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首页> 外文期刊>Proceedings of the Royal Society. Mathematical, physical and engineering sciences >Quasi-incompressible Cahn-Hilliard fluids and topological transitions
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Quasi-incompressible Cahn-Hilliard fluids and topological transitions

机译:拟不可压缩的Cahn-Hilliard流体和拓扑转换

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One of the fundamental problems in simulating the motion of sharp interfaces between immiscible fluids is a description of the transition that occurs when the interfaces merge and reconnect. It is well known that classical methods involving sharp interfaces fail to describe this type of phenomena. Following some previous work in this area, we suggest a physically motivated regularization of the Euler equations which allows topological transitions to occur smoothly. In this model, the sharp interface is replaced by a narrow transition layer across which the fluids may mix. The model describes a flow of a binary mixture, and the internal structure of the interface is determined by both diffusion and motion. An advantage of our regularization is that it automatically yields a continuous description of surface tension, which can play an important role in topological transitions. An additional scalar held is introduced to describe the concentration of one of the fluid components and the resulting system of equations couples the Euler (or Navier-Stokes) and the Cahn-Hilliard equations. The model takes into account weak non-locality (dispersion) associated with an internal length scale and localized dissipation due to mixing. The non-locality introduces a dimensional surface energy; dissipation is added to handle the loss of regularity of solutions to the sharp interface equations and to provide a mechanism for topological changes. In particular, we study a nontrivial limit when both components are incompressible, the pressure is kinematic but the velocity field is non-solenoidal (quasi-incompressibility). To demonstrate the effects of quasi-incompressibility, we analyse the linear stage of spinodal decomposition in one dimension. We show that when the densities of the fluids are not perfectly matched, the evolution of the concentration field causes fluid motion even if the fluids are inviscid. In the limit of infinitely thin and well-separated interfacial layers, an appropriately scaled quasi-incompressible Euler-Cahn-Hilliard system converges to the classical sharp interface model. In order to investigate the behaviour of the model outside the range of parameters where the sharp interface approximation is sufficient, we consider a simple example of a change of topology and show that the model permits the transition to occur without an associated singularity. [References: 63]
机译:模拟不混溶流体之间尖锐界面运动的基本问题之一是描述界面合并和重新连接时发生的过渡。众所周知,涉及尖锐界面的经典方法无法描述这种现象。在此领域中的一些先前工作之后,我们建议对Euler方程进行物理上的正则化,以使拓扑转换能够平稳进行。在此模型中,尖锐的界面被狭窄的过渡层代替,流体可以在过渡层上混合。该模型描述了二元混合物的流动,界面的内部结构由扩散和运动决定。我们进行正则化的一个优点是,它可以自动产生对表面张力的连续描述,这可以在拓扑转换中发挥重要作用。引入了一个附加的标量来描述一种流体成分的浓度,并且所得方程组将Euler(或Navier-Stokes)方程和Cahn-Hilliard方程耦合在一起。该模型考虑了与内部长度尺度相关的弱非局部性(分散性)和由于混合引起的局部性耗散。非局部性引入了维数表面能;增加了耗散以处理尖锐接口方程解的规则性损失,并提供了拓扑更改的机制。特别地,当两个分量都是不可压缩的,压力是运动学的,但是速度场是非电磁的(准不可压缩性)时,我们研究一个非平凡的极限。为了证明准不可压缩性的影响,我们在一个维度上分析了旋节线分解的线性阶段。我们表明,当流体的密度不完全匹配时,即使流体不粘稠,浓度场的演化也会引起流体运动。在无限薄且分离良好的界面层的限制下,适当缩放的准不可压缩的Euler-Cahn-Hilliard系统收敛于经典的锐利界面模型。为了研究参数的范围(其中尖锐的界面近似值已足够)的模型行为,我们考虑了拓扑变化的简单示例,并显示了该模型允许在没有相关奇点的情况下进行过渡。 [参考:63]

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