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Casimir amplitudes and capillary condensation of near-critical fluids between parallel plates: Renormalized local functional theory

机译:卡西米尔振幅和近临界流体的毛细凝聚   平行板之间:重整化局部泛函理论

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摘要

We investigate the critical behavior of a near-critical fluid confinedbetween two parallel plates in contact with a reservoir by calculating theorder parameter profile and the Casimir amplitudes (for the force density andfor the grand potential). Our results are applicable to one-component fluidsand binary mixtures. We assume that the walls absorb one of the fluidcomponents selectively for binary mixtures. We propose a renormalized localfunctional theory accounting for the fluctuation effects. Analysis is performedin the plane of the temperature T and the order parameter in the reservoir\psi_{\infty} . Our theory is universal if the physical quantities are scaledappropriately. If the component favored by the walls is slightly poor in thereservoir, there appears a line of first-order phase transition of capillarycondensation outside the bulk coexistence curve. The excess adsorp- tionchanges discontinuously between condensed and noncondensed states at thetransition. With increasing T, the transition line ends at a capillary criticalpoint T = T_c^{ca} slightly lower than the bulk critical temperature T_c. TheCasimir amplitudes are larger than their critical-point values by 10-100 timesbetween the transition line and the bulk coexistence curve and slightly abovethe capillary critical point.
机译:我们通过计算阶次参数曲线和卡西米尔振幅(对于力密度和大势能)来研究封闭在与储层接触的两个平行板之间的近临界流体的临界行为。我们的结果适用于单组分流体和二元混合物。我们假设壁对二元混合物有选择地吸收一种流体成分。我们提出了一个重新归一化的局部函数理论来说明波动的影响。在温度T的平面和储层\ psi _ {\ infty}中的阶数参数中进行分析。如果物理量适当地缩放,我们的理论是通用的。如果壁所偏爱的成分在储层中略微较差,则在整体共存曲线外会出现一串毛细管冷凝的一级相变线。过渡时,过剩的吸附在凝聚态和非凝聚态之间不连续地变化。随着T的增加,过渡线的终点为毛细管临界点T = T_c ^ {ca},略低于整体临界温度T_c。在过渡线和本体共存曲线之间,Casimir振幅比其临界点值大10-100倍,在毛细管临界点稍高一点。

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