Search PubMed⌕ Search

SEARCH · Search PubMed

Results for “Molecular Dynamic simulation”

Search indexed PubMed citations on genomics, clinical trials, systematic reviews and public health. Explore titles, authors and supplied subject terms, then open the PubMed record.

Quote a phrase for an exact phrase match. Source license links do not imply unrestricted reuse.

At least 973 records · Page 54Linked to original sources

Tyr-317 phosphorylation increases Shc structural rigidity and reduces coupling of domain motions remote from the phosphorylation site as revealed by molecular dynamics simulations.

Activated receptor tyrosine kinases bind the Shc adaptor protein through its N-terminal phosphotyrosine-binding (PTB) and C-terminal Src homology 2 (SH2) domains. After binding, Shc is phosphorylated within the central collagen-homology (CH) linker region on Tyr-317, a residue remote to both the PTB and SH2 domains. Shc phosphorylation plays a pivotal role in the initiation of mitogenic signaling through the Ras/Raf/MEK/ERK pathway, but it is unclear if Tyr-317 phosphorylation affects Shc-receptor interactions through the PTB and SH2 domains. To investigate the structural impact of Shc phosphorylation, molecular dynamics simulations were carried out using special-purpose Molecular Dynamics Machine-Grape computers. After a 1-nanosecond equilibration, atomic motions in the structures of unphosphorylated Shc and Shc phosphorylated on Tyr-317 were calculated during a 2-nanosecond period. The results reveal larger phosphotyrosine-binding domain fluctuations and more structural flexibility of unphosphorylated Shc compared with phosphorylated Shc. Collective motions between the PTB-SH2, PTB-CH, and CH-SH2 domains were highly correlated only in unphosphorylated Shc. Dramatic changes in domain coupling and structural rigidity, induced by Tyr-317 phosphorylation, may alter Shc function, bringing about marked differences in the association of unphosphorylated and phosphorylated Shc with its numerous partners, including activated membrane receptors.

Adaptor Proteins, Signal Transducing↗

Molecular dynamics simulation study of the negative correlation in antibody AZ28-catalyzed oxy-cope rearrangement.

The oxy-Cope rearrangement reaction in the antibody AZ28 is investigated using ab initio molecular orbital calculations and molecular mechanical molecular dynamics simulations. This antibody, AZ28, is known as one of the few systems where the mature catalytic antibody shows a negative correlation between the transition state analogue (TSA) binding affinity and the catalytic rate of the oxy-Cope rearrangement compared to the germ line catalytic antibody. The ab initio optimized structure shows that the transition state structure has a more planar configuration than the TSA. The favorable electrostatic interactions between AZ28 and the transition state analogue overcome the unfavorable van der Waals interactions; thus, AZ28 shows higher binding affinity for the TSA than the germ line. However, the AZ28 is not flexible enough to accept the relatively planar transition state structure. Because the lower flexibility causes poorer antibody-hapten interaction energies, the activation free energy of the oxy-Cope rearrangement becomes larger in the mature antibody than the germ line. We show that the differences in flexibility between the germ line and the mature form and the differences in structure between TSA and the transition state are the origin of the negative correlation in AZ28-catalyzed oxy-Cope rearrangement. The mutation of residue 34 of the light chain, 34(L), affects the binding free energies through the interresidue interaction because it is the closest to the hapten among the six mutatable residues. However, it does not affect the negative correlation.

Alanine↗

Molecular dynamics simulation of double proton transfer: adenine-thymine base pair.

Molecular dynamics of proton transfer was simulated from normal (N) to tautomeric (T) form of the base pair (bp) adenine-thymine (A-T). The results for the model system, consisting of one A-T base pair in SPC/E water, was analysed in terms of its hydration properties, difference on free energy, conformational changes, and magnetic properties. It is suggested that during proton transfer the base pair remains on the same conformational state. The free energy of the protons transfer appears to be almost insensitive to the presence of water. The overall hydrophobicity of the A-T pairs is slightly modified by the proton transfer the N form being a little more hydrophobic. The behavior of the magnetic shielding suggests that a current is produced in the ring of the hydrogen bonds due to strong pi -electron delocalization in the amide-amidine complex.

Adenine↗

Berry pseudorotation mechanism for the interpretation of the 19F NMR spectrum in PF5 by ab initio molecular dynamics simulations.

For the first time, theoretical evidence that confirms the importance of the Berry pseudorotation process in the interpretation of the 19F NMR spectrum of phosphorus pentafluoride (PF5) is presented. Ab initio molecular dynamics simulations have been performed to generate a large number of configurations used for NMR parameter computations at the density functional theory level. Two different temperatures were set to highlight the effect of pseudorotation process on the NMR spectrum. Average 19F chemical shifts and spin-spin coupling constants calculated for the five fluorine atoms converge towards the NMR equivalence of the five atoms when the Berry pseudorotation mechanism is accounted for.

Journal Article↗

Molecular-dynamics simulation of model polymer nanocomposite rheology and comparison with experiment.

The shear-rate dependence of viscosity is studied for model polymer melts containing various concentrations of spherical filler particles by molecular-dynamics simulations, and the results are compared with the experimental results for calcium-carbonate-filled polypropylene. Although there are some significant differences in scale between the simulated model polymer composite and the system used in the experiments, some important qualitative similarities in shear behavior are observed. The trends in the steady-state shear viscosities of the simulated polymer-filler system agree with those seen in the experimental results; shear viscosities, zero-shear viscosities, and the rate of shear thinning are all seen to increase with filler content in both the experimental and simulated systems. We observe a significant difference between the filler volume fraction dependence of the zero-shear viscosity of the simulated system and that of the experimental system that can be attributed to a large difference in the ratio of the filler particle radius to the radius of gyration of the polymer molecules. In the simulated system, the filler particles are so small that they only have a weak effect on the viscosity of the composite at low filler volume fraction, but in the experimental system, the viscosity of the composite increases rapidly with increasing filler volume fraction. Our results indicate that there exists a value of the ratio of the filler particle radius to the polymer radius of gyration such that the zero-shear-rate viscosity of the composite becomes approximately independent of the filler particle volume fraction.

Journal Article↗

Evidence of a double-lid movement in Pseudomonas aeruginosa lipase: insights from molecular dynamics simulations.

Pseudomonas aeruginosa lipase is a 29-kDa protein that, following the determination of its crystal structure, was postulated to have a lid that stretched between residues 125 and 148. In this paper, using molecular dynamics simulations, we propose that there exists, in addition to the above-mentioned lid, a novel second lid in this lipase. We further show that the second lid, covering residues 210-222, acts as a triggering lid for the movement of the first. We also investigate the role of hydrophobicity in the movement of the lids and show that two residues, Phe214 and Ala217, play important roles in lid movement. To our knowledge, this is the first time that a double-lid movement of the type described in our manuscript has been presented to the scientific community. This work also elucidates the interplay of hydrophobic interactions in the dynamics, and hence the function, of an enzyme.

Computer Simulation↗

Asymmetric structural motions of the homomeric alpha7 nicotinic receptor ligand binding domain revealed by molecular dynamics simulation.

A homology model of the ligand binding domain of the alpha7 nicotinic receptor is constructed based on the acetylcholine-binding protein crystal structure. This structure is refined in a 10 ns molecular dynamics simulation. The modeled structure proves fairly resilient, with no significant changes at the secondary or tertiary structural levels. The hypothesis that the acetylcholine-binding protein template is in the activated or desensitized state, and the absence of a bound agonist in the simulation suggests that the structure may also be relaxing from this state to the activatable state. Candidate motions that take place involve not only the side chains of residues lining the binding sites, but also the subunit positions that determine the overall shape of the receptor. In particular, two nonadjacent subunits move outward, whereas their partners counterclockwise to them move inward, leading to a marginally wider interface between themselves and an overall asymmetric structure. This in turn affects the binding sites, producing two that are more open and characterized by distinct side-chain conformations of W54 and L118, although motions of the side chains of all residues in every binding site still contribute to a reduction in binding site size, especially the outward motion of W148, which hinders acetylcholine binding. The Cys loop at the membrane interface also displays some flexibility. Although the short simulation timescale is unlikely to sample adequately all the conformational states, the pattern of observed motions suggests how ligand binding may correlate with larger-scale subunit motions that would connect with the transmembrane region that controls the passage of ions. Furthermore, the shape of the asymmetry with binding sites of differing affinity for acetylcholine, characteristic of other nicotinic receptors, may be a natural property of the relaxed, activatable state of alpha7.

Acetylcholine↗

Role of hydrogen bonds in the fast dynamics of binary glasses of trehalose and glycerol: a molecular dynamics simulation study.

Trehalose-glycerol mixtures are known to be effective in the long time preservation of proteins. However, the microscopic mechanism of their effective preservation abilities remains unclear. In this article we present a molecular dynamics simulation study of the short time, less than 1 ns, dynamics of four trehalose-glycerol mixtures at temperatures below the glass transition temperature. We found that a mixture of 5% glycerol and 95% trehalose has the most suppressed short time dynamics (fast dynamics). This result agrees with the experimental analysis of the mean-square displacement of the hydrogen atoms, as measured via neutron scattering, and correlates with the experimentally observed enhancement of the stability of some enzymes at this particular concentration. Our microscopic analysis suggests that the formation of a robust intermolecular hydrogen bonding network is most effective at this concentration and is the main mechanism for the suppression of the fast dynamics.

Binding Sites↗

Surface binding of alamethicin stabilizes its helical structure: molecular dynamics simulations.

Alamethicin is an amphipathic alpha-helical peptide that forms ion channels. An early event in channel formation is believed to be the binding of alamethicin to the surface of a lipid bilayer. Molecular dynamics simulations are used to compare the structural and dynamic properties of alamethicin in water and alamethicin bound to the surface of a phosphatidylcholine bilayer. The bilayer surface simulation corresponded to a loosely bound alamethicin molecule that interacted with lipid headgroups but did not penetrate the hydrophobic core of the bilayer. Both simulations started with the peptide molecule in an alpha-helical conformation and lasted 2 ns. In water, the helix started to unfold after approximately 300 ps and by the end of the simulation only the N-terminal region of the peptide remained alpha-helical and the molecule had collapsed into a more compact form. At the surface of the bilayer, loss of helicity was restricted to the C-terminal third of the molecule and the rod-shaped structure of the peptide was retained. In the surface simulation about 10% of the peptide/water H-bonds were replaced by peptide/lipid H-bonds. These simulations suggest that some degree of stabilization of an amphipathic alpha-helix occurs at a bilayer surface even without interactions between hydrophobic side chains and the acyl chain core of the bilayer.

Alamethicin↗

Molecular dynamics simulation of protein denaturation: solvation of the hydrophobic cores and secondary structure of barnase.

The transition in barnase from the native state to a compact globule has been studied with high-temperature molecular dynamics simulations. A partial destruction of the alpha-helices and the outer strands of the beta-sheet is observed with water molecules replacing the hydrogen bonds of the secondary structural elements. Simultaneously, the main alpha-helix moves away from the beta-sheet and exposes the principal hydrophobic core, many of whose nonpolar side chains, beginning with the ones near the surface, become solvated by hydrogen-bonded water molecules. This step involves a significant increase in the solvent-exposed surface area; the resulting loss of stability due to the hydrophobic effect may be the major source of the activation barrier in the unfolding reaction. The detailed mechanism described here for the first stage of the denaturation of barnase, including the essential role of water molecules, is likely to be representative of protein denaturation, in general.

Bacillus↗

TRAJELIX: a computational tool for the geometric characterization of protein helices during molecular dynamics simulations.

We have developed a computer program with the necessary mathematical formalism for the geometric characterization of distorted conformations of alpha-helices proteins, such as those that can potentially be sampled during typical molecular dynamics simulations. This formalism has been incorporated into TRAJELIX, a new module within the SIMULAID framework (http://inka.mssm.edu/~mezei/simulaid/) that is capable of monitoring distortions of alpha-helices in terms of their displacement, global and local tilting, rotation around their axes, compression/extension, winding/unwinding, and bending. Accurate evaluation of these global and local structural properties of the helix can help study possible intramolecular and intermolecular changes in the helix packing of alpha-helical membrane proteins, as shown here in an application to the interacting helical domains of rhodopsin dimers. Quantification of the dynamic structural behavior of alpha-helical membrane proteins is critical for our understanding of signal transduction, and may enable structure-based design of more specific and efficient drugs.

Algorithms↗

Ricin A-chain structural determinant for binding substrate analogues: a molecular dynamics simulation analysis.

Ricin A-chain is a cytotoxic protein that attacks ribosomes by hydrolyzing a specific adenine base from a highly conserved, single-stranded rRNA hairpin containing the tetraloop sequence GAGA. Molecular-dynamics simulation methods are used to analyze the structural determinant for three substrate analogues bound to the ricin A-chain molecule. Simulations were applied to the binding of the dinucleotide adenyl-3',5'-guanosine employing the x-ray crystal structure of the ricin complex and a modeled CGAGAG hexanucleotide loop taken from the NMR solution structure of a 29-mer oligonucleotide hairpin. A third simulation model is also presented describing a conformational search of the docked 29-mer structure by using a simulated-annealing method. Analysis of the structural interaction energies for each model shows the overall binding dominated by nonspecific interactions, which are mediated by specific arginine contracts from the highly basic region on the protein surface. The tetraloop conformation of the 29-mer was found to make specific interactions with conserved protein residues, in a manner that favored the GAGA sequence. A comparison of the two docked loop conformations with the NMR structure revealed significant positional deviations, suggesting that ricin may use an induced fit mechanism to recognize and bind the rRNA substrate. The conserved Tyr-80 may play an important conformational entropic role in the binding and release of the target adenine in the active site.

Binding Sites↗

Molecular dynamics simulations of human carbonic anhydrase II: insight into experimental results and the role of solvation.

In this paper, the carbonic anhydrase II (CA II) enzyme active site is modeled using ab initio calculations and molecular dynamics simulations to examine a number of important issues for the enzyme function. It is found that the Zn2+ ion is dominantly tetrahedrally coordinated, which agrees with X-ray crystallographic studies. However, a transient five-fold coordination with an extra water molecule is also found. Studies of His64 conformations upon a change in the protonation states of the Zn-bound water and the His64 residue also confirm the results of an X-ray study which suggest that the His64 conformation is quite flexible. However, the degree of water solvation is found to affect this behavior. Water bridge formation between the Zn-bound water and the His64 residue was found to involve a free energy barrier of 2-3 kcal/mol and an average lifetime of several picoseconds, which supports the concept of a proton transfer mechanism through such a bridge. Mutations of various residues around the active site provide further insight into the corresponding experimental results and, in fact, suggest an important role for the solvent water molecules in the CA II catalytic mechanism.

Carbonic Anhydrases↗

Fast lipid disorientation at the onset of membrane fusion revealed by molecular dynamics simulations.

Membrane fusion is a key event in vesicular trafficking in every cell, and many fusion-related proteins have been identified. However, how the actual fusion event occurs has not been elucidated. By using molecular dynamics simulations we found that when even a small region of two membranes is closely apposed such that only a limited number of water molecules remain in the apposed area (e.g., by a fusogenic protein and thermal membrane fluctuations), dramatic lipid disorientation results within 100 ps-2 ns, which might initiate membrane fusion. Up to 12% of phospholipid molecules in the apposing layers had their alkyl chains outside the hydrophobic region, lying almost parallel to the membrane surface or protruding out of the bilayer by 2 ns after two membranes were closely apposed.

Cell Membrane↗

Molecular dynamics simulation of continuous current flow through a model biological membrane channel.

The conductance of sodium ions through a simplified channel-membrane system immersed in a reservoir of 1M NaCl in SPC/E water is examined by molecular dynamics simulation. An applied external potential of 1.1 V drives the ions and water through a channel of length 25 A producing a current of 19.6 pA, in reasonable agreement with experimental findings. The stream of ions and water molecules flows continuously because of the constant applied field and periodic boundary conditions. We also examine the potential profile across the simulation cell, the average density distributions of the various species in the reservoir and radially in the channel, and the ion velocity in the channel.

Biophysical Phenomena↗

Molecular dynamics simulations of asialoglycoprotein receptor ligands.

Several recent studies have implicated carbohydrates in cell adhesion, inflammation, clearance of glycoproteins from blood circulation, embryonic development, and metastasis among others. Understanding the conformation of these carbohydrate recognition elements and their interaction at the molecular level is essential for the design of oligosaccharide inhibitors/drugs. Given the difficulty in solving carbohydrate structures by X-ray crystallography and since NMR experiments give only time-averaged conformation, molecular dynamics simulations are well suited to determine all the accessible conformations of oligosaccharides. Present communication reports the simulation of some of the oligosaccharide ligands of asialoglycoprotein receptor for 1 ns using Biosym's Insight II molecular modeling package on NCI-FCRDC's Y-MP 8D/8128 supercomputer. Results obtained from these simulations, in addition to explaining the observed differences in the binding affinities of these ligands to the asialoglycoprotein receptor, have led to a modified model for the recognition of the oligosaccharides by the receptor. Accordingly, only the two terminal galactose residues on the 1,3-arm of the triantennary oligosaccharide (GlcNAc2Man3 core of the N-linked oligosaccharides with N-acetyllactosamine in beta 1,2- and beta 1,4-linkages on the 1,3-linked core mannose) are primarily required for recognition, and the terminal galactose on the 1,6-arm (N-acetyllactosamine in beta 1,2-linkage on the 1,6-linked core mannose) provides additional binding energy. It has been shown that the oligosaccharides studied here have significant flexibility and the flexibility is more around the 1,3-linkage than the 1,6-linkage. The need for simulation for longer periods and with multiple initial conformations is also discussed in the present report.

Asialoglycoprotein Receptor↗

Nonequilibrium Molecular Dynamics Simulations of Steady-State Heat and Mass Transport in Condensation.

We present evidence for the hypothesis of local equilibrium for a liquid-vapor interface in a one-component fluid, using molecular dynamics simulations. Lennard-Jones/spline particles are studied in a two-phase system that is out of global equilibrium. Equilibrium simulations are first used to establish the equation of state for the vapor and interface. A procedure is developed to define the boundaries of the interface. Finally it is shown that the equation of state for the interface applies also when there is heat and mass transport through the interface. The temperature gradient in the vapor was 10(8) K/m in these studies. Copyright 2000 Academic Press.

Journal Article↗

Analysis of active site motions from a 175 picosecond molecular dynamics simulation of camphor-bound cytochrome P450cam.

The structure and internal motions of the active site residues of camphor-bound cytochrome P450cam have been evaluated on the basis of a 175 psec molecular dynamics simulation. The active site residues generally show very small deviations away from their starting crystal positions. These residues also generally show much smaller fluctuations than for the enzyme as a whole. Phe 87 is dynamically very unusual and is suggested to play a role in substrate movement into and/or out of the active site. The average distance between the heme iron and atoms C5, C6, and C3 of camphor is 5.3, 6.0, and 7.0 A, respectively. This trend is consistent with the experimentally observed stereospecificity of the hydroxylation reaction. On the basis of distance and angle criteria, both 5-exo and 5-endo hydrogen abstraction are predicted to occur during the hydroxylation reaction; although the 5-exo pathway is expected to be 3-fold more likely.

Binding Sites↗