Chapter 08-Electrical Circuit Analysis-Problem Solutions, Exercises of Electrical Circuit Analysis

This is solution to problems related Electrical Circuit Analysis course. It was given by Prof. Gurnam Kanth at Punjab Engineering College. Its main points are: Steady, State, Equivalent, Circuit, KVL, Equivalent, KCL, Solution, Node, KVL, Mesh

Typology: Exercises

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Chapter 8, Problem 1.
For the circuit in Fig. 8.62, find:
(a)
๎˜‹
๎˜Œ
๎˜Ž
0i and
๎˜‹
๎˜Œ
๎˜Ž
0v,
(b)
๎˜‹
๎˜Œ
dtdi /0๎˜Žand
๎˜‹
๎˜Œ
dtdv /0๎˜Ž,
(c)
๎˜‹๎˜Œ
fiand
๎˜‹๎˜Œ
fv.
Figure 8.62
For Prob. 8.1.
docsity.com
pf3
pf4
pf5
pf8
pf9
pfa
pfd
pfe

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Chapter 8, Problem 1.

For the circuit in Fig. 8.62, find: (a) i 0  and v 0  , (b) di 0 ^ / dt and dv 0 ^ / dt , (c) i fand v f.

Figure 8. For Prob. 8.1.

Chapter 8, Solution 1.

(a)shown in Figure (a). At t = 0-, the circuit has reached steady state so that the equivalent circuit is

i(0-) = 12/6 = 2A, v(0-) = 12V At t = 0+, i(0+) = i(0-) = 2A , v(0+) = v(0-) = 12V (b) For t > 0, we have the equivalent circuit shown in Figure (b). v (^) L = Ldi/dt or di/dt = v (^) L/L Applying KVL at t = 0+, we obtain, vL(0+) โ€“ v(0+) + 10i(0+) = 0 vL(0+) โ€“ 12 + 20 = 0, or v (^) L(0+) = - Hence, di(0+)/dt = -8/2 = -4 A/s Similarly, i (^) C = Cdv/dt, or dv/dt = i (^) C /C i (^) C (0+) = -i(0+) = - dv(0+)/dt = -2/0.4 = -5 V/s (c) As t approaches infinity, the circuit reaches steady state. i(f) = 0 A , v(f) = 0 V

VS^ + ^6 :

(a) (b)

v 10 H (^) 

10 P F

vL 

By the current division principle, i (^) L(0-) = 60(2mA)/(60 + 20) = 1.5 mA vC (0-) = 0 At t = 0+, vC (0+) = vC (0-) = 0 i (^) L(0+) = i (^) L(0-) = 1.5 mA 80 = i (^) R (0+)(25 + 20) + vC (0-) i (^) R (0+) = 80/45k = 1.778 mA But, i (^) R = i (^) C + i (^) L 1.778 = iC (0+) + 1.5 or iC (0+) = 0.278 mA (b) vL(0+) = vC (0+) = 0 But, vL = LdiL/dt and di (^) L(0+)/dt = vL(0+)/L = 0 di (^) L(0+)/dt = 0 Again, 80 = 45iR + vC 0 = 45diR /dt + dvC /dt But, dvC (0+)/dt = i (^) C (0+)/C = 0.278 mohms/1 PF = 278 V/s Hence, diR (0+)/dt = (-1/45)dvC (0+)/dt = -278/ di (^) R (0+)/dt = -6.1778 A/s Also, i (^) R = i (^) C + i (^) L di (^) R (0+)/dt = di (^) C (0+)/dt + di (^) L(0+)/dt -6.1788 = di (^) C (0+)/dt + 0, or di (^) C (0+)/dt = -6.1788 A/s (c) As t approaches infinity, we have the equivalent circuit in Figure (b). i (^) R (f) = i (^) L(f) = 80/45k = 1.778 mA

Chapter 8, Problem 3.

Refer to the circuit shown in Fig. 8.64. Calculate: (a) i (^) L 0  , v (^) c 0  and vR 0  , (b) di (^) L 0 ^ / dt , dv (^) c 0 ^ / dt , and dv (^) R 0 ^ / dt , (c) i (^) L f, v (^) c fand vR f

Figure 8. For Prob. 8.3.

Chapter 8, Solution 3. At t = 00. But, -v-, u(t) = 0. Consider the circuit shown in Figure (a). iL(0-) = 0, and vR (0-) = R (0-) + vC (0-) + 10 = 0, or vC (0-) = -10V.

(a) At t = 0+, since the inductor current and capacitor voltage cannot change abruptly, the inductor current must still be equal to 0A , the capacitor has a voltage equal to โ€“10V. Since it is in series with the +10V source, together they represent a direct short at t = 0+. This means that the entire 2A from the current source flows through the capacitor and not the resistor. Therefore, vR (0+) = 0 V.

Chapter 8, Problem 4. In the circuit of Fig. 8.65, find: (a) v 0  and i 0  , (b) dv 0 ^ / dt and di 0 ^ / dt , (c) v f and i f.

Figure 8.65 For Prob. 8.4.

Chapter 8, Solution 4. (a) At t = 0-, u(-t) = 1 and u(t) = 0 so that the equivalent circuit is shown in Figure (a). i(0-) = 40/(3 + 5) = 5A, and v(0-) = 5i(0-) = 25V.

Hence, i(0+) = i(0 - ) = 5A v(0+) = v(0-) = 25V 3 :

(a)

i (^) + v 

40V + 

4 A

0.1F

(b)

i (^) + vL  40V + 

0.25 H

i (^) C i (^) R

(b) i (^) C = Cdv/dt or dv(0+)/dt = iC(0+)/C For t = 0Since i and v cannot change abruptly,+, 4u(t) = 4 and 4u(-t) = 0. The equivalent circuit is shown in Figure (b).

i (^) R = v/5 = 25/5 = 5A, i(0+) + 4 =i (^) C (0+) + i (^) R (0+) 5 + 4 = iC (0+) + 5 which leads to iC (0+) = 4 dv(0+)/dt = 4/0.1 = 40 V/s

Similarly, vL = Ldi/dt which leads to di(0+)/dt = vL(0+)/L 3i(0+) + vL(0+) + v(0+) = 0 15 + vL(0+) + 25 = 0 or vL(0+) = - di(0+)/dt = -40/0.25 = -160 A/s (c) As t approaches infinity, we have the equivalent circuit in Figure (c).

i(f) = -5(4)/(3 + 5) = -2.5 A v(f) = 5(4 โ€“ 2.5) = 7.5 V

4 A

(c)

i (^) + v 

Chapter 8, Solution 5. (a) For t < 0, 4u(t) = 0 so that the circuit is not active (all initial conditions = 0). i (^) L(0-) = 0 and vC (0-) = 0. For t = 0+, 4u(t) = 4. Consider the circuit below.

Since the 4-ohm resistor is in parallel with the capacitor, i(0+) = vC (0+)/4 = 0/4 = 0 A Also, since the 6-ohm resistor is in series with the inductor, v(0+) = 6i (^) L(0+) = 0V.

(b) di(0+)/dt = d(v (^) R (0+)/R)/dt = (1/R)dvR (0+)/dt = (1/R)dvC(0+)/dt = (1/4)4/0.25 A/s = 4 A/s v = 6iL or dv/dt = 6diL/dt and dv(0+)/dt = 6diL(0+)/dt = 6vL(0+)/L = 0 Therefore dv(0+)/dt = 0 V/s (c) As t approaches infinity, the circuit is in steady-state. i(f) = 6(4)/10 = 2.4 A v(f) = 6(4 โ€“ 2.4) = 9.6 V

i

A

vC 

4A 4 : 0.25F

v 

1 H

i (^) C + vL 

i (^) L

Chapter 8, Problem 6.

In the circuit of Fig. 8.67, find: (a) v (^) R 0  and vL 0  , (b) dv (^) R 0 ^ / dt and dv (^) L 0 ^ / dt , (c) v (^) R f and vL f,

Figure 8. For Prob. 8.6.

Chapter 8, Problem 7. A series RLC circuit has R 10 kศ, L 0. 1 mH, and C 10 PF. What type of damping is exhibited by the circuit? Chapter 8, Solution 7. (^36)

D 2^ R L^ 2 0.1 10 x 10 10 x^ x^  3 50 10 x

Z o LC 0.1 10 x  x 10 10 x  x

D! Z o o overdamped

Chapter 8, Problem 8. A branch current is described by ddt^2 i 2 t  4 didtt  10 it 0

Determine: (a) the characteristic equation, (b) the type of damping exhibited by the circuit, (c) i t given that i 0 1 and di 0 / dt 2. Chapter 8, Solution 8.

(a) The characteristic equation is s^2^  4 s  10 0 (b) s 1,2^ ^4 r^162 ^40  2 r j 2. This is underdamped case. (c ) i t ( ) ( A cos 2.45 t  B sin2.45 ) t e ^2 t di (^) ( 2 A cos 2.45 t  2 B sin2.45 t  2.45 A sin2.45 t  2.45 B cos 2.45 ) t e  2 t dt i(0) =1 = A di(0)/dt = 2 = โ€“2A + 2.45B = โ€“2 + 2.45B or B = 1. i(t) = {cos(2.45t) + 1.6327sin(2.45t)}e โ€“2t^ A. Please note that this problem can be checked using MATLAB.

Chapter 8, Problem 9.

The current in an RLC circuit is described by (^) dtd^22 i  (^10) dtdi  25 i 0 If i 0 10 and di 0 / dt 0 find i t for t! 0.

Chapter 8, Solution 9.

s 2 + 10s + 25 = 0, thus s (^) 1,2 = ^10 r 210 ^10 = -5, repeated roots. i(t) = [(A + Bt)e -5t^ ], i(0) = 10 = A di/dt = [Be -5t^ ] + [-5(A + Bt)e -5t^ ] di(0)/dt = 0 = B โ€“ 5A = B โ€“ 50 or B = 50. Therefore, i(t) = [(10 + 50t)e -5t] A

Chapter 8, Problem 10.

The differential equation that describes the voltage in an RLC network is ddt^22 v  5 dvdt  4 v 0

Given that v 0 0 , dv 0 / dt 10 obtain v t.

Chapter 8, Solution 10.

s 2 + 5s + 4 = 0, thus s1,2 =