The unwinding coil (teaching experience sharing)

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It is just for teaching experience sharing. Consider a uniform disk. A stretchless and massless wire has been wound on the disk. The end of the wire is attached to the ceiling. Initially the system is at rest as it is shown at the picture. Then the disk is released. It falls down and rotates and the wire unwinds.
Prove that the unwound part of the wire keeps being vertical for all the time.
This fact is evident (I do not know why), nevertheless to provide a correct proof one must write the Lagrange equations for the system with two degrees of freedom and make sure that the corresponding motion satisfies the equations.

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wrobel said:
This fact is evident (I do not know why), ...
Intuitively, because there are no horizontal forces.
 
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A.T. said:
Intuitively, because there are no horizontal forces.
Yes but if the coil has an elliptic shape then there are also no horizontal forces at the beginning but then they appear. I do not know if there are trivial explanations which do not refer equations of motion

hutchphd said:
Aren't there stability issues?
I believe that the Lyapunov stability is a very hard problem here.
 
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wrobel said:
Yes but if the coil has an elliptic shape then there are also no horizontal forces at the beginning but then they appear.
Okay. But if the coil is circular, the only way to make the wire not vertical is to accelerate the center of mass of the coil horizontally. And for this you need horizontal forces away from the vertical. But here any horizontal forces would oppose the deviation from the vertical.

So it's not like the ball on the top of the sphere, which is indeterminate. But rather like a ball at the bottom of a spherical bowl.
 
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Obviously it depends on the initial conditions, whether the wire stays vertical or not. I'd expect the complete solution to give a pendulum-like oscillation together with the motion of the cylinder unwinding the wire. That could be an interesting problem for the analytical-mechanics lecture. I'm pretty sure it can be found in some textbooks.
 
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Once the disk is released, what prevents the center of mass of the disk, after some oscillations, to tend to vertically get aligned with the point of anchorage of the wire to the ceiling?
There is an initial restitutive torque respect to that anchorage point.
 
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wrobel said:
There is a pretty big difference between " my intuition prompts me something" and "Basing on the given mathematical model I can prove the following theorem..."
Yes, I was mainly replying to the question, why it's intuitively self-evident.
 
A.T. said:
Yes, I was mainly replying to the question, why it's intuitively self-evident.
I'm not sure that 'intuitively' is an appropriate word. Your explanation is very reasonable and I have to accept it but, as with a lot of explanations, writing the equations and concluding something is not always intuitive - until you are at a level where you can suspend your disbelief and accept that description of things. I just made a comment on another thread that 'intuition' is, in fact the use of learned knowledge . If you don't have the knowledge then your 'intuition' may be like the intuition Jacob Rees-Mogg describes (virtual ignorance).
I accept that the string must stay vertical but when I look at the diagram, I 'see' the drum swinging like a pendulum. Would I risk my life, relying on your prediction? Hmmm. (Virtual ignorance :wink: )
 
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wrobel said:
It is just for teaching experience sharing. Consider a uniform disk. A stretchless and massless wire has been wound on the disk. The end of the wire is attached to the ceiling. Initially the system is at rest as it is shown at the picture. Then the disk is released. It falls down and rotates and the wire unwinds.

pic-jpg.jpg
Alternative question: What if the wire is not mass-less? Will the coil drift horizontally? If yes, in which direction?
 
I think the main problem is not so much tha mass but the stiffness of the wire. I'd rather think about a massive or massless thread, for which stiffness can be neglected. With a massive thread it's a bit tricky though. For a massless thread it seems to be a straight-forward problem perfectly suitable for the Lagrange or Hamilton formalism (action principle).