论文标题
稳定和不稳定的步骤分层扰动后湍流的扩散
Diffusion of turbulence following both stable and unstable step stratification perturbations
论文作者
论文摘要
在正常温度失去率的稳定和不稳定的扰动的情况下,已经研究了两相,空气和不饱和水蒸气,时间衰减,无剪切,湍流层的演变。在没有水滴的情况下,温暖的蒸气云与透明空气之间的顶界面被认为是参考动力学。直接的3D数值模拟在6m x 6m宽和12m的高云部分内进行,该部分位于温暖的云和透明空气之间的界面附近。泰勒微型雷诺的数字在云部分内为250。平方弗洛德的数字在[0.4的间隔内变化; 1038.5]和[-4.2; -20.8]。观察到足够强烈的分层可以改变混合动力学。观察到无剪切层内的子层的形成。在稳定的热分层条件下,子层的表现就像动能的坑。另一方面,观察到动能瞬态生长发生在不稳定的条件下,从而导致在无剪切层中心下方的能量峰形成。量化了界面区域内能量时间变化的缩放定律:这是一个代数定律,其指数取决于扰动分层强度。与未分层的情况相比,纵向速度衍生物的统计行为差异增加了不稳定的分层的存在。由于在稳定的情况下抑制了混合过程,因此小尺度各向异性也会被抑制。
The evolution of a two-phase, air and unsaturated water vapor, time decaying, shearless, turbulent layer has been studied in the presence of both stable and unstable perturbations of the normal temperature lapse rate. The top interface between a warm vapor cloud and clear air in the absence of water droplets was considered as the reference dynamics. Direct, 3D numerical simulations were performed within a 6m x 6m wide and 12m high cloud portion, which was hypothesized to be located close to an interface between the warm cloud and clear air. The Taylor micro-scale Reynolds' number was 250 inside the cloud portion. The squared Froude's number varied over intervals of [0.4; 1038.5] and [-4.2; -20.8]. A sufficiently intense stratification was observed to change the mixing dynamics. The formation of a sub-layer inside the shearless layer was observed. The sub-layer, under a stable thermal stratification condition, behaved like a pit of kinetic energy. On the other hand, it was observed that kinetic energy transient growth took place under unstable conditions, which led to the formation of an energy peak just below the center of the shearless layer. The scaling law of the energy time variation inside the interface region was quantified: this is an algebraic law with an exponent that depends on the perturbation stratification intensity. The presence of an unstable stratification increased the differences in statistical behavior among the longitudinal velocity derivatives, compared with the unstratified case. Since the mixing process is suppressed in stable cases, small-scale anisotropy is also supressed.