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Everything remains the same as in Problem 8.2 except the second initial condition, which is now di Q0 di 100 2500=50 500 A=s V or 0 L dt C dt 0:1

Mdb 20 log |Amid| 20 Decade 0 L B ib rp (rb e) Cp (Cb e) + _

The initial values are half those in Problem 8.2, and so, by linearity, i e 250t 1:35 sin 370:8t A

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2. The diagrams are left for the reader. (a) The line parallel to the banks and midway between them (b) The perpendicular bisector of the segment joining the two oats (c) The bisector of the angle between the roads (d) The pair of bisectors of the angles between the roads 3. The diagrams are left for the reader. (a) A circle having the sun as its center and the xed distance as its radius (b) A circle concentric to the coast, outside it, and at the xed distance from it (c) A pair of parallel lines on either side of the row and 20 ft from it (d) A circle having the center of the clock as its center and the length of the clock hand as its radius. 4. (a) EF; (b) GF; (c) EF; (d) GH; (e) EF; ( f ) GH; (g) AB; (h) a 90 arc from A to G with B as center 5. (a) AC; (b) BD; (c) BD; (d) AC; (e) E 6. In each case, the letter refers to the circumference of the circle. (a) A; (b) C; (c) B; (d) A; (e) C; ( f ) A and C; (g) B 7. The description of each locus is left for the reader.

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rx (rbb )

A parallel RLC network, with R 50:0

9. The explanation is left for the reader. 10. (a) (b) (c) (d) (e) The intersection of two of the angle bisectors The intersection of two of the bisectors of the sides The intersection of the bisector of AB and the bisector of jB The intersection of the bisector of jC and a circle with C as center and 5 as radius The intersections of two circles, one with B as center and 5 as radius and the other with A as center and 10 as radius

, C 200 mF, and L 55:6 mH, has an initial charge Q0 5:0 mC on the capacitor. Obtain the expression for the voltage across the network.

Fig. 8-7

11. (a) 1; (b) 1; (c) 4; (d) 2; (e) 2; ( f ) 1

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1 8:99 104 s 2 LC q Since !2 > 2 , the voltage function is oscillatory and so !d !2 2 296 rad/s. 0 0 expression is !2 0 v e 50t A1 cos 296t A2 sin 296t With Q0 5:0 10 3 C, V0 25:0 V. At t 0, v 25:0 V. Then, A1 25:0. 1 50 s 1 2RC

Because of capacitance that is inherent within the transistor, ampli er current- and voltage-gain ratios decrease in magnitude as the frequency of the input signal increases beyond the midfrequency p range. The high-frequency cuto point !H is the frequency at which the gain ratio equals 1= 2 times its midfrequency value [see Fig. 8-1(a)], or at which Mdb has decreased by 3 db from its midfrequency value. The range of frequencies above !H is called the high-frequency region. Like !L , !H is a break frequency. The most useful high-frequency model for the BJT is called the hybrid- equivalent circuit (see Fig. 8-8). In this model, the reverse voltage ratio hre and output admittance hoe are assumed negligible. The base ohmic resistance rbb 0 , assumed to be located between the base terminal B and the base junction B 0 ,

dv 50e 50t A1 cos 296t A2 sin 296t 296e 50t A1 sin 296t A2 cos 296t dt At t 0, dv=dt V0 =RC !d A2 A1 , from which A2 4:22. v e

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