I Meaning of the Hamiltonian when it is not energy

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The discussion centers on the interpretation of the Hamiltonian, denoted as ##E##, when it is not equivalent to the energy of the system. Participants explore the implications of a negative value for ##E##, suggesting it represents the energy of the system plus work done on it, with a constant that is negative. The conversation highlights that the kinetic energy is not conserved due to external work maintaining a constant angular velocity, leading to confusion about why ##E## is not labeled as the total energy of the bead. The distinction in definitions of energy between the textbook and participants is acknowledged, emphasizing the need for clarity in terminology. Ultimately, the discussion reveals differing perspectives on energy definitions within the context of Hamiltonian mechanics.
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Suppose the initial radial position and radial velocity of the bead are ##r_0>0## and ##0## respectively. Then ##E## is negative. Is there any significance to the negative value of ##E##? Note that ##E## is defined by (5.52) and given by (5.144) below.

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Hi happy,
Well what do you think of the paragraph 'The main point here ... ' ?
 
BvU said:
Hi happy,
Well what do you think of the paragraph 'The main point here ... ' ?

Hi BvU,

It suggests that ##E## is the energy of the system ##+## work done on the system ##+## a constant, right? And in this case, that constant is negative.
 
In this case L = T (there is no V). That is all the energy in the system. If the driving force to keep ##\omega## constant stops acting, then I suppose T will remain constant.
I think you have to solve the EL equations to find the constraint forces and that way you'll find their work input is ##m\omega^2##. All the kinetic energy change comes from the driving force (torque).
 
BvU said:
In this case L = T (there is no V). That is all the energy in the system. If the driving force to keep ##\omega## constant stops acting, then I suppose T will remain constant.
I think you have to solve the EL equations to find the constraint forces and that way you'll find their work input is ##m\omega^2##. All the kinetic energy change comes from the driving force (torque).

I can't find the constraint force using the standard method of EL equations with Lagrange undetermined multipliers:

$$\frac{d}{dt}\frac{\partial L}{\partial\dot q_i}=\frac{\partial L}{\partial q_i}+F_i\frac{\partial\eta}{\partial q_i}$$

where ##F_i## is the generalized constraint force and ##\eta=0## is the constraint equation. In this case, ##\eta=\dot\theta-\omega=0##. Since ##\eta## does not depend on ##r## or ##\theta##, ##\frac{\partial\eta}{\partial q_i}=0## and the above equations reduce to the usual EL equations without ##F##.

How do you solve for the constraint force?
 
I do not understand, why the textbook says, ##E## is not the energy of the bead. It depends on the definition of the book. For me energy is the conserved quantity defined via Noether's theorem as the generator of spatial translations, and that's the Hamiltonian. It's clear that the kinetic energy for itself is not conserved since you apply work via the external force to keep ##\omega=\text{const}##, but why ##E## is not called the total energy of the bead here, is not clear to me.
 
vanhees71 said:
I do not understand, why the textbook says, ##E## is not the energy of the bead. It depends on the definition of the book. For me energy is the conserved quantity defined via Noether's theorem as the generator of spatial translations, and that's the Hamiltonian. It's clear that the kinetic energy for itself is not conserved since you apply work via the external force to keep ##\omega=\text{const}##, but why ##E## is not called the total energy of the bead here, is not clear to me.

Your question is answered by the following remark.

Screen Shot 2016-08-28 at 1.46.49 am.png
 
Ok, then the book uses a different definition of energy than I do. Then it's of course consistent in itself.
 
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