Molecular dynamics (MD) simulations in explicit solvent allow studying receptor-ligand binding processes including full flexibility of the binding partners and an explicit inclusion of solvation effects. However, in MD simulations, the search for an optimal ligand-receptor complex geometry is frequently trapped in locally stable non-native binding geometries. A Hamiltonian replica-exchange (H-REMD)-based protocol has been designed to enhance the sampling of putative ligand-receptor complexes. It is based on softening nonbonded ligand-receptor interactions along the replicas and one reference replica under the control of the original force field. The efficiency of the method has been evaluated on two receptor-ligand systems and one protein-peptide complex. Starting from misplaced initial docking geometries, the H-REMD method reached in each case the known binding geometry significantly faster than a standard MD simulation. The approach could also be useful to identify and evaluate alternative binding geometries in a given binding region with small relative differences in binding free energy.
A detailed understanding of the drug-receptor association process is of fundamental importance for drug design. Due to the long time scales of typical binding kinetics, the atomistic simulation of the ligand traveling from bulk solution into the binding site is still computationally challenging. In this work, we apply a multiscale approach of combined Molecular Dynamics (MD) and Brownian Dynamics (BD) simulations to investigate association pathway ensembles for the two prominent H1N1 neuraminidase inhibitors oseltamivir and zanamivir. Including knowledge of the approximate binding site location allows for the selective confinement of detailed but expensive MD simulations and application of less demanding BD simulations for the diffusion controlled part of the association pathway. We evaluate a binding criterion based on the residence time of the inhibitor in the binding pocket and compare it to geometric criteria that require prior knowledge about the binding mechanism. The method ranks the association rates of both inhibitors in qualitative agreement with experiment and yields reasonable absolute values depending, however, on the reaction criteria. The simulated association pathway ensembles reveal that, first, ligands are oriented in the electrostatic field of the receptor. Subsequently, a salt bridge is formed between the inhibitor's carboxyl group and neuraminidase residue Arg368, followed by adopting the native binding mode. Unexpectedly, despite oseltamivir's higher overall association rate, the rate into the intermediate salt-bridge state was found to be higher for zanamivir. The present methodology is intrinsically parallelizable and, although computationally demanding, allows systematic binding rate calculation on selected sets of potential drug molecules.
Molecular dynamics (MD) and Monte Carlo (MC) simulations have emerged as a valuable tool to investigate statistical mechanics and kinetics of biomolecules and synthetic soft matter materials. However, major limitations for routine applications are due to the accuracy of the molecular mechanics force field and due to the maximum simulation time that can be achieved in current simulations studies. For improving the sampling a number of advanced sampling approaches have been designed in recent years. In particular, variants of the parallel tempering replica-exchange methodology are widely used in many simulation studies. Recent methodological advancements and a discussion of specific aims and advantages are given. This includes improved free energy simulation approaches and conformational search applications.
Limited proteolysis of RNase-A yields a short N-terminal S-peptide segment and the larger S-protein. Binding of S-peptide to S-protein results in the formation of an enzymatically active RNase-S protein. S-peptide undergoes a transition from intrinsic disorder to an ordered helical state upon association with S-protein to form RNase-S and is an excellent model system to study coupled folding and binding. To better understand the dynamics of the RNases-S complex and its isolated partners, comparative molecular dynamics simulations have been performed. In agreement with experiment, we find significant conformational fluctuations of the isolated S-peptide compatible with a disordered regime and only little residual helical structure. In the RNase-S complex, the N-terminal helix of S-peptide unfolds and refolds repeatedly on the microsecond timescale, indicating that the α-helical structure is only part of the equilibrium regime for these residues whereas the C-terminal residues are confined to the helical conformation that is found in the x-ray structure. This is also in line with systematic, in silico Alanine scanning free-energy simulations, which indicate that the major contribution to complex stability emerges from the C-terminal helical turn, consisting of residues 8-13 in S-peptide whereas the N-terminal S-peptide residues 1-7 make only minor contributions. Comparative simulations of S-protein in the presence and absence of S-peptide reveal that the isolated S-protein is significantly more flexible than in the complex, and undergoes a global pincerlike conformational change that narrows the S-peptide binding cleft. The narrowed binding cleft adds a barrier for complex formation likely influencing the binding kinetics. This conformational change is reversed by S-peptide association, which also stabilizes conformational fluctuations in S-protein. Such global motions associated with binding are also likely to play a role for other coupled peptide folding and binding processes at peptide binding regions on protein surfaces.
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