Section VI: Load Flow By Newton-Raphson Method
Let us assume that an n -bus power system contains a total np number of P-Q buses while the number of P-V (generator) buses be ng such that n = np + ng + 1. Bus-1 is assumed to be the slack bus. We shall further use the mismatch equations of ΔPi and ΔQi given in (4.9) and (4.10) respectively. The approach to Newton-Raphson load flow is similar to that of solving a system of nonlinear equations using the Newton-Raphson method: At each iteration we have to form a Jacobian matrix and solve for the corrections from an equation of the type given in (4.27). For the load flow problem, this equation is of the form
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(4.30) |
where the Jacobian matrix is divided into submatrices as
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(4.31) |
It can be seen that the size of the Jacobian matrix is ( n + np − 1) x ( n + np −1). For example for the 5-bus problem of Fig. 4.1 this matrix will be of the size (7 x 7). The dimensions of the submatrices are as follows:
J11: (n - 1) ´ (n - 1), J12: (n - 1) ´ np, J21: np ´ (n - 1) and J22: np ´ np
The submatrices are

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(4.32) |

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(4.33) |

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(4.34) |
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(4.35) |
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