双扩散过程中精细结构的形成与破坏

P.F. Linden
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引用次数: 33

摘要

通过在包含两个分量的相反的均匀梯度的区域上施加不稳定浮力通量来形成层状结构进行了检查。Turner (Journal of Fluid Mechanics, 33,183 - 200,1968)研究了稳定盐度梯度从下方加热时地层的形成。目前的工作是他的延伸,允许在流体内部存在不稳定的温度梯度。实验采用两种溶质(糖和盐)作为密度场的组成部分。从理论上发现,并通过实验证实,层的规模取决于内部两个密度梯度的比例Gϱ。观察到,随着距离施加浮力通量的边界的距离增加,这些层依次形成。在第一层形成过程中,由边界通量提供的能量和储存在不稳定分量中的能量的相对贡献取决于Gϱ,而不取决于边界通量的大小。当Gϱ=0,且不存在不稳定密度梯度时,能量全部来自施加的通量。当Gϱ→1时,来自不稳定分量的能量变得更加重要,提供了极限内的全部能量。报道了一些精细结构破坏的观察结果。观察到两种。一种类型的特点是界面垂直迁移到相邻的界面,从而破坏了中间的层。另一种是通过原位界面的破裂来确定的,这显然是由于两侧两层的密度均匀造成的。最后与海洋精细结构作了简要比较。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
The formation and destruction of fine-structure by double-diffusive processes

The formation of layered structure by the imposition of an unstable buoyancy flux on a region containing opposing, uniform gradients of two components is examined. Turner (Journal of Fluid Mechanics, 33, 183–200, 1968) investigated the formation of layers when a stable salinity gradient is heated from below. The present work is an extension of his, allowing for the presence of a destabilizing temperature gradient in the interior of the fluid. Experiments were carried out using two solutes (sugar and salt) as the components contributing to the density field. It is found theoretically, and confirmed by experiment, that the scale of the layers depends on the ratio of the two density gradients in the interior Gϱ. The layers were observed to form sequentially with increasing distance from the boundary across which the buoyancy flux was applied. The relative contributions of the energy provided by the boundary flux and that stored in the destabilizing component during the formation of the first layer are found to depend on Gϱ but not on the magnitude of the boundary flux. When =0, and there is no destabilizing density gradient, all the energy comes from the imposed flux. As →1, the energy from the destabilizing component becomes more important, providing all the energy in the limit. Some observations of destruction of fine-structure are reported. Two kinds were observed. One type was characterized by the vertical migration of an interface to an adjacent one thereby destroying the layer in between. The other kind was identified by a breakdown of an interface in situ, apparently resulting from an equalization of the density of the two layers on either side. Finally some brief comparisons with oceanic fine-structure are made.

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