Page 151 - Schaum's Outline of Theory and Problems of Electric Circuits
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                       For t > 1 ms,            FIRST-ORDER CIRCUITS                            [CHAP. 7
                                                                 t
                                              v ¼ 0:632e  ðt 1Þ  ¼ 1:72e , and i ¼ 1:72e  t
               (b) V 0 ¼ 10 V, T ¼ 0:1 ms.
                       For 0 < t < 0:1 ms,
                                                   t       t                0:1
                                        v ¼ 10ð1   e Þ; i ¼ 10e , and V T ¼ 10ð1   e  Þ¼ 0:95 V
                       For t > 0:1 ms,
                                                                 t
                                              v ¼ 0:95e  ðt 0:1Þ  ¼ 1:05e , and i ¼ 1:05e  t
               (c)  V 0 ¼ 100 V, T ¼ 0:01 ms.
                       For 0 < t < 0:01 ms,
                                          t
                              v ¼ 100ð1   e Þ  100t; i ¼ 100e  t    100ð1   tÞ, and V T ¼ 100ð1   e  0:01 Þ¼ 0:995 V
                       For t > 0:01 ms,
                                             v ¼ 0:995e  ðt 0:01Þ  ¼ 1:01e  t  and i ¼ 1:01e  t
                                                                                                 t
                   As the input voltage pulse approaches an impulse, the capacitor voltage and current approach v ¼ e uðtÞ (V)
                            t
               and i ¼  ðtÞ  e uðtÞ.


               7.11  IMPULSE RESPONSE OF RC AND RL CIRCUITS
                   A narrow pulse can be modeled as an impulse with the area under the pulse indicating its strength.
               Impulse response is a useful tool in analysis and synthesis of circuits.  It may be derived in several ways:
               take the limit of the response to a narrow pulse, to be called limit approach, as illustrated in Examples
               7-11 and 7-12; take the derivative of the step response; solve the differential equation directly.  The
               impulse response is often designated by hðtÞ.

               EXAMPLE 7.12   Find the limits of i and v of the circuit Fig. 7-17(a) for a voltage pulse of unit area as the pulse
               duration is decreased to zero.
                   We use the pulse responses in (14) and (15) with V 0 ¼ 1=T and find their limits as T approaches zero. From
               (14c) we have
                                             lim V T ¼ lim ð1   e  T=RC Þ=T ¼ 1=RC
                                            T!0     T!0
               From (15) we have:
                   For t < 0;                   h v ¼ 0  and   h i ¼ 0
                                                        1               1
                              þ

                   For 0 < t < 0 ;              0   h v       and   h i ¼   ðtÞ
                                                       RC               R
                                                       1                        1
                   For t > 0;                   h v ðtÞ¼  e  t=RC  and  h i ðtÞ¼    e  t=RC
                                                                                2
                                                      RC                       R C
               Therefore,
                                       1                            1       1
                                 h v ðtÞ¼  e  t=RC uðtÞ  and   h i ðtÞ¼   ðtÞ   e  t=RC uðtÞ
                                                                            2
                                      RC                            R      R C
               EXAMPLE 7.13   Find the impulse responses of the RC circuit in Fig. 7-17(a) by taking the derivatives of its unit
               step responses.
                   A unit impulse may be considered the derivative of a unit step.  Based on the properties of linear differential
               equations with constant coefficients, we can take the time derivative of the step response to find the impulse
               response.  The unit step responses of an RC circuit were found in (6)tobe
                                      vðtÞ¼ ð1   e  t=RC ÞuðtÞ  and  iðtÞ¼ ð1=RÞe  t=RC uðtÞ
               We find the unit impulse responses by taking the derivatives of the step responses.  Thus
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