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Problems 13 through 16 deal with the effect of a sequence of impulses on an undamped oscillator. Suppose that y ty-f(t), y(0

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Answer #1

y''+y=\sum_{k=1}^{20}\delta(t-k\pi)

And so L(y'')+L(y)=\sum_{k=1}^{20}L(\delta(t-k\pi))

We note that L(y'')=s^2L(y)-sy(0)-y'(0)=s^2L(y)

Therefore, s^2L(y)+L(y)=\sum_{k=1}^{20}e^{-k\pi s}

Which means (s^2+1)L(y)=\sum_{k=1}^{20}e^{-k\pi s}

So L(y)=\frac{\sum_{k=1}^{20}e^{-k\pi s}}{s^2+1}

Taking inverse Laplace transform, we have y(t)=\sum_{k=1}^{20} u(t-k\pi)\sin(t-k\pi) which is plotted below:

a K H(x) = {x 20:1.0} 20 20 30 40 50 60 70

\blacksquare

Please do rate this answer positively if you found it helpful. Thanks and have a good day!

Add a comment
Answer #1

y''+y=\sum_{k=1}^{20}\delta(t-k\pi)

And so L(y'')+L(y)=\sum_{k=1}^{20}L(\delta(t-k\pi))

We note that L(y'')=s^2L(y)-sy(0)-y'(0)=s^2L(y)

Therefore, s^2L(y)+L(y)=\sum_{k=1}^{20}e^{-k\pi s}

Which means (s^2+1)L(y)=\sum_{k=1}^{20}e^{-k\pi s}

So L(y)=\frac{\sum_{k=1}^{20}e^{-k\pi s}}{s^2+1}

Taking inverse Laplace transform, we have y(t)=\sum_{k=1}^{20} u(t-k\pi)\sin(t-k\pi) which is plotted below:

a K H(x) = {x 20:1.0} 20 20 30 40 50 60 70

\blacksquare

Please do rate this answer positively if you found it helpful. Thanks and have a good day!

Add a comment
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