2001
DOI: 10.1016/s0017-9310(01)00084-9
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Pool-boiling CHF enhancement by modulated porous-layer coating: theory and experiment

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Cited by 439 publications
(220 citation statements)
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“…Submerged pool boiling from porous surfaces has been extensively characterized for a number of surface geometries, working fluids, and flooded porous wick structures often found in heat pipes [15][16][17][18][19][20][21][22][23][24][25][26][27][28]. The fundamental mechanism of heat transfer during boiling from a porous surface submerged in a liquid pool differs from that from a wick that is passively fed by capillary action.…”
Section: Nucleate Boiling In Porous Wick Structuresmentioning
confidence: 99%
“…Submerged pool boiling from porous surfaces has been extensively characterized for a number of surface geometries, working fluids, and flooded porous wick structures often found in heat pipes [15][16][17][18][19][20][21][22][23][24][25][26][27][28]. The fundamental mechanism of heat transfer during boiling from a porous surface submerged in a liquid pool differs from that from a wick that is passively fed by capillary action.…”
Section: Nucleate Boiling In Porous Wick Structuresmentioning
confidence: 99%
“…15 The basic idea is that the hydrodynamic limit model based on Rayleigh-Taylor instability wavelength ͑ RT,c ͒ on the plain surface originally proposed by Zuber 16 can be extended to a surface with microstructure coating and the capillary limit. The onset of CHF based on the hydrodynamic limit is due to the instability of vapor columns.…”
mentioning
confidence: 99%
“…The wavelength can be a geometrically determined factor according to the surface condition. 15 As the result, the change in wavelength prolongs the wetting of the surface by allowing the liquid to break through which means the enhancement of CHF. Recognizing that the CHF enhancement and wavelengths reported in the literature are not exactly matched with the prediction of Eq.…”
mentioning
confidence: 99%
“…A similar analysis has been employed by others with satisfactory predictions [17,34]. Using a volumetric porosity ε of 0.5±0.02, an average breakthrough bubble diameter d br of 42 μm (determined from the average pore diameter ), and thermophysical properties of water at saturation temperature (100 °C), the hydrodynamic limit of the bare sample is estimated to be 906±102 W/cm 2 using: …”
Section: Mechanism Of Dryoutmentioning
confidence: 92%
“…The hydrodynamic instability limit is reached when the interfaces of the liquid-vapor counterflow columns become Helmholtz-unstable. Liter and Kaviany [34] demonstrated that the hydrodynamic limit can be significantly increased using modulated porous structures which provide preferential flow paths for liquid and vapor, thereby reducing the liquid/vapor counterflow situations and aiding non-hydrodynamical determination of the critical instability wavelength. Various other studies also report a significant increase in critical heat flux (CHF) of uniformly coated porous surfaces compared to plain surfaces investigated under natural convection boiling conditions [17,35].…”
Section: Mechanism Of Dryoutmentioning
confidence: 99%