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arXiv 0704.0544cond-mat.softcond-mat.stat-mech
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库仑作用下流体的交叉行为

Crossover behavior in fluids with Coulomb interactions

O. V. Patsahan, J. -M. Caillol, I. M. Mryglod

摘要:

根据大量的实验发现,离子流体的金斯堡温度$t_{G}$与非离子流体的金斯堡温度显著不同[Schröer W.,魏格特纳河2004 { \it Pure Appl. Chem.} { \bf 76} 19]。在这里提出了一个理论研究的结果是由平均场分析的相互作用的短期和长期的价值$t_{G}$。我们考虑一个相当普遍的连续电荷不对称模型,由带电硬球与额外的短程相互作用(没有静电相互作用的模型属于相同的普适性类的三维伊辛模型)。导出了整个体系在气液临界点附近的有效Landau-Ginzburg哈密顿量,并由此计算了Ginzburg温度随离子性的变化。以这种方式获得的结果为$t_{G}$是在良好的定性和足够的定量协议与现有的实验数据。

英文摘要:

According to extensive experimental findings, the Ginzburg temperature $t_{G}$ for ionic fluids differs substantially from that of nonionic fluids [Schröer W., Weigärtner H. 2004 {\it Pure Appl. Chem.} {\bf 76} 19]. A theoretical investigation of this outcome is proposed here by a mean field analysis of the interplay of short and long range interactions on the value of $t_{G}$. We consider a quite general continuous charge-asymmetric model made of charged hard spheres with additional short-range interactions (without electrostatic interactions the model belongs to the same universality class as the 3D Ising model). The effective Landau-Ginzburg Hamiltonian of the full system near its gas-liquid critical point is derived from which the Ginzburg temperature is calculated as a function of the ionicity. The results obtained in this way for $t_{G}$ are in good qualitative and sufficient quantitative agreement with available experimental data.

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