id	author	title	date	pages	extension	mime	words	sentence	flesch	summary	cache	txt
cet-9236		cet-9236		6	.pdf	application/pdf	2917	95	47	The boundary conditions for the velocity field are given by 0v 0xz,L = = , 0v Wxz,L = = , 0v 0yz,L = = , 0v LHyz,L = = , (11) and those for the concentration field by 0 x c 0x L = ∂ ∂ = , 0 x c Wx L = ∂ ∂ = , 0 y c 0y L = ∂ ∂ = and LHy L D N y c L −= ∂ ∂ = , with Wx0 ≤≤ and LHy0 ≤≤ . In reason of the similarity between the transport mechanisms in both fluid channels, only the equations for the liquid channel are presented in this section as follows: The Navier-Stokes equation writes 674 dz dp1 y v x v L L 2 z,L 2 2 z,L 2 ⋅−= ∂ ∂ + ∂ ∂ μ .	cache/cet-9236.pdf	txt/cet-9236.txt