Closed form expressions for the fully developed velocity, temperature and concentration profiles in a vertical channel are found by solving the equations for a cavity in the limit as the aspect ratio tends to infinity. We consider plane, steady, laminar, Boussinesq flow of an ideal gas-vapour mixture. The vertical walls are held at different constant temperatures and compositions, are impermeable to the gas and non-slip. The finite mass transfer effects of interfacial velocity and interdiffusion of enthalpy are included.
Description
Heat and mass transfer across tall cavities filled with gas-vapour mixtures: the fully developed regime - ScienceDirect
%0 Journal Article
%1 mcbain1998transfer
%A McBain, G.D.
%D 1998
%J International Journal of Heat and Mass Transfer
%K 76r10-free-convection 80a20-heat-and-mass-transfer
%N 11
%P 1397-1403
%R https://doi.org/10.1016/S0017-9310(97)00270-6
%T Heat and mass transfer across tall cavities filled with gas-vapour mixtures: the fully developed regime
%U https://www.sciencedirect.com/science/article/pii/S0017931097002706
%V 41
%X Closed form expressions for the fully developed velocity, temperature and concentration profiles in a vertical channel are found by solving the equations for a cavity in the limit as the aspect ratio tends to infinity. We consider plane, steady, laminar, Boussinesq flow of an ideal gas-vapour mixture. The vertical walls are held at different constant temperatures and compositions, are impermeable to the gas and non-slip. The finite mass transfer effects of interfacial velocity and interdiffusion of enthalpy are included.
@article{mcbain1998transfer,
abstract = {Closed form expressions for the fully developed velocity, temperature and concentration profiles in a vertical channel are found by solving the equations for a cavity in the limit as the aspect ratio tends to infinity. We consider plane, steady, laminar, Boussinesq flow of an ideal gas-vapour mixture. The vertical walls are held at different constant temperatures and compositions, are impermeable to the gas and non-slip. The finite mass transfer effects of interfacial velocity and interdiffusion of enthalpy are included.},
added-at = {2022-03-14T00:43:36.000+0100},
author = {McBain, G.D.},
biburl = {https://www.bibsonomy.org/bibtex/2d1eb7f0666bbee5e46a6778f047ad644/gdmcbain},
description = {Heat and mass transfer across tall cavities filled with gas-vapour mixtures: the fully developed regime - ScienceDirect},
doi = {https://doi.org/10.1016/S0017-9310(97)00270-6},
interhash = {a864b51077527c69ec772aa220dda78b},
intrahash = {d1eb7f0666bbee5e46a6778f047ad644},
issn = {0017-9310},
journal = {International Journal of Heat and Mass Transfer},
keywords = {76r10-free-convection 80a20-heat-and-mass-transfer},
number = 11,
pages = {1397-1403},
timestamp = {2022-03-14T00:43:36.000+0100},
title = {Heat and mass transfer across tall cavities filled with gas-vapour mixtures: the fully developed regime},
url = {https://www.sciencedirect.com/science/article/pii/S0017931097002706},
volume = 41,
year = 1998
}