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Local linear viscoelasticity of confined fluids

机译:密闭流体的局部线性粘弹性

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In this paper the authors propose a novel method to study the local linear viscoelasticity of fluids confined between two walls. The method is based on the linear constitutive equation and provides details about the real and imaginary parts of the local complex viscosity. They apply the method to a simple atomic fluid undergoing zero mean oscillatory flow using nonequilibrium molecular dynamics simulations. The method shows that the viscoelastic properties of the fluid exhibit dramatic spatial changes near the wall-fluid boundary due to the high density in this region. It is also shown that the real part of the viscosity converges to the frequency dependent local shear viscosity sufficiently far away from the wall. This also provides valuable information about the transport properties in the fluid, in general. The viscosity is compared with predictions from the local average density model. The two methods disagree in that the local average density model predicts larger viscosity variations near the wall-fluid boundary than what is observed through the method presented here. (c) 2007 American Institute of Physics.
机译:在本文中,作者提出了一种新颖的方法来研究封闭在两壁之间的流体的局部线性粘弹性。该方法基于线性本构方程,并提供有关局部复数粘度的实部和虚部的详细信息。他们使用非平衡分子动力学模拟将该方法应用于经历零平均振荡流的简单原子流体。该方法表明,由于该区域的高密度,流体的粘弹性质在壁-流体边界附近显示出剧烈的空间变化。还表明,粘度的实部收敛到足够远离壁的频率相关的局部剪切粘度。通常,这也提供有关流体中传输特性的有价值的信息。将粘度与局部平均密度模型的预测值进行比较。两种方法的不同之处在于,与通过此处介绍的方法观察到的结果相比,局部平均密度模型预测壁流体边界附近的粘度变化更大。 (c)2007年美国物理研究所。

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