\begin{document}$ 5^{\circ} $\end{document} and \begin{document}$ 75^{\circ}$\end{document}, the following conclusions are obtained. When colliding with the wall at an angle close to vertical, both components of the momentum of the gas molecules are lost. The normal energy transfers to the tangential direction, and when the molecular velocity is not less than 2.0, the transfer rate is not significantly affected by the incident energy of the molecule and the surface roughness. The total energy loss of gas molecules after scattering becomes significant with the increase of incident velocity, and it is not sensitive to changes of surface roughness. When the gas molecules are incident at \begin{document}$ 75^{\circ} $\end{document}, the roughness of the surface has a significant impact on the conversion mechanism of molecular momentum and energy. After colliding with a smooth wall, the momentum and energy values of the gas molecules remain basically unchanged, only the direction of the momentum is reversed. The motion state of molecules is close to the mirror reflection, and the conversion between momentum and energy components is not obvious. The introduction of roughness enhances the degree of accommodation between gas molecules and metal surface, and promotes the transfer of molecular tangential momentum and kinetic energy to the normal direction. When incident at a large polar angle, as opposed to the small-angle cases, the total energy loss of molecules is not sensitive to changes of incident velocity, it goes up significantly with the surface roughness increasing. The research in this article not only explores the gas-surface interaction mechanism, but also provides a useful reference for the high-fidelity simulation of rare gas flow and the development of appropriate gas-surface interaction models."> - 必威体育下载

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Citation:

    Yu Hang, Zhang Ran, Yang Fan, Li Hua
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    • Abstract views:4960
    • PDF Downloads:84
    • Cited By:0
    Publishing process
    • Received Date:24 July 2020
    • Accepted Date:31 August 2020
    • Available Online:13 January 2021
    • Published Online:20 January 2021

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