.. _Mass-Transfer: Mass transfer through interfaces ================================ .. _Gibbs-Thomson-Condition: Gibbs-Thomson condition ----------------------- Gibbs-Thomson condition for a curved interface """""""""""""""""""""""""""""""""""""""""""""" .. admonition:: Gibbs-Thomson condition For a curved interface at equilibrium: .. math:: :label: Equilib_mu_Curved \mu_{in}^{eq}(\phi_{in})=\mu_{out}^{eq}(\phi_{out})=\mu_{i}^{eq} where the index :math:`i` is for "interface". The pressure difference is given by the Laplace's law: .. math:: :label: Equilib_p_Curved p_{in}(\phi_{in})-p_{out}(\phi_{out})=\sigma\kappa With its definition: With its def (Eq. ([eq:Def_p-c_local])), Eq. ([eq:Equilib_p_Curved]) writes .. math:: :label: \phi_{in}\mu_{in}^{eq}-f(\phi_{in})-\phi_{out}\mu_{out}^{eq}+f(\phi_{out})=\sigma\kappa Using common tangent construction Eq. :eq:`Mu-Common-Tangent` for :math:`f_{dw}(\phi_{out})-f_{dw}(\phi_{in})`: .. math:: :label: \mu_{i}^{eq}(\phi_{in}-\phi_{out})+\mu^{eq}(\phi_{out}-\phi_{in})=\sigma\kappa and finally: .. math:: :label: \boxed{\mu_{i}^{eq}=\mu^{eq}+\frac{\sigma\kappa}{(\phi_{out}-\phi_{in})}} This is the Gibbs-Thomson condition which means that the equilibrium chemical potential of a curved interface is equal to the equilibrium chemical potential for a flat interface corrected by the curvature and the surface tension. Ostwald ripening ---------------- Consequence of Gibbs-Thomson condition with :math:`\boldsymbol{j}_{CH}`: Ostwald ripening """"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""" .. admonition:: Ostwald ripening The Gibbs-Thomson condition writes: .. math:: :label: Gibbs-Thomson_jCH \mu_{i}=\mu^{eq}+\frac{1}{(\phi_{out}-\phi_{in})}\frac{2\sigma}{R} If we consider two droplets of radius :math:`R_{1}` and :math:`R_{2}` with :math:`R_{1}