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The recent mu-opioid receptor (MOPr) and kappa-opioid receptor (KOPr) crystal structures have inspired hypotheses of physiologically relevant dimerization contacts, specifically: a closely packed interface involving transmembrane (TM) helices TM5 and TM6, and a less compact interface, involving TM1, TM2, and helix 8 (H8). While the former was only found in MOPr crystals, similar arrangements of the latter were identified for both KOPr and MOPr. The relevance of these interfaces outside of a crystal lattice is called into question by the possibility that they might be influenced by the specific crystallization conditions. In this study, we have employed umbrella sampling molecular dynamics simulations of coarse-grained representations of the interacting MOPr or KOPr crystallographic structures, in the absence of the T4 lysozyme, and in an explicit lipid-water environment, to determine the strength of receptor dimerization at the different crystallographic interfaces. We note that the shape of the interface plays a dominant role in the strength of the interaction, and the pattern of contacting residues defines the shape of the potential of mean force. This information can be used to guide experiments aimed at exploring the role of dimerization in opioid receptor function. [ABSTRACT FROM AUTHOR]

Despite many years of dedicated efforts, high-resolution structural determination of membrane proteins lags far behind that of soluble proteins. Computational methods in general, and molecular dynamics (MD) simulations in particular, have represented important alternative resources over the years to advance understanding of membrane protein structure and function. However, it is only recently that much progress has been achieved owing to new high-resolution membrane protein structures, specialized parallel computer architectures, and efficient simulation algorithms. This has definitely been the case for G protein-coupled receptors (GPCRs), which have assumed a leading role in the area of structural biology with several new structures appearing in the literature during the past five years. We provide here a concise overview of recent developments in computational biophysics of membrane proteins, using GPCRs as an example to showcase important information that can be derived from modern MD simulations. [ABSTRACT FROM AUTHOR]

The mitochondrial ADP/ATP carrier is a six helix bundle membrane transport protein, which couples the exit of ATP from the mitochondrial matrix to the entry of ADP. Extended (4×20 ns) molecular dynamics simulations of the carrier, in the presence and absence of bound inhibitor (carboxyatractyloside), have been used to explore the conformational dynamics of the protein in a lipid bilayer environment, in the presence and absence of the carboxyatractyloside inhibitor. The dynamic flexibility (measured as conformational drift and fluctuations) of the protein is reduced in the presence of bound inhibitor. Proline residues in transmembrane helices H1, H3 and H5 appear to form dynamic hinges. Fluctuations in inter-helix salt bridges are also observed over the time course of the simulations. Inhibitor-protein and lipid-protein interactions have been characterised in some detail. Overall, the simulations support a transport mechanism in which flexibility about the proline hinges enables a transition between a 'closed' and an 'open' pore-like state of the carrier protein. [ABSTRACT FROM AUTHOR]