help button home button Biophys. J.
HOME HELP FEEDBACK SUBSCRIPTIONS ARCHIVE SEARCH TABLE OF CONTENTS

Biophysical Journal 15: 533-551 (1975)
© 1975 the Biophysical Society

This Article
Right arrow Full Text (PDF)
Right arrow Alert me when this article is cited
Right arrow Alert me if a correction is posted
Services
Right arrow Similar articles in this journal
Right arrow Similar articles in PubMed
Right arrow Alert me to new issues of the journal
Right arrow Download to citation manager
Right arrow reprints & permissions
Citing Articles
Right arrow Citing Articles via HighWire
Right arrow Citing Articles via Google Scholar
Google Scholar
Right arrow Articles by Levitt, D G
Right arrow Search for Related Content
PubMed
Right arrow PubMed Citation
Right arrow Articles by Levitt, D G

General continuum analysis of transport through pores. I. Proof of Onsager's reciprocity postulate for uniform pore.

D G Levitt

ABSTRACT

The nonelectrolyte (Js) and volume (Jv) flux across a membrane is usually described in terms of two equations derived from the theory of irreversible thermodynamics: (see article) where delta c and delta P are the concentration and pressure difference; omega and Lp are the diffuse and hydraulic permeability; and sigma s and sigma v are the reflection coefficients. If Onsager's reciprocity postulate is assumed, it can be shown that signa s and sigma v are equal. This is an important assumption because it allows one to apply the continuum theory relationship between sigma s and the pore radius to experimental measurements of sigma v. In this paper, general continuum expressions for both the Jv (a new result) and Js equation will be derived and the equality of sigma s and sigma v proved. The proof uses only general hydrodynamic results and does not require explicit solutions for the drag coefficients or, for example, the assumption that the solute is in the center of the pore. The proof applys to arbitrarily shaped solutes and any pore whose shape is independent of axial position (uniform). In addition, new expressions for the functional dependence of omega and sigma on the pore radius are derived (including the effect of the particle lying off the pore axis). These expressions differ slightly from earlier results and are probably more accurate.




This article has been cited by other articles:


Home page
J. Gen. Physiol.Home page
A. L. Harris
Connexin Specificity of Second Messenger Permeation: Real Numbers At Last
J. Gen. Physiol., March 31, 2008; 131(4): 287 - 292.
[Full Text] [PDF]


Home page
Biophys. JHome page
N. S. Heyman and J. M. Burt
Hindered Diffusion through an Aqueous Pore Describes Invariant Dye Selectivity of Cx43 Junctions
Biophys. J., February 1, 2008; 94(3): 840 - 854.
[Abstract] [Full Text] [PDF]


Home page
Biophys. JHome page
J. M. Nitsche, H.-C. Chang, P. A. Weber, and B. J. Nicholson
A Transient Diffusion Model Yields Unitary Gap Junctional Permeabilities from Images of Cell-to-Cell Fluorescent Dye Transfer Between Xenopus Oocytes
Biophys. J., April 1, 2004; 86(4): 2058 - 2077.
[Abstract] [Full Text] [PDF]


Home page
Biophys. JHome page
H. Lecar, H. P. Larsson, and M. Grabe
Electrostatic Model of S4 Motion in Voltage-Gated Ion Channels
Biophys. J., November 1, 2003; 85(5): 2854 - 2864.
[Abstract] [Full Text] [PDF]




HOME HELP FEEDBACK SUBSCRIPTIONS ARCHIVE SEARCH TABLE OF CONTENTS
Copyright © 1975 by the Biophysical Society.