gluon1988
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Homework Statement
A bead of mass, m is threaded on a frictionless, straight rod, which lies in the horizontal plane and is forced to spin with constant angular velocity, \omega, about a fixed vertical axis through the midpoint of the rod. Find the Hamiltonian for the bead and show that it does not equal T+U
Homework Equations
\mathcal{L}=T-U
\frac{d}{dt}\frac{\partial\mathcal{L}}{\partial\dot{q}}=\frac{\partial\mathcal{L}}{\partial{q}}
p=\frac{\partial\mathcal{L}}{\partial\dot{q}}
\mathcal{H}=\sum p_{i}\dot{q}_{i}-\mathcal{L}
The Attempt at a Solution
The bead is threaded onto the road, so the radius is fixed. So is the z-axis. The only degree of freedom for the bead is \phi, the angle it is located at in reference to a starting point.
\mathcal{L}=\frac{1}{2}m(\dot{\phi} R)^{2}-U(\phi)
p=\frac{\partial\mathcal{L}}{\partial\dot{\phi}}=m{R^2}{\dot{\phi}}
\mathcal{H}=m{R^2}{{\dot{\phi}}^2}-\frac{1}{2}m(\dot{\phi} R)^{2}-U(\phi)=\frac{1}{2}m(\dot{\phi} R)^{2}+U(\phi)\rightarrow\mathcal{H}=T+U??
I'm assuming I am getting the kinetic energy wrong but I really don't see what it could be with z and R fixed. Please help