On the existence, uniqueness, and new analytic approximate solution of the modified error function in two‐phase Stefan problems

Author(s):  
Lazhar Bougoffa ◽  
Randolph C. Rach ◽  
Abdelaziz Mennouni
2019 ◽  
Vol 43 (14) ◽  
pp. 7948-7960
Author(s):  
Miguel A. Piqueras ◽  
Rafael Company ◽  
Lucas Jódar
Keyword(s):  

Author(s):  
Olawanle P. Layeni ◽  
Olusoji Ilori ◽  
Ebenezer O. B. Ajayi

The classical Stefan problem proffers a suitable model for determining the temperature regimes as well as conjugate interfacial positions for multiphase problems. Obtaining the solutions to these problems exactly, especially in systems with cylindrical or spherical symmetry, is often an arduous task. This is largely due to inherent nonlinearities in the mathematical statements of Stefan problems. In this paper, a tractable and effective approach is proposed. Subsequent to a recast as a system of differential-difference equations, and a methodical reduction to constant coefficient difference equations, exact similarity solutions are derived for a class of heterogeneous two-phase Stefan problems with cylindrical or spherical symmetry in one spatial dimension, under either Gaussian or hypergeometric perturbations.


2000 ◽  
Vol 11 (2) ◽  
pp. 153-169 ◽  
Author(s):  
A. A. LACEY ◽  
L. A. HERRAIZ

A mushy region is assumed to consist of a fine mixture of two distinct phases separated by free boundaries. For simplicity, the fine structure is here taken to be periodic, first in one dimension, and then a lattice of squares in two dimensions. A method of multiple scales is employed, with a classical free-boundary problem being used to model the evolution of the two-phase microstructure. Then a macroscopic model for the mush is obtained by an averaging procedure. The free-boundary temperature is taken to vary according to Gibbs–Thomson and/or kinetic-undercooling effects.


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