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A theoretical study of structure and thermodynamics of fluids with long-range competing interactions exhibiting pattern formation

机译:具有长距离竞争相互作用并表现出模式形成的流体的结构和热力学的理论研究

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We study the structure and phase behavior of a model fluid with competing short-range attraction and long-range repulsion, constituted by hard spheres interacting by means of two opposite Kac potentials. We use, to this purpose, a thermodynamically self-consistent integral equation approach developed by one of the authors [J.-M. Bomont and J.-L. Bretonnet, J. Chem. Phys. 119, 2188 (2003)]10.1063/1.1583675, which proven accurate in predicting the properties of other competing fluids. We choose the potential parameters in such a way that, upon appropriate thermodynamic conditions, the fluid displays microphase separation terminating, at sufficiently low temperatures, with a phase transition into an ordered-pattern fluid. The propensity toward the pattern formation is indicated by long-wavelength, slowly decaying oscillations in the pair correlation function, and by the presence of a sharp peak in the structure factor S(q) at a small but finite wavevector q c. The limits of stability of the micro-separated phase are identified by a drastic, diverging-like, increase of S(q c) as the temperature drops. The behavior of S(q) in the disordered-pattern phase suggests that different morphologies of the ordered patterns should be expected, depending on the ratio between the strengths of competing interactions. The structural predictions are confirmed, at the thermodynamic level, by the change of sign observed in the "residual multi-particle entropy", according to the one-phase ordering criterion developed by Giaquinta and Giunta [Physica A 187, 145 (1992)]10.1016/0378-4371(92)90415-M, and by the trend shown by the chemical potential. Our self-consistent approach succeeds in describing the thermodynamic regime where the phase transition occurs, whereas, as reported in the literature, other sophisticated schemes within the same theoretical framework generally fail; reasons of this outcome and putative remedies are discussed.
机译:我们研究了具有竞争性的短程吸引和长程排斥的模型流体的结构和相行为,后者由硬质球体通过两个相对的Kac电位相互作用而构成。为此,我们使用由一位作者开发的热力学自洽积分方程方法[J.博蒙特和J.-L. Bretonnet,J.Chem。物理119,2188(2003)] 10.1063 / 1.1583675,事实证明它在预测其他竞争性流体的性质方面是准确的。我们选择潜在参数的方式是,在适当的热力学条件下,流体显示出微相分离,在足够低的温度下终止,并发生相转变为有序模式的流体。通过长波长,对相关函数中的缓慢衰减的振荡以及在小的但有限的波矢q c处的结构因子S(q)中存在一个尖锐的峰,表明了对图形形成的倾向。当温度下降时,S(q c)急剧增加,呈发散状,增加了微分离相稳定性的极限。 S(q)在无序模式阶段的行为表明,应根据竞争性相互作用的强度之比来预期有序模式的不同形态。根据Giaquinta和Giunta提出的单相有序标准,在热力学水平上,通过在“残留多粒子熵”中观察到的符号变化,可以确认结构预测[Physica A 187,145(1992)]。 10.1016 / 0378-4371(92)90415-M,并通过化学势显示趋势。我们的自洽方法成功地描述了发生相变的热力学状态,而正如文献所报道的那样,同一理论框架内的其他复杂方案通常会失败;讨论了这种结果的原因和可能的补救措施。

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