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(a) In polar form, the given frequency transfer function is 1 1 q j tan 1 ! A j! q 2 1 1 ! j tan ! =1 1 ! 2 Hence, and tan 1 ! 1 Mdb 20 log jA j! j 20 log q 10 log 1 ! 2 1 ! 2 (8.5) (8.6)

35.16 Solve the following equations for x: (a) e3x = 2 (b) ln x 3 = 1 (c) ex 2e x = 1 (d) ln ln x = 1 (e) ln x 1 = 0 (a) the area of R;

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(b) If values of (8.5) and (8.6) are calculated and plotted for various values of !, then a Bode plot is generated. This is done in Fig. 8-2, where ! is given in terms of time constants rather than, say, hertz. This particular system is called a lag network because its phase angle is negative for all !.

Mdb T (s) = A(s) =

35.17 Consider the region R under the curve y = ex , above the x-axis, and between x = 0 and x = 1. Find: (b) the volume of the solid generated by revolving R about the x-axis. 35.18 Consider the region R bounded by the curve y = ex/2 , the y-axis, and the line y = e. Find: volume of the solid generated by revolving R about the x-axis.

1 +1

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When both trade and cash discounts are offered, the cash discount is computed after the trade dis count has been taken.

(a) Show that, if continuously compounded at r percent per year, P dollars become Per/100 dollars after 1 year. [Hint: Use Problem 35.30.] Then, after t years, P dollars would become Pert/100 dollars. (b) Continuously compounded at 6 percent per year, how long would it take to double a given amount of money (c) GC When r = 5 percent, compare the result of continuous compounding with that obtained by compounding once a year and with that obtained by compounding monthly. 35.36 GC Use Newton s method to approximate a solution of: 35.37 GC Use Simpson s rule with n = 4 to approximate

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_ 45

36.1 L H PITAL S RULE The following theorem allows us to compute limits of the form lim f (x) g(x)

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Fig. 8-2 Example 8.2. A simple rst-order network has Laplace-domain transfer function and frequency transfer function A s s 1 and A j! 1 j! Determine the network phase angle and the amplitude ratio Mdb , and discuss the nature of the Bode plot. After A j! is converted to polar form, it becomes apparent that tan 1 ! q 20 log jA j! j 20 log 1 ! 2 10 log 1 ! 2 8:7 (8.8)

in the indeterminate case when the numerator f (x) and the denominator g(x) both approach 0 or both approach . Theorem 36.1 (L H pital s Rule): If f (x) and g(x) either both approach 0 or both approach , then lim f (x) f (x) = lim g(x) g (x)

Comparison of (8.5) and (8.7) reveals that the network phase angle is the mirror image of the phase angle for the network of Example 8.1. (As ! increases, ranges from 08 to 908.) Further, (8.8) shows that the amplitude ratio is the mirror image of the amplitude ratio of Example 8.1. (As ! increases, Mdb ranges from 0 to positive values.) Thus, the complete Bode plot consists of the mirror images about zero of Mdb and of Fig. 8-2. Since here the phase angle is everywhere positive, this network is called a lead network.

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A break frequency or corner frequency is the frequency 1= . For a simple lag or lead network, it is the frequency at which M 2 jA j! j2 has changed by 50 percent from its value at ! 0; at that frequency, Mdb has changed by 3 db from its value at ! 0. Corner frequencies serve as key points in the construction of Bode plots.

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