Page 214 - Solutions Manual to accompany Electric Machinery Fundamentals
P. 214

Therefore, the current per path is
                            I    120 A
                         I   A         15 A
                             a     8

                 (b) Duplex lap-wound:
                         a   mP     8   16 paths
                                  2
                      Therefore, the current per path is
                            I    120 A
                         I   A         7.5 A
                             a    16

                 (c) Simplex wave-wound:
                         a   2m     1   2  paths
                                  2
                      Therefore, the current per path is
                            I    120 A
                         I   A         60 A
                             a     2

          7-5.   How many parallel current paths will there be in the armature of an 20-pole machine if the armature is (a)
                 simplex lap-wound, (b) duplex wave-wound, (c) triplex lap-wound, (d) quadruplex wave-wound?

                 SOLUTION
                 (a) Simplex lap-wound:
                                        
                         a   mP   (1)(20) 20  paths
                 (b) Duplex wave-wound:
                         a   2m   (2)(2)   4  paths

                 (c) Triplex lap-wound:
                                        
                         a   mP   (3)(20) 60  paths
                 (d) Quadruplex wave-wound:
                         a   2m   (2)(4) 8  paths
                                       
          7-6.   The power converted from one form to another within a dc motor was given by
                                       P conv    E I   AA   
                                                         m
                                                      ind
                 Use the equations for  E A  and  ind   [Equations (7-38) and (7-49)] to prove that  EI   =   ; that is,
                                                                                                      m
                                                                                                   ind
                                                                                           AA
                 prove  that  the  electric power disappearing at the point of power conversion is exactly equal to the
                 mechanical power appearing at that point.
                 SOLUTION
                         P conv    E I
                                AA
                 Substituting Equation (8-38) for  E
                                                A
                              P  K       I
                          conv          A
                               P  K      I 
                          conv       A
                                                 
                 But from Equation (7-49),     K    I , so
                                          ind       A
                                                           208
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