Pyramidal and toroidal water drops after impact on a solid surface

By Yuriko Renardy, Stéphane Popinet, L. Duchemin, Michael Renardy, S. Zaleski, C. Josserand, M. A. Drumright-Clarke, D. Richard, C. Clanet, D. Quéré. Journal of Fluid Mechanics, 2003

201 citations recorded by the source corpus.

Subfields: Computational Mechanics, Surfaces, Coatings and Films

View Paper: https://www.semanticscholar.org/paper/b134f1dd059558c4c58fe8f6d84a9d94cce1c7f4

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In Computational Mechanics

In Surfaces, Coatings and Films

Citations in the corpus

Droplet impact dynamics on micropillared hydrophobic surfaces (2016, background): “[11] t osc , present measurements t b , present measurements t osc , t b , Refs.”
On the elasticity of an inertial liquid shock (2006, background): “Numerical simulations, well-adapted to these slippery states of water where the absence of any contact lines simplifies the approach (Renardy et al. 2003) might be very useful.”
Secondary breakup of a drop at moderate Weber numbers (2015, result): “This behaviour is also in agreement with earlier experimental studies [8,48] (also see [49]).”
Contact angle dynamics in droplets impacting on flat surfaces with different wetting characteristics (2006, methodology): “Renardy et al. (2003) reported that the capillary wave of maximal amplification has a phase speed equal to the droplet impact speed, hence, the corresponding wavelength is Λ = σ/(ρV 2 0 ).”
Numerical studies of the influence of the dynamic contact angle on a droplet impacting on a dry surface (2009, methodology): “Droplet impacts onto dry and flat surfaces have been studied by many researchers from both theoretical and practical aspects [1–19].”
Drop Impact on a Solid Surface (2016, unknown): “In particular, when the impact is performed on a (super)-hydrophobic surface the retraction of the drop can lead to partial or complete rebound and even to singular jet formation (Bartolo et al. (2006); Renardy et al. (2003)), as shown in Figure 3 .”
Drop impact on a solid surface: short-time self-similarity (2015, unknown): “When the initial kinetic energy of the drop can no more be neglected in front of the surface energy (We ∼ 1), a surface wavefield starts to develop on the drop, shaping it into a characteristic liquid pyramid or torus (Renardy et al. 2003).”