We consider a mass transfer induced buoyancy force, superimposed on a thermally induced one, in a flow generated adjacent to a vertical surface. Flow and stability were investigated for a Prandtl number of 0.7; for Schmidt numbers of 2.0, 0.94, and 0.2; and for different magnitudes of the buoyancy effects.
SCOPEMass transfer occurring in a body of fluid gives rise to a buoyancy force if the concentration gradient causes density differences. If the concentration of the diffusing species is sufficiently small, the equations governing the phenomenon are identical to those governing a thermally induced flow. A frequently occurring circumstance in our environment and in technological applications is the simultaneous transport of both thermal energy and a chemical constituent. The two buoyancy effects may be in the same direction or opposing. They may even have different spatial extent in the fluid if the Prandtl and Schmidt numbers are different.The consequences, the effects on the resulting flow and on its stability to disturbances whose growth determines transition to turbulence, were investigated for a gas. Mass transfer effects were determined over the known range of mass transfer rates, that is, of Schmidt number.The analyses predict transport rates as well as the conditions of instability and the actual disturbance growth rates. These results amount to an assessment of those complicated and interacting effects over a wide range of practical applications. Previous developments are summarized in a later section, preceding the analysis.
PREVIOUS WORKOne of the first investigations of the flow resulting from combined buoyancy modes was by Somers (1956), who applied integral method analysis to predict the flow that would arise adjacent to a wetted isothermal surface. Mathers et al. (1957) and Wilcox (1961) using, respectively, an analogue and an integral analysis, follow Somers in as- Gebhart. the total buoyancy term in the momentum equation. Such All correspondence concerning this paper should be addressed to B. signing a factor +% to the transport contribution to formation and predicted the observed weak temperature dependence of fuel nitrogen conversion, as well as a significant effect of particle size,