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Nature 436, 848-851 (11 August 2005) | doi:10.1038/nature03819; Received 6 March 2005; Accepted 18 May 2005

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Small vertical movement of a K+ channel voltage sensor measured with luminescence energy transfer

David J. Posson1, Pinghua Ge1, Christopher Miller2, Francisco Bezanilla3 & Paul R. Selvin1

  1. Department of Physics and Biophysics Center, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801, USA
  2. Department of Biochemistry, Howard Hughes Medical Institute, Brandeis University, Waltham, Massachusetts 02454, USA
  3. Department of Physiology and Department of Anesthesiology, UCLA School of Medicine, Los Angeles, California 90095, USA

Correspondence to: Paul R. Selvin1 Correspondence and requests for materials should be addressed to P.R.S. (Email: selvin@uiuc.edu).

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Voltage-gated ion channels open and close in response to voltage changes across electrically excitable cell membranes1. Voltage-gated potassium (Kv) channels are homotetramers with each subunit constructed from six transmembrane segments, S1–S6 (ref. 2). The voltage-sensing domain (segments S1–S4) contains charged arginine residues on S4 that move across the membrane electric field2, 3, modulating channel open probability. Understanding the physical movements of this voltage sensor is of fundamental importance and is the subject of controversy. Recently, the crystal structure of the KvAP4 channel motivated an unconventional 'paddle model' of S4 charge movement, indicating that the segments S3b and S4 might move as a unit through the lipid bilayer with a large (15–20-Å) transmembrane displacement5. Here we show that the voltage-sensor segments do not undergo significant transmembrane translation. We tested the movement of these segments in functional Shaker K+ channels by using luminescence resonance energy transfer to measure distances between the voltage sensors and a pore-bound scorpion toxin. Our results are consistent with a 2-Å vertical displacement of S4, not the large excursion predicted by the paddle model. This small movement supports an alternative model in which the protein shapes the electric field profile, focusing it across a narrow region of S4 (ref. 6).

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