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9 241 19.4 8.81 6.00 4.77 4.10 3.68 3.39 3.18 3.02 2.90 2.80 2.71 2.65 2.59 2.54 2.49 2.46 2.42 2.39 2.37 2.34 2.32 2.30 2.28 2.27 2.25 2.24 2.22 2.21 2.12 2.04 1.96 1.88

10 242 19.4 8.79 5.96 4.74 4.06 3.64 3.35 3.14 2.98 2.85 2.75 2.67 2.60 2.54 2.49 2.45 2.41 2.38 2.35 2.32 2.30 2.27 2.25 2.24 2.22 2.20 2.19 2.18 2.16 2.08 1.99 1.91 1.83

Find i, the current drawn from the battery, in Problem 7.50. Ans: a i 1 0:5e t=2 ; b i 0:5; c i 1 0:5et

12 244 19.4 8.74 5.91 4.68 4.00 3.57 3.28 3.07 2.91 2.79 2.69 2.60 2.53 2.48 2.42 2.38 2.34 2.31 2.28 2.25 2.23 2.20 2.18 2.16 2.15 2.13 2.12 2.10 2.09 2.00 1.92 1.83 1.75

8.1 INTRODUCTION In 7, RL and RC circuits with initial currents or charge on the capacitor were examined and rst-order di erential equations were solved to obtain the transient voltages and currents. When two or more storage elements are present, the network equations will result in second-order di erential equations. In this chapter, several examples of second-order circuits will be presented. This will then be followed by more direct methods of analysis, including complex frequency and pole-zero plots.

15 246 19.4 8.70 5.86 4.62 3.94 3.51 3.22 3.01 2.85 2.72 2.62 2.53 2.46 2.40 2.35 2.31 2.27 2.23 2.20 2.18 2.15 2.13 2.11 2.09 2.07 2.06 2.04 2.03 2.01 1.92 1.84 1.75 1.67

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20 248 19.4 8.66 5.80 4.56 3.87 3.44 3.15 2.94 2.77 2.65 2.54 2.46 2.39 2.33 2.28 2.23 2.19 2.16 2.12 2.10 2.07 2.05 2.03 2.01 1.99 1.97 1.96 1.94 1.93 1.84 1.75 1.66 1.57

R. Harrison, S. Counsell, R. Nithi. An Evaluation of the MOOD Set of Object-oriented Software Metrics. IEEE TOSE 24:6, June 1998, 491 496.

The second-order di erential equation, which will be examined shortly, has a solution that can take three di erent forms, each form depending on the circuit elements. In order to visualize the three possibilities, a second-order mechanical system is shown in Fig. 8-1. The mass M is suspended by a spring with a constant k. A damping device D is attached to the mass M. If the mass is displaced from its rest position and then released at t 0, its resulting motion will be overdamped, critically damped, or underdamped (oscillatory). Figure 8-2 shows the graph of the resulting motions of the mass after its release from the displaced position z1 (at t 0).

24 249 19.5 8.64 5.77 4.53 3.84 3.41 3.12 2.90 2.74 2.61 2.51 2.42 2.35 2.29 2.24 2.19 2.15 2.11 2.08 2.05 2.03 2.01 1.98 1.96 1.95 1.93 1.91 1.90 1.89 1.79 1.70 1.61 1.52

Fig. 8-1

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40 251 19.5 8.59 5.72 4.46 3.77 3.34 3.04 2.83 2.66 2.53 2.43 2.34 2.27 2.20 2.15 2.10 2.06 2.03 1.99 1.96 1.94 1.91 1.89 1.87 1.85 1.84 1.82 1.81 1.79 1.69 1.59 1.50 1.39

Fig. 8-2

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The series RLC circuit shown in Fig. 8-3 contains no voltage source. the closed loop after the switch is closed is vR vL vC 0 di 1 i dt 0 Ri L dt C

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ilities (maintainability, readability, testability, quality, complexity, etc.) cannot be measured directly, and indirect measures for these attributes are the goal of many metrics programs. The following are criteria for valid indirect metrics: 1. 2. 3. 4. The model must be explicitly de ned. The model must be dimensionally consistent. There should be no unexpected discontinuities. Units and scale types must be correct.

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