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

This Article
Right arrow Full Text
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 Lecar, H.
Right arrow Articles by Grabe, M.
Right arrow Search for Related Content
PubMed
Right arrow PubMed Citation
Right arrow Articles by Lecar, H.
Right arrow Articles by Grabe, M.
Biophysical Journal 85:2854-2864 (2003)
© 2003 The Biophysical Society

Electrostatic Model of S4 Motion in Voltage-Gated Ion Channels

Harold Lecar *, H. Peter Larsson {dagger} and Michael Grabe {ddagger}

* Department of Molecular and Cell Biology, University of California at Berkeley, Berkeley, California; {dagger} Neurological Sciences Institute, Oregon Health Sciences University, Beaverton, Oregon; and {ddagger} Howard Hughes Medical Institute, University of California, San Francisco, California

Correspondence: Address reprint requests to Harold Lecar, Dept. of Cell and Molecular Biology, 134 LSA, MC# 3200, University of California at Berkeley, Berkeley, CA 94720. E-mail: hlecar{at}uclink4.berkeley.edu.

The S4 transmembrane domain of the family of voltage-gated ion channels is generally thought to be the voltage sensor, whose translocation by an applied electric field produces the gating current. Experiments on hSkMI Na+ channels and both Shaker and EAG K+ channels indicate which S4 residues cross the membrane-solution interface during activation gating. Using this structural information, we derive the steady-state properties of gating-charge transfer for wild-type and mutant Shaker K+ channels. Assuming that the energetics of gating is dominated by electrostatic forces between S4 charges and countercharges on neighboring transmembrane domains, we calculate the total energy as a function of transmembrane displacement and twist of the S4 domain. The resulting electrostatic energy surface exhibits a series of deep energy minima, corresponding to the transition states of the gating process. The steady-state gating-charge distribution is then given by a Boltzmann distribution among the transition states. The resulting gating-charge distributions are compared to experimental results on wild-type and charge-neutralized mutants of the Shaker K+ channel.




This article has been cited by other articles:


Home page
J. Gen. Physiol.Home page
M. Pathak, L. Kurtz, F. Tombola, and E. Isacoff
The Cooperative Voltage Sensor Motion that Gates a Potassium Channel
J. Gen. Physiol., December 28, 2004; 125(1): 57 - 69.
[Abstract] [Full Text] [PDF]


Home page
Proc. Natl. Acad. Sci. USAHome page
M. Grabe, H. Lecar, Y. N. Jan, and L. Y. Jan
A quantitative assessment of models for voltage-dependent gating of ion channels
PNAS, December 21, 2004; 101(51): 17640 - 17645.
[Abstract] [Full Text] [PDF]


Home page
J. Gen. Physiol.Home page
C. A. Ahern and R. Horn
Specificity of Charge-carrying Residues in the Voltage Sensor of Potassium Channels
J. Gen. Physiol., February 23, 2004; 123(3): 205 - 216.
[Abstract] [Full Text] [PDF]


Home page
J. Gen. Physiol.Home page
R. Horn
How S4 Segments Move Charge. Let Me Count the Ways
J. Gen. Physiol., December 29, 2003; 123(1): 1 - 4.
[Full Text] [PDF]




HOME HELP FEEDBACK SUBSCRIPTIONS ARCHIVE SEARCH TABLE OF CONTENTS
Copyright © 2003 by the Biophysical Society.