Page 311 - Solutions Manual to accompany Electric Machinery Fundamentals
P. 311

2
                             3 VE           3 V   X   X 
                         P       A   sin          d  q   sin 2
                                                                  
                                                                
                                                          
                                                
                               X  d          2    XX   q 
                                                     d
                                                         
                                                          2
                             3     7621  9890   3 7621   . 0  62   . 0  40 
                         P                  sin                          sin   2
                                                           
                                   . 0  62                   2   62    . 0  . 0   40  
                         P    364    7 .  sin    77    3 .  sin 2       MW
                 A plot of power supplied as a function of torque angle is shown below:


























                 The peak power occurs at an angle of 70.6, and the maximum power that the generator can supply is
                 392.4 MW.

                 (d)  If this generator were non-salient,  P MAX   would occur when  = 90, and  P MAX   would be 364.7
                 MW.  Therefore, the salient-pole generator has a higher maximum power than an equivalent non-salint
                 pole generator.

          C-3.   Suppose that a salient-pole m achine is to be used as a motor.
                 (a) Sketch the phasor diagram of a salient- pole synchronous machine used as a motor.
                 (b) Write the equations describing the voltages and currents in this motor.

                 (c)  Prove that the torque angle  between E  and  V  on this  motor is given by
                                                                
                                                         A
                                                             
                                                           
                                                 IX    cos    I R     sin 
                                         tan -1  A  q          A  A
                                                V     I X  q  sin     I R A  cos 
                                                                  A
                                                     A
                 SOLUTION











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