Page 145 - Schaum's Outline of Theory and Problems of Electric Circuits
P. 145

FIRST-ORDER CIRCUITS
               134


















                                                        Fig. 7-10                               [CHAP. 7


               7.7  COMPLEX FIRST-ORDER RL AND RC CIRCUITS
                   A more complex circuit containing resistors, sources, and a single energy storage element may be
               converted to a The ´ venin or Norton equivalent as seen from the two terminals of the inductor or
               capacitor.  This reduces the complex circuit to a simple RC or RL circuit which may be solved accord-
               ing to the methods described in the previous sections.
                   If a source in the circuit is suddently switched to a dc value, the resulting currents and voltages are
               exponentials, sharing the same time constant with possibly different initial and final values. The time
               constant of the circuit is either RC or L=R, where R is the resistance in the The ´ venin equivalent of the
               circuit as seen by the capacitor or inductor.

               EXAMPLE 7.5 Find i, v, and i 1 in Fig. 7-11(a).
















                                                        Fig. 7-11

                   The The ´ venin equivalent of the circuit to the left of the inductor is shown in Fig. 7-11(b) with R Th ¼ 4 
 and
                                                                       3
               v Th ¼ 3uðtÞ (V).  The time constant of the circuit is   ¼ L=R Th ¼ 5ð10 Þ=4s ¼ 1:25 ms.  The initial value of the
               inductor current is zero.  Its final value is
                                                            3V
                                                       v Th
                                                 ið1Þ ¼   ¼    ¼ 0:75 A
                                                       R Th  4
               Therefore,

                                                   di     800t              9   v  1     800t
                               800t
                   i ¼ 0:75ð1   e  ÞuðtÞ  ðAÞ  v ¼ L  ¼ 3e  uðtÞ  ðVÞ    i 1 ¼   ¼ ð3   e   ÞuðtÞðAÞ
                                                   dt                        12    4
                                                         þ
               v can also be derived directly from its initial value vð0 Þ¼ ð9   6Þ=ð12 þ 6Þ¼ 3 V, its final value vð1Þ ¼ 0 and the
               circuit’s time constant.
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