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A. Rabinovich, G. Dagan, T. Miloh
International Journal of Heat and Mass Transfer Volume 55, Issue 4, 31 January 2012, Pages 618–628
Abstract
We solve the problem of heat conduction in a homogeneous media below a planar boundary subjected to time-periodic temperature (of frequency ω), in the presence of a spherical inhomogeneity (of radius R), whose center is at distance d > R from the boundary. In the absence of the sphere, the well known one dimensional solution can be regarded as an oscillating thermal boundary layer of displacement thickness δ = sqrt(2*α/ω), where α is the heat diffusivity. The general solution depends on four dimensionless parameters: d/R, δ/R, the heat conductivity ratio κ and the heat capacity ratio C. An analytical solution is derived as an infinite series of Bessel functions, which converges quickly. The results are illustrated and analyzed for a given accuracy and for a few values of the governing parameters. The general solution can be simplified considerably for asymptotic values of the parameters. A first approximation, obtained for R/d ≪ 1, pertains to an unbounded domain. A further approximate solution, for R/δ ≪ 1, while κ and C are fixed, can be regarded as pertaining to a quasi-steady regime, and is similar in structure to Maxwell’s solution for steady state. However, its accuracy deteriorates for κ ≪ 1, and a solution, coined as the insulated sphere approximation, is derived for this case. Comparison with the exact solution shows that these approximations are accurate for a wide range of parameter values. Besides providing insight, they can be employed for solving in a simple manner more complex problems, e.g. effective properties of a heterogeneous medium made of an ensemble of spherical inclusions.
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