Loose Leaf for Engineering Circuit Analysis Format: Loose-leaf
Loose Leaf for Engineering Circuit Analysis Format: Loose-leaf
9th Edition
ISBN: 9781259989452
Author: Hayt
Publisher: Mcgraw Hill Publishers
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Chapter 17, Problem 61E

(a)

To determine

The value of output voltage, v0(t).

(a)

Expert Solution
Check Mark

Answer to Problem 61E

The value of output voltage, v0(t)=5.444e0.625t(cos(1.45t+23.32ο))V.

Explanation of Solution

Given data:

The input voltage is, vi(t)=5u(t)V

The given diagram is shown in Figure 1.

Loose Leaf for Engineering Circuit Analysis Format: Loose-leaf, Chapter 17, Problem 61E , additional homework tip  1

Calculation:

Mark the loop current i in the given figure.

The required diagram is shown in Figure 2.

Loose Leaf for Engineering Circuit Analysis Format: Loose-leaf, Chapter 17, Problem 61E , additional homework tip  2

The conversion of mH into H is given as,

1mH=1×103H

The conversion of 800mH into H is given as,

800mH=800×103H=0.8H

Hence, the value of the inductor, L=0.8H

The conversion of mF into F is given as,

1mF=1×103F

The conversion of 500mH into F is given as,

500mF=500×103F=0.5F

Hence, the value of the capacitor, C=0.5F

The expression for output voltage using KVL is given by,

i(t)+0.8di(t)dt+10.5i(t)dt=vi(t)

Substitute 5u(t) for vi(t) in the above expression.

i(t)+0.8di(t)dt+10.5i(t)dt=5u(t)

Apply Fourier transform to the above expression.

I(jω)+0.8jωI(jω)+2jωI(jω)=F[5u(t)]I(jω)[jω+0.8(jω)2+2jω]=F[5u(t)]        (1)

The Fourier transform of 5u(t) is given by,

F[5u(t)]=5(πδ(ω)+1jω)

Substitute 5(πδ(ω)+1jω) for F[5u(t)] in equation (1).

I(jω)[jω+0.8(jω)2+2jω]=5(πδ(ω)+1jω)I(jω)[jω+0.8(jω)2+2]=5[(jω)πδ(ω)+1]I(jω)0.8[(jω)2+1.25jω+2.5]=5[(jω)πδ(ω)+1]I(jω)=6.25[(jω)πδ(ω)(jω)2+1.25jω+2.5+1(jω)2+1.25jω+2.5]

Further solve as,

I(jω)=6.25[πδ(ω)[(jω+0.625j1.45)0.625+j1.45](jω+0.625j1.45)(jω+0.625+j1.45)+1(jω+0.625+j1.45)(jω+0.625j1.45)]=6.25[πδ(ω)(jω+0.625+j1.45)(πδ(ω)(0.625j1.45)(jω+0.625j1.45)(jω+0.625+j1.45))+1(jω+0.625+j1.45)(jω+0.625j1.45)]=6.25[πδ(ω)(jω+0.625+j1.45)+(πδ(ω)(0.5+j0.215)(jω+0.625j1.45))πδ(ω)(0.5+j0.215)jω+0.625+j1.45+6.25j2.91(jω+0.625+j1.45)1jω+0.625j1.45]=3.125[2πδ(ω)(jω+0.625+j1.45)+(2πδ(ω)(0.5+j0.215)(jω+0.625j1.45))2πδ(ω)(0.5+j0.215)jω+0.625+j1.45+2.155j1(jω+0.625+j1.45)1jω+0.625j1.45]

Apply shifting property for ω0 in δ(ω) terms.

Further solve as,

I(jω)=[3.125(2πδ(ω))[((0.5j0.215)(0.625+j1.45))+(0.5+j0.215)0.625j1.45]+2.155j1(jω+0.625+j1.45)1jω+0.625j1.45]=[3.125(2πδ(ω))[(0.2j0.0865)+(0.2j0.0865)]+2.155j1(jω+0.625+j1.45)1jω+0.625j1.45]=[3.125(2πδ(ω))[0.4]+2.155j1(jω+0.625+j1.45)1jω+0.625j1.45]=1.25(2πδ(ω))+2.155j1(jω+0.625+j1.45)1jω+0.625j1.45        (2)

The inverse Fourier transform for the 2πδ(ω) is given by,

F1[2πδ(ω)]=1

The inverse Fourier transform for the 1jω+0.625+j1.45 is given by,

F1[ 1jω+0.625+j1.45 ]=e(0.625+j1.45)tu(t)

The inverse Fourier transform for the 1jω+0.625j1.45 is given by,

F1[1jω+0.625j1.45]=e(0.625j1.45)tu(t)

Substitute 1 for 2πδ(ω), e(0.625+j1.45)tu(t) for 1jω+0.625+j1.45 and e(0.625j1.45)tu(t) for 1jω+0.625j1.45 in equation (2).

i(t)=1.25+j2.155[e(0.625+j1.45)te(0.625j1.45)t]u(t)

The expression for the output voltage from the figure is given by,

v0(t)=0.8di(t)dt

Substitute 1.25+j2.155[e(0.625+j1.45)te(0.625j1.45)t]u(t) for i(t) in the above expression.

v0(t)=0.8ddt[1.25+j2.155[e(0.625+j1.45)te(0.625j1.45)t]u(t)]=0.8(j2.155)[(0.625+j1.45)e(0.625+j1.45)t+(0.625j1.45)e(0.625j1.45)t]=2.5j1.0775e(0.625+j1.45)t+2.5+j1.0775e(0.625j1.45)t=e0.625t(2.72223.32ο)ej1.45t+e0.625t(2.72223.32ο)ej1.45t

Further solve as,

v0(t)=2(2.2722)e0.625t(cos(1.45t+23.32ο))=5.444e0.625t(cos(1.45t+23.32ο))

Conclusion:

Therefore, the value of output voltage, v0(t)=5.444e0.625t(cos(1.45t+23.32ο))V.

(b)

To determine

The value of output voltage, v0(t).

(b)

Expert Solution
Check Mark

Answer to Problem 61E

The value of output voltage, v0(t)=5.134e0.625t(cos(1.45t+136.1ο))V.

Explanation of Solution

Given data:

The input voltage is, vi(t)=3δ(t)V

Calculation:

The expression for output voltage using KVL is given by,

i(t)+0.8di(t)dt+10.5i(t)dt=vi(t)

Substitute 3δ(t) for vi(t) in the above expression.

i(t)+0.8di(t)dt+10.5i(t)dt=3δ(t)

Apply Fourier transform to the above expression.

I(jω)+0.8jωI(jω)+2jωI(jω)=F[3δ(t)]I(jω)[jω+0.8(jω)2+2jω]=F[3δ(t)]        (3)

The Fourier transform of 3δ(t) is given by,

F[3δ(t)]=3

Substitute 3 for F[3δ(t)] in equation (3).

I(jω)[jω+0.8(jω)2+2jω]=3I(jω)[jω+0.8(jω)2+2]=3jωI(jω)0.8[(jω)2+1.25jω+2.5]=3jωI(jω)=3.75[jω(jω)2+1.25jω+2.5]

Further solve as,

I(jω)=3.75[jω(jω+0.625+j1.45)(jω+0.625j1.45)]=3.75[0.5+j0.215(jω+0.625j1.45)+0.5j0.215jω+0.625+j1.45]=1.875+j0.7875(jω+0.625j1.45)+1.875j0.7875jω+0.625+j1.45        (4)

The inverse Fourier transform for the 1jω+0.625+j1.45 is given by,

F1[1jω+0.625+j1.45]=e(0.625+j1.45)tu(t)

The inverse Fourier transform for the 1jω+0.625j1.45 is given by,

F1[1jω+0.625j1.45]=e(0.625j1.45)tu(t)

Substitute e(0.625+j1.45)tu(t) for 1jω+0.625+j1.45 and e(0.625j1.45)tu(t) for 1jω+0.625j1.45 in equation (4).

i(t)=[(1.875+j0.7875)e(0.625j1.45)t+(1.875j0.7875)e(0.625+j1.45)t]u(t)

The expression for the output voltage from the figure is given by,

v0(t)=0.8di(t)dt

Substitute [(1.875+j0.7875)e(0.625j1.45)t+(1.875j0.7875)e(0.625+j1.45)t]u(t) for i(t) in the above expression.

v0(t)=0.8ddt[(1.875+j0.7875)e(0.625j1.45)t+(1.875j0.7875)e(0.625j1.45)t]u(t)=[(1.5+j0.63)(0.625j1.45)e(0.625j1.45)t(1.5j0.63)(0.625+j1.45)e(0.625+j1.45)t]=(1.85j1.78)e(0.625j1.45)t(1.85+j1.78)e(0.625+j1.45)t=e0.625t(2.567136.1ο)ej1.45t+e0.625t(2.567136.1ο)ej1.45t

Further solve as,

v0(t)=2(2.567)e0.625t(cos(1.45t+136.1ο))=5.134e0.625t(cos(1.45t+136.1ο))

Conclusion:

Therefore, the value of output voltage, v0(t)=5.134e0.625t(cos(1.45t+136.1ο))V.

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Chapter 17 Solutions

Loose Leaf for Engineering Circuit Analysis Format: Loose-leaf

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