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 A7, Problem 1P
To determine

The Laplace transform of the given periodic function.

Expert Solution & Answer
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Answer to Problem 1P

The Laplace transform of the given periodic function is 8s2+π24(s+π2es+π2e3sse4s1e4s).

Explanation of Solution

Given data:

The given periodic waveform is shown in Figure 1.

Loose Leaf for Engineering Circuit Analysis Format: Loose-leaf, Chapter A7, Problem 1P

The time period of this waveform is T=4 s.

Calculation:

The function expression calculated from the figure is written as,

f1(t)={8cos(ωt) 0t1 s0 1t3 s8cos(ω(t4)) 3t4 s        (1)

Here,

ω is the angular frequency.

The angular frequency is given by,

ω=2πT

Substitute 4 for T in the above equation.

ω=2π4=π2

Substitute π2 for ω in equation (1).

f1(t)={8cos((π2)t) 0t1 s0 1t3 s8cos(π2(t4)) 3t4 s        (2)

The Laplace transform of a periodic signal is written as,

L{f(t)}=11eTsL{f1(t)}        (3)

The Laplace transform of the function f1(t) can be expressed as,

L{f1(t)}=04f1(t)estdt

Substitute {8cos((π2)t) 0t1 s0 1t3 s8cos(π2(t4)) 3t4 s for f1(t) in the above equation.

L{f1(t)}=018cos(π2t)estdt+130estdt+348cos(π2(t4))estdt        (4)

The general form of cosθ is expressed as,

cosθ=ejθ+ejθ2

Substitute π2t for θ in the above relation.

cos(π2t)=ejπ2t+ejπ2t2

Substitute ejπ2t+ejπ2t2 for cos(π2t) in equation (4).

L{f1(t)}=018ejπ2t+ejπ2t2estdt+348ejπ2t+ejπ2t2estdt=401(ejπ2t+ejπ2t)estdt+434(ejπ2(t4)+ejπ2(t4))estdt

The above equation is divided into two parts as,

L{f1(t)}=I1+I2        (5)

The first part I1 is expressed as,

I1=401(ejπ2t+ejπ2t)estdt

The second part I2 is expressed as,

I2=434(ejπ2(t4)+ejπ2(t4))estdt        (6)

Solve for I1.

I1=401(ejπ2t+ejπ2t)estdt=401ejπ2testdt+401ejπ2testdt=401e(sjπ2)tdt+401e(s+jπ2)tdt=4[e(sjπ2)t(sjπ2)]01+4[e(s+jπ2)t(s+jπ2)]01

Solve further as,

I1=4[e(sjπ2)1(sjπ2)]+4[e(s+jπ2)1(s+jπ2)]=4[(e(sjπ2)1)(s+jπ2)+(sjπ2)(e(s+jπ2)1)(s+jπ2)(sjπ2)]=4[(esejπ21)(s+jπ2)+(sjπ2)(esejπ21)(s+jπ2)(sjπ2)]=4[(jes1)(s+jπ2)+(sjπ2)(jes1)(s2+(π2)2)]

Solve further as,

I1=4[s(jes1jes1)+jπ2(jes1jes+1)(s2+(π2)2)]=4[2s+jπ2(2jes)(s2+(π2)2)]=8(s+π2es)(s2+(π2)2)

Solve equation (6) for I2 as,

I2=434(ejπ2(t4)+ejπ2(t4))estdt=434ejπ2(t4)estdt+434ejπ2(t4)estdt=434ej2πe(sjπ2)tdt+434ej2πe(s+jπ2)tdt=434e(sjπ2)tdt+434e(s+jπ2)tdt

Solve further as,

I2=4[e(sjπ2)t(sjπ2)]34+4[e(s+jπ2)t(s+jπ2)]34=4[e(sjπ2)4e(sjπ2)3(sjπ2)]+4[e(s+jπ2)4e(s+jπ2)3(s+jπ2)]=4[(e4sej2πe3sej3π2)(s+jπ2)+(sjπ2)(e4sej2πe3sej3π2)(s+jπ2)(sjπ2)]=4[(e4s+je3s)(s+jπ2)+(sjπ2)(e4sje3s)(s2+(π2)2)]

Solve further as,

I2=4[s(e4s+je3s+e4sje3s)+jπ2(e4s+je3s+e4sje3s)(s2+(π2)2)]=4[2se4sπ22e3s(s2+(π2)2)]=8(se4sπ2e3s)s2+(π2)2

Substitute 8(s+π2es)(s2+(π2)2) for I1 and 8(se4sπ2e3s)s2+(π2)2 for I2 in equation (5).

L{f1(t)}=8(s+π2es)(s2+(π2)2)+8(se4sπ2e3s)s2+(π2)2

The Laplace transform of f(t) is F(s) and the Laplace transform of f1(t) is F1(s).

Substitute F1(s) for L{f1(t)} in the above equation.

F1(s)=8(s+π2esse4s+π2e3s)s2+(π2)2=8s2+π24(s+π2es+π2e3sse4s)

Substitute F(s) for L{f(t)} and F1(s) for L{f1(t)} in equation in equation (3).

F(s)=11eTsF1(s)

Substitute 8s2+π24(s+π2es+π2e3sse4s) for F1(s) in the above equation.

F(s)=11eTs(8s2+π24(s+π2es+π2e3sse4s))=8s2+π24(s+π2es+π2e3sse4s1eTs)

Substitute 4 for T in the above equation.

F(s)=8s2+π24(s+π2es+π2e3sse4s1e4s)

Conclusion:

Therefore, the Laplace transform of the given periodic function is. 8s2+π24(s+π2es+π2e3sse4s1e4s).

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