The Journal of General Physiology
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Published online Nov 29 2004. doi:10.1085/jgp.200409111
The Rockefeller University Press, 0022-1295 $8.00
JGP, Volume 124, Number 6, 679-690
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On the Importance of Atomic Fluctuations, Protein Flexibility, and Solvent in Ion Permeation

Toby W. Allen1, O.S. Andersen1, and Benoit Roux1,2

1 Department of Physiology and Biophysics, Weill Medical College of Cornell University, New York, NY 10021
2 Department of Biochemistry, Weill Medical College of Cornell University, New York, NY 10021

Address correspondence to Benoit Roux, Department of Physiology and Biophysics, Weill Medical College of Cornell University, 1300 York Ave., New York, NY 10021. Fax: 212-746-4843; email: benoit.roux{at}med.cornell.edu

Proteins, including ion channels, often are described in terms of some average structure and pictured as rigid entities immersed in a featureless solvent continuum. This simplified view, which provides for a convenient representation of the protein's overall structure, incurs the risk of deemphasizing important features underlying protein function, such as thermal fluctuations in the atom positions and the discreteness of the solvent molecules. These factors become particularly important in the case of ion movement through narrow pores, where the magnitude of the thermal fluctuations may be comparable to the ion pore atom separations, such that the strength of the ion channel interactions may vary dramatically as a function of the instantaneous configuration of the ion and the surrounding protein and pore water. Descriptions of ion permeation through narrow pores, which employ static protein structures and a macroscopic continuum dielectric solvent, thus face fundamental difficulties. We illustrate this using simple model calculations based on the gramicidin A and KcsA potassium channels, which show that thermal atomic fluctuations lead to energy profiles that vary by tens of kcal/mol. Consequently, within the framework of a rigid pore model, ion-channel energetics is extremely sensitive to the choice of experimental structure and how the space-dependent dielectric constant is assigned. Given these observations, the significance of any description based on a rigid structure appears limited. Creating a conducting channel model from one single structure requires substantial and arbitrary engineering of the model parameters, making it difficult for such approaches to contribute to our understanding of ion permeation at a microscopic level.

Key Words: crystallographic B factors • continuum electrostatics • Poisson-Boltzmann theory • ion solvation • free energy profile


T.W. Allen's present address is Department of Chemistry, University of California, Davis, Davis, CA 95616-5295.

Abbreviations used in this paper: gA, gramicidin A; MD, molecular dynamics; NMR, nuclear magnetic resonance; PMF, potential of mean force; RMS, root-mean-square.


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