We study the capillary rise of viscous liquids into sharp corners formed by two surfaces whose geometry is described by power laws hᵢ(x) = cᵢ xⁿ , $i = 1,2$ , where c₂ > c₁ for n ≥ 1 . Prior investigations of capillary rise in sharp corners have shown that the meniscus altitude increases with time as t1/3 , a result that is universal, i.e. applies to all corner geometries. The universality of the phenomenon of capillary rise in sharp corners is revisited in this work through the analysis of a partial differential equation for the evolution of a liquid column rising into power-law-shaped corners, which is derived using lubrication theory. Despite the lack of geometric similarity of the liquid column cross-section for $n>1$ , there exist a scaling and a similarity transformation that are independent of cᵢ and n , which gives rise to the universal t1/3 power law for capillary rise. However, the prefactor, which corresponds to the tip altitude of the self-similar solution, is a function of n , and it is shown to be bounded and monotonically decreasing as n→ ∞ . Accordingly, the profile of the interface radius as a function of altitude is also independent of cᵢ and exhibits slight variations with n . Theoretical results are compared against experimental measurements of the time evolution of the tip altitude and of profiles of the interface radius as a function of altitude.
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Wu et al. (2024) studied this question.
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