Incorporating dipolar solvents with variable density in Poisson-Boltzmann electrostatics.
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Molecular docking as a popular tool in drug design, an in silico travelUnderstanding nucleic acid-ion interactionsBiomolecular electrostatics and solvation: a computational perspectiveStructural basis for ion permeation mechanism in pentameric ligand-gated ion channelsNonlocal Electrostatics in Spherical Geometries Using Eigenfunction Expansions of Boundary-Integral Operators.Validating solution ensembles from molecular dynamics simulation by wide-angle X-ray scattering data.Communication: modeling charge-sign asymmetric solvation free energies with nonlinear boundary conditionsNonlinear Poisson equation for heterogeneous media.Adapting Poisson-Boltzmann to the self-consistent mean field theory: application to protein side-chain modeling.The ionic atmosphere around A-RNA: Poisson-Boltzmann and molecular dynamics simulations.Formulation of a new and simple nonuniform size-modified Poisson-Boltzmann description.The electrostatic response of water to neutral polar solutes: implications for continuum solvent modeling.Investigating Mutations to Reduce Huntingtin Aggregation by Increasing Htt-N-Terminal Stability and Weakening Interactions with PolyQ Domain.AQUASOL: An efficient solver for the dipolar Poisson-Boltzmann-Langevin equation.Computing ion solvation free energies using the dipolar Poisson modelDifferential geometry based solvation model. III. Quantum formulation.Computational assembly of polymorphic amyloid fibrils reveals stable aggregatesAquaSAXS: a web server for computation and fitting of SAXS profiles with non-uniformally hydrated atomic models.On the ability of molecular dynamics simulation and continuum electrostatics to treat interfacial water molecules in protein-protein complexes.Comparing the Predictions of the Nonlinear Poisson-Boltzmann Equation and the Ion Size-Modified Poisson-Boltzmann Equation for a Low-Dielectric Charged Spherical Cavity in an Aqueous Salt Solution.Influence of nonelectrostatic ion-ion interactions on double-layer capacitance.Molecular density functional theory of water describing hydrophobicity at short and long length scales.Dipolar Poisson-Boltzmann approach to ionic solutions: a mean field and loop expansion analysis.Electric double layer force between charged surfaces: effect of solvent polarization.Poisson-Helmholtz-Boltzmann model of the electric double layer: analysis of monovalent ionic mixtures.The Poisson-Helmholtz-Boltzmann model.Polarizable Poisson-Boltzmann equation: the study of polarizability effects on the structure of a double layer.Molecular density functional theory of solvation: from polar solvents to water.Charged particles at fluid interfaces as a probe into structural details of a double layer.Beyond the Poisson-Boltzmann model: modeling biomolecule-water and water-water interactions.
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P2860
Incorporating dipolar solvents with variable density in Poisson-Boltzmann electrostatics.
description
article científic
@ca
article scientifique
@fr
articolo scientifico
@it
artigo científico
@pt
bilimsel makale
@tr
scientific article published on 26 September 2008
@en
vedecký článok
@sk
vetenskaplig artikel
@sv
videnskabelig artikel
@da
vědecký článek
@cs
name
Incorporating dipolar solvents with variable density in Poisson-Boltzmann electrostatics.
@en
Incorporating dipolar solvents with variable density in Poisson-Boltzmann electrostatics.
@nl
type
label
Incorporating dipolar solvents with variable density in Poisson-Boltzmann electrostatics.
@en
Incorporating dipolar solvents with variable density in Poisson-Boltzmann electrostatics.
@nl
prefLabel
Incorporating dipolar solvents with variable density in Poisson-Boltzmann electrostatics.
@en
Incorporating dipolar solvents with variable density in Poisson-Boltzmann electrostatics.
@nl
P2093
P2860
P1433
P1476
Incorporating dipolar solvents with variable density in Poisson-Boltzmann electrostatics.
@en
P2093
Cyril Azuara
Henri Orland
Marc Delarue
Michael Bon
Patrice Koehl
P2860
P304
P356
10.1529/BIOPHYSJ.108.131649
P407
P577
2008-09-26T00:00:00Z