Lagrangian and Hamiltonian Methods
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A particle moves in one dimension with action \[ S=\int_{t_1}^{t_2}\left(\frac{1}{2}m\dot{x}^2 - V(x)\right)\,dt. \] The endpoint times \(t_1,t_2\) are fixed, but the endpoint positions \(x(t_1)\) and \(x(t_2)\) are free to vary. What additional condition must the extremal path satisfy at the endpoints?
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