Classical Mechanics (Goldstein) · Problem 35

The Hamilton Equations of Motion — Herbert Goldstein, Charles Poole, John Safko

Physics — Mechanics · exponential-lagrangian-hamiltonian-motion

Problem

Consider a Lagrangian of the form L=12m(x˙2−ω2x2)eγt,L = \tfrac{1}{2}m(\dot{x}^2 - \omega^2 x^2)e^{\gamma t}, where the particle of mass mm moves in one direction. Assume all constants are positive. (a) Find the equations of motion. (b) Interpret the equations by giving a physical interpretation of the forces acting on the particle. (c) Find the canonical momentum and construct the Hamiltonian. Is this Hamiltonian a constant of the motion? (d) If initially x(0)=0x(0) = 0 and dx/dt=0dx/dt = 0, what is x(t)x(t) as tt approaches large values?

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