I've started this, but I'm getting a bit stuck. When a mass of \(2kg\) is attached to a spring whose spring constant is \(32 N/m\) it comes to a rest in the equilibrium position. Starting at \(t=0s\), a force equal to \(Q(t)=68e^{-2t}cos(4t)\) is applied to the system. Find the equation of motion in the absence of damping. \[m\ddot x +\beta \dot x + kx=Q(t), 2\lambda=\frac{\beta}{m}=0,\omega_0^2=\frac{k}{m}=16\] \[\ddot x +16x=68e^{-2t}\cos(4t)\] \[x_c=c_1\cos(\omega_0 t)+c_2\sin(\omega_0 t)=c_1\cos(4t)+c_2\sin(4t)\]
Correction on one of the equations I noticed now. \[\ddot x + 16x = 34e^{-2t}\cos(4t)\] With this I was able to work out \(x_p\) \[x_p=\frac{1}{2}e^{-2t}\cos(4t) -2e^{-2t}\sin(4t)\] This gives: \[x=c_1\cos(4t)+c_2\sin(4t) + \frac{1}{2}e^{-2t}\cos(4t)-2e^{-2t}\sin(4t)\] Not sure how to find the constants from the problem description though.
u have two constants here so u have to differentiate \( x\) two times
Okay, so I see the first I think \(Q(0)=m\ddot x\) I also see that as time goes on (\(\lim_{t \to \infty}\))? \(x\rightarrow 0\). Not sure I know how to take care of that one, either that or I don't remember how to. If so, \(x_p\) goes toward 0, so the components of \(x_c\) would need to be opposite of each other.
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