Abstract

In this paper, we investigated the melting process with moving boundary (MB) for the solid material occupying the finite region 0≤y*≤l. The melting material is a mixture consisting of two fluids, with constant thermal conductivities are constants. The melting process is on a slab, and the temperature T at the fixed boundary y*=0 is exponentially proportional to time. The MB can be determined by the coordinate transformation ξ=y∗S∗(t∗) first proposed by Landau[1], where, S*(t*) is the position of the moving boundary. We solved the second order two coupled partial differential equations which describe this problem by using the finite-difference scheme[2] which was first applied to a finite-difference scheme by Crank[3, 4]. Using the finite-difference we can transform the partial differential equations to a system of non-linear algebraic equations. The system of non-linear algebraic equations can be linearized by using (Newton's linearization methods). This system is solved with an initial guess Sn+1,0 where, Sn+1,0 is the moving boundary of the zero level (e.g by Taylor's projection method from the two previous time levels) to find Tn+1,1 where, Tn+1,1 is the temperature of the first level, and hence, Sn+1,1 from both of the MB conditions and the scheme aterated until convergence.

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