2020
DOI: 10.1016/j.ijheatmasstransfer.2020.119661
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Heat transfer during drop impingement onto a hot wall: The influence of wall superheat, impact velocity, and drop diameter

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Cited by 51 publications
(23 citation statements)
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“…The heat transfer from single drop impacts was characterized in dependence of impact parameters and material parameters, expressed in dimensionless form [12]. This work was then extended to the case of multiple drop impacts, either vertically coalescing or side-by-side.…”
Section: Droplet and Spray Interactions With Hot Wallsmentioning
confidence: 99%
“…The heat transfer from single drop impacts was characterized in dependence of impact parameters and material parameters, expressed in dimensionless form [12]. This work was then extended to the case of multiple drop impacts, either vertically coalescing or side-by-side.…”
Section: Droplet and Spray Interactions With Hot Wallsmentioning
confidence: 99%
“…A thermal boundary layer in the vapour region close to the wall is initialised prior to the simulation. Dimensions of the domain are chosen such that boundary conditions do not influence the drop impingement process [1] It is shown in associated experiments in [6,7] that no three-dimensional effects (like splash) are observed for the investigated parameter range. Hence, a static, structured 2D axis-symmetric grid with local grid refinement at the solid-fluid interface is chosen.…”
Section: Model Descriptionmentioning
confidence: 99%
“…12). The experimental setup and procedure are described in [6,7]. After the impact and coalescence of two drops, the combined drop spreads.…”
Section: Vertical Coalescencementioning
confidence: 99%
“…The heat conduction equation is solved using the finite volume method. The details of the above procedure for determination of heat flux distribution and its accuracy are discussed in [8,22].…”
Section: Data Reductionmentioning
confidence: 99%
“…Numerical simulations [11,12,21] and experimental studies [8,11] reveal that, if the drop impinges an impermeable and rigid substrate in drop deposition (in the absence of splashing and bouncing phenomena) and film evaporation regimes, its evolution can be subdivided into three subsequent phases: (i) the drop spreading phase, in which the contact line advances radially outwards due to action of inertia; (ii) the drop receding phase, in which the contact line moves inwards due to surface tension; and (iii) the phase of sessile drop evaporation, in which the drop is at a state of mechanical equilibrium. During all three phases, heat is transferred by conduction, convection, and evaporation.…”
Section: Introductionmentioning
confidence: 99%