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p Phase is minimum at ! 1000= 11 301:5 rad/s 8.50 In the circuit of Fig. 8-46 nd the relationship between v2 and v1 for (a) k 103 , case nd its unit-step response; that is, v2 for v1 u t . 6 dv2 4 106 v2 4 107 v1 ; v2 10 1 e 4 10 t u t Ans: a dt 9 dv2 4 108 v2 4 109 v1 ; v2 10 1 e 4 10 t u t b dt (b) k 105 . In each

Fig. 2-31

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The second-stage gain follows directly from (6.46) if RL is replaced with RC2 : Av2 Consequently, the overall gain is

Fig. 8-46

Fig. 2-32

Substituting (1) into (7) and simplifying yield the desired gain: Av s hfe1 hfe2 RC1 RC2 Req sZin2 C2 hie1 hie2 Req Ri sC2 Zin2 Zo1 1 8

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 17.

2.6. In Fig. 2-33 AD and BC are trisected (divided into 3 equal parts).

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The voltage-current relationships for the single elements R, L, and C were examined in 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, ! 2 f , where f is the frequency with unit cycle/s, or more commonly hertz (Hz). Consider an inductance L with i I cos !t 458 A [see Fig. 9-1(a)]. The voltage is vL L di !LI sin !t 458 !LI cos !t 1358 dt V

In the cascaded ampli er of Problem 8.7 (Fig. 6-22 with C1 ; CE ! 1), let hie1 hie2 1500 , hfe1 hfe2 40; C2 1 F; Ri 1k ; RC1 10 k ; RC2 20 k , and RB1 RB2 5 k . Determine (a) the low-frequency gain, (b) the midfrequency gain, and (c) the low-frequency cuto point.

(2.7)

Fig. 9-1

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(a) Letting s ! 0 in (8) of Problem 8.7 makes apparent the fact that the low-frequency gain Av 0 0. (b) The midfrequency gain is determined by letting s ! 1 in (8) of Problem 8.7: From (2), (3), and (4) of Problem 8.7, Av 1 lim Av s

Fig. 2-33

A comparison of vL and i shows that the current lags the voltage by 908 or =2 rad. The functions are sketched in Fig. 9-1(b). Note that the current function i is to the right of v, and since the horizontal scale is !t, events displaced to the right occur later in time. This illustrates that i lags v. The horizontal scale is in radians, but note that it is also marked in degrees ( 1358; 1808, etc.). This is a case of mixed units just as with !t 458. It is not mathematically correct but is the accepted practice in circuit analysis. The vertical scale indicates two di erent quantities, that is, v and i, so there should be two scales rather than one. While examining this sketch, it is a good time to point out that a sinusoid is completely de ned when its magnitude V or I , frequency (! or f ), and phase (458 or 1358) are speci ed. In Table 9-1 the responses of the three basic circuit elements are shown for applied current i I cos !t and voltage v V cos !t. If sketches are made of these responses, they will show that for a resistance R, v and i are in phase. For an inductance L, i lags v by 908 or =2 rad. And for a capacitance C, i leads v by 908 or =2 rad.

(a) If AD > BC, why is AE > BF (b) If EG > FH, why is AG > BH (c) If GD > HC, why is AD > BC (d) If ED > FC, why is EG > FH 2.7. In Fig. 2-34 j BCD and j ADC are trisected. (a) If mj BCD (b) If mj 1 mj ADC, why does mj FCD mj FDC

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