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arXiv 1402.2069cond-mat.stat-mech
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具有屏蔽库仑相互作用的二元离子流体的气液相共存和交叉行为:相互作用范围的影响

Gas-liquid phase coexistence and crossover behavior of binary ionic fluids with screened Coulomb interactions: The effect of an interaction range

O. Patsahan

摘要:

我们研究了气-液相图和一个简单的离子流体模型的交叉行为:一个等摩尔的二元混合物的等尺寸的硬球相互作用,通过屏蔽库仑势是排斥粒子之间的相同物种和吸引力的不同物种的粒子。利用我们以前的结果,我们得到了显式表达式的有效$φ^{4}$ Ginzburg-Landau哈密顿量在一个循环近似的相关系数。在这个近似的框架内,我们计算的临界参数和气液共存曲线的无量纲的反屏蔽长度$z$的不同值。由Yukawa势接触值标度的临界温度以及临界堆积分数随着相互作用范围的增加而迅速降低,然后对于$z<0.05$缓慢地接近纯离子模型的值,即,一种受限基元模型(RPM)。这两种趋势与蒙特卡罗模拟的结果定性一致。我们发现气液共存区随着$z$的增加而缩小,在$z\simeq 2.781$处完全消失。这与蒙特卡罗模拟的结果定性地一致,表明$z\leq 4$的稳定的气液共存。它还表明,从一个典型的简单流体的一个典型的离子流体的相互作用范围的增加导致交叉温度的降低。对于$z\simeq 0.01$,交叉温度与RPM相同。对于$z\simeq 2.781$,我们的结果表明了一个三临界点。

英文摘要:

We study the gas-liquid phase diagram and the crossover behavior of a simple model of ionic fluid: an equimolar binary mixture of equisized hard spheres interacting through screened Coulomb potentials which are repulsive between particles of the same species and attractive between particles of different species. Using our previous results, we obtain explicit expressions for the relevant coefficients of the effective $φ^{4}$ Ginzburg-Landau Hamiltonian in a one-loop approximation. Within the framework of this approximation, we calculate the critical parameters and gas-liquid coexistence curves for different values of the dimensionless inverse screening length $z$. The critical temperature scaled by the Yukawa potential contact value as well as the critical packing fraction rapidly decrease with an increase of the interaction range and then for $z<0.05$ slowly approach the values found for a purely ionic model, i.e., a restricted primitive model (RPM). The both trends are qualitatively consistent with the results of Monte Carlo simulations. We find that gas-liquid coexistence region reduces with an increase of $z$ and completely vanishes at $z\simeq 2.781$. This qualitatively agrees with the results of Monte Carlo simulations indicating a stable gas-liquid coexistence for $z\leq 4$. It is also shown that an increase in the interaction range from the one typical of simple fluids to the one typical of ionic fluids leads to a decrease of the crossover temperature. For $z\simeq 0.01$, the crossover temperature is the same as for the RPM. For $z\simeq 2.781$, our results indicate a tricritical point.

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