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Nonequilibrium fluctuations in the Rayleigh-Benard problem for binary fluid mixtures

机译:二元流体混合物的Rayleigh-Benard问题中的非平衡波动

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We have employed a simple Galerkin-approximation scheme to calculate nonequilibrium temperature and concentration fluctuations in a binary fluid subjected to a temperature gradient with realistic boundary conditions. When a fluid mixture is driven outside thermal equilibrium, there are two instability mechanisms, namely a Rayleigh (stationary) and a Hopf (oscillatory) instability, causing long-ranged fluctuations. The competition of these two mechanisms causes the structure factor associated with the temperature fluctuations to exhibit two maxima as a function of the wave number q of the fluctuations, in particular, close to the convective instability. In the presence of thermally conducting but impermeable walls the intensity of the temperature fluctuations vanishes as q goes to zero, while the intensity of the concentration fluctuations remains finite in the limit of vanishing q. Finally, we propose a simpler small-Lewis-number approximation scheme, which is useful to represent nonequilibrium concentration fluctuations for mixtures with positive separation ratio, even close to (but below) the convective instability.
机译:我们采用了一种简单的Galerkin逼近方案来计算二元流体在具有实际边界条件的温度梯度下的非平衡温度和浓度波动。当将流体混合物驱使到热平衡之外时,存在两种不稳定性机制,即瑞利(平稳)和霍普夫(振荡)不稳定性,从而导致长期波动。这两种机制的竞争使得与温度波动相关的结构因子呈现出两个最大值,这是波动的波数q的函数,特别是接近对流不稳定性。在存在导热但不可渗透的壁的情况下,温度波动的强度随着q变为零而消失,而浓度波动的强度在q消失的范围内保持有限。最后,我们提出了一种更简单的小刘易斯数逼近方案,该方案可用于代表具有正分离比(甚至接近(但低于)对流不稳定性)的混合物的非平衡浓度波动。

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