Particle motion when wrapped around drum; elastic string

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The discussion focuses on the dynamics of a mass attached to an elastic cable wrapped around a rotating drum. Participants analyze the Lagrangian formulation to derive equations of motion, noting that the mass experiences uniform acceleration superimposed with oscillation. The angular frequency of the oscillation is confirmed as ω² = k(M + 2m)/Mm, while the amplitude of oscillation is debated, with one participant asserting it should be Mmg/k(M + 2m) instead of the book's value. There is also criticism regarding the realism of the elastic potential energy expression used in the problem. Ultimately, the correct approach to finding the underlying constant acceleration is clarified, leading to a resolution of the amplitude discrepancy.
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Homework Statement


A uniform cylindrical drum of mass M and radius a is free to rotate about its axis, which i is horizontal. An elastic cable of negligible mass and length l is wrapped around the drum and carries on its free end a mass m. The cable has elastic potential energy \tfrac12 kx^2 where x is the extension of the cable. The cable is initially fully wound up. Show that the motion of the mass m is a uniform acceleration the same as it would be if the cable were inelastic, but it is superimposed with an oscillation of angular frequency given by \omega^2 = k(M +2m)/Mm. Find the amplitude of the oscillation if the system is released from rest with the cable unextended.

Homework Equations

The Attempt at a Solution



The Lagrangian is
<br /> L = \tfrac14 Ma^2 \dot{\theta}^2 + \tfrac{m}{2} (a\dot{\theta} +\dot{x})^2 + mg(a\theta +x) -\tfrac12 k x^2<br />
where \theta is the angle rotated from its rest position such that a positive angle results in the mass moving downwards. From this we get the equations
<br /> m(a \ddot{\theta} + \ddot{x} ) =mg -kx<br />
and
<br /> Ma \ddot{\theta} +2m(a \ddot{\theta} +\ddot{x}) = 2mg<br />

We can eliminate \ddot{\theta} to get
<br /> \ddot{x} = -\frac{k(M+2m)}{mM}x + g<br />
We can eliminate g by intorducing a new variable but the key point is the angular frequency is the one given in the question. The amplitude then becomes Mmg/k(M+2m), whereas the one given in the book is M^2mg/k(M+2m)^2. Solving for \ddot{\theta} I get
<br /> a \ddot{\theta} = \frac{2k}{M}x<br />
which isn't the uniform acceleration they asked for. The uniform acceleration I think should be 2mg/(M+2m).
 
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I think you have some signs wrong in your Lagrangian.

I really do not like this question. The expression for elastic PE is completely unrealistic here. It is only correct for uniformly stretched elastic. If k is the elastic constant for the whole string, then for the unwound piece of length y it is kl/y. If the extension is x then the PE is klx2/(2y).
 
haruspex said:
I think you have some signs wrong in your Lagrangian.

I really do not like this question. The expression for elastic PE is completely unrealistic here. It is only correct for uniformly stretched elastic. If k is the elastic constant for the whole string, then for the unwound piece of length y it is kl/y. If the extension is x then the PE is klx2/(2y).

I've looked at it a bit and I'm not sure what the sign error would be.
 
Dazed&Confused said:
I've looked at it a bit and I'm not sure what the sign error would be.
Sorry, your signs are correct. I also agree with your amplitude.
Why do you think ##a\ddot\theta## would give the underlying constant acceleration? Can you think of another way to find it?
 
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I did combine two questions here. The previous question was without the string being inelastic and the constant acceleration term was a \ddot{\theta}. I guess there is no other acceleration with the coordinates I have chosen.
 
If I find the acceleration a \ddot{\theta} perhaps then combining the two it will be obvious.
 
Dazed&Confused said:
If I find the acceleration a \ddot{\theta} perhaps then combining the two it will be obvious.
You know that x is a sin function of t, plus a constant, no? Can you not simply discard the sine function and solve for ##\ddot\theta##?
 
I'm not sure what you mean, but I found the answer they were looking for. From a \ddot{\theta} = 2kx/M I found a \theta and then added it to x from which we get a term corresponding to a constant acceleration of 2mg/(M+2m) and an oscillation with the same frequency but with amplitude as given in the book.
 
Dazed&Confused said:
I'm not sure what you mean, but I found the answer they were looking for. From a \ddot{\theta} = 2kx/M I found a \theta and then added it to x from which we get a term corresponding to a constant acceleration of 2mg/(M+2m) and an oscillation with the same frequency but with amplitude as given in the book.
Ah, of course, it's the amplitude of the aθ+x oscillation you want, which is not the same as that of x.
Well done. Sorry I wasn't more helpful.
 

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