DYNAMICS OF PARTIAL WETTING

DYNAMICS OF PARTIAL WETTING
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DOI:
10.1016/0001-8686(92)80052-y
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发表时间:
1992-04-06
影响因子:
15.6
通讯作者:
DEGENNES, PG
DEGENNES, PG
中科院分区:
化学1区
文献类型:
--
作者:
BROCHARDWYART, F;DEGENNES, PG

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当接触角θ偏离平衡值θ(e)时,两大类模型已被用于描述接触线的运动:a)Eyring方法,强调尖端处单个分子的微观跳跃。B)流体动力学方法,集中于角θ的液体楔内的粘性损失。在本综述中,我们比较了两个模型的预测,为两个关键的实验:1)从静止的流体中拉出垂直板-显示(对于有限的θ(e))临界速度V(c),在该速度以上的板是完全润湿的。2)在小θ(e)下,由平坦液膜覆盖的非光滑表面的干斑的生长速度,其变化类似于θ(e)3。净结论是,在小θ(e)和低速度V下,流体动力学损失占主导地位,而在大θ(e)和大V下,分子特征可能是重要的。
Two broad classes of models have been used to describe the motion of a contact line when the contact angle-theta deviates from the equilibrium value-theta(e): a) an Eyring approach, emphasizing the microscopic jump of a single molecule at the tip. b) a hydrodynamic approach, concentrating on the viscous losses inside the liquid wedge of angle-theta. In the present review, we compare the predictions from both models, for two critical experiments :1) The pull out of a vertical plate from a fluid at rest -showing (for finite-theta(e)) a critical velocity V(c) above which the plate is completely wet.2) The velocity of growth of a dry patch for a non wettable surface covered by a flat liquid film which turns out to vary like theta(e)3 at small-theta(e).The net conclusion is that, at small-theta(e) and for low velocities V, the hydrodynamic losses dominate, while at large-theta(e) and large V, the molecular features are probably important.