1-2-oleoylphosphatidylcholine and decalin

1-2-oleoylphosphatidylcholine has been researched along with decalin* in 2 studies

Other Studies

2 other study(ies) available for 1-2-oleoylphosphatidylcholine and decalin

ArticleYear
A Parameterization of Cholesterol for Mixed Lipid Bilayer Simulation within the Amber Lipid14 Force Field.
    The journal of physical chemistry. B, 2015, Sep-24, Volume: 119, Issue:38

    The Amber Lipid14 force field is expanded to include cholesterol parameters for all-atom cholesterol and lipid bilayer molecular dynamics simulations. The General Amber and Lipid14 force fields are used as a basis for assigning atom types and basic parameters. A new RESP charge derivation for cholesterol is presented, and tail parameters are adapted from Lipid14 alkane tails. 1,2-Dimyristoyl-sn-glycero-3-phosphocholine (DMPC), 1,2-dioleoyl-sn-glycero-3-phosphocholine (DOPC), and 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) bilayers are simulated at a range of cholesterol contents. Experimental bilayer structural properties are compared with bilayer simulations and are found to be in good agreement. With this parameterization, another component of complex membranes is available for molecular dynamics with the Amber Lipid14 force field.

    Topics: Alkanes; Cholesterol; Dimyristoylphosphatidylcholine; Glycerylphosphorylcholine; Lipid Bilayers; Molecular Dynamics Simulation; Naphthalenes; Neutron Diffraction; Phosphatidylcholines; Temperature; X-Ray Diffraction

2015
Update of the cholesterol force field parameters in CHARMM.
    The journal of physical chemistry. B, 2012, Jan-12, Volume: 116, Issue:1

    A modification of the CHARMM36 lipid force field (C36) for cholesterol, henceforth, called C36c, is reported. A fused ring compound, decalin, was used to model the steroid section of cholesterol. For decalin, C36 inaccurately predicts the heat of vaporization (~10 kJ/mol) and molar volume (~10 cc/mol), but C36c resulted in near perfect comparison with experiment. MD simulations of decalin and heptane at various compositions were run to estimate the enthalpy and volumes of mixing to compare to experiment for this simple model of cholesterol in a chain environment. Superior estimates for these thermodynamic properties were obtained with C36c versus C36. These new parameters were applied to cholesterol, and quantum mechanical calculations were performed to modify the torsional potential of an acyl chain torsion for cholesterol. This model was tested through simulations of DMPC/10% cholesterol, DMPC/30% cholesterol, and DOPC/10% cholesterol. The C36 and C36c results were similar for surface areas per lipid, deuterium order parameters, electron density profiles, and atomic form factors and generally agree well with experiment. However, C36 and C36c produced slightly different cholesterol angle distributions with C36c adopting a more perpendicular orientation with respect to the bilayer plane. The new parameters in the C36c modification should enable more accurate simulations of lipid bilayers with cholesterol, especially for those interested in the free energy of lipid flip/flop or transfer of phospholipids and/or cholesterol.

    Topics: Cholesterol; Dimyristoylphosphatidylcholine; Heptanes; Lipid Bilayers; Molecular Dynamics Simulation; Naphthalenes; Phosphatidylcholines; Phospholipids; Quantum Theory; Thermodynamics

2012