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At least 55 records · Page 3Linked to original sources

MD simulations of anthrax edema factor: calmodulin complexes with mutations in the edema factor "switch a" region and docking of 3'-deoxy ATP into the adenylyl cyclase active site of wild-type and mutant edema factor variants.

Bacillus anthracis, a spore-forming infectious bacterium, produces an exotoxin, called the edema factor (EF), that functions in part by disrupting internal signalling pathways. When complexed with human host cell calmodulin (CaM), EF becomes an active adenylyl cyclase, producing the internal signal substance cyclic-AMP in an uncontrolled fashion. Recently, the crystal structures for uncomplexed EF and EF:CaM complexes in the presence and absence of a substrate analog (3'-deoxy-ATP), were reported. EF mutational studies have implicated a number of residues important in CaM binding and/or in the generation of the adenylyl cyclase active site, formed by the movements of the EF switch A, B and C regions upon CaM binding. Here we report on the results of molecular dynamics (MD) simulations on two EF:CaM complexes, one containing wild-type EF and the other containing EF in which a cluster of residues in the switch A region (L523, K525, Q526 and V529) have been mutated to alanine. The switch A mutations cause a large increase in the flexibility of the switch C region, the rupture of a number of EF-CaM interactions, an expansion of the carboxyl-terminal domain of CaM, and a change in the Ca(2+) ion binding abilities of the CaM that is in complex with EF. The results indicate the importance of the mutated switch A residues in maintaining a compact EF:CaM complex that appears to be a prerequisite for the generation of a fully-functional adenylyl cyclase active site. The effects of mutating key residues (K346, K353, H577, E588, D590 and N639) in the active site region of EF (to alanine) on the ability of EF to bind the 3'-deoxy-ATP substrate analog were also examined. Active-site residue substitutions at positions 583 (N583A) and 577 (H577A) were found to be particularly disruptive for the placement of the adenine ring moiety into the position found in the x-ray crystal structure of the ligand-protein complex.

Adenylyl Cyclases↗

Exploring the potential of complex formation between a mutant DNA and the wild type protein counterpart: a MM and MD simulation approach.

We have demonstrated that the methods of molecular modeling and molecular dynamics simulation might be used to assess whether a specific mutation in the DNA would destabilize a known DNA-protein complex. The approach is based on probing the changes in the interaction that would be induced into the complex if within the already formed wild type complex the mutation could be introduced. We have used Hoxc8-DNA complex as a test system where it is known that the Hoxc8 binding affinity of the DNA is completely lost upon mutation of the DNA by replacing TAAT stretch to GCCG. Mutation was obtained by changing the relevant base pairs into the DNA of the model of the corresponding wild type complex developed by homology modeling and MD simulation in water for 2.0 ns. Comparison of the structure, dynamics and interactions between the hypothetical mutant model with those of the similarly refined wild type model shows that the loss of affinity of the mutant DNA to Hoxc8 has two different origins: (i) loss of several strong H-bonds as the direct consequences of mutation and (ii) reduced H-bonds in the common parts due to a net loss or inferior H-bonding geometry induced by the mutation as indirect effects. The net change in the interaction energy between the DNA and the protein in the best possible configuration indicated the experimentally observed destabilization effects. No significant change in the groove width was observed and no correlation was found between the water-bridges and the loss of affinity.

Amino Acid Sequence↗

Structure and dynamics of the pore-lining helix of the nicotinic receptor: MD simulations in water, lipid bilayers, and transbilayer bundles.

Multiple nanosecond duration molecular dynamics simulations on the pore-lining M2 helix of the nicotinic acetylcholine receptor reveal how its structure and dynamics change as a function of environment. In water, the M2 helix partially unfolds to form a molecular hinge in the vicinity of a central Leu residue that has been implicated in the mechanism of ion channel gating. In a phospholipid bilayer, either as a single transmembrane helix, or as part of a pentameric helix bundle, the M2 helix shows less flexibility, but still exhibits a kink in the vicinity of the central Leu. The single M2 helix tilts relative to the bilayer normal by 12 degrees, in agreement with recent solid state NMR data (Opella et al., Nat Struct Biol 6:374-379, 1999). The pentameric helix bundle, a model for the pore domain of the nicotinic receptor and for channels formed by M2 peptides in a bilayer, is remarkably stable over a 2-ns MD simulation in a bilayer, provided one adjusts the pK(A)s of ionizable residues to their calculated values (when taking their environment into account) before starting the simulation. The resultant transbilayer pore shows fluctuations at either mouth which transiently close the channel. Proteins 2000;39:47-55.

Computer Simulation↗

High propeller twist and unusual hydrogen bonding patterns from the MD simulation of (dG)6.(dC)6.

A molecular dynamics (MD) study of (dG)6.(dC)6 including counter ions and 292 water molecules was made. The hydrogen bonding pattern and propeller twist angles for the mini-helix are reported as averages for times spanning 21-30, 31-40, 41-50, and 51-60 ps. The propeller twist angles range from 18 degrees to 38 degrees. Bifurcated and interstrand neighboring base (twisted) hydrogen bonding patterns were found.

Hydrogen Bonding↗

MD simulations of a 5-HT2A receptor model in DOPC membranes.

This work presents MD calculations on a model 5-HT2A G protein-coupled receptor embedded in DOPC membrane bilayers at different lipid:protein ratios. The primary purpose is to evaluate physical properties of the system to probe membrane dynamics and the solvation interactions. This showed several kinds of apparent cooperativity phenomena in distributions, lipid dynamics, and hydrogen bond interactions. The integral protein appears to cause a disordered condensation of the local lipid structure which does not extend far beyond the surface layer of lipids. This, and changes in the lipid-protein interaction profiles give a start toward understanding membrane-protein selectivity. The presence of a partially immobilized surface layer of lipids may generally slow down kinetics of solute-solute interactions in similar liquid-crystal membranes. A hydration algorithm was also applied to the GPCR model producing a detailed water structure in some of the internal cavities, including in the areas proposed for ligand binding. Other properties examined included the distributions of lipid groups, the membrane electrostatic potential, and some of the short-time protein dynamics.

Algorithms↗

An atomistic MD simulation and pair-distribution-function study of disorder and reactivity of alpha-AlF3 nanoparticles.

Cubic nanoparticles of alpha-AlF(3) containing 864 and 2048 atoms were investigated by using molecular dynamics simulations. Significant structural rearrangements of these particles occurred, primarily at the edges and corners of the particles, and 3 and 5 membered (Al-F-)(n) ring structures were observed in addition to the 4-membered rings seen in bulk alpha-AlF(3). These 3 and 5 membered ring structures are, however, present in other metastable forms of AlF(3), which are formed at low temperatures from high surface area precursors. The surfaces of the nanoparticles were very dynamic on the timescale of the MD run, Al-F bonds being continually broken and formed, resulting in the movement of the low coordinate Lewis acid Al sites on the surfaces of the particles. The Lewis acid sites, which represent the catalytically active sites for F/Cl exchange reactions, are largely present at the corners and edges of the particles. The particles show larger rhombohedral distortions than present in the bulk phase and do not undergo a rhombohedral to cubic phase transition at elevated temperatures. The results are compared with pair distribution function (PDF) analysis results from fluorinated gamma-Al(2)O(3), nanoparticles of AlF(3) prepared by plasma routes and alpha- and beta-AlF(3). Broad peaks between 3.3 and 4.5 A in the PDF plots of the fluorinated Al(2)O(3) and the nanoparticles indicate a distribution of Al-F distances arising from Al and F atoms in connected AlF(6) octahedra; this is consistent with the presence of ring structures other than those found in alpha-AlF(3).

Aluminum Compounds↗

Operator recognition by the phage 434 cI repressor: MD simulations of free and bound 50-bp DNA reveal important differences between the OR1 and OR2 sites.

Using molecular dynamics simulations in explicit solvent, we investigated the behavior of a 50-bp DNA sequence containing the 434 bacteriophage operators OR1 and OR2 separated by an 8-bp spacer. Two simulations of 1 ns each were carried out, with DNA alone and with DNA complexed to dimers of the R1-69 DNA binding domain of the phage 434 cI repressor protein at the OR1 and OR2 sites. Strong correlations among average structural parameters are observed between our simulations and available experimental data for the bound OR1/OR2 subsites. In the free state, some differences appear between the three relevant fragments (OR1, the spacer, and OR2). Unbound OR1 exhibits a large, shallow major groove into which the base atoms protrude and is also bent toward the major groove. This structure is maintained because structural fluctuations are weak. Unbound OR2 resembles canonical B-DNA although the structural parameters show greater fluctuations, essentially due to a malleable step (the innermost CpA/TpG), absent in OR1. Complexation with the proteins slightly alters the base positions but strongly modifies the sugar and backbone motions. The most crucial repressor effects are changes in the flexibility of the OR1/OR2 sites. Structural fluctuations are enhanced for OR1, conferring a favorable energetic contribution to the OR1 binding, whereas they are reduced for OR2. Therefore, both structural and dynamic properties of DNA suggest OR1 is the most attractive site for the repressor, which may explain the different binding association constants observed for the OR1 and OR2 sites. Finally, we also investigated the impact of the protein on the DNA backbone dynamics and find that direct or indirect interactions facilitate the DNA structural variations required for achieving complementarity with the protein.

Bacteriophage lambda↗

MD simulations of acyclic and macrocyclic Gd3+-based MRI contrast agents: influence of the internal mobility on water proton relaxivity.

Classical molecular dynamics simulations with a force field adapted to the family of Gd(3+) polyaminocarboxylate complexes have been successfully applied on two macrocyclic ([Gd(DOTA)(H(2)O)](-) and [Gd(DO3A)(H(2)O)(2)]) and two acyclic ([Gd(DTPA)(H(2)O)](2-) and [Gd(EGTA)(H(2)O)](-)) complexes in aqueous solution (DOTA=1,4,7,10-tetrakis(carboxymethyl)-1,4,7,10-tetraazacyclododecane, DO3A=1,4,6-tris(carboxymethyl)-1,4,7,10-tetraazacyclododecane, DTPA=1,1,4,7,7-pentakis(carboxymethyl)-1,4,7-triazaheptane, EGTA=1,1,10,10-tetrakis(carboxymethyl)-1,10-diaza-4,7-dioxadecane). In both macrocylic complexes the Gd(3+) coordination polyhedron remains close to a monocapped square antiprism (MSA) during the entire simulation time. For the stereolabile acyclic complexes different interconverting sets of geometries are observed: three sets close to tricapped trigonal prisms (TTP) for [Gd(EGTA)(H(2)O)](-) and three sets intermediate between MSA and TTP (distorted C(2v) symmetry) for [Gd(DTPA)(H(2)O)](2-). The fast conformational changes observed in the acyclic complexes might weaken the hydration of the second water shell and therefore disfavour the outer-sphere relaxivity. Moreover, the motions of the chelate observed in both acyclic complexes involve the reorientation of the symmetry elements over time. This reorientation, occurring on a picosecond timescale, can be associated with the correlation time for modulation of the zero field splitting and might participate in the electron spin relaxation mechanisms of the Gd(3+) ion. The internal motion of the inner-sphere water molecule can be quantified by the ratio tau(R)(GD-HW)/tau(R)(GD-OW) which increases slightly from 0.7 for the acyclic to 0.8 for the macrocyclic complexes. This increase for the macrocylic chelates is favourable for a higher relaxivity and can be related to their rigidity. The water exchange rate on the four complexes has been related to the steric constraint of the ligand on the inner-sphere water molecule(s), which is inversely proportional to a geometrical descriptor, the solid angle psi. A range of psi values is given (2<<psi<3.3) where the exchange should be optimal. The observations made on the picosecond timescale give general directions for the design of more efficient magnetic resonance imaging contrast agents.

Journal Article↗

Essential domain motions in barnase revealed by MD simulations.

The wealth of data accumulated on the bacterial ribonuclease barnase is complemented by molecular dynamics trajectories starting from four different experimental structures and covering a total of >10 ns. Using principal component analysis, the simulations are interpreted in view of dynamic domains and hinges promoting relative motions of these domains. Two domains with residues 7-22 and 52-108 for the first domain and residues 25-51 for the second domain were consistently observed. Hinge regions consist primarily of Tyr24, Ser50, Ile51, and Gly52. Earlier mutation studies have demonstrated that the residues of the hinge regions play essential roles for the stability and activity of barnase. The domain motions are correlated to inter-domain interactions involving functionally important active site residues, such as Lys27 and Glu73. A model is presented that combines the observation of dynamic domains and their motions with the extensive mutation data from the literature. Enthalpic energy contributions originating from specific inter-domain interactions as well as entropic energy contributions due to the domain motions are discussed in the frame of this model and compared with destabilization energies measured for corresponding mutants.

Bacterial Proteins↗

Specific DNA recognition by the Antp homeodomain: MD simulations of specific and nonspecific complexes.

Four molecular dynamics simulation trajectories of complexes between the wild-type or a mutant Antennapedia homeodomain and 2 DNA sequences were generated in order to probe the mechanisms governing the specificity of DNA recognition. The starting point was published affinity measurements showing that a single protein mutation combined with a replacement of 2 base pairs yields a new high-affinity complex, whereas the other combinations, with changes on only 1 macromolecule, exhibited lower affinity. The simulations of the 4 complexes yielded fluctuating networks of interaction. On average, these networks differ significantly, explaining the switch of affinity caused by the alterations in the macromolecules. The network of mostly hydrogen-bonding interactions involving several water molecules, which was suggested both by X-ray and NMR structures of the wild-type homeodomain and its DNA operator sequence, could be reproduced in the trajectory. More interestingly, the high-affinity complex with alterations in both the protein and the DNA yielded again a dynamic but very tight network of intermolecular interactions, however, attributing a significantly stronger role to direct hydrophobic interactions at the expense of water bridges. The other 2 homeodomain-DNA complexes, with only 1 molecule altered, show on average over the trajectories a clearly reduced number of protein-DNA interactions. The observations from these simulations suggest specific experiments and thus close the circle formed by biochemical, structural, and computational studies. The shift from a water-dominated to a more "dry" interface may prove important in the design of proteins binding DNA in a specific manner.

Antennapedia Homeodomain Protein↗

Conformation of N-terminal HIV-1 Tat (fragment 1-9) peptide by NMR and MD simulations.

The N-terminal portion of HIV-1 Tat covering residues 1-9 is a competitive inhibitor of dipeptidyl peptidase IV (DP IV). We have used 1H NMR techniques, coupled with molecular dynamics methods, to determine the conformation of this peptide in the three diverse media: DMSO-d6, water (pH 2.7) and 40% HFA solution. The results indicate that in both DMSO-d6 and HFA the peptide has a tendency to acquire a type I beta-turn around the segment Asp5-Pro6-Asn7-IIe8. The N-terminal end is seen to be as a random coil. In water, the structure is best described as a left-handed polyproline type II (PPII) helix for the mid segment region Asp2 to Pro6. The structures obtained in this study have been compared with an earlier report on Tat (1-9).

Acetone↗

Hierarchy of structure loss in MD simulations of src SH3 domain unfolding.

To complement experimental studies of the src SH3 domain folding, we studied 30 independent, high-temperature, molecular dynamics simulations of src SH3 domain unfolding. These trajectories were observed to differ widely from each other. Thus, rather than analyzing individual trajectories, we sought to identify the recurrent features of the high-temperature unfolding process. The conformations from all simulations were combined and then divided into groups based on the number of native contacts. Average occupancies of each side-chain hydrophobic contact and hydrogen bond in the protein were then determined. In the symmetric funnel limit, the occupancies of all contacts should decrease in concert with the loss in total number of native contacts. If there is a lack of symmetry or hierarchy to the unfolding process, the occupancies of some contacts should decrease more slowly, and others more rapidly. Despite the heterogeneity of the individual trajectories, the ensemble averaging revealed an order to the unfolding process: contacts between the N and C-terminal strands are the first to disappear, whereas contacts within the distal beta-hairpin and a hydrogen-bonding network involving the distal loop beta-turn and the diverging turn persist well after the majority of the native contacts are lost. This hierarchy of events resembles but is somewhat less pronounced than that observed in our experimental studies of the folding of src SH3 domain.

Computer Simulation↗

On using oscillating time-dependent restraints in MD simulation.

The use of time-dependent restraints in molecular simulation in order to generate a conformational ensemble for molecules that is in accordance with measured ensemble averages for particular observable quantities is investigated. Using a model system consisting of liquid butane and the cyclic peptide antamanide the reproduction of particular average (3) J-coupling constant values in a molecular dynamics simulation is analysed. It is shown that the multiple-valuedness and the sizeable gradients of the Karplus curve relating (3) J-coupling constants measured in NMR experiments to the corresponding torsional-angle values cause severe problems when trying to restrain a (3) J-coupling constant to a value close to the extrema of the Karplus curve. The introduction of a factor oscillating with time into the restraining penalty function alleviates this problem and enhances the restrained conformational sampling.

Algorithms↗

Mechanical unfolding of TNfn3: the unfolding pathway of a fnIII domain probed by protein engineering, AFM and MD simulation.

Protein engineering Phi-value analysis combined with single molecule atomic force microscopy (AFM) was used to probe the molecular basis for the mechanical stability of TNfn3, the third fibronectin type III domain from human tenascin. This approach has been adopted previously to solve the forced unfolding pathway of a titin immunoglobulin domain, TI I27. TNfn3 and TI I27 are members of different protein superfamilies and have no sequence identity but they have the same beta-sandwich structure consisting of two antiparallel beta-sheets. TNfn3, however, unfolds at significantly lower forces than TI I27. We compare the response of these proteins to mechanical force. Mutational analysis shows that, as is the case with TI I27, TNfn3 unfolds via a force-stabilised intermediate. The key event in forced unfolding in TI I27 is largely the breaking of hydrogen bonds and hydrophobic interactions between the A' and G-strands. The mechanical Phi-value analysis and molecular dynamics simulations reported here reveal that significantly more of the TNfn3 molecule contributes to its resistance to force. Both AFM experimental data and molecular dynamics simulations suggest that the rate-limiting step of TNfn3 forced unfolding reflects a transition from the extended early intermediate to an aligned intermediate state. As well as losses of interactions of the A and G-strands and associated loops there are rearrangements throughout the core. As was the case for TI I27, the forced unfolding pathway of TNfn3 is different from that observed in denaturant studies in the absence of force.

Computer Simulation↗

Exploring models of the influenza A M2 channel: MD simulations in a phospholipid bilayer.

The M2 protein of influenza A virus forms homotetrameric helix bundles, which function as proton-selective channels. The native form of the protein is 97 residues long, although peptides representing the transmembrane section display ion channel activity, which (like the native channel) is blocked by the antiviral drug amantadine. As a small ion channel, M2 may provide useful insights into more complex channel systems. Models of tetrameric bundles of helices containing either 18 or 22 residues have been simulated while embedded in a fully hydrated 1-palmitoyl-2-oleoyl-sn-glycerol-3-phosphatidylcholine bilayer. Several different starting models have been used. These suggest that the simulation results, at least on a nanosecond time scale, are sensitive to the exact starting structure. Electrostatics calculations carried out on a ring of four ionizable aspartate residues at the N-terminal mouth of the channel suggest that at any one time, only one will be in a charged state. Helix bundle models were mostly stable over the duration of the simulation, and their helices remained tilted relative to the bilayer normal. The M2 helix bundles form closed channels that undergo breathing motions, alternating between a tetramer and a dimer-of-dimers structure. Under these conditions either the channel forms a pocket of trapped waters or it contains a column of waters broken predominantly at the C-terminal mouth of the pore. These waters exhibit restricted motion in the pore and are effectively "frozen" in a way similar to those seen in previous simulations of a proton channel formed by a four-helix bundle of a synthetic leucine-serine peptide (, Biophys. J. 77:2400-2410).

Amino Acid Sequence↗

Myoglobin-CO conformational substate dynamics: 2D vibrational echoes and MD simulations.

Two-dimensional (2D) infrared vibrational echoes were performed on horse heart carbonmonoxymyoglobin (MbCO) in water over a range of temperatures. The A(1) and A(3) conformational substates of MbCO are found to have different dephasing rates with different temperature dependences. A frequency-frequency correlation function derived from molecular dynamics simulations on MbCO at 298 K is used to calculate the vibrational echo decay. The calculated decay shows substantial agreement with the experimentally measured decays. The 2D vibrational echo probes protein dynamics and provides an observable that can be used to test structural assignments for the MbCO conformational substates.

Animals↗

MD simulation of protein-ligand interaction: formation and dissociation of an insulin-phenol complex.

Complexes of proteins with small ligands are of utmost importance in biochemistry, and therefore equilibria, formation, and decay have been investigated extensively by means of biochemical and biophysical methods. Theoretical studies of the molecular dynamics of such systems in solution are restricted to 10 ns, i.e., to fast processes. Only recently new theoretical methods have been developed not to observe the process in real time, but to explore its pathway(s) through the energy landscape. From the profiles of free energy, equilibrium and kinetic quantities can be determined using transition-state theory. This study is dedicated to the pharmacologically relevant insulin-phenol complex. The distance of the center of mass chosen as a reaction coordinate allows a reasonable description over most of the pathway. The analysis is facilitated by analytical expressions we recently derived for distance-type reaction coordinates. Only the sudden onset of rotations at the very release of the ligand cannot be parameterized by a distance. They obviously require a particular treatment. Like a preliminary study on a peptide, the present case emphasizes the contribution of internal friction inside a protein, which can be computed from simulation data. The calculated equilibrium constant and the friction-corrected rates agree well with experimental data.

Binding Sites↗

Conformation of a model peptide of the tandem repeat decapeptide in mussel adhesive protein by NMR and MD simulations.

The conformation of a model peptide (Ala-Lys-Pro-Ser-Tyr-Hyp-Hyp-Thr-Tyr-Lys) of the tandem repeat decapeptide sequence of Mytilus edulis foot protein-1 (mefp-1) has been studied by 1H and 13C 2D-NMR in three diverse media-DMSO-d6, water (pH 3.5) and 40% hexafluoroacetone (HFA). Various NMR parameters that were used to deduce the secondary structure were chemical shift (1H and 13C) temperature coefficients of NH chemical shifts, 3J(NH alpha) coupling constants and the pattern of intra and inter-residue NOEs. Molecular dynamics simulations making integral use of the NMR data shows that the conformation of the peptide is conserved in all the three media. The structure in the three solvents is best defined as a left-handed polyproline II helix (PPII).

Amino Acid Sequence↗