Classical Mechanics (Kibble & Berkshire) · Problem 13.2

Hamilton's equations and phase space — T.W.B. Kibble, F.H. Berkshire

Physics — Mechanics · euler-lagrange-equation

Problem

Find the extremal of the functional J[y]=∫0π(2xsin⁡t−x˙2) dtJ[y] = \int_0^{\pi} (2x \sin t - \dot{x}^2)\, dt that satisfies x(0)=x(π)=0x(0) = x(\pi) = 0. Show that this extremal provides the global maximum of JJ.

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