A bead threaded on a circular wire of circumference (in metres) has its transverse…

PHYSICS · Multi-part · Fermi University Physics · Mathematical Methods for Physics · Linear algebra and vector spaces · Linear algebra and vector spaces

Conditions of Validity, Ch Inner products, orthogonality and the adjoint

Problem

A bead threaded on a circular wire of circumference LL (in metres) has its transverse displacement modelled by the eigenvalue problem for Ly=−y′′\mathcal{L}y = -y'' on [0,L][0,L], with domain D(T)={y:y(0)=y(L), y′(0)=y′(L)}\mathcal{D}(T) = \{y : y(0)=y(L),\ y'(0)=y'(L)\} (periodic boundary conditions, matching position and slope round the loop). Someone argues: "the only self-adjoint domain for −d2/dx2-\mathrm{d}^2/\mathrm{d}x^2 on an interval is the Dirichlet one, y(0)=y(L)=0y(0)=y(L)=0, because that is the case where the boundary form visibly vanishes term by term. Since the periodic conditions do not set yy or y′y' to zero at either endpoint separately, this operator cannot be self-adjoint." ((a)) Write down the boundary form B(f,g)=[f∗g′−f∗′g]0LB(f,g) = [f^*g'-f^{*\prime}g]_0^L for two functions f,g∈D(T)f,g \in \mathcal{D}(T), and evaluate it using the periodic conditions. ((b)) State whether the quoted argument is correct, and give the correct classification of (L,D(T))(\mathcal{L},\mathcal{D}(T)).

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