Page 39 - Schaum's Outline of Theory and Problems of Electric Circuits
P. 39

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               3.6  VOLTAGE DIVISION                CIRCUIT LAWS                                [CHAP. 3

                   A set of series-connected resistors as shown in Fig. 3-5 is referred to as a voltage divider.  The
               concept extends beyond the set of resistors illustrated here and applies equally to impedances in series, as
               will be shown in Chapter 9.


















                                                        Fig. 3-5
                   Since v 1 ¼ iR 1 and v ¼ iðR 1 þ R 2 þ R 3 Þ,

                                                             R 1
                                                  v 1 ¼ v
                                                        R þ R þ R  3
                                                          1
                                                              2
               EXAMPLE 3.7.  A voltage divider circuit of two resistors is designed with a total resistance of the two resistors
               equal to 50.0 
. If the output voltage is 10 percent of the input voltage, obtain the values of the two resistors in the
               circuit.
                                               v 1                 R 1
                                                 ¼ 0:10   0:10 ¼
                                                v               50:0   10 3
               from which R 1 ¼ 5:0 
 and R 2 ¼ 45:0 
.




               3.7  CURRENT DIVISION
                   A parallel arrangement of resistors as shown in Fig. 3-6 results in a current divider. The ratio of the
               branch current i 1 to the total current i illustrates the operation of the divider.














                                                        Fig. 3-6

                                               v    v   v                 v
                                           i ¼   þ    þ       and    i 1 ¼
                                              R 1  R 2  R 3              R 1
                                      i 1        1=R 1               R 2 R 3
               Then                     ¼                   ¼
                                       i  1=R 1 þ 1=R 2 þ 1=R 3  R 1 R 2 þ R 1 R 3 þ R 2 R 3
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