A rod of length is held at zero temperature at both ends

PHYSICS · Multi-part · Fermi University Physics · Mathematical Methods for Physics · Fourier analysis and integral transforms · Function spaces and operator theory

Conditions of Validity, Ch Eigenfunction expansions, convergence and the Rayleigh quotient

Problem

A rod of length LL is held at zero temperature at both ends, so its temperature profiles are expanded in the Dirichlet eigenfunctions yn(x)=sin⁡(nπx/L)y_n(x)=\sin(n\pi x/L), weight w=1w=1, λn=(nπ/L)2\lambda_n=(n\pi/L)^2. Two candidate initial profiles both vanish at x=0x=0 and x=Lx=L: ((a)) f(x)=x(L−x)2f(x)=x(L-x)^2, a smooth (infinitely differentiable) cubic. Apply the boundary-matching chain: check whether ff satisfies the Dirichlet conditions, then whether Lf=−f′′\mathcal{L}f=-f'' also satisfies them, and hence predict the power-law decay of ff's sine coefficients. ((b)) g(x)=L2−∣x−L2∣g(x)=\dfrac{L}{2}-\left|x-\dfrac{L}{2}\right|, a triangular "tent" profile that is continuous but has a discontinuous first derivative (a corner) at x=L/2x=L/2. Explain why the boundary-matching chain of part (a) cannot be carried past its first step for gg, and state, from the standard Fourier decay rate of a triangular wave, whether gg's coefficients decay faster or slower than ff's. ((c)) ff is infinitely differentiable, yet its coefficients fall only as a fixed power of nn. State briefly what this shows about the claim that the decay rate of an eigenfunction expansion is set by the smoothness of the expanded function alone.

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