For a variation with at both endpoints, the first variation isTwo applications of integration by parts remove derivatives from . The boundary terms vanish, and the fundamental lemma of the calculus of variations gives the higher-order Euler-Lagrange equation
For the stated integrand,so the equation reduces toThe general solution of this linear ordinary differential equation isDecay and finiteness of the integral force ; gives , and gives . Hence the unique stationary function is
Articles by others on the same topic
There are currently no matching articles.