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Sinusoidal Steady-




                       State Circuit Analysis














               9.1  INTRODUCTION
                   This chapter will concentrate on the steady-state response of circuits driven by sinusoidal sources.
               The response will also be sinusoidal.  For a linear circuit, the assumption of a sinusoidal source
               represents no real restriction, since a source that can be described by a periodic function can be replaced
               by an equivalent combination (Fourier series) of sinusoids. This matter will be treated in Chapter 17.



               9.2  ELEMENT RESPONSES

                   The voltage-current relationships for the single elements R, L,and C were examined in Chapter 2
               and summarized in Table 2-1. In this chapter, the functions of v and i will be sines or cosines with the
               argument !t. ! is the angular frequency and has the unit rad/s. Also, ! ¼ 2 f , where f is the frequency
               with unit cycle/s, or more commonly hertz (Hz).
                   Consider an inductance L with i ¼ I cos ð!t þ 458Þ A [see Fig. 9-1(a)]. The voltage is
                                        di
                                 v L ¼ L  ¼ !LI½  sin ð!t þ 458ފ ¼ !LI cos ð!t þ 1358Þ  ðVÞ
                                        dt



















                                                        Fig. 9-1

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