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The Laplace-domain transfer functions that serve as bases for Bode plots of the voltage- and currentgain ratios are, respectively, (3) of Problem 8.9 and (3) of Problem 8.10. Under the given assumptions, inspection shows that the two transfer functions share a break frequency at ! 1= CC RL RC and the voltage-gain transfer function has another at a higher frequency. Moreover, the voltage plot rises at 40 db per decade to its rst break point, and the current plot at 20 db per decade. With !1v !1i !Li 1 CC RL RC and !2v !Lv RE hib CC RE hib

(Angle-Side-Angle, ASA) If two angles and the included side of one triangle are congruent to the corresponding parts of another, then the triangles are congruent.

EXAMPLE 9.3 A series combination of R 10 and L 20 mH has a current i 5:0 cos 500t 108) (A). Obtain the voltages v and V, the phasor current I and sketch the phasor diagram. Using the methods of Example 9.1, vR 50:0 cos 500t 108 di 50:0 cos 500t 1008 dt v vR vL 70:7 cos 500t 558 V vL L

Fig. 3-4

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the low-frequency asymptotic Bode plots of voltage and current gain are sketched in Fig. 8-19. The given assumption assures a separation of at least a decade between !1v and !2v and between ! 1 and !1v . Since the parameter values are not known, the sketches were made under the assumption that Kb 1 in both plots. When values become known, the Bode plots must be shifted upward by 20 log Kbv 20 log

CHAP. 9]

PRINCIPLE 4:

Fig. 8-19

The phase angle of 458 can be seen in the time-domain graphs of i and v shown in Fig. 9-6(a), and the phasor diagram with I and V shown in Fig. 9-6(b).

(Side-Side-Side, SSS) If three sides of one triangle are congruent to three sides of another, then the triangles are congruent.

Fig. 9-6

0 For the CE ampli er of Fig. 3-10, determine (a) Zin , (b) Zin , and (c) Zo if CC ! 1 but CE cannot be neglected.

Fig. 3-5

Phasors can be treated as complex numbers. When the horizontal axis is identi ed as the real axis of a complex plane, the phasors become complex numbers and the usual rules apply. In view of Euler s identity, there are three equivalent notations for a phasor. polar form rectangular form exponential form The cosine expression may also be written as v V cos !t Re Ve j !t Re Ve j!t The exponential form suggests how to treat the product and quotient of phasors. V1 e j 1 V2 e j 2 V1 V2 e j 1 2 , V1 1 V2 2 V1 V2 1 2 Since V V V V cos j sin V Ve j

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