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. Author manuscript; available in PMC: 2006 Dec 28.
Published in final edited form as: J Membr Biol. 2005 Nov;208(1):39–53. doi: 10.1007/s00232-005-0817-9

Fig. 2.

Fig. 2

A simple two-membrane model of epithelial transport. (A) Secretion of fluid without boundary conditions on the secretion. The basolateral membranes are washed with a well-stirred solution of osmolarity co; the intracellular osmolarity Ci(X) is allowed to vary across the epithelium, but the calculations suggest it is essentially constant because difiusion is very effective over short distances; the secreted solution has osmolarity cs, which is determined by the membrane water permeability and the rate of salt transport, j. Since the flux of salt in the secretion is carried entirely by convection, it is given by j = ucs. Hence the boundary condition on the osmolarity of the secretion is cs = j/u for model A. (B) The same simple model of an epithelium, but now each side is washed with a well-stirred solution whose osmolarity is co. Thus the difference in the two models is the boundary condition on the secretion, which is cs = co for model B.