Model of Boundary Conditions on Metal Surfaces for Rarefied Gas

E. Prozorova
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Abstract

Currently, the classical theory discusses issues related to the sliding of liquid and gas along a wall at low external flow velocities. These questions become especially relevant when the surface size is reduced to the nanoscale. The article discusses the formation of sliding conditions and an adsorption layer for an ideal crystalline surface. For gas, the Knudsen layer is proposed to be divided into two parts: an adjacent layer with a thickness of several molecular interaction radii, in which molecules do not collide with each other, and a layer in which the Chapman-Enskog method is defined. The solution for this layer can be found by the small parameter method. For water, there is no Knudsen layer, but adhesion and the formation of a thin stationary layer are possible. Various possible causes of slipping are discussed. The formation of a dislocation from a point defect near the surface, which is a vacancy, is considered. An analysis of the causes of pore clogging during water movement near the surface was carried out. The emphasis is on the change in stress in the metal, taking into account the influence of the moment that occurs when the position of the molecules changes.
稀薄气体金属表面边界条件模型
目前,经典理论讨论的是液体和气体在低外部流速下沿壁滑动的相关问题。当表面尺寸缩小到纳米级时,这些问题变得尤为重要。文章讨论了理想结晶表面的滑动条件和吸附层的形成。对于气体,建议将 Knudsen 层分为两部分:厚度为几个分子相互作用半径的相邻层(其中分子不会相互碰撞)和 Chapman-Enskog 方法定义的层。这一层的解可以用小参数法求得。对于水来说,不存在克努森层,但有可能发生粘附并形成薄的静止层。讨论了滑动的各种可能原因。考虑了由表面附近的点缺陷(即空位)形成的位错。分析了表面附近水运动过程中孔隙堵塞的原因。重点是金属中应力的变化,同时考虑到分子位置变化时产生的力矩的影响。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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