论文标题

在非局部Cahn- hilliard方程上,具有非局部动态边界条件和边界惩罚

On the nonlocal Cahn--Hilliard equation with nonlocal dynamic boundary condition and boundary penalization

论文作者

Knopf, Patrik, Signori, Andrea

论文摘要

cahn--hilliard方程是描述二进制混合物中相位分离过程的最常见模型之一。最近,已经引入了各种动态边界条件,以更精确地模型材料与边界的相互作用。为了考虑材料的长期相互作用,我们提出了一个新模型,该模型由非本地cahn--hilliard方程组成,受到非局部动态边界条件的约束,该方程也属于cahn--hilliard类型,并包含额外的边界惩罚项。我们严格地将模型推导为非局部总自由能的梯度流,相对于合适的内部产物$ h^{ - 1} $,其中包含批量和表面贡献。总自由能被认为是非局部性的,因为它包含与某些相互作用内核的散装和相场变量的卷积。主要困难是由于在表面上定义合适的内核以及处理所得的边界卷积而产生的。在主要模型中,根据与化学反应速率相关的特定弛豫参数,散装和表面上的化学电位与罗宾型边界条件结合。我们证明了该系统的弱且强大的体系,并研究了当弛豫参数趋于零或无穷大时达到的奇异极限。通过这种方法,我们还获得了相应极限系统的弱且强大的稳定性。

The Cahn--Hilliard equation is one of the most common models to describe phase segregation processes in binary mixtures. In recent times, various dynamic boundary conditions have been introduced to model interactions of the materials with the boundary more precisely. To take long-range interactions of the materials into account, we propose a new model consisting of a nonlocal Cahn--Hilliard equation subject to a nonlocal dynamic boundary condition that is also of Cahn--Hilliard type and contains an additional boundary penalization term. We rigorously derive our model as the gradient flow of a nonlocal total free energy with respect to a suitable inner product of order $H^{-1}$ which contains both bulk and surface contributions. The total free energy is considered as nonlocal since it comprises convolutions in the bulk and on the surface of the phase-field variables with certain interaction kernels. The main difficulties arise from defining a suitable kernel on the surface and from handling the resulting boundary convolution. In the main model, the chemical potentials in the bulk and on the surface are coupled by a Robin type boundary condition depending on a specific relaxation parameter related to the rate of chemical reactions. We prove weak and strong well-posedness of this system, and we investigate the singular limits attained when the relaxation parameter tends to zero or infinity. By this approach, we also obtain weak and strong well-posedness of the corresponding limit systems.

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