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PubMed1990

Molecular dynamics simulations in biology.

Molecular dynamics--the science of simulating the motions of a system of particles--applied to biological macromolecules gives the fluctuations in the relative positions of the atoms in a protein or in DNA as a function of time. Knowledge of these motions provides insights into biological phenomena such as the role of flexibility in ligand binding and the rapid solvation of the electron transfer state in photosynthesis. Molecular dynamics is also being used to determine protein structures from NMR, to refine protein X-ray crystal structures faster from poorer starting models, and to calculate the free energy changes resulting from mutations in proteins.

Chemical Phenomena↗
PubMed1998

Ab initio modeling and molecular dynamics simulation of the alpha 1b-adrenergic receptor activation.

This work describes the ab initio procedure employed to build an activation model for the alpha 1b-adrenergic receptor (alpha 1b-AR). The first version of the model was progressively modified and complicated by means of a many-step iterative procedure characterized by the employment of experimental validations of the model in each upgrading step. A combined simulated (molecular dynamics) and experimental mutagenesis approach was used to determine the structural and dynamic features characterizing the inactive and active states of alpha 1b-AR. The latest version of the model has been successfully challenged with respect to its ability to interpret and predict the functional properties of a large number of mutants. The iterative approach employed to describe alpha 1b-AR activation in terms of molecular structure and dynamics allows further complications of the model to allow prediction and interpretation of an ever-increasing number of experimental data.

Amino Acid Sequence↗
PubMed1992

Application of restrained minimization, simulated annealing and molecular dynamics simulations for the conformational analysis of oligosaccharides.

The purpose of the present study was to determine the confidence with which the small number of 1H NMR nuclear Overhauser effect (NOE) distance constraints measurable across glycosidic linkages in oligosaccharides could be used for solution conformational analysis. This was assessed by use of these constraints in restrained molecular mechanical minimization of the tetrasaccharide Gal beta 1----4(Fuc alpha 1----3)Glc-NAc beta 1----3Gal, a model compound of the Lewis-X antigenic determinant. This presents a particularly severe test case in view of extreme resonance overlap and a dearth of inter-residue distance constraints. It is concluded that these constraints, when used in conventional restrained minimization, result in the generation of 'virtual conformations' and local minima about glycosidic linkages. However, these restraints are nevertheless found to be useful in the initial stages of a conformational analysis strategy involving restrained minimization combined with dynamical simulated annealing to define more accurately the global minimum energy configuration, together with molecular dynamics simulation to explore conformational mobility about this minimum. Theoretical ROE values calculated over the time course of the MD simulation, using a formalism appropriate for the time scale of the internal motion, are compared with those obtained experimentally in the oligosaccharide.

Carbohydrate Conformation↗
PubMed2003

A recent development in computational chemistry: chemical reactions from first principles molecular dynamics simulations.

First-principles molecular dynamics simulations have recently been found an effective tool to study a large variety of chemical problems. Finite temperature simulations reveal unique information, including explicit dynamical effects and the evaluation of proper free energy differences. Moreover, dynamics simulations reveal information on the flexibility of molecular systems, and elucidate, often otherwise inaccessible, mechanistic details of chemical reactions. In addition this methodology allows the study of larger, periodic, systems, revealing computationally unique information which may be directly compared to experiments on realistic chemical systems. A variety of examples will be given, although most focus on the important field of catalysis.

Biochemistry↗
PubMed1998

Locally accessible conformations of proteins: multiple molecular dynamics simulations of crambin.

Multiple molecular dynamics (MD) simulations of crambin with different initial atomic velocities are used to sample conformations in the vicinity of the native structure. Individual trajectories of length up to 5 ns sample only a fraction of the conformational distribution generated by ten independent 120 ps trajectories at 300 K. The backbone atom conformational space distribution is analyzed using principal components analysis (PCA). Four different major conformational regions are found. In general, a trajectory samples only one region and few transitions between the regions are observed. Consequently, the averages of structural and dynamic properties over the ten trajectories differ significantly from those obtained from individual trajectories. The nature of the conformational sampling has important consequences for the utilization of MD simulations for a wide range of problems, such as comparisons with X-ray or NMR data. The overall average structure is significantly closer to the X-ray structure than any of the individual trajectory average structures. The high frequency (less than 10 ps) atomic fluctuations from the ten trajectories tend to be similar, but the lower frequency (100 ps) motions are different. To improve conformational sampling in molecular dynamics simulations of proteins, as in nucleic acids, multiple trajectories with different initial conditions should be used rather than a single long trajectory.

Computer Simulation↗
PubMed2001

Investigation of the mechanism of domain closure in citrate synthase by molecular dynamics simulation.

Six, 2 ns molecular dynamics simulations have been performed on the homodimeric enzyme citrate synthase. In three, both monomers were started from the open, unliganded X-ray conformation. In the remaining three, both monomers started from a closed, liganded X-ray conformation, with the ligands removed. Projecting the motion from the simulations onto the experimental domain motion revealed that the free-energy profile is rather flat around the open conformation, with steep sides. The most closed conformations correspond to hinge-bending angles of 12-14 compared to the 20 degrees that occurs upon the binding of oxaloacetate. It is also found that the open, unliganded X-ray conformation is situated at the edge of the steep rise in free energy, although conformations that are about 5 degrees more open were sampled. A rigid-body essential dynamics analysis of the combined open trajectories has shown that domain motions in the direction of the closed X-ray conformation are compatible with the natural domain motion of the unliganded protein, which has just two main degrees of freedom. The simulations starting from the closed conformation suggest a free-energy profile with a small barrier in going from the closed to open conformation. A combined essential dynamics and hinge-bending analysis of a trajectory that spontaneously converts from the closed to open state shows an almost exact correspondence to the experimental transition that occurs upon ligand binding. The simulations support the conclusion from an earlier analysis of the experimental transition that the beta-hairpin acts as a mechanical hinge by attaching the small domain to the large domain through a conserved main-chain hydrogen bond and salt-bridges, and allowing rotation to occur via its two flexible termini. The results point to a mechanism of domain closure in citrate synthase that has analogy to the process of closing a door.

Citrate (si)-Synthase↗
PubMed1999

Mouse acetylcholinesterase unliganded and in complex with huperzine A: a comparison of molecular dynamics simulations.

A 1 ns molecular dynamics simulation of unliganded mouse acetylcholinesterase (AChE) is compared to a previous simulation of mouse AChE complexed with huperzine A (HupA). Several common features are observed. In both simulations, the active site gorge fluctuates in size during the 1 ns trajectory and is completely pinched off several times. Many of the residues in the gorge that formed hydrogen bonds with HupA in the simulation of the complex now form hydrogen bonds with other protein residues and water molecules in the gorge. The opening of a "backdoor" entrance to the active site that was found in the simulation of the complex is also observed in the unliganded simulation. Differences between the two simulations include overall lower structural rms deviations for residues in the gorge in the unliganded simulation, a smaller diameter of the gorge in the absence of HupA, and the disappearance of a side channel that was frequently present in the liganded simulation. The differences between the two simulations can be attributed, in part, to the interaction of AChE with HupA.

Acetylcholinesterase↗
PubMed1998

Non-native interactions in protein folding intermediates: molecular dynamics simulations of hen lysozyme.

Molecular dynamics simulations of protein denaturation can complement and extend experimental studies of protein folding by providing atomic-level structural information about conformational transitions and any conformational states along the unfolding pathway. Previous unfolding simulations of hen egg-white lysozyme have resulted in intermediate structures with an unfolded alpha-domain and a structured beta-domain, which is inconsistent with experiment. In contrast, the beta-domain unfolded first in the two simulations presented here leaving a structured alpha-domain. Following this, intermediate states were identified that differ with respect to the packing of the helices and the elements of non-native structure adopted. The non-native structure is critical for explaining many of the experimental observations. Overall, the pooled ensemble of these intermediates is in agreement with the experimental data for the major kinetic intermediate, suggesting that the kinetic intermediate may be made up of distinct, but rapidly interconverting, partially folded conformations distinguished primarily by differences in helix packing.

Amino Acid Sequence↗
PubMed2001

Induced fit DNA recognition by a minor groove binding analogue of Hoechst 33258: fluctuations in DNA A tract structure investigated by NMR and molecular dynamics simulations.

NMR analysis and molecular dynamics simulations of d(GGTAATTACC)(2) and its complex with a tetrahydropyrimidinium analogue of Hoechst 33258 suggest that DNA minor groove recognition in solution involves a combination of conformational selection and induced fit, rather than binding to a preorganised site. Analysis of structural fluctuations in the bound and unbound states suggests that the degree of induced fit observed is primarily a consequence of optimising van der Waals contacts with the walls of the minor groove resulting in groove narrowing through: (i) changes in base step parameters, including increased helical twist and propeller twist; (ii) changes to the sugar-phosphate backbone conformation to engulf the bound ligand; (iii) suppression of bending modes at the TpA steps. In contrast, the geometrical arrangement of hydrogen bond acceptors on the groove floor appears to be relatively insensitive to DNA conformation (helical twist and propeller twist). We suggest that effective recognition of DNA sequences (in this case an A tract structure) appears to depend to a significant extent on the sequence being flexible enough to be able to adopt the geometrically optimal conformation compatible with the various binding interactions, rather than involving 'lock and key' recognition.

Base Sequence↗
PubMed1999

Structure, interaction, dynamics and solvent effects on the DNA-EcoRI complex in aqueous solution from molecular dynamics simulation.

A 0.7-ns molecular dynamics simulation of the DNA-EcoRI complex in a 7.0-A solvent shell indicated a stable behavior of the system. No significant evaporation or smearing of the solvent's outer boundary occurred. The structure and the intermolecular interactions were found to be well maintained during the simulation. The interaction pattern in the simulation was found to be very similar to that in the crystal structure. Most of the specific interactions between the DNA and the protein were found to be enhanced in the simulation compared to that in the crystal structure as a result of improved interaction geometry. The nonspecific interactions were found to be stronger than the specific ones. The specific interactions between the N7 atoms of Gua(4) or Ade(5) or Ade(6) and the protein were found to be present over almost the entire time of the simulation, whereas hydrogen bonds involving the amino groups of the Ade(5) and Ade(6) with the protein were found to be relatively weaker, with lower probability and shorter lifetime. The time evolution of the root mean square deviations of the DNA and the protein were highly correlated even at the later part of the simulation, showing the tight binding between them. Several long-lived water bridges were found between the DNA backbone atoms and the protein and also between the two protein monomers, which increased the overall stability of the complex. The two protein monomers were found to interact strongly with each other. The energy of the DNA kink deformation was estimated as approximately 31 kcal/mol.

Binding Sites↗
PubMed1992

Characterization of "native" apomyoglobin by molecular dynamics simulation.

We have used molecular dynamics simulation methods to study the structure and fluctuations of "native" apomyoglobin in aqueous solution for a period of greater than 0.5 nanosecond. This work was motivated by the recent attempts of Hughson et al. to characterize the structure and motion of both this molecule and the less compact, acid stabilized I stage, using methods of pulsed H/2H exchange. The study of these systems provides new insights into protein folding intermediates and our simulation has yielded a detailed model for structure and fluctuations in apomyoglobin which complements the experimental studies. We find that local (short-time) fluctuations agree well with fluctuations observed for the holoprotein in aqueous solution, as well as results from the crystallographic B-factors. In addition, the structural features we observe for native apomyoglobin are very similar to the holoprotein, in basic agreement with the findings of Hughson et al. By examining larger-scale motions, developing only over timescales in excess of a 100 picoseconds, we are able to identify conformationally "labile" and "non-labile" regions within native apomyoglobin. These regions correspond extremely well to those identified in the nuclear magnetic resonance experiments as unstable and stable "folding subdomains" in the I state of apomyoglobin. Overall we find that helices A, B, E, G and H show the least amount of motion and helices C, D and F move substantially over the timescales examined. The major motions, and the primary difference between the holo and apo structures as we have observed them, are due to the shifting motion of helices C, D and F into the vacant heme cavity. We also find that motions at the interface of helical segments can be large, with one important exception being the chain segment connecting helices G and H. This segment of chain interacts with the conformationally "non-labile" helix A to form a relatively rigid subdomain composed of helices A, G and H. We believe that these findings provide direct support for the suggestion of Hughson et al. that helices A, G and H constitute a compact subdomain that remains in a native-like conformation as the protein begins to unfold in environments of decreasing pH.

Apoproteins↗
PubMed2000

Transitions from alpha to pi helix observed in molecular dynamics simulations of synthetic peptides.

Molecular dynamics simulations were carried out for three 13-residue peptides of the form AcNH-A-A-E-X-A-E-A-H-A-A-E-K-A-CONH(2) with X = A, F, and W. All three peptides exhibited unexpected dynamical behavior, undergoing a transition from an alpha-helical to a pi-helical structure in the course of 5-ns trajectories in aqueous solution. Analysis of peptide length, accessible surface, interaction energies, hydrogen bonding, and dihedral angles was consistent with alpha --> pi transitions at 2800, 500, and 800 ps for X = A, F and W, respectively. The transitions occurred sequentially and cooperatively, propagating from the C- to the N-terminus for X = A and W and from the center toward both termini for X = F. The time scale of the overall transition ranged from 300 to 500 ps. For all three peptides the backbone structural transition was accompanied by a concerted rearrangement of the charged side chains, including a 3 A increase in the distance between carboxylate groups of Glu-3 and Glu-6. During the transition the peptide backbone hydrogen-bonding patterns were disrupted at the interface between the alpha-helical and nascent pi-helical regions, with peptide groups forming water-bridged hydrogen bonds. The peptide structures exhibited significant fluidity, with individual residues sampling alpha-, pi-, and 3(10)-helical conformations, as well as a "coil" state, without any intramolecular hydrogen bonds. The studied peptides have been designed to form alpha-helices when incorporated in novel hemoprotein model compounds, peptide-sandwiched mesohemes, which consist of two identical peptides covalently attached to an Fe(III) mesoporphyrin [Liu, D., Williamson, D. A., Kennedy, M. L., Williams, T. D., Morton, M. M., and Benson, D. R. (1999) J. Am. Chem. Soc. 121, 11798-11812]. The possibility of adopting pi-helical structures by the constituent peptides may influence the properties of the hemoprotein models.

Computer Simulation↗
PubMed2002

Structure and dynamics of liquid water with different long-range interaction truncation and temperature control methods in molecular dynamics simulations.

We have used molecular dynamics simulations to study the physical properties of modified TIP3P water model included in the CHARMM program, using four different methods-the Ewald summation technique, and three different spherical truncation methods-for the treatment of the long-range interactions. Both the structure and dynamics of the liquid water model were affected by the methods used to truncate the long-range interactions. For some of the methods artificial structuring of the model liquid was observed around the cutoff radius. The model liquid properties were also affected by the commonly applied temperature control methods. Four different methods for controlling the temperature of the system were studied, and the effects of these methods on the bulk properties for liquid water were analyzed. The system size was also found to change the dynamics of the model liquid water. Two control simulations with the SPC/E water model were carried out. The self-diffusion coefficient (D), the radial distribution function (g(OO)), the distance dependent Kirkwood G-factor [G(k)(r)] and the intermolecular potential energy (E(pot)) were determined from the different trajectories and compared with the experimental data.

Journal Article↗
PubMed1993

Dynamical properties of bovine pancreatic trypsin inhibitor from a molecular dynamics simulation at 5000 atm.

Molecular dynamics simulations of bovine pancreatic trypsin inhibitor in water have been performed with coupling to pressure baths at 1 atm and at 5000 atm. The positional fluctuations of atoms in the alpha- and gamma-positions are slightly decreased at 5000 atm. The mobility of the backbone phi- and psi-angles is not affected with respect to the root mean square fluctuations and the rate of torsional angle transitions. The amplitude of libration of sidechain chi-angles remains nearly the same for both pressures, but the rate of torsional angle transitions decreases on average by 30% when increasing the hydrostatic pressure to 5000 atm.

Amino Acid Sequence↗
PubMed1995

Rigid-body motions of sub-units in DNA: a correlation analysis of a 200 ps molecular dynamics simulation.

A 200 ps molecular dynamics simulation of the B-form double stranded self-complementary octanucleotide d(CTGATCAG) is analyzed in terms of correlated motions using the canonical analysis approach. Each nucleotide is decomposed in three sub-units corresponding to the base, the sugar ring and the backbone respectively. The correlation between the full dynamics of two sub-units was found to decrease as their mutual distance increases. The interpretation of the full dynamics of sub-units as the superimposition of rigid-body motions (translation and orientation) and deformation shows that the main source of correlation is rigid-body motions. Correlation between sub-units deformation is weak and practically vanishes for sub-units belonging to non-adjacent nucleotides. It is also shown that the correlation is much more important for sub-units of the same strand than of opposite strands. We conclude that the internal dynamics of the octanucleotide may be well described by rigid-body motions, the sub-units deformation having only local influence whereas sub-units translation and rotation have repercussion to long distances. The results presented in this study suggest how the number of degrees of freedom may be reduced for simulating long-time dynamics of oligonucleotides.

Computer Simulation↗
PubMed2002

Measuring kinetic coefficients by molecular dynamics simulation of zone melting.

Molecular dynamics simulations are performed to measure the kinetic coefficient at the solid-liquid interface in pure gold. Results are obtained for the (111), (100), and (110) orientations. Both Au(100) and Au(110) are in reasonable agreement with the law proposed for collision-limited growth. For Au(111), stacking fault domains form, as first reported by Burke, Broughton, and Gilmer [J. Chem. Phys. 89, 1030 (1988)]. The consequence on the kinetics of this interface is dramatic: the measured kinetic coefficient is three times smaller than that predicted by collision-limited growth. Finally, crystallization and melting are found to be always asymmetrical and here again the effect is much more pronounced for the (111) orientation.

Journal Article↗
PubMed2002

Complex formation in systems of oppositely charged polyelectrolytes: a molecular dynamics simulation study.

Results of molecular dynamics simulations for systems with two flexible, oppositely charged polymer chains are presented. The lengths N and interaction strength lambda of the chains are varied. We find that the chains remain separated for small values of lambda. For large interaction strengths, i.e., large Bjerrum lengths, we find glasslike structures and order on the length scale of a few monomer diameters. Between these two limits of the interaction strengths, the chains of various lengths collapse into compact complexes that exhibit self-similar structures. The scaling behavior of the radius of gyration is discussed as a function of chain length and interaction strength. In addition, the local structure of the collapsed systems is analyzed and the dependence of the density of the aggregate on the interaction strength is discussed.

Journal Article↗
PubMed2003

Nonequilibrium molecular dynamics simulations of a bubble.

Molecular dynamics simulations are performed to investigate the microscopic dynamics of a bubble when liquids are locally heated. We successfully observe that the heated atoms scatter the neighboring nonheated atoms and make a bubble, and then the bubble is cooled and compressed by the surrounding liquids. The bubble dynamics in this process agrees with the results of the Rayleigh-Plesset equation which describes the dynamics of a bubble in terms of macroscopic hydrodynamics. In this way, we clarify that the hydrodynamic description is reliable even for a microscopic bubble.

Journal Article↗