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 - 8.5 Oscillations of a Mechanical System - Problems - Page 539: 2

Answer

See below

Work Step by Step

Given: $\frac{d^2y}{dt^2}+w_0^2y=0$ The time interval: $T=\frac{2 \pi}{w_0}=\pi$ The complementary function for the given equation is: $y(t)=c_1\sin w_0t+c_2\cos w_0t$ Since $y(0)=y_0,y'(0)=v_0$ We have $c_2=y_0,c_1=\frac{v_0}{w_0}$ Hence, the general solution is $y(t)=\frac{v_0}{w_0}\sin w_0t+y_0\cos w_0t=\sqrt (\frac{v_0}{w_0})^2+y_0^2\cos(wt+\tan^{-1}\frac{v_0}{y_0w_0})$ The amplitude is $A=\sqrt (\frac{v_0}{w_0})^2+y_0^2$ Phase $\phi=tan^{-1}(\frac{v_0}{y_0w_0})$
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