consider the unforced, undamped spring system, modelled by m(d^2x/dt^2)+kx=0, and take w=sqt(k/m). Given initial conditions x(0)=xo and x'(0)=vo not both zero, show that x(t)+Acos(wt-a) for A= sqrt(xo^2+(vo/w)^2) and a defined by cosa=xo/A, sina=vo/wA
I'm so confused, how am I supposed to show this?
\[x(t) = A\cos(\omega t - \alpha)\]
find the second derivative and plug it in the differential equation
Ohhhh... I was finding the derivative to the general solution lol I'll try that, thanks
I get (-mw^2+k)(Acos(wt-alpha) :S
right, which is same as : \[(-m\omega^2 + k )x = 0\] yes ?
solve \(\omega \)
Ohhh, same as what's given. What does the A and the alpha part have to do with it?
Okay, so do we agree x(t) = Acos(wt-alpha) satisfies the given differential equation if we assume w = sqrt(k/m) ?
Yes
plugin the initial conditions and find out A and alpha
\(x(0) = x_0 \) \[x_0 = A\cos(0-\alpha)\] \[x_0^2 = A^2\cos^2\alpha\tag {1}\]
get another equation using the other initial condition and solve A and alpha
why did you square it?
you will see it after getting the second equation
I got the second equation, I know that w is squared but I don't see how that helps. I got \[x'(0)=-Aw^2\cos(-\alpha)=v _{o}\]
i think you're substituting in the wrong equation
and then \[A=\frac{ \cos^{-1}(-\alpha)v_o }{ w^2 }\]
looks you're using x''(t) instead of x'(t)
Oh yeah haha
So when you square it alpha doesn't square?
wait dumb question
Okay I still don't see it, \[x'(0)=-Awsin(\alpha)=v_o\] are you squaring both sides then adding them together?
square it and eliminate alpha because that what the problem wants
\[\sin^2\alpha = \left(\frac{v_0}{A\omega}\right)^2\] \[\cos^2\alpha = 1-\left(\frac{v_0}{A\omega}\right)^2\tag{2}\]
solve (1) and (2) for A
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