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: 14

Answer

See below

Work Step by Step

Given: $\frac{d^2y}{dt^2}+4y=F_0\cos 3t$ At $t=5$ $Force=-4\delta(t-5)$ The equation becomes: $\frac{d^2y}{dt^2}+4y=F_0\cos 3t -4\delta(t-5)$ Taking the Laplace transform of both sides of the given differential equation and imposing the initial conditions yields: $[s^2(Y)-sY(0)-y'(0)]+4Y(s)=\frac{F_0s}{s^2+9}-4e^{-5s}\\ s(Y)(s^2+4)=\frac{F_0s}{s^2+9}-4e^{-5s}$ which implies that: $Y(s)=\frac{F_0s}{s^2+9}-\frac{4e^{-5s}}{s^2+4}$ Taking the inverse Laplace transform of both sides gives $y(t)=L^{-1}[\frac{F_0s}{s^2+9}-\frac{4e^{-5s}}{s^2+4}]$ We finally obtain $y(t)=\frac{-1}{5}F_0\cos 2t+\frac{1}{5}F_0\cos 3t-2\sin 3(t-5)u_5(t)$
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