Proving Hamiltonian ≠ Energy for Rotating Ball

AI Thread Summary
The discussion centers on the dynamics of a ball of mass m rotating around a vertical axis with a constant radius r. The Lagrangian is derived as L = (1/2) m r² dot(φ)², leading to the Hamiltonian H expressed as H(q,p) = p²/(2 m r²), which equals the kinetic energy T of the system. The confusion arises regarding the assertion that the Hamiltonian differs from the total energy, particularly in the context of the angular velocity of the ring. The mention of the angular velocity suggests a potential distinction between the system's kinetic energy and the total mechanical energy when considering external influences or constraints. Clarifying these points is essential for understanding the relationship between Hamiltonian mechanics and energy in this rotating system.
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Consider a ball of mass m rotating around an axis Oz (vertical). This ball is on a circle whose center is the same O.
Given: Angular velocity of ring is d∅/dt = ω.
Mind explaining it so we can prove that Hamiltonian here is different from Energy?!
 
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The question is, is your assertion true? Let's start from the Lagrangian, using \phi as the generalized coordinate. The motion on a circle is then described by

\vec{x}=\begin{pmatrix}<br /> r \cos \phi \\ r \sin \phi<br /> \end{pmatrix}<br />

with r=\text{const}. The Lagrangian is

L=T=\frac{m}{2} r^2 \dot{\phi}^2.

The Hamiltonian is then defined as

H(q,p)=\dot{q} p-L

with the canonical momentum

p=\frac{\partial L}{\partial \dot{\phi}}=m r^2 \dot{\phi}.

The Hamiltonian is thus

H(q,p)=\frac{p^2}{2 m r^2}.

Written in terms of \dot{q}=\partial_p H=p/(m r^2) one sees that H=T, and thus H is the energy of the system.
 
Thank you for your reply, very organized, and this is so true! But why did he ask us to prove that H different from E?
 
And why did he mention "Angular velocity of ring is d∅/dt = ω"?
 
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