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Phase Field Modelling - Department of Materials Science and ...

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e chosen to represent strain <strong>and</strong> hence can be used to model phasechanges <strong>and</strong> the associated microstructure evolution.In the phase field modelling <strong>of</strong> solidification, there is no distinctionmade between the solid, liquid <strong>and</strong> the interface. All regions are describedin terms <strong>of</strong> the order parameter. This allows the whole domainto be treated simultaneously. In particular, the interface is not trackedbut is given implicitly by the chosen value <strong>of</strong> the order parameter as afunction <strong>of</strong> time <strong>and</strong> space. The classical formulation <strong>of</strong> the free boundaryproblem is replaced by equations for the temperature <strong>and</strong> phasefield.Appendix 1Recall (MP4–6) that a Taylor expansion for a single variable aboutX = 0 is given byJ{X} = J{0} + J ′ {0} X 1! + J ′′ {0} X22!...A Taylor expansion like this can be generalised to more than one variable.Cahn assumed that the free energy due to heterogeneities in asolution can be expressed by a multivariable Taylor expansion:g{y, z, . . .} =g{c 0 } + y ∂g∂y + z ∂g∂z + ...+ 1 []y 2 ∂2 g2 ∂y 2 + z2 ∂2 g∂z 2 +2yz ∂2 g∂y∂z + ... + ...in which the variables, y, z, . . . in our context are the spatial compositionderivatives (dc/dx, d 2 c/dx 2 , etc). For the free energy <strong>of</strong> a small volumeelement containing a one–dimensional composition variation (<strong>and</strong>

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