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Self-similarity and scaling transitions during rupture of thin free films of Newtonian fluids

机译:牛顿流体自由薄膜破裂过程中的自相似和水垢转变

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摘要

Rupture of thin liquid films is crucial in many industrial applications and nature such as foam stability in oil-gas separation units, coating flows, polymer processing, and tear films in the eye. In some of these situations, a liquid film may have two free surfaces (referred to here as a free film or a sheet) as opposed to a film deposited on a solid substrate that has one free surface. The rupture of such a free film or a sheet of a Newtonian fluid is analyzed under the competing influences of inertia, viscous stress, van derWaals pressure, and capillary pressure by solving a system of spatially one-dimensional evolution equations for film thickness and lateral velocity. The dynamics close to the space-time singularity where the film ruptures is asymptotically self-similar and, therefore, the problem is also analyzed by reducing the transient partial differential evolution equations to a corresponding set of ordinary differential equations in similarity space. For sheets with negligible inertia, it is shown that the dominant balance of forces involves solely viscous and van der Waals forces, with capillary force remaining negligible throughout the thinning process in a viscous regime. On the other hand, for a sheet of an inviscid fluid for which the effect of viscosity is negligible, it is shown that the dominant balance of forces is between inertial, capillary, and van der Waals forces as the film evolves towards rupture in an inertial regime. Real fluids, however, have finite viscosity. Hence, for real fluids, it is further shown that the viscous and the inertial regimes are only transitory and can only describe the initial thinning dynamics of highly viscous and slightly viscous sheets, respectively. Moreover, regardless of the fluid's viscosity, it is shown that for sheets that initially thin in either of these two regimes, their dynamics transition to a late stage or final inertial-viscous regime in which inertial, viscous, and van derWaals forces balance each other while capillary force remains negligible, in accordance with the results of Vaynblat, Lister, and Witelski. Published by AIP Publishing.
机译:薄液膜的破裂对于许多工业应用和自然界至关重要,例如油气分离单元中的泡沫稳定性,涂层流动,聚合物加工以及眼中的泪膜。在这些情况中的某些情况下,与沉积在具有一个自由表面的固体基材上的膜相反,液体膜可具有两个自由表面(在此称为自由膜或片)。通过求解膜厚和侧向速度的空间一维演化方程组,在惯性,粘性应力,范德华压力和毛细管压力的竞争影响下分析了这种自由膜或牛顿流体的破裂。 。接近膜破裂时空奇点的动力学是渐近自相似的,因此,还可以通过将瞬态偏微分演化方程简化为相似空间中相应的一组常微分方程组来分析该问题。对于具有可忽略的惯性的片材,表明力的主要平衡仅涉及粘性力和范德华力,而在粘性状态下,在整个变薄过程中,毛细管力仍然可以忽略不计。另一方面,对于一片粘性流体可以忽略不计的无粘性流体,结果表明,当薄膜在惯性中朝破裂方向发展时,力的主要平衡在惯性力,毛细管力和范德华力之间政权。但是,实际流体具有有限的粘度。因此,对于真实流体,进一步表明粘性和惯性态只是暂时的,只能分别描述高粘性和轻微粘性薄板的初始稀化动力学。此外,无论流体的粘度如何,都表明,对于在这两种情况下最初变薄的薄板,其动力学都会过渡到后期或最终的惯性粘稠状态,在此状态下惯性,粘性和范德华力相互平衡根据Vaynblat,Lister和Witelski的结果,毛细作用力仍然可以忽略不计。由AIP Publishing发布。

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