: the minimum topological relation matrix of the load node-black start power supply shown in the table 1 is constructed
TABLE 1 topological relationship matrix
|
w1 |
w2 |
…
|
wj |
…
|
wN
|
B1 |
d11 |
d12 |
…
|
d1j |
…
|
d1N |
B2 |
d21 |
d22 |
…
|
d2j |
…
|
d2N |
…
|
…
|
…
|
…
|
…
|
…
|
…
|
Bi |
di1 |
di2 |
…
|
dij |
…
|
diN |
…
|
…
|
…
|
…
|
…
|
…
|
…
|
BM |
dM1 |
dM2 |
…
|
dMj |
…
|
dMN |
In Table 1, w1~wNFor the load nodes in the system, B1~BMThe number of the power nodes capable of being started in black is M, and the power nodes are referred to as black-start power nodes in the following text, wherein N is the number of load nodes, M is the number of the black-start power nodes, i is the serial number of the black-start power nodes, i is more than or equal to 1 and less than or equal to M, j is the serial number of the load nodes, and j is more than or equal to 1 and less than or equal to N. For each unit in Table 1 dijAnd (4) showing. dijThe minimum topological distance from the black-start power source node i to the load node j is defined as the minimum power supply path of the black-start power source node i connected to the load j in an extensive search mode.
Step two: establishing a load node relation matrix table as shown in table 2 according to the incidence relation of each load node, wherein each unit in the table 2 uses EjkAnd (4) showing.
TABLE 2 node relationship matrix
|
w1 |
w2 |
…
|
wk |
…
|
wN |
w1 |
E11 |
E12 |
…
|
E1k |
…
|
E1N |
w2 |
E21 |
E22 |
…
|
E1k |
…
|
E2N |
…
|
…
|
…
|
…
|
…
|
…
|
…
|
wj |
Ej1 |
Ej2 |
…
|
Ejk |
…
|
EjN |
…
|
…
|
…
|
…
|
…
|
…
|
…
|
wN |
EN1 |
EN2 |
…
|
ENk |
…
|
ENN |
EjkRepresenting the connection state of a load node j and a load node k, wherein k is the serial number of the load node, k is more than or equal to 1 and less than or equal to N, EjkThe mathematical description of (a) is:
step three: introducing variable vipjAnd variable conjDefined as shown in formula (2) and formula (3), respectively:
step four: with B1~BMIndicating that the power nodes can be black-started, a partition range table is constructed as shown in table 3.
TABLE 3 partition Range Table
|
w1 |
w2 |
…
|
wj
|
…
|
wN |
B1 |
v11 |
v12 |
…
|
…
|
…
|
v1N |
B2 |
v21 |
v22 |
…
|
…
|
…
|
v2N |
…
|
…
|
…
|
…
|
…
|
…
|
…
|
Bi |
vi1 |
vi2 |
…
|
vij |
…
|
viN |
…
|
…
|
…
|
…
|
…
|
…
|
…
|
BM |
vM1 |
…
|
…
|
vMj |
…
|
vMN |
vijThe unit value v of (i, j) in Table 3ijA partition dependency value v of the power supply partition in which the black start power supply node i is positioned and the load node jijTaking the value of 0 or 1. In Table 3, only one element in each column is 1, and the others are 0, i.e., the sum of the elements in each column is 1. v. ofijWhen 1, it indicates the load node wjRow-in black start power node BiV. power supply section ofijWhen 0 denotes the load node wjNon-intrusive black start power node BiThe power supply partition of (1).
Step five: an energy function represented by the formula (4) is constructed.
Wherein E is an energy function value, E1-E5 are coefficients greater than 0, v
mnThe partition relation value of a black start power source node M and a load node N is shown, M is the serial number of the black start power source node, M is more than or equal to 1 and less than or equal to M, M is not less than i, N is the serial number of the load node, N is more than or equal to 1 and less than or equal to N, and N is not less than j. E
jnTo indicate the connection state of the load node j and the load node n. Gamma ray
iIs an intermediate variable, τ
iIs the intermediate variable(s) of the variable,
w
jis the capacity of node j, s
iIs B
iAnd Δ is a scale factor, and may be 0.01 or less.
α
iPower supply node B for black start
iThe minimum force coefficient of (c).
The first term of the energy function is 0 only in one case, namely the sum of the numerical values of each column in table 3 is 1, namely only one unit of each column in table 3 is 1, and the rest are 0, so that each load node is ensured to be powered by a black start power supply. In the second term constraint of the energy function, the capacity of the black-start power supply node i is greater than the total amount of a class of loads in the power supply area
And if the value is 0, otherwise, the value is 1, and the power supply power balance of the power supply area is ensured.
It can be found that the capacity of the black-start power supply node i is less than the total amount of adjustable load in its supply area
Is 0, otherwise is 1. The third term can restrict the adjustable load of each partitionThe charge is larger than the output of the black start power supply. The fourth term constrains the losses incurred when powering each load node to be as small as possible. The fifth item ensures that the nodes of each zone are wired to the black start power supply node of that zone.
Step six: solving formula (4) using formula (5)
Wherein u isijTo solve for vijThe solving method of the intermediate variable (2) is shown in the formula (6).
Step seven: from equations (4) and (5), the dynamic equation for equation (4) can be solved as follows:
wherein u isvFor the normalization coefficient, it may be taken as 0.01 or less. Solving the formula (6) by using an Eulerian method, calculating an energy function value E according to the formula (4) after each iterative solution, and stopping iterative calculation when the E is not reduced any more. According to vijThe power supply partition, v, of each black start power supply node can be determinedijWhen 1, it indicates the load node wjRow-in black start power node BiV. power supply section ofijWhen 0 denotes the load node wjNon-intrusive black start power node BiThe power supply partition of (1). E does not terminate the iteration when it is decreasing for each element v in Table 3ijAnd the element value and the corresponding energy function E are minimum, the tie line of each partition is also minimum, and the partition is divided into the optimal partition.
Referring to fig. 10, a power supply network black-start partitioning scheme calculation system includes a memory and a processor, the memory stores a computer program that can be executed on the processor, and the processor executes the computer program to implement the power supply network black-start partitioning scheme calculation method.
Example 1
The invention will be described in detail with reference to specific examples, a power supply network of which is shown in FIG. 1, w2And w7Is a type of load, w4And w6For adjustable loading, w1、w3、w5Is a non-categorical and non-adjustable load, B1And B2For the black start power supply, the grid parameters are shown in table 4.
TABLE 4 Power grid parameter Table
|
w1 |
w2 |
w3 |
w4 |
w5 |
w6 |
w7 |
B1 |
B2 |
α1 |
α2 |
Capacity/size (MW)
|
60
|
50
|
75
|
40
|
55
|
40
|
80
|
70
|
90
|
0.3
|
0.3 |
The method comprises the following steps: firstly, a node-black start power supply minimum topology relation matrix shown in table 5 is constructed
TABLE 5 topological relationship matrix
|
w1 |
w2 |
w3 |
w4 |
w5 |
w6 |
w7 |
B1 |
1
|
1
|
2
|
3
|
3
|
2
|
4
|
B 2 |
3
|
3
|
2
|
1
|
1
|
2
|
1 |
Step two: establishing a load node relation matrix table as shown in table 6 according to the incidence relation of each node, wherein each unit in the table uses EjkAnd (4) showing.
TABLE 6 node relationship matrix
|
w1 |
w2 |
w3 |
w4 |
w5 |
w6 |
w7 |
w1 |
0
|
0
|
0
|
0
|
0
|
1
|
0
|
w2 |
0
|
0
|
1
|
0
|
0
|
0
|
0
|
w3 |
0
|
1
|
0
|
1
|
0
|
0
|
0
|
w4 |
0
|
0
|
1
|
0
|
0
|
0
|
0
|
w5 |
0
|
0
|
0
|
0
|
0
|
1
|
1
|
w 6 |
1
|
0
|
0
|
0
|
1
|
0
|
0
|
w7 |
0
|
0
|
0
|
0
|
1
|
0
|
0 |
Step three: introducing variable vipjAnd conj,w2And w7Is a type of load, w4And w6Is an adjustable load.
Step four: a partition range table as shown in table 7 was constructed.
TABLE 7 partition Range Table
|
w1 |
w2 |
w3 |
w4 |
w5 |
w6 |
w7 |
B1 |
v11 |
v12 |
v13 |
v14 |
v15 |
v16 |
v17 |
B2 |
v21 |
v22 |
v23 |
v24 |
v25 |
v26 |
v27 |
In Table 7, vijTaking the value of 0 or 1. In Table 7, only one element in each column is 1, and the others are 0, i.e., the sum of the elements in each column is 1. v. ofijWhen 1, it indicates the load node wjStrike-in black start power supply BiV. power supply section ofijWhen 0 denotes the load node wjNon-strike-in black start power supply BiThe power supply partition of (1). A cell of 1 indicates that the corresponding column node is assigned to the partition in which the corresponding row black start power supply is located.
Step five: an energy function shown in formula (1) is constructed.
Wherein, E1-1000, E2-200, E3-200, E4-20.0, and E5-80.0.
s
iIs B
iAnd Δ is a scale factor, and may be 0.01 or less.
Step six: solving formula (1) using formula (2)
Wherein v isijTable 7 for meaning synchronization; u. ofijTo solve for vijThe solving method of the intermediate variable (2) is shown in the formula (3).
Step seven: from equations (1), (2), the dynamic equation for equation (1) can be solved as follows:
wherein u isv0.01 or less. Solving the formula (3) by using an Eulerian method, calculating an energy function value E according to the formula (1) after each iterative solution, and stopping iterative calculation when the E is not reduced any more. From the calculated vijAnd obtaining each black start power supply partition table 8.
TABLE 8 partition Range Table
|
w1 |
w2 |
w3 |
w4 |
w5 |
w6 |
w7 |
B1 |
1
|
1
|
1
|
0
|
0
|
1
|
0
|
B2 |
0
|
0
|
0
|
1
|
1
|
0
|
1 |
The partition map obtained from Table 8 is shown in FIG. 2, i.e., black start power supply B1Load node w1Load node w2Load node w3And load node w6Is the same partition, black start power supply B2Load node w4Load node w5And load node w7Are the same partition.
Other partition schemes can be searched in a traversal mode, as shown in fig. 3-5, the number of the connection lines of the partition scheme shown in fig. 3 is 4, which is more than the partition scheme obtained by the method of the present invention, and the requirement of ensuring power supply to a class of loads is not satisfied. The number of the partitioning scheme links shown in fig. 4 is 4, which is more than the partitioning scheme obtained by the present invention. The number of the partition scheme connecting lines shown in fig. 5 is 2, which is the same as the partition scheme connecting lines obtained by the invention, but does not satisfy the constraint condition that the adjustable load is larger than the minimum output of the black-start power supply. As can be seen from a comparison of fig. 2 to 5, the partition scheme calculated by the present invention is due to other partition schemes.
The verification is as follows:
example 2
In the following, the detailed description of the present invention is made by referring to specific examples, an IEEE-39 node grid is shown in fig. 6, nodes 12 and 17 are a class of loads, the adjustable loads are numbered (7,20,21,23,24,25,28,31,34,35), the node 30 and the node 33 are black-start power supplies B1 and B2, both sets α are 0.3, and grid parameters are shown in table 9.
TABLE 9 electric network parameter table
The method comprises the following steps: firstly, a node-black start power supply minimum topology relation matrix shown in a table 10 is constructed (after the load point number is deleted, the black start power supply number is sequentially sequenced according to the original order, and the load point number in the subsequent step is the same)
TABLE 10 topological relationship matrix
|
w1
|
w2
|
w3
|
w4
|
w5
|
w6
|
w7
|
w8
|
w9
|
w10
|
w11
|
w12
|
w13
|
B1
|
2
|
1
|
2
|
3
|
4
|
5
|
6
|
5
|
4
|
7
|
6
|
7
|
5
|
B2
|
7
|
6
|
6
|
5
|
6
|
7
|
8
|
7
|
8
|
6
|
8
|
6
|
5
|
|
w14
|
w15
|
w16
|
w17
|
w18
|
w19
|
w20
|
w21
|
w22
|
w23
|
w24
|
w25
|
w26
|
B1
|
4
|
5
|
6
|
4
|
3
|
6
|
7
|
6
|
7
|
8
|
6
|
2
|
3
|
B2
|
4
|
3
|
2
|
3
|
4
|
1
|
2
|
3
|
4
|
5
|
3
|
7
|
5
|
|
w27
|
w28
|
w29
|
w30
|
w31
|
w32
|
w33
|
w34
|
w35
|
w36
|
w37
|
|
|
B1
|
5
|
4
|
5
|
6
|
7
|
8
|
8
|
8
|
3
|
5
|
3
|
|
|
B2
|
4
|
6
|
7
|
8
|
7
|
3
|
5
|
5
|
7
|
7
|
9
|
|
|
Step two: based on the association relationship of each node, a load node relationship matrix table is established as shown in Table 11, wherein each unit in the table uses EjkAnd (4) showing.
TABLE 11 node relationship matrix
Step three: introducing variable vipjAnd conj。
Step four: a partition range table as shown in table 12 was constructed.
TABLE 12 partition Range Table
|
w1
|
w2
|
w3
|
w4
|
w5
|
w6
|
w7
|
w8
|
w9
|
w10
|
w11
|
w12
|
w13
|
B1
|
v1,1 |
v1,2 |
v1,3 |
v1,4 |
v1,5 |
v1,1 |
v1,2 |
v1,8 |
v1,9 |
v1,10 |
v1,11 |
v1,12 |
v1,13 |
B2
|
v2,1 |
v2,2 |
v2,3 |
v2,4 |
v2,5 |
v2,1 |
v2,2 |
v2,8 |
v2,9 |
v2,10 |
v2,11 |
v2,12 |
v2,13 |
|
w14
|
w15
|
w16
|
w17
|
w18
|
w19
|
w20
|
w21
|
w22
|
w23
|
w24
|
w25
|
w26
|
B1
|
v1,14 |
v1,15 |
v1,16 |
v1,17 |
v1,18 |
v1,19 |
v1,20 |
v1,21 |
v1,22 |
v1,23 |
v1,24 |
v1,25 |
v1,26 |
B2
|
v2,14 |
v2,15 |
v2,16 |
v2,17 |
v2,18 |
v2,19 |
v2,20 |
v2,21 |
v2,22 |
v2,23 |
v2,24 |
v2,25 |
v2,26 |
|
w27
|
w28
|
w29
|
w30
|
w31
|
w32
|
w33
|
w34
|
w35
|
w36
|
w37
|
|
|
B1
|
v1,27 |
v1,28 |
v1,29 |
v1,30 |
v1,31 |
v1,32 |
v1,33 |
v1,34 |
v1,35 |
v1,36 |
v1,37 |
|
|
B2
|
v2,27 |
v2,28 |
v2,29 |
v2,30 |
v2,31 |
v2,32 |
v2,33 |
v2,34 |
v2,35 |
v2,36 |
v2,37 |
|
|
In Table 12, vijTaking the value of 0 or 1. In Table 7, only one element in each column is 1, and the others are 0, i.e., the sum of the elements in each column is 1. v. ofijWhen 1, it indicates the load node wjStrike-in black start power supply BiV. power supply section ofijWhen 0 denotes the load node wjNon-strike-in black start power supply BiThe power supply partition of (1). A cell of 1 indicates that the corresponding column node is assigned to the partition in which the corresponding row black start power supply is located.
Step five: an energy function represented by the formula (4) is constructed.
Wherein, E1-1000, E2-200, E3-200, E4-20.0, and E5-80.0.
s
iIs B
iAnd Δ is a scale factor, and may be 0.01 or less.
Step six: solving formula (4) using formula (5)
Wherein v isijThe meaning synchronization table 12; u. ofijTo solve for vijThe solving method of the intermediate variable (2) is shown in the formula (6).
Step seven: from equations (4) and (5), the dynamic equation for equation (4) can be solved as follows:
wherein u isv0.01 or less. Solving the formula (6) by using an Eulerian method, calculating an energy function value E according to the formula (3) after each iterative solution, and stopping iterative calculation when the value E is not reduced. From the calculated vijA black start power supply partition table 13 is obtained.
Table 13 partition range table
|
w1
|
w2
|
w3
|
w4
|
w5
|
w6
|
w7
|
w8
|
w9
|
w10
|
w11
|
w12
|
w13
|
B1
|
1
|
1
|
1
|
1
|
1
|
1
|
1
|
1
|
1
|
0
|
0
|
0
|
0
|
B2
|
0
|
0
|
0
|
0
|
0
|
0
|
0
|
0
|
0
|
1
|
1
|
1
|
1
|
|
w14
|
w15
|
w16
|
w17
|
w18
|
w19
|
w20
|
w21
|
w22
|
w23
|
w24
|
w25
|
w26
|
B1
|
0
|
0
|
0
|
0
|
1
|
0
|
0
|
0
|
0
|
0
|
0
|
1
|
0
|
B2
|
1
|
1
|
1
|
1
|
0
|
1
|
1
|
1
|
1
|
1
|
1
|
0
|
1
|
|
w27
|
w28
|
w29
|
w30
|
w31
|
w32
|
w33
|
w34
|
w35
|
w36
|
w37
|
|
|
B1
|
0
|
0
|
0
|
1
|
0
|
0
|
0
|
0
|
1
|
0
|
1
|
|
|
B2
|
1
|
1
|
1
|
0
|
1
|
1
|
1
|
1
|
0
|
1
|
0
|
|
|
The partition map obtained from table 13 is shown in fig. 7, and the number of links is 4. Other partitioning schemes with few links can be searched in a traversal mode, as shown in fig. 8 and 9, the number of the partitioning scheme links in fig. 8 and 9 is 5, which is more than the partitioning scheme calculated by the present invention. The partition scheme calculated by the present invention is due to other partition schemes.
The above-mentioned contents are only for illustrating the technical idea of the present invention, and the protection scope of the present invention is not limited thereby, and any modification made on the basis of the technical idea of the present invention falls within the protection scope of the claims of the present invention.