Cahn–Hilliard equation

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CahnHilliard OstwaldRipening

Cahn–Hilliard equation is a partial differential equation that describes the process of phase separation, by which the components of a binary fluid mixture separate into distinct regions of different properties (phases), over time. It was first introduced by John W. Cahn and John E. Hilliard in the late 1950s to model the phase separation process in alloys. The equation is a fundamental model in the study of materials science, particularly in the analysis of the microstructure of alloys, and has applications in various other fields such as biology, geophysics, and fluid dynamics.

Formulation[edit | edit source]

The Cahn–Hilliard equation is given by:

\[ \frac{\partial \phi}{\partial t} = \nabla \cdot \left( M \nabla \left( \frac{\delta F}{\delta \phi} \right) \right) \]

where \(\phi\) represents the concentration of one of the components of the mixture, \(t\) is time, \(M\) is the mobility (a measure of how fast the components can move), and \(F\) is the free energy of the system, which is typically a functional that depends on \(\phi\) and its gradients. The term \(\frac{\delta F}{\delta \phi}\) represents the functional derivative of \(F\) with respect to \(\phi\), indicating how the free energy changes with changes in the concentration.

The free energy \(F\) is often modeled as:

\[ F[\phi] = \int_V \left( f(\phi) + \frac{\kappa}{2}|\nabla \phi|^2 \right) dV \]

where \(f(\phi)\) is a local free energy density that has a double-well potential, representing two stable phases, \(\kappa\) is a positive constant that penalizes gradients in \(\phi\) (thus modeling the energy cost of interfaces between phases), and \(V\) is the volume of the system.

Applications[edit | edit source]

The Cahn–Hilliard equation is used to model and predict the behavior of phase-separating systems in a wide range of applications. In materials science, it helps in understanding the formation of microstructures during the cooling of alloys, which is crucial for determining their mechanical properties. In biology, the equation can describe the separation of cellular components during processes such as cytokinesis. In geophysics, it has been applied to model the formation of patterns in geological formations. Additionally, in fluid dynamics, the equation is used to study the phase separation in binary fluid mixtures, such as oil and water.

Numerical Solutions[edit | edit source]

Solving the Cahn–Hilliard equation, especially in three dimensions or over large time scales, typically requires numerical methods. Common approaches include finite difference methods, finite element methods, and spectral methods. These numerical solutions allow for the simulation of complex phase separation phenomena in various materials and systems.

Challenges and Research Directions[edit | edit source]

Despite its wide applicability, the Cahn–Hilliard equation poses several challenges, particularly in terms of computational resources required for solving it in complex systems. Research in this area focuses on developing more efficient numerical algorithms, understanding the equation's behavior in different physical contexts, and extending the model to include additional effects such as temperature dependence, anisotropy, and external fields.

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Contributors: Prab R. Tumpati, MD