Page 54 - Schaum's Outline of Theory and Problems of Electric Circuits
P. 54

43
                                                  ANALYSIS METHODS
               CHAP. 4]
               the network provides a very clear picture of the overall functioning of the network in terms of voltages,
               currents, and power.  The reduction begins with a scan of the network to pick out series and parallel
               combinations of resistors.


               EXAMPLE 4.6 Obtain the total power supplied by the 60-V source and the power absorbed in each resistor in the
               network of Fig. 4-8.
                                                    R ab ¼ 7 þ 5 ¼ 12
                                                         ð12Þð6Þ
                                                    R cd ¼     ¼ 4
                                                         12 þ 6















                                                         Fig. 4-8
               These two equivalents are in parallel (Fig. 4-9), giving
                                                         ð4Þð12Þ
                                                    R ef ¼     ¼ 3
                                                         4 þ 12
               Then this 3-
 equivalent is in series with the 7-
 resistor (Fig. 4-10), so that for the entire circuit,
                                                    R eq ¼ 7 þ 3 ¼ 10















                                  Fig. 4-9
                                                                               Fig. 4-10

                   The total power absorbed, which equals the total power supplied by the source, can now be calculated as
                                                      V  2  ð60Þ 2
                                                 P T ¼   ¼     ¼ 360 W
                                                      R eq  10
               This power is divided between R ge and R ef as follows:

                                             7                         3
                                  P ge ¼ P 7
 ¼  ð360Þ¼ 252 W    P ef ¼   ð360Þ¼ 108 W
                                            7 þ 3                     7 þ 3
               Power P ef is further divided between R cd and R ab as follows:

                                           12                        4
                                    P cd ¼     ð108Þ¼ 81 W    P ab ¼     ð108Þ¼ 27 W
                                         4 þ 12                    4 þ 12
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