Abstract
A general mathematical approach to the rigorous treatment of experimental data on nonstationary‐state diffusion in solids of complex shape is developed. The general solution for a uniform initial concentration, c0, and a constant surface concentration, cs, at times greater than zero is shown to be of the form in the neighborhood of time zero, and in the neighborhood of time infinity, where c is the average concentration at time t; S and V are the surface area and volume of the solid, respectively; D is the diffusion coefficient; and f″ (0), α, and β are constants dependent on solid shape. The vacuum drying of wheat has been studied, and it is shown that, for the wheat kernel, f″ (0) = 0.588, α = 0.862; and β2 = 1.301. The diffusion coefficient is an Arrhenius‐type function of temperature given by D = D0 exp {‐E/RT} where D0 = 76.8 cm.2/sec. and E = 12.20 kcal./mole.

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