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A rigorous derivation of mean-field models for diblock copolymer melts

机译:对二嵌段共聚物熔体的均值场模型的严格推导

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We study the free boundary problem describing the micro phase separation of diblock copolymer melts in the regime that one component has small volume fraction such that micro phase separation results in an ensemble of small balls of one component. Mean-field models for the evolution of a large ensemble of such spheres have been formally derived in Glasner and Choksi (Physica D, 238:1241-1255, 2009), Helmers et al. (Netw Heterog Media, 3(3):615-632, 2008). It turns out that on a time scale of the order of the average volume of the spheres, the evolution is dominated by coarsening and subsequent stabilization of the radii of the spheres, whereas migration becomes only relevant on a larger time scale. Starting from the free boundary problem restricted to balls we rigorously derive the mean-field equations in the early time regime. Our analysis is based on passing to the homogenization limit in the variational framework of a gradient flow.
机译:我们研究了自由边界问题,该问题描述了一种嵌段共聚物熔体的微相分离,该体系中一种组分的体积分数较小,以致微相分离导致一种组分的小球团聚。 Helmers等人在Glasner和Choksi(Physica D,238:1241-1255,2009)中正式推导了此类球体大集合演化的平均场模型。 (Netw Heterog Media,3(3):615-632,2008)。结果表明,在球体平均体积量级的时间尺度上,演化主要由球半径的粗化和随后的稳定所决定,而迁移仅在较大的时间尺度上才有意义。从限于球的自由边界问题开始,我们严格地推导了早期状态下的均场方程。我们的分析是基于在梯度流变分框架中达到均质化极限。

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