Consider an Atwood machine, in which two blocks \(m_1\) and \(m_2\) are suspended by an inextensible string (length \(l\)) which passes over a pulley with moment of inertia \(I\) and radius R. The pulley has frictionless bearings.
Starting from Newton's 2nd Law, find the acceleration of the system.
(modified from Taylor 7.21)
The center of a long frictionless rod is pivoted at the origin, and the rod is forced to rotate in a horizontal plane with constant angular velocity \(\omega\). Consider a bead with mass \(m\) that is free to move frictionlessly along the rod. Find the position of the bead as a function of time using the polar coordinate \(s\) as your generalized coordinate.
(adapted from Taylor 7.20)
A smooth wire is bent into the shape of a helix, with cylindrical polar coordinates \(s=R\) and \(z=\lambda\phi\), where \(R\) and \(\lambda\) are constants and \(z\) is the vertically up (and gravity vertically down). Using \(z\) as your generalized coordinate, write down the Lagrangian for a bead of mass \(m\) threaded on the wire.
Find the bead's vertical acceleration \(\ddot{z}\).
Use three sensemaking strategies to evaluate your answer to part (a). (Don't forget to articulate your expected result for each strategy.)
In the limit that \(\lambda\rightarrow 0\), what is \(\ddot{z}\)? Explain conceptually how this makes sense.