This paper introduces a novel methodology for the mathematical modelling of first and second order phase transformations. It will be shown that this methodology can be related to certain limiting cases of the Cahn-Hilliard equation, specifically the cases of having (i) a convex molar free energy function and (ii) a convex molar free energy function with no regularization. The latter case is commonly regarded as unstable; however, by modifying the variational approach and solving for rate-dependent variables, we obtain a stabilized method capable of handling the missing regularization. While the specific numerical method used to solve the equations (a mixed finite element approach) has been previously employed in related contexts (e.g., to stabilize solutions of the Laplace equation), its application to diffusion and diffusional phase transformations is novel. We prove the thermodynamic consistency of the derived method and discuss several use cases. Our work contributes to the development of new mathematical tools for modeling complex phase transformations in materials science.
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