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Molecular dynamics simulation of the contact angle of liquids on solid surfaces

机译:液体在固体表面接触角的分子动力学模拟

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Solid-liquid-vapor interaction phenomena have an important role in phase change heat transfer. In 2005, Sinha1 carried out simulation of contact angle using argon and a virtual solid wall. He modeled the solid-liquid interaction by a (9,3) potential and assumed that the solid surface is semi-infinite,nnwhere R0 is the lattice constant of a fcc(111) solid surface, z is the distance from wall, and ϵsf and σsf are Lennard-Jones parameters, respectively. In that study, it was found that the contact angle decreased with increasing temperature and no matter how the potential was changed, the trend was the same. Earlier in 2002, Maruyama et al.2 also simulated the contact angle of argon liquid on a virtual solid wall. They calculated various contact angles by changing the parameter ϵ in the potential between argon fluid and the virtual solid wall. They found that the contact angle decreased with an increase in interface potential and became 0° when the potential was set to a large enough value.nResults of limited molecular dynamics simulation studies have been reported in literature on the contact angle of water and a realistic solid wall. In 2003, Kimura and Maruyama3 first simulated a water droplet on a platinum surface. They used two different potentials between water and platinum. By using Spohr–Heinzinger4 potential, they found that the contact angle is always 0°, which suggests that this potential is not suitable to predict the contact angle. By using Zhu–Philpott5 potential, they successfully calculated the contact angle variation with the orientation of the crystal structure of a platinum wall at a temperature of 350 K.nIn this paper, the particle-particle particle-mesh (PPPM) method6 is applied to minimize the error in long range terms in both the Coulombic and Lennard-Jones potentials. Higher accuracy simulation is performed to obtain the contact angle variation with temperature and wall potential.
机译:固液汽相互作用现象在相变传热中具有重要作用。 2005年,Sinha1使用氩气和虚拟实心壁进行了接触角的模拟。他用(9,3)电势对固液相互作用进行建模,并假设固体表面是半无限大的,其中R0是fcc(111)固体表面的晶格常数,z是与壁的距离,distancesf和σsf分别是Lennard-Jones参数。在该研究中,发现接触角随温度升高而减小,并且无论电位如何变化,其趋势都是相同的。在2002年初,Maruyama等人2还模拟了氩气在虚拟固体壁上的接触角。他们通过改变氩气和虚拟固体壁之间的电势参数calculated来计算各种接触角。他们发现接触角随着界面电位的增加而减小,并且当电位设置为足够大的值时变为0°。n关于水和实际固体的接触角的文献报道了有限的分子动力学模拟研究的结果。壁。 2003年,Kimura和Maruyama3首先在铂金表面上模拟了水滴。他们在水和铂之间使用了两种不同的电势。通过使用Spohr–Heinzinger4电势,他们发现接触角始终为0°,这表明该电势不适合预测接触角。利用Zhu–Philpott5电势,他们成功地计算了在350 K温度下接触角随铂壁晶体结构取向的变化。n本文将粒子-粒子-粒子网(PPPM)方法6用于最大限度地减小库伦比势和Lennard-Jones势的长期误差。执行更高精度的仿真以获得接触角随温度和壁电势的变化。

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  • 来源
    《J. Chem. Phys》 |2009年第3期|p.1-5|共5页
  • 作者

    Bo Shi and Vijay K. Dhir;

  • 作者单位

    Department of Mechanical and Aerospace Engineering, Henry Samueli School of Engineering and Applied Science, University of California, Los Angeles, California 90095, USA (Received 5 August 2008, accepted 3 December 2008, published online 21 January 2009),;

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