Differential Equations and Linear Algebra (4th Edition)

Published by Pearson
ISBN 10: 0-32196-467-5
ISBN 13: 978-0-32196-467-0

Chapter 10 - The Laplace Transform and Some Elementary Applications - 10.8 Impulsive Driving Terms: The Dirac Delta Function - Problems - Page 710: 8

Answer

See below

Work Step by Step

Taking the Laplace transform of both sides of the given differential equation and imposing the initial conditions yields: $[s^2(Y)-sY(0)-y'(0)]-4[sY(s)-y(0)]+13Y(s)=e^{-\frac{\pi s}{4}}\\ s(Y)(s^2-4s+13)-3s+12=e^{-\frac{\pi s}{4}}$ which implies that: $Y(s)=\frac{e^{-\frac{\pi s}{4}}}{(s-2)^2+9}+\frac{3s}{(s-2)^2+9}-\frac{12}{(s-2)^2+9}$ Taking the inverse Laplace transform of both sides gives $y(t)=L^{-1}[\frac{e^{-\frac{\pi s}{4}}}{(s-2)^2+9}+\frac{3(s-2)}{(s-2)^2+9}-\frac{6}{(s-2)^2+9}]$ We finally obtain $y(t)=\frac{1}{3}e^{2(t-\frac{\pi}{4})}\sin 3(t-\frac{\pi}{4})u_{\frac{\pi}{4}}(t)+3\cos 3t e^{2t}-2\sin 3te^{2t}$
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