1992
DOI: 10.1016/0017-9310(92)90262-q
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Heat and mass transfer on a rough surface with gas blowing at the wall

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Cited by 6 publications
(3 citation statements)
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“…Now using the relation for V s = 0, given by (4.105) Kays and Crawford (1993) show that both the friction coefficient and the Stanton number predicted by (4.221) and (4.223) agree weIl with the experimental results for a large range of Band B t . Recent studies of Faraco- Medeiros and Silva-Freire (1992) and Puzach (1992) address the effect of the pressure gradient and the surface roughness.…”
Section: (B) Turbulent Boundary Layersmentioning
confidence: 99%
“…Now using the relation for V s = 0, given by (4.105) Kays and Crawford (1993) show that both the friction coefficient and the Stanton number predicted by (4.221) and (4.223) agree weIl with the experimental results for a large range of Band B t . Recent studies of Faraco- Medeiros and Silva-Freire (1992) and Puzach (1992) address the effect of the pressure gradient and the surface roughness.…”
Section: (B) Turbulent Boundary Layersmentioning
confidence: 99%
“…For Re > Recr, the flow is established in a pseudoturbulent manner, and a turbulent diffusivity operates instead of the molecular diffusivity. Determination of the value of the critical number Recr needs special experimental studies (Puzach, 1992).…”
Section: Dimensionless Numbers That Govern the Mass Transfermentioning
confidence: 99%
“…Of late, the influence of surface roughness on mass transfer rates was analyzed by Dawson and Trass (1972) by considering a series of geometrically similar rough surfaces. As an initial approach, Sedahmed and Shemilt (1976) have analyzed the impacts of surface roughness on forced convection flow, while Puzach (1992) has studied the effects of blowing over rough surfaces. The study on surface roughness is then continued by Kandlikar et al (2003) and their analysis was mainly focused on fluid flow over small diameter tubes.…”
Section: Introductionmentioning
confidence: 99%