Heat conduction along a thin circular cooling fin

PHYSICS · Multi-part · Fermi University Physics · Mathematical Methods for Physics · Ordinary differential equations · Special functions and orthogonal polynomials

Conditions of Validity, Ch Sturm-Liouville theory: the spectral theorem for a differential operator

Problem

Heat conduction along a thin circular cooling fin, with heat lost sideways proportional to temperature, gives the dimensionless equation xy′′+y′−(x+ν2x)y=0,0<x≤X,xy''+y'-\left(x+\frac{\nu^2}{x}\right)y=0,\qquad 0<x\le X, where xx is a dimensionless radial coordinate and ν>0\nu>0 is a fixed (dimensionless) constant. Its two independent solutions are Iν(x)I_\nu(x), which behaves like c1xνc_1x^\nu (finite, in fact tending to zero) as x→0x\to0, and Kν(x)K_\nu(x), which behaves like c2x−νc_2x^{-\nu} (diverging) as x→0x\to0, for constants c1,c2≠0c_1,c_2\ne0 and ν>0\nu>0. ((a)) Write this equation in Sturm-Liouville form −(py′)′+qy=0-(py')'+qy=0 and identify p(x)p(x) and q(x)q(x). ((b)) Show that p(0)=0p(0)=0, so x=0x=0 is a singular endpoint of exactly the same character as the ordinary Bessel equation's endpoint at the axis. ((c)) Using Abel's identity for the Wronskian of two solutions of a self-adjoint second-order equation, show that p(x)(fg′−f′g)p(x)\big(fg'-f'g\big) is the same constant for every x>0x>0 when f,gf,g are any two independent solutions. Hence show that a self-adjoint domain cannot contain both IνI_\nu and KνK_\nu with independent coefficients, and state the condition, with its physical reason, that decides which of the two is kept.

Related theory

Browse the problem library