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Heat Transfer, Volume 2 2006
DOI: 10.1115/imece2006-13899
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Characteristics of an Evaporating Thin Film in a Microchannel

Abstract: An evaporating meniscus in a microchannel is investigated through an augmented Young-Laplace model and the kinetic theory-based expression for mass transport across a liquid-vapor interface. The complete expression for mass transport is employed without any approximations and boundary conditions for the film profile are developed. The thin-film and the intrinsic-meniscus regions are distinguished based on the disjoining pressure variation along the meniscus. While heat transfer in the thin-film region is found… Show more

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Cited by 10 publications
(56 citation statements)
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References 19 publications
(28 reference statements)
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“…The heat exhibition of the heat pipe for expanding and diminishing heat motions are contrasted and refined water while using 10 wt % of Al 2 O 3 NF falls apart the heat pipe heat execution Wang, Garimella [20]. When the heat transfer effectiveness with thermo siphon has own importance the rate of heat transfer can be calculated Wilson, Q. Yu et al [21].…”
Section: Performance Of Heat Pipe With Different Parametersmentioning
confidence: 99%
“…The heat exhibition of the heat pipe for expanding and diminishing heat motions are contrasted and refined water while using 10 wt % of Al 2 O 3 NF falls apart the heat pipe heat execution Wang, Garimella [20]. When the heat transfer effectiveness with thermo siphon has own importance the rate of heat transfer can be calculated Wilson, Q. Yu et al [21].…”
Section: Performance Of Heat Pipe With Different Parametersmentioning
confidence: 99%
“…The fourth‐order Runge–Kutta procedure and the shooting method were used to solve the equations. The guessed initial conditions (∂δ/∂ x )| x =0 and $\dot{m}$ v | x =0 are determined iteratively to satisfy the boundary conditions at x = L 2, 3, 7: …”
Section: Theoretical Modelmentioning
confidence: 99%
“…1 can be typically divided into three regions: the intrinsic meniscus region where capillary forces dominate, the evaporating thin film region which is affected by both long‐range intermolecular forces (the disjoining pressure) and capillary forces, and the non‐evaporating film region governed by the disjoining pressure. Strong evaporation and most of the interfacial temperature drop occur in the thin film region due to the very small thermal resistance 1–3. The liquid pressure gradient is caused by the capillary pressure gradient due to variation in the film curvature and the disjoining pressure gradient resulting from film thickness changes in the evaporating thin film region.…”
Section: Introductionmentioning
confidence: 99%
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“…These assumptions for the adsorbed region allow for the determination of initial conditions by inspection. As the film cannot evaporate, the mass flux balance for the adsorbed region has a net mass exchange of zero, despite being subjected to an applied superheat [7,10,12,15]. Thus it may be inferred that the principal mode of heat transfer is conduction through the adsorbed layer [7,12,15].…”
Section: Adsorbed Regionmentioning
confidence: 99%