Page 157 - Schaum's Outline of Theory and Problems of Electric Circuits
P. 157

[CHAP. 7
                                                FIRST-ORDER CIRCUITS
               146
               7.2   In Problem 7.1, obtain the power and energy in the resistor, and compare the latter with the initial
                     energy stored in the capacitor.
                                          p R ¼ v R i ¼ 25e  125t  ðWÞ
                                               ð       ð
                                                t       t
                                          w R ¼  p R dt ¼  25e  125t  dt ¼ 0:20ð1   e  125t Þ  ðJÞ
                                                0       0
                     The initial stored energy is
                                                                   2
                                                              6
                                                   2
                                                      1
                                               1
                                          W 0 ¼ CV 0 ¼ ð40   10 Þð100Þ J ¼ 0:20 ¼ w R ð1Þ
                                               2      2
                     In other words, all the stored energy in the capacitor is eventually delivered to the resistor, where it is
                     converted into heat.
               7.3   An RC transient identical to that in Problems 7.1 and 7.2 has a power transient
                                                              t=0:00001
                                                    p ¼ 360e         ðWÞ
                                                     R
                     Obtain the initial charge Q 0 ,if R ¼ 10 
.
                                                              2
                                        p R ¼ P 0 e  2t=RC  or  ¼ 10 5  or   C ¼ 2 mF
                                                             RC
                                                   ð  t
                                                                   t=0:00001
                                               w R ¼  p R dt ¼ 3:6ð1   e  Þ  ðmJÞ
                                                    0
                                          2
                     Then, w R ð1Þ ¼ 3:6mJ ¼ Q 0 =2C, from which Q 0 ¼ 120 mC.

               7.4   The switch in the RL circuit shown in Fig. 7-21 is moved from position 1 to position 2 at t ¼ 0.
                     Obtain v R and v L with polarities as indicated.













                                                        Fig. 7-21

                         The constant-current source drives a current through the inductance in the same direction as that of the
                     transient current i.  Then, for t > 0,
                                                     i ¼ I 0 e  Rt=L  ¼ 2e  25t  ðAÞ
                                                    v R ¼ Ri ¼ 200e  25t  ðVÞ
                                                    v L ¼ v R ¼ 200e  25t  ðVÞ




               7.5   For the transient of Problem 7.4 obtain p R and p L .

                                                    p R ¼ v R i ¼ 400e  50t  ðWÞ
                                                    p L ¼ v L i ¼ 400e  50t  ðWÞ

                     Negative power for the inductance is consistent with the fact that energy is leaving the element.  And, since
                     this energy is being transferred to the resistance, p R is positive.
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