Something about configuration manifolds in classical mechanics

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I think it could be interesting.

Consider a mechanical system

Screenshot from 2021-02-25 09-30-39.png
A circle of mass M can rotate about the vertical axis. The angle of rotation is coordinated by the angle ##\psi##. A bead of mass m>0 can slide along this circle. The position of the bead relative the circle is given by the angle ##\theta##.

It is interesting to note that if M>0 the Lagrangian of this system is defined on the tangent bundle ##T\mathbb{T}^2##. But if M=0 then the Lagrangian is defined on the tangent bundle ##TS^2##.
 
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