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Convective instabilities in liquid layers with free upper surface under the action of an inclined temperature gradient

机译:倾斜温度梯度作用下具有自由上表面的液体层的对流不稳定性

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We present the result of an experimental study of convective instabilities in a horizontal liquid layer with free upper surface under the action of an inclined temperature gradient, i.e.. when horizontal and vertical temperature gradients are applied tit the same time. Silicone oil of 10 cSt (Prandtl number Pr = 102) was employed as the test fluid. We investigated the layers with different thicknesses to examine the influence of gravity on the formation of the convective patterns. It is found out that the system appreciably depends on the dynamic Bond number, which shows a relation of buoyancy and thermocapillary forces In the case of small dynamic Bond numbers, when the influence of buoyancy is minimal. four different flow patterns, according to the combination of the vertical and horizontal Marangoni numbers. have been found: steady parallel flow, Benard-Marangoni cells, drifting Benard-Marangoni cells. and longitudinal rolls At larger dynamic Bond number, when the influence of buoyancy becomes considerable, new convective structures, named by us the "Surface longitudinal rolls" and the "Surface drifting cells," appear in addition to the patterns listed above These instabilities exist only in the Surface part of the thermocapillary flow. whereas the return flow remains stable. Under large enough dynamic Bond number these patterns become the dominating ones. forcing out the classical Benard-Marangoni instability. We give a phenomenological description of the obtained convective patterns and present the stability diagram in the plane of the vertical and the horizontal Marangoni numbers (C) 2009 American Institute of Physics.
机译:我们介绍了在倾斜的温度梯度作用下(即同时施加水平和垂直温度梯度时)具有自由上表面的水平液层中对流不稳定性的实验研究结果。将10cSt的硅油(Prandtl数Pr = 102)用作测试流体。我们研究了具有不同厚度的层,以检查重力对流模式形成的影响。发现该系统明显地依赖于动态邦定数,这表明了浮力和热毛细力的关系。在动态邦定数小的情况下,当浮力的影响最小时。根据垂直和水平Marangoni数的组合,有四种不同的流动模式。已经发现:稳定的平行流,Benard-Marangoni细胞,漂移的Benard-Marangoni细胞。在较大的动态Bond数下,当浮力的影响变得很大时,除了上面列出的模式以外,还出现了新的对流结构,我们称其为“表面纵向辊”和“表面漂移单元”。这些不稳定性仅存在在热毛细管流的表面部分。而回流保持稳定。在足够大的动态邦德数下,这些模式成为主导模式。迫使经典的Benard-Marangoni不稳定性。我们对获得的对流模式进行了现象学描述,并在垂直和水平Marangoni数(C)2009美国物理研究所的平面上给出了稳定性图。

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