Thus, we can compute lD and LF via: lD=LD-kMF; lF=LF-kMF; A similar treatment for the Q-axis quantities results in: lQ=LQ-kMQ; lG=LG-kMQ; Recall the data given for Example 4.2 Calculations given in the book (p. 113) to address without G-winding are: In addition, we need the terms LMD, LMQ which can be obtained from ; (See (4.119) and (4.122), and notes on “FluxLinkageEquations”, p. 4 and p. 6). These calculations are provided in the book for the case without the G-winding, as follows (p. 113): The complete calculation is done, without the G-winding, is provided in the book as follows: and we get for the state-space equation for the first six variables, with = 0 D Example 4.4 What is below is exactly what is in the book. We will modify it to accommodate the G-winding. Extend Examples 4.2 and 4.3 to include the effect of the transmission line and torque equations. The line constants are , rad. The infinite bus voltage constant and the damping torque coefficient are left unspecified. K D
Thus, we can compute lD and LF via: lD=LD-kMF; lF=LF-kMF; A similar treatment for the Q-axis quantities results in: lQ=LQ-kMQ; lG=LG-kMQ; Recall the data given for Example 4.2 Calculations given in the book (p. 113) to address without G-winding are: In addition, we need the terms LMD, LMQ which can be obtained from ; (See (4.119) and (4.122), and notes on “FluxLinkageEquations”, p. 4 and p. 6). These calculations are provided in the book for the case without the G-winding, as follows (p. 113): The complete calculation is done, without the G-winding, is provided in the book as follows: and we get for the state-space equation for the first six variables, with D = 0 Example 4.4 What is below is exactly what is in the book. We will modify it to accommodate the G-winding. Extend Examples 4.2 and 4.3 to include the effect of the transmission line and torque equations. The line constants are , rad. The infinite bus voltage constant K and the damping torque coefficient D are left unspecified.
Example4.2-3.docx