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When a 4 kg mass is attached to a spring whose constant is 100 N/m, it comes to rest in the equilibrium position. Starting at

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Answer #1

Since there is no damping the differential equation governing the mass spring system is

4 {d^2x(t)\over dt^2}+100x(t)=12e^{-3t}\cos 6t with x(0)=0~,~x'(0)=0

a) The aboce differential equation can be written as

{d^2x(t)\over dt^2}+25x(t)=3e^{-3t}\cos 6t--------------------(1)

The characteristic equation for this equation is

m2 + 25 = 0 m= +52

So the complementary function is 2 (t) = ci cos(5t) + C sin(5t)

The particular solution is given by

x_p(t)= e^{-3t}[A\cos (6t)+B\sin (6t)]

Then, {d^2x_p(t)\over dt^2}= e^{-3t}[9(4A-3B)\sin (6t)-9(4B+3A)\cos (6t)]

Use in equation (1) we get

e^{-3t}[ (36A-2B)\sin (6t)+ (-36B-2A)\cos (6t)] =3e^{-3t}\cos(6t)

Equate coefficients we get A=-{3\over 74}~,~B=-{9\over 37}

So we get x_{p}(t)=e^{-3t}\left ( -{3\over 74}\cos (6t)-{9\over 37}\sin (6t) \right )

So the solution is

x(t)=x_c(t)+ x_{p}(t)= c_1\cos (5t)+c_2\sin (5t)+e^{-3t}\left ( -{3\over 74}\cos (6t)-{9\over 37}\sin (6t) \right )

x(0)=0 gives c_1={3\over 74} also

x'(0)=0 gives c_2=-{99\over 370}

x(t)= {3\over 74}\cos (5t)-{99\over 370}\sin (5t)+e^{-3t}\left ( -{3\over 74}\cos (6t)-{9\over 37}\sin (6t) \right )

At t=\pi

x(\pi)=- {3\over 74} +e^{-3\pi}\left ( -{3\over 74} \right )=-{3\over 74}[1+e^{-3\pi}]

b) The amplitude after very long time

A= \sqrt{{3^2\over 74^2}+{(99)^2\over (370)^2}}={1\over 370}\sqrt{10,026 }

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