Differential Equations and Linear Algebra (4th Edition)

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

Chapter 8 - Linear Differential Equations of Order n - 8.10 Chapter Review - Additional Problems - Page 575: 21

Answer

See below

Work Step by Step

We can notice that: $y'''-6y''+25y'=\sin 4x$ Obtain: $(D^3-6D^2+25D)y=\sin 4x$ Solve the auxiliary equation for the differential equation. $r^3-6r^2+25r=0\\ r(r^2-6r+25)=0$ Roots are: $r_1=0$ as a multiplicity of 1, $r_2=3-4i$ as a multiplicity of 1 and $r_3=3+4i$ as a multiplicity of 1. Therefore, the general solution for the given differential equation is: $y(x)=c_1+c_2e^{3x}\cos 4x+c_3e^{3x}\sin 4x$ We can see that $D^2+16$ is the annihilator of $G(x)=\sin 4x$ Multiply $D^2+16$ to both sides of the given equation we get $(D^2+16)(D^3-6D^2+25D)=0$ Solve the auxiliary equation for the differential equation. $(r^2+16)(r^3-6r^2+25r)=0$ Roots are: $r_1=3-4i$ as a multiplicity of 1, $r_2=3+4i$ as a multiplicity of 1 and $r_2=-4i$ as a multiplicity of 1, $r_4=4i$ as a multiplicity of 1. The general solution to $(D^2+16)(D^3-6D^2+25D)=0$ is $y(x)=c_1e^{3x}\cos 4x+c_2e^{3x}\sin 4x+c_3\cos 4x+c_4\sin 4x$ The trial solution to initial solution is $y_p=c_3\cos x4+c_4\sin 4x$. We obtain the same trial solution with the use of annihilators.
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