2012
DOI: 10.1016/j.ijthermalsci.2011.09.017
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Modeling of heat and mass transfer in the liquid film of rotating heat pipes

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Cited by 29 publications
(32 citation statements)
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“…where the first equation is the no-slip boundary condition at the inner wall [23][24][25], the second equation is the negligible shear stress boundary condition at the liquid/vapor interface [24,36] and the third equation describes the average velocity as the velocity profile integrated over the liquid film divided by the cross-sectional area.…”
Section: Liquid Componentmentioning
confidence: 99%
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“…where the first equation is the no-slip boundary condition at the inner wall [23][24][25], the second equation is the negligible shear stress boundary condition at the liquid/vapor interface [24,36] and the third equation describes the average velocity as the velocity profile integrated over the liquid film divided by the cross-sectional area.…”
Section: Liquid Componentmentioning
confidence: 99%
“…For RHPs, steady-state modelling has been extensively addressed [23][24][25], with recent studies focusing on the use of nanofluids [26,27]. On the other hand, transient modelling studies are scarce.…”
Section: Introductionmentioning
confidence: 99%
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“…When a film is flowing down the outside of a rotating cylinder, it has been shown [25][26][27] that the first azimuthal mode may be the most unstable one under different circumstances. Nevertheless, for flow inside the cylinder (as in [28]) the most unstable mode is the axial one. The relevance of the azimuthal modes is also found in the instability of inviscid stratified fluids in a rotating annulus [29].…”
Section: Introductionmentioning
confidence: 99%