Hamiltons Principle proving Newtons laws?

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Hamilton's principle demonstrates that the path a particle takes minimizes the action integral of the Lagrangian, which can be generalized to accommodate various coordinate systems. This generalization is essential because it allows for the application of symmetries in complex systems, making it easier to derive Newton's laws for multiple particles. The Lagrangian and Hamiltonian formulations utilize different mathematical structures, specifically the tangent and cotangent bundles, to represent configurations and velocities or momenta, respectively. Understanding these concepts requires a shift in perspective regarding how space and motion are represented in physics. Grasping Hamilton's principle is crucial for connecting classical mechanics with more advanced formulations.
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My teacher asked us too prove that Hamiltons principle proves that Newtons equations of motion hold for N particles. I'm not sure that i fully grasp the concept but this is my understanding so far:

Using the lagrangian we can prove Newtons law for specific situations, however Hamiltons principle allows us to make the specific situation into generalized coordintes. This is my understanding so far, but i feel that i don't completely understand. Why do we need it to be in generalized coordinates? Why does hamiltons principle allow it to change to generalized coordinates?
 
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One of the strengths of the Lagrangian and Hamiltonian formulations is the ability to use generalized coordinates, which can often be chosen to take advantage of symmetries in the system. To recover Newton's equations, you should choose the generalized coordinates to be the rectangular coordinates associated with Euclidean space.

The above formulations can be given a geometrical interpretation in which the "space" associated with the Lagrangian formulation is a certain manifold called the tangent-bundle and the Hamiltonian formulation with the cotangent-bundle (more generally, a symplectic manifold).
 
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I'm sorry but i was not referring to the Hamiltonian, but to Hamilton's principle. The principle that states that the path that a particle follows is such that the action integral of the Lagrangian from point 1 to point 2 is stationary. I am not sure if you were referring to that and i simply didn't understand it or if there was a miscommunication
 
the configuration of the system is described using a "configuration space" Q (which could be described in any convenient set of coordinates for it)
the tangent-bundle is essentially the "space of configurations and velocities" (TQ)
the cotangent-bundle is essentially the "space of configurations and momenta" (T*Q)

possibly useful:
http://books.google.com/books?id=I2...P79&sig=UrhQn9eZ_avFCBudNiPHYVjRjIM#PPA226,M1
 
thank you. I think my problem stems from me having difficulty wrapping my mind around this concept of changing the way we look at space.
 
I have recently been really interested in the derivation of Hamiltons Principle. On my research I found that with the term ##m \cdot \frac{d}{dt} (\frac{dr}{dt} \cdot \delta r) = 0## (1) one may derivate ##\delta \int (T - V) dt = 0## (2). The derivation itself I understood quiet good, but what I don't understand is where the equation (1) came from, because in my research it was just given and not derived from anywhere. Does anybody know where (1) comes from or why from it the...
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