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Departure from Navier-Stokes hydrodynamics in confined liquids

机译:在密闭液体中偏离 Navier-Stokes 流体动力学

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摘要

In this work we use nonequilibrium molecular dynamics (NEMD) to simulate an atomic liquid undergoing gravity-fed flow down a narrow channel. We compare the simulation results against the predictions of classical Navier-Stokes theory for two different channel widths. For a channel width of 5.1 molecular diameters, we find that the velocity profile deviates significantly from the hydrodynamic prediction. The shape of this velocity profile is found to be independent of the applied field (pressure gradient). We find that the heat flux profile does not agree with the cubic profile predicted, by Navier-Stokes hydrodynamics, but shows significant oscillations located about one molecular diameter from the walls. This result differs from the earlier work of Todd and Evans B. D. Todd and D. J. Evans, J. Chem. Phys. 103, 9804 (1995), in which an assumption of a purely quadratic velocity profile resulted in very weak oscillations in the heat flux. We fmd that in narrow channels the viscosity cannot be described by a linear, local constitutive relation. However, classical Navier-Stokes behavior is approached for a channel width of >similar to 10 molecular diameters.
机译:在这项工作中,我们使用非平衡分子动力学(NEMD)来模拟在狭窄通道下经历重力馈送流动的原子液体。我们将仿真结果与经典Navier-Stokes理论对两种不同通道宽度的预测进行了比较。对于分子直径为5.1的通道宽度,我们发现速度分布与流体动力学预测有显著偏差。发现该速度曲线的形状与施加的磁场(压力梯度)无关。我们发现热通量分布与Navier-Stokes流体动力学预测的立方分布不一致,但显示出距离壁约一个分子直径的显着振荡。这一结果与Todd和Evans的早期工作[B. D. Todd and D. J. Evans, J. Chem. Phys. 103, 9804 (1995)]不同,后者假设纯二次速度分布导致热通量振荡非常微弱。我们认为,在狭窄的通道中,粘度不能用线性的局部本构关系来描述。然而,经典的 Navier-Stokes 行为接近通道宽度>类似于 10 个分子直径。

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