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Chapter 07-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: Time, Required, Voltage, Decay, RC, Circuit, Constant, Source, Free, Switch, Inductor

Typology: Exercises

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Chapter 7, Problem 1.
In the circuit shown in Fig. 7.81
()
,V56 200t
etv
= t > 0
()
,mA8 200t
eti
= t > 0
(a) Find the values of R and C.
(b) Calculate the time constant
τ
.
(c) Determine the time required for the voltage to decay half its initial value at
t = 0.
Figure 7.81
For Prob. 7.1
Chapter 7, Solution 1.
(a) τ=RC = 1/200
For the resistor, V=iR= 200 200 3 56
56 8Re 10 7 k
8
tt
ex R
−−
=
⎯⎯→==
3
11
0.7143
200 200 7 10
CF
R
X
X
µ
== =
(b) τ =1/200= 5 ms
(c) If value of the voltage at = 0 is 56 .
=⎯→=
200 200
156 56 2
2tt
xe e
=⎯→==
1
200 ln2 ln2 3.466 ms
200
oo
tt
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Chapter 7, Problem 1.

In the circuit shown in Fig. 7.

v ( ) t = 56 e −^200 t V, t > 0

i ( ) t = 8 e −^200 t mA, t > 0

(a) Find the values of R and C.

(b) Calculate the time constant τ.

(c) Determine the time required for the voltage to decay half its initial value at

t = 0.

Figure 7.

For Prob. 7.

Chapter 7, Solution 1.

(a) τ=RC = 1/

For the resistor, V=iR=

56 8Re 10 7 k 8

t t e x R

− − − = ⎯⎯→ = = Ω

3

C F

R X X

(b) τ =1/200= 5 ms (c) If value of the voltage at = 0 is 56.

− = ⎯⎯→ =

t t x e e

200 ln2 ln2 3.466 ms 200

t o to

Chapter 7, Problem 2.

Find the time constant for the RC circuit in Fig. 7.82.

Figure 7.

For Prob. 7.2.

Chapter 7, Solution 2.

τ=R (^) th C

where R (^) th is the Thevenin equivalent at the capacitor terminals.

R (^) th= 120 || 80 + 12 = 60 Ω

τ = × × =

60 0. 5 10 30 ms

Chapter 7, Problem 3.

Determine the time constant for the circuit in Fig. 7.83.

Figure 7.

For Prob. 7.3.

Chapter 7, Solution 3.

R = 10 +20//(20+30) =10 + 40x50/(40 + 50)=32.22 kΩ

3 12

τ RC 32.22 X 10 X 100 X 10 3.222 μS

− = = =

Figure 7.

For Prob. 7.5.

Chapter 7, Solution 5.

Let v be the voltage across the capacitor.

For t <0,

4 (0 ) (24) 16 V 2 4

v

− = =

For t >0, we have a source-free RC circuit as shown below.

i

4 Ω

v 1/3 F

τ = RC = + = s

/ / 3 ( ) (0) 16

t t v t v e e

− τ − = =

(^1 1) / 3 / 3 ( ) ( ) 16 1.778 A 3 3

dv t t i t C e e dt

− − = − = − − =

Figure 7.

For Prob. 7.6.

Chapter 7, Solution 6.

v(t) 4 e V

v(t) v e , RC 40 x 10 x 2 x 10

( 24 ) 4 V

v v( 0 )

  1. 5 t

t/ 6 3 o

o

− τ −

= τ= = =

Figure 7.

For Prob. 7.8.

Chapter 7, Solution 8.

(a) 4

τ=RC =

dt

dv

  • i=C
  • 0.2e = C( 10 )(-4)e ⎯⎯→ C =

-4t -4t 5 mF

4 C

R 50 Ω

(b) τ = = = 4

RC 0. 25 s

(c) = = ( 5 × 10 )( 100 )= 2

CV

w (^) C ( 0 ) 02 -^3 250 mJ

(d) (^ )

τ = × = −^0 2 - 2t 0

2 R 0 CV^1 e 2

CV

w

  1. 5 1 e^0 e^0
  • 8t - 8t = − ⎯⎯→ =

or e 0 2

8t

= ln( 2 ) = 8

t 0 86. 6 ms

Figure 7.

For Prob. 7.9.

Chapter 7, Solution 9.

For t < 0, the switch is closed so that

4 (0) (6) 4 V 2 4

v o = =

For t >0, we have a source-free RC circuit. 3 3

τ RC 3 10 x x 4 10 x 12 s

− = = =

/ / ( ) (0) 4 V

t t vo t vo e e

− τ − = =

Chapter 7, Problem 11.

For the circuit in Fig. 7.91, find i (^) 0 for t > 0.

Figure 7.

For Prob. 7.11.

Chapter 7, Solution 11.

For t<0, we have the circuit shown below.

3 Ω 4H

24 V 8 Ω

4H

i (^) o

8 A 3 Ω 8 Ω

3//4= 4x3/7=1.

i o

− = =

A

For t >0, we have a source-free RL circuit. 4 1/ 3 4 8

L

R

/ 3 ( ) (0) 1.4118 A

t t io t io e e

− τ − = =

Chapter 7, Problem 12.

The switch in the circuit of Fig. 7.92 has been closed for a long time. At t = 0 the switch

is opened. Calculate i ( t ) for t > 0.

Figure 7.

For Prob. 7.12.

Chapter 7, Solution 12.

When t < 0, the switch is closed and the inductor acts like a short circuit to dc. The 4 Ω

resistor is short-circuited so that the resulting circuit is as shown in Fig. (a).

4 A

i( 0 )= =

Since the current through an inductor cannot change abruptly,

i( 0 )= i( 0 )=i( 0 )= 4 A

− +

When t > 0, the voltage source is cut off and we have the RL circuit in Fig. (b).

R

L

τ= = =

Hence,

= =

  • tτ i( t) i( 0 )e 4 e A

-2t

(b)

12 V

(a)

i(

- )