A FAST NUMERICAL METHOD FOR A SIMPLIFIED PHASE FIELD MODEL
We consider the phase field model consisting of the system of p.d.e' s \begin{array}{l} q(\theta)\phi t = \nabla \cdot (A\nabla\phi) + f(\phi, u)\,,\\[2pt] u_t = \Delta u + [p(\phi)]_t\,, \end{array} where ϕ = ϕ(x,y,t) is the phase indicator function, θ = arctan $\frac{\phi_{y}}{\phi_{x}}$, u =...
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Published in | Mathematical Methods In Scattering Theory And Biomedical Engineering pp. 208 - 215 |
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Main Authors | , |
Format | Book Chapter |
Language | English |
Published |
WORLD SCIENTIFIC
01.08.2006
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Subjects | |
Online Access | Get full text |
ISBN | 9812568603 9812773193 9789812773197 9789814477598 9814477591 9789812568601 |
DOI | 10.1142/9789812773197_0022 |
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Summary: | We consider the phase field model consisting of the system of p.d.e' s
\begin{array}{l}
q(\theta)\phi t = \nabla \cdot (A\nabla\phi) + f(\phi, u)\,,\\[2pt]
u_t = \Delta u + [p(\phi)]_t\,,
\end{array}
where ϕ = ϕ(x,y,t) is the phase indicator function, θ = arctan $\frac{\phi_{y}}{\phi_{x}}$, u = u(x,y,t) is the temperature, q, p, and f are given scalar functions, and A is a 2 × 2 matrix of suitable functions of θ. This system describes the evolution of phase and temperature in a two phase medium, and is posed for t ≥ 0 on a rectangle in the x, y space with appropriate boundary and initial conditions. We solve the system numerically by a finite difference ADI method and show the results of relevant numerical experiments in the semi-anisotropic case, where A = I. In the case of an isotropic medium with q = 1, and A a diagonal matrix of functions of ϕ, we prove an error estimate of second order accuracy in space and time. |
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ISBN: | 9812568603 9812773193 9789812773197 9789814477598 9814477591 9789812568601 |
DOI: | 10.1142/9789812773197_0022 |