2016
DOI: 10.1016/j.ijheatfluidflow.2016.10.003
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Effects of temperature-dependent contact angle on the flow dynamics of an impinging droplet on a hot solid substrate

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Cited by 13 publications
(3 citation statements)
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“…3) Although pesticide use can increase crop yields in the short term, their excessive use leaves many hidden dangers that can be easy to ignore. For example, pesticide droplets can easily roll off the surface of rice leaves, 4,5) causing only 20-30% of the pesticides to be deposited on the target. The remaining 70-80% is lost to the soil, 6) which leads to the pesticide having a low degree of wet spreading on the plant foliage 7,8) and causing ecological pollution.…”
Section: Introductionmentioning
confidence: 99%
“…3) Although pesticide use can increase crop yields in the short term, their excessive use leaves many hidden dangers that can be easy to ignore. For example, pesticide droplets can easily roll off the surface of rice leaves, 4,5) causing only 20-30% of the pesticides to be deposited on the target. The remaining 70-80% is lost to the soil, 6) which leads to the pesticide having a low degree of wet spreading on the plant foliage 7,8) and causing ecological pollution.…”
Section: Introductionmentioning
confidence: 99%
“…So called generalized Navier boundary conditions (GNBC) derived from the molecular dynamics (MD) theory for the Navier-Stokes equations have been proven to capture the dynamics of the triple contact line adequately (see [16,17,18,19]). GNBC have already been successfully applied for simulating free surface flows with ALE FEM for various multiphysics phenomena such as free surface flows in [13], sliding/rolling droplets kinematics in [20,21], droplets kinematics on non-isothermal surfaces in [22], chemotaxis phenomena in [23,24], to name a few. The main goal of this paper is the derivation of the energy stable numerical scheme based on the mathematical model incorporating GNBC and not the investigation of GNBC themselves.…”
Section: Introductionmentioning
confidence: 99%
“…In practice, ALE velocity may be constructed solving the following problem: for t > 0 and v h fluid velocity,−∆ w h = 0 in Ω h , w h = v h • ν h k h • ν h k h on ∂Ω h ,(3.5)where k h : ∂Ω h → R d is some user defined vector and depends on the physics of the problem.The trivial choice of k h is k h = v h which, formally, yields w h = v h on ∂Ω h . This is a very common choice for simulating the kinematics of droplets with FEM (see, e.g.,[22,20,21]). In this paper, we use implicit discretization in time for the domain evolution.…”
mentioning
confidence: 99%