Annual Meeting of the APS Four Corners Section
Volume 60, Number 11
Friday–Saturday, October 16–17, 2015;
Tempe, Arizona
Session I10: Biological Physics V: Advances in Spectroscopic Techniques
11:00 AM–12:12 PM,
Saturday, October 17, 2015
Room: PSA106
Chair: Carrie Moon, University of Denver
Abstract ID: BAPS.2015.4CF.I10.1
Abstract: I10.00001 : Biophysics of G-Protein-Coupled Receptor Activation in Membranes*
11:00 AM–11:24 AM
Preview Abstract
Abstract
Author:
Michael Brown
(Department of Physics, University of Arizona; Department of Chemistry and Biochemistry, University of Arizona)
G-protein\textbf{-}coupled receptors (GPCRs) comprise almost 50{\%} of all
pharmaceutical drug targets and afford enormous opportunities in biophysics.
Here the visual protein rhodopsin is an important prototype and occurs
naturally in lipid membranes. Photoactivation of rhodopsin entails 11-\textit{cis} to
all-\textit{trans} isomerization of the bound retinal cofactor, yielding equilibrium
between inactive Meta-I and active Meta-II states. We are employing
solid-state nuclear magnetic resonance (NMR) spectroscopy as a powerful
method to study rhodopsin activation in a membrane lipid environment [1].
For aligned membranes containing rhodopsin, the solid-state $^{\mathrm{2}}$H
NMR lineshapes of the retinal cofactor determine its average conformation
and orientation bound to the protein. Solid-state NMR data together with
theoretical molecular dynamics (MD) simulations detect increased local
mobility of retinal upon light activation [2]. The resulting changes in
local dynamics of the cofactor initiate large-scale fluctuations of
transmembrane helices that expose recognition sites for the
signal-transducing G-protein. Moreover the lipids and water comprise the
so-called "dark matter" of cellular membranes. Effects of membrane lipids on
G-protein-coupled receptors (GPCRs) are revealed by UV-visible and FTIR
spectroscopic studies of how they govern the conformational energetics of
rhodopsin in visual signaling [3]. A new flexible surface model (FSM)
describes how the curvature stress field of the membrane governs the
energetics of active rhodopsin, due to the spontaneous monolayer curvature
of the lipids [4]. The new biomembrane model challenges the standard fluid
mosaic model. The FSM describes elastic coupling of membrane lipids to the
conformational energetics of rhodopsin. Additional influences of osmotic
pressure dictate that a large number of bulk water molecules are implicated
in rhodopsin activation. An ensemble-mediated activation mechanism is
proposed for rhodopsin in a natural membrane lipid environment, which
includes a role of bulk water in the activation of rhodopsin-like GPCRs [4].
Ion channels, transporters, and membrane-bound peptides are all affected by
elastic deformation of the bilayer, thus giving a new paradigm for membrane
lipid-protein interactions in structural biophysics. [1] A. V. Struts et al.
(2011)~\textit{PNAS}$~$\textbf{108}, 8263. [2] N. Leioatts et al. (2014)\textit{ Biochemistry} \textbf{53}, 376.
[3] M. Mahalingam et al. (2008) \textit{PNAS} \textbf{105}, 17795. [4] M. F. Brown (2012)
\textit{Biochemistry} \textbf{51}, 9782.
*Research supported by NIH.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2015.4CF.I10.1