1953
DOI: 10.1021/ie50519a048
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Mass Transfer between Solid Wall and Fluid Streams. Mechanism and Eddy Distribution Relationships in Turbulent Flow.

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Cited by 241 publications
(69 citation statements)
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“…In addition, a continuous correlation for the eddy viscosity was used instead of the correlation proposed by Lin et al (1953). The assumptions in this free-flight model are more physically satisfying than those in Friedlander & Johnstone's work because the initial free-flight velocity is not assigned arbitrarily, but is equal to the local fluid velocity fluctuations at the point at which free flight begins.…”
Section: 54a Free-flight Models For Smooth Surfacesmentioning
confidence: 99%
“…In addition, a continuous correlation for the eddy viscosity was used instead of the correlation proposed by Lin et al (1953). The assumptions in this free-flight model are more physically satisfying than those in Friedlander & Johnstone's work because the initial free-flight velocity is not assigned arbitrarily, but is equal to the local fluid velocity fluctuations at the point at which free flight begins.…”
Section: 54a Free-flight Models For Smooth Surfacesmentioning
confidence: 99%
“…Based on continuity arguments, it is now well accepted that ξ a is proportional to (y + ) 3 in the close vicinity of a wall (Chapman & Kuhn, 1986). The eddy viscosity correlations of Lin et al (1953), Davies (1966a) (with Re = 10 4 ) and Lai & Nazaroff (2000) are plotted in Figure 13 and general agreement among the expressions is observed. …”
Section: Eddy Viscositymentioning
confidence: 68%
“…In addition, a continuous correlation for the eddy viscosity was utilized instead of the correlation proposed by Lin et al (1953). The assumptions in this free-flight model are much more physically satisfying than those in Friedlander & Johnstone's work because the initial free-flight velocity is not assigned arbitrarily, but is equal to the local fluid velocity fluctuations at the point at which free flight begins.…”
mentioning
confidence: 99%
“…According to the Boussinesq eddy viscosity assumption (Boussinesq, 1877), the logarithmic law for velocity profile was solved by using the mixing length method (Prandtl, 1925;Khan et al, 2017;Zawar et al, 2017). Some vertical velocity distribution laws, such as the power law and the exponential law, are based on experimental considerations or semi-empirical theories (Lin et al, 1953;Deissler, 1954;Afzal et al, 2007). Other laws for turbulent velocity profile or concentration profile are based on an indirect turbulence model (Bucci et al, 2008;Nucci and Fiorucci, 2011).…”
Section: Introductionmentioning
confidence: 99%