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Approximate expression of Young's equation and molecular dynamics simulation for its applicability 被引量:1
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作者 Shu-Wen Cui Jiu-An Wei +2 位作者 Wei-Wei Liu Ru-Zeng Zhu Qian Ping 《Chinese Physics B》 SCIE EI CAS CSCD 2019年第1期527-531,共5页
In 1805, Thomas Young was the first to propose an equation(Young's equation) to predict the value of the equilibrium contact angle of a liquid on a solid. On the basis of our predecessors, we further clarify that ... In 1805, Thomas Young was the first to propose an equation(Young's equation) to predict the value of the equilibrium contact angle of a liquid on a solid. On the basis of our predecessors, we further clarify that the contact angle in Young's equation refers to the super-nano contact angle. Whether the equation is applicable to nanoscale systems remains an open question. Zhu et al. [College Phys. 4 7(1985)] obtained the most simple and convenient approximate formula, known as the Zhu–Qian approximate formula of Young's equation. Here, using molecular dynamics simulation, we test its applicability for nanodrops. Molecular dynamics simulations are performed on argon liquid cylinders placed on a solid surface under a temperature of 90 K, using Lennard–Jones potentials for the interaction between liquid molecules and between a liquid molecule and a solid molecule with the variable coefficient of strength a. Eight values of a between 0.650 and 0.825 are used. By comparison of the super-nano contact angles obtained from molecular dynamics simulation and the Zhu–Qian approximate formula of Young's equation, we find that it is qualitatively applicable for nanoscale systems. 展开更多
关键词 molecular dynamics simulation Young’s EQUATION surface tension Zhu–Qian APPROXIMATE FORMULA of Young’s EQUATION
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Tolman length of simple droplet: Theoretical study and molecular dynamics simulation
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作者 Shu-Wen Cui Jiu-An Wei +3 位作者 Qiang Li Wei-Wei Liu Ping Qian Xiao Song Wang 《Chinese Physics B》 SCIE EI CAS CSCD 2021年第1期443-448,共6页
In 1949, Tolman found the relation between the surface tension and Tolman length, which determines the dimensional effect of the surface tension. Tolman length is the difference between the equimolar surface and the s... In 1949, Tolman found the relation between the surface tension and Tolman length, which determines the dimensional effect of the surface tension. Tolman length is the difference between the equimolar surface and the surface of tension. In recent years, the magnitude, expression, and sign of the Tolman length remain an open question. An incompressible and homogeneous liquid droplet model is proposed and the approximate expression and sign for Tolman length are derived in this paper. We obtain the relation between Tolman length and the radius of the surface of tension(R_(s)) and found that they increase with the Rs decreasing. The Tolman length of plane surface tends to zero. Taking argon for example, molecular dynamics simulation is carried out by using the Lennard–Jones(LJ) potential between atoms at a temperature of 90 K. Five simulated systems are used, with numbers of argon atoms being 10140, 10935, 11760, 13500, and 15360, respectively. By methods of theoretical study and molecular dynamics simulation, we find that the calculated value of Tolman length is more than zero, and it decreases as the size is increased among the whole size range. The value of surface tension increases with the radius of the surface of tension increasing, which is consistent with Tolman’s theory. These conclusions are significant for studying the size dependence of the surface tension. 展开更多
关键词 Tolman length surface tension radius of surface of tension radius of equimolecular surface molecular dynamics simulation
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纳观接触角的确定方法 被引量:1
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作者 崔树稳 朱如曾 +4 位作者 魏久安 王小松 杨洪秀 徐升华 孙祉伟 《物理学报》 SCIE EI CAS CSCD 北大核心 2015年第11期351-359,共9页
对纳观接触角的确定曾有过许多研究工作,本文对各种理论进行分析评论,指出其各自的优缺点甚至错误,认为最为简单实用的理论是朱如曾于1995年在《大学物理》((Vol.14(2)))的文章中对前人的宏观接触角的错误理论采用澄清接触角概念的方法... 对纳观接触角的确定曾有过许多研究工作,本文对各种理论进行分析评论,指出其各自的优缺点甚至错误,认为最为简单实用的理论是朱如曾于1995年在《大学物理》((Vol.14(2)))的文章中对前人的宏观接触角的错误理论采用澄清接触角概念的方法所得到的纳观接触角的近似理论及近似公式α=(1-2EPS/EPL)π(其中EPL和EPS分别表示液体内部一个液体分子的势能和固体表面一个液态分子与固体的相互作用势能,并可用分子动力学(MD)模拟得到),此理论属于纳观接触角的分子动力学理论的近似简化形式,值得进一步发展.为此,本文根据物理分析假设Gibbs张力表面上位于非三相接触区的一个液体分子的势能为EPL/2x,三相接触线上一个液体分子与其余液体的相互作用势能为(1+k EPS/EPL)αEPL/2xπ,其中x和k为优化参数.根据Gibbs分界面上处处势能相等条件,得到改进的纳观接触角的近似公式α=π(1-2x EPS/EPL)/(1+k EPS/EPL).对固体表面的氩纳米液柱,在温度90K下对液体分子之间采用林纳德-琼斯(L-J)势,液体分子与固体原子间采用带有可变强度参数a的L-J势,对0.650<a<0.825范围内的8种a值进行了MD模拟.得到了相应的Gibbs张力面.将其纳观底角视为近似纳观接触角,结合物理条件(当EPS/EPL=0时,α=π)用最小二乘法得到优化参数值x=0.7141,k=1.6051和相关系数0.9997.这一充分接近于1的相关系数表明,对于不同相互作用强度的纳米液固接触系统,优化参数x和k确实可近似视为常数,由此确认我们提出的利用MD模拟来确定纳观接触角近似公式中优化参数的可行性和该近似公式的一般适用性. 展开更多
关键词 纳观接触角 分子动力学模拟 表面张力 实用公式
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