2018
DOI: 10.1017/jfm.2018.60
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Droplet impact onto an elastic plate: a new mechanism for splashing

Abstract: During a droplet impact onto a substrate, splashing is known to be caused by the presence of surrounding gas or by surface roughness. Impact occurring in a vacuum onto a smooth rigid wall results in droplet spreading, rather than development of a corona or prompt splash. Here we present an analytical and numerical study of a third potential splashing mechanism, namely elastic deformation of the substrate. An axisymmetric Wagner-style model of droplet impact is formulated and solved using the method of normal m… Show more

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Cited by 42 publications
(43 citation statements)
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“…The outcomes of a droplet impact on solid surfaces, such as deposition, rebounding, splashing, depend on both the micro/nanostructures and chemical property of the solid. Diverse strategies have been exploited by nature as well as artificial materials to regulate the droplet impact processes as well as the subsequent droplet motions 1013 . For example, various superhydrophobic surfaces are fabricated to accelerate the droplet bouncing off solids after impact 1416 ; topological heterogeneity is utilized for directional transportation of impacting droplets 17,18 .…”
Section: Introductionmentioning
confidence: 99%
“…The outcomes of a droplet impact on solid surfaces, such as deposition, rebounding, splashing, depend on both the micro/nanostructures and chemical property of the solid. Diverse strategies have been exploited by nature as well as artificial materials to regulate the droplet impact processes as well as the subsequent droplet motions 1013 . For example, various superhydrophobic surfaces are fabricated to accelerate the droplet bouncing off solids after impact 1416 ; topological heterogeneity is utilized for directional transportation of impacting droplets 17,18 .…”
Section: Introductionmentioning
confidence: 99%
“…The solution of the hydrodynamic problem (4.1)-(4.3) is given by (4.19) see Appendix A in Korobkin & Scolan (2006). It is convenient to introduce the functions Q n (x) and the coefficients W nk by (4.20) see equations (3.19) and (3.37) in Pegg et al (2018). In particular, Q 0 (x) = √ 2.…”
Section: Formulation Of the Axisymmetric Exit Problem And Its Solutionmentioning
confidence: 99%
“…In particular, Q 0 (x) = √ 2. The functions Q n (x) and the coefficients W nk are expressed through the Bessel, trigonometric and hyperbolic functions similar to those in Pegg et al (2018), Appendixes B and C, where the corresponding integrals were evaluated for a simply supported circular elastic disc.…”
Section: Formulation Of the Axisymmetric Exit Problem And Its Solutionmentioning
confidence: 99%
“…One of the earliest models investigated a droplet impacting onto an elastic halfspace by imposing a constant uniform pressure over a circle whose radius increased in proportion to the square root of time [35]. The full hydroelastic problem of the impact of a two-dimensional wave onto an Euler-Bernoulli beam has previously been studied using Wagner theory [36], and more recently this analytical model has been extended to study the axisymmetric impact of a droplet onto an elastic plate, where the elastic plate has a radius much smaller than the droplet and its deflection governed by thin-plate theory [37]. A thorough parameter study was conducted for different types of plate, and regimes where the elasticity of the plate could cause splashing of the droplet at early times, defined as the detachment of the splash sheet from the surface of the plate, have been identified.…”
Section: Introductionmentioning
confidence: 99%