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arXiv 1905.08052physics.flu-dyn
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双流体多尺度非局部模型压力稳态解析解

Analytical steady-state solutions for pressure with a multiscale non-local model for two-fluid systems

Amanda A. Howard, Yongcheng Zhou, Alexandre M. Tartakovsky

摘要:

我们认为表面张力的非局部多尺度模型\citep{Tartakovsky2018}作为替代(宏观)杨拉普拉斯定律。非局部模型的形式得到的支持$\varepsilon$添加到Navier-Stokes动量守恒方程的分子力的功能的积分。利用这个模型,我们计算的稳态平衡压力梯度和压力分布的圆形和球形气泡和平面界面在二维和三维的解析形式。根据解析解,压力在界面上以与MD模拟中观察到的定量相似的方式连续变化。此外,对于大于$3\varepsilon$的曲率半径,压力差$P_{\varepsilon, in} - P_{\varepsilon, out}$满足杨-拉普拉斯定律,否则偏离杨-拉普拉斯定律(即,当曲率半径变为零时,$P_{\varepsilon, in} - P_{\varepsilon, out}$变为零,其中$P_{\varepsilon, out}$是气泡外部距离界面大于$3\varepsilon$的压力,$P_{\varepsilon, in}$是气泡中心处的压力)。后者表明,所提出的模型中的表面张力随曲率半径的减小而减小,这与分子动力学模拟和实验室实验的纳米气泡。因此,我们的研究结果表明,非局部模型的行为微观尺度小于$\varepsilon$和宏观,否则。

英文摘要:

We consider the nonlocal multiscale model for surface tension \citep{Tartakovsky2018} as an alternative to the (macroscale) Young-Laplace law. The nonlocal model is obtained in the form of an integral of a molecular-force-like function with support $\varepsilon$ added to the Navier-Stokes momentum conservation equation. Using this model, we calculate analytical forms for the steady-state equilibrium pressure gradient and pressure profile for circular and spherical bubbles and flat interfaces in two and three dimensions. According to the analytical solutions, the pressure changes continuously across the interface in a way that is quantitatively similar to what is observed in MD simulations. Furthermore, the pressure difference $P_{\varepsilon, in} - P_{\varepsilon, out}$ satisfies the Young-Laplace law for the radius of curvature greater than $3\varepsilon$ and deviates from the Young-Laplace law otherwise (i.e., $P_{\varepsilon, in} - P_{\varepsilon, out}$ goes to zero as the radius of the curvature goes to zero, where $P_{\varepsilon, out}$ is the pressure outside of the bubble at the distance greater than $3\varepsilon$ from the interface and $P_{\varepsilon, in}$ is the pressure at the center of the bubble). The latter indicates that the surface tension in the proposed model decreases with the decreasing radius of curvature, which agrees with molecular dynamics simulations and laboratory experiments with nanobubbles. Therefore, our results demonstrate that the nonlocal model behaves microscopically at scales smaller than $\varepsilon$ and macroscopically, otherwise.

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