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Solutions to Homework Problems CH4 and CH4.5: Circuit Theory, Exams of Electrical and Electronics Engineering

The solutions to homework problems ch4 and ch4.5, covering topics such as differential equations, capacitance, inductance, and circuit theory. The solutions include equations, constants, and initial conditions.

Typology: Exams

Pre 2010

Uploaded on 08/30/2009

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Download Solutions to Homework Problems CH4 and CH4.5: Circuit Theory and more Exams Electrical and Electronics Engineering in PDF only on Docsity! HomeWork #4 Due on Oct 11 (Tue) at 9:30am. (do not turn in) means that the grader does not check, thus no points are assigned. However these questions are also very useful for preparation to Midterm II. CH4.1 P4.4* The solution is of the form of Equation 4.17:      322 10exp100exp  tKRCtKVtv sC in which 2K is a constant to be determined. At 0t , we have   2100500 KvC  Solving, we find that 1502 K and the solution is    310exp150100  ttvC CH4.2 P4.15* In steady state, the equivalent circuit is: Thus, we have A 2 0 23 1   ii i CH4.3 P4.24 The general form of the solution is    LtRKKtiL  exp21 At 0t , we have     2100(0 KKii LL  At t , the inductance behaves as a short circuit, and we have   11.0 KiL  Thus, the solution for the current is     0 for 10-0.1exp-0.1 0 for 0 6   tt ttiL The voltage is       0 for 10exp100 0 for 0 6    tt t dt tdi Ltv CH4.3 (do not turn in) P4.30* (no points) In steady state with the switch closed, we have   0 for 0  tti because the closed switch shorts the source. In steady state with the switch open, the inductance acts as a short circuit and the current becomes   A 1i . The current is of the form     0 for exp21  tLRtKKti in which  20R , because that is the Thévenin resistance seen looking back from the terminals of the inductance with the switch open. Also, we have       1 21 1 000 Ki KKii   Thus, 12 K and the current (in amperes) is given by     0 for 20exp1 0 for 0   tt tti CH4.4 P4.37*Applying KVL, we obtain the differential equation:       0 for exp5  tttRi dt tdi L (1) We try a particular solution of the form:    tAtip  exp (2) in which A is a constant to be determined. Substituting Equation (2) into Equation (1), we have      ttRAtLA  exp5expexp which yields
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