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Molecular dynamics simulations of the enzyme Cu, Zn superoxide dismutase.

The enzyme Cu, Zn superoxide dismutase (Cu,Zn-SOD) is a ubiquitous oxireductase, which is responsible for the cellular defense against oxidative stress caused by the high toxicity of the superoxide radical, and has been also linked to some cases of familiar amyotrophic lateral sclerosis. In the present study a set of molecular mechanics parameters for the active site of Cu,Zn-SOD has been derived. Afterward, an extensive molecular dynamics simulation has been carried out in an aqueous environment. The obtained results shed a further light on the structural flexibility of the backbone, where the active site is nested, and the solvation shell occupancy. The relatively small backbone deviation, shown by a root-mean-square deviation below 1.0 A, confirms the accuracy of the parameters. The solvent shell analysis has shown that the first solvation shell is located at about 5 A from the copper ion, generating an empty cavity with enough space to accommodate the superoxide radical. The low residence time means that a high permutation rate of water molecules in both solvation shells is consistent with the efficiency of this catalytic mechanism. Hybrid studies using ONIOM methodologies can now be done to evaluate the mechanistic implications of the explicit inclusion of the whole system.

Computer Simulation↗

Effect of pressure on the conformation of proteins. A molecular dynamics simulation of lysozyme.

The effect of pressure on the structure and mobility of lysozyme was studied by molecular dynamics computer simulation at 1 and 3 kbar (1 atm = 1.01325 bar = 101.325 kPa). The results have good agreement with the available experimental data, allowing the analysis of other features of the effect of pressure on the protein solution. The studies of mobility show that although the general mobility is restricted under pressure this is not true for some particular residues. From the analysis of secondary structure along the trajectories it is observed that the conformation under pressure is more stable, suggesting that pressure acts as a 'conformer selector' on the protein. The difference in solvent-accessed surface (SAS) with pressure shows a clear inversion of the hydrophilic/hydrophobic SAS ratio, which consequently shows that the hydrophobic interaction is considerably weaker under high hydrostatic pressure conditions.

Carbon↗

Improving the performance of molecular dynamics simulations on parallel clusters.

In this article a procedure is derived to obtain a performance gain for molecular dynamics (MD) simulations on existing parallel clusters. Parallel clusters use a wide array of interconnection technologies to connect multiple processors together, often at different speeds, such as multiple processor computers and networking. It is demonstrated how to configure existing programs for MD simulations to efficiently handle collective communication on parallel clusters with processor interconnections of different speeds.

Journal Article↗

Shear viscosity of molten alkali halides from equilibrium and nonequilibrium molecular-dynamics simulations.

The shear viscosity of molten NaCl and KCl was calculated through equilibrium (EMD) and nonequilibrium molecular-dynamics (NEMD) simulations in the canonical (N,V,T) ensemble. Two rigid-ion potentials were investigated, namely, the Born-Mayer-Huggins-Tosi-Fumi potential and the Michielsen-Woerlee-Graaf-Ketelaar potential with the parameters proposed by Ladd. The NEMD simulations were performed using the SLLOD equations of motion [D. J. Evans and G. P. Morriss, Phys. Rev. A 30, 1528 (1984)] with a Gaussian isokinetic thermostat and the results are compared with those obtained from Green-Kubo EMD (N,V,T) simulations and experimental shear viscosity data. The NEMD zero strain rate shear viscosity, eta(0), was obtained by fitting a simplified Carreau-type equation and by application of mode-coupling theory, i.e., a eta-gamma(1/2) linear relationship. The values obtained from the first method are found to be significantly lower than those predicted by the second. The agreement between the EMD and NEMD results with experimental data is satisfactory for the two potentials investigated. The ion-ion radial distribution functions obtained with the two rigid-ion potentials for both molten salts are discussed in terms of the differences between the two models.

Journal Article↗

Conformational analysis of furanoid epsilon-sugar amino acid containing cyclic peptides by NMR spectroscopy, molecular dynamics simulation, and X-ray crystallography: evidence for a novel turn structure.

Sugar amino acids (SAAs) are useful building blocks for the design of peptidomimetics and peptide scaffolds. The three-dimensional structures of cyclic hybrid molecules containing the furanoid epsilon-SAA III and several amino acids were elucidated to study the preferred conformation of such an epsilon-SAA and its conformational influence on the backbone of cyclic peptides. NMR-based molecular dynamics simulations and empirical calculations of the cyclic tetramer 1, consisting of two copies of the SAA residue and two amino acids, revealed that it is conformationally restrained. The two SAA residues adopt different conformations. One of them forms an unusual turn, stabilized by an intraresidue nine-member hydrogen bond. The methylene functionalities of the other SAA residue are positioned in such a way that an intraresidue H bond is not possible. The X-ray crystal structure of 1 strongly resembles the solution conformation. Molecular dynamics calculations in combination with NMR analysis were also performed for compounds 2 and 3, which contain the RGD (Arg-Gly-Asp) consensus sequence and were previously shown to inhibit alpha(IIb)beta(3)-receptor-mediated platelet aggregation. The biologically most active compound 2 adopts a preferred conformation with the single SAA residue folded into the nine-member H bond-containing turn. Compound 3, containing an additional valine residue, as compared with compound 2, is conformational flexible. Our studies demonstrate that the furanoid epsilon-SAA III is able to introduce an unusual intraresidue hydrogen bond-stabilized beta-turn-like conformation in two of the three cyclic structures.

Amino Acids↗

Kinking occurs during molecular dynamics simulations of small DNA minicircles.

Recent experiments on minicircle formation suggest that a conformational mechanism other than smooth deformation may be playing a role in enhancing DNA flexibility. Both local base unpairing and kink formation have been suggested as possible explanations. Although kinks within isolated DNA were proposed 30 years ago, they have, until now, only been observed within DNA complexed with proteins. In order to test how DNA behaves in the strong bending regime, we have carried out molecular dynamics simulations of a 94 base pair minicircle in explicit solvent with two different linking numbers, corresponding to a torsionally relaxed state and a positively supercoiled state. The simulations suggest that sharp kinks can indeed arise in small minicircles. The relaxed minicircle is generally associated with a single kink, while two kinks occur with the supercoiled state. No evidence is seen of base unpaired regions.

Base Composition↗

Conformational analysis of globomycin with a signal peptidase II inhibitory activity using molecular dynamics simulation.

Globomycin (1), a 19-membered cyclic depsipeptide, exhibited an antibiotic activity against gram-negative bacteria by inhibiting signal peptidase II in the cytoplasmic membrane. Although only one conformation of 1 was observed for the crystal structure, it was revealed by 1H NMR spectroscopic analysis that 1 exists as a mixture of two rotational isomers in solution (CDCl3 and CD3OD). A conformational analysis of 1 was, therefore, performed by high-temperature molecular dynamics simulation in combination with 1H NMR analysis to elucidate the conformations in solution. The relative ratio of the major and minor isomers present, which differs depending on the solvent, was then derived from their relative energy differences obtained in the conformational analysis. The difference in the relative ratios corresponded with that calculated from the 1H NMR analysis. Finally, the predicted conformations in solution were compared with that of the X-ray crystal structure to find local and global differences that characterize these conformations.

Aspartic Acid Endopeptidases↗

Molecular dynamics simulations of C2F6 effects on gramicidin A: implications of the mechanisms of general anesthesia.

It was recently postulated that the effects of general anesthetics on protein global dynamics might underlie a unitary molecular mechanism of general anesthesia. To verify that the specific dynamics effects caused by general anesthetics were not shared by nonanesthetic molecules, two parallel 8-ns all-atom molecular dynamics simulations were performed on a gramicidin A (gA) channel in a fully hydrated dimyristoylphosphatidylcholine membrane in the presence and absence of hexafluoroethane (HFE), which structurally resembles the potent anesthetic molecule halothane but produces no anesthesia. Similar to halothane, HFE had no measurable effects on the gA channel structure. In contrast to halothane, HFE produced no significant changes in the gA channel dynamics. The difference between halothane and HFE on channel dynamics can be attributed to their distinctly different distributions within the lipid bilayer and consequently to the different interactions of the anesthetic and the nonanesthetic molecules with the channel-anchoring tryptophan residues. The study further supports the notion that anesthetic-induced changes in protein global dynamics may play an important role in mediating anesthetic actions on proteins.

Anesthesia, General↗

Critical temperature T(c) and memory kernel in molecular-dynamics-simulated glass-forming Ni(0.2)Zr(0.8).

The mode-coupling theory (MCT) of dense liquids marks the dynamical glass transition by a critical temperature T(c) that is reflected in the temperature dependence of a number of physical quantities. Here, molecular-dynamics simulation data of a model adapted to Ni0.2Zr0.8 are analyzed to deduce T(c) from different quantities and to check the consistency of the estimated values. Analyzed are the critical temperature T(c) from (i). the nonvanishing nonergodicity parameters as asymptotic solutions of the MCT equations in the arrested state, (ii). the g(m) parameters describing the approach of the melt towards the arrested state on the ergodic side, (iii). the diffusion coefficients in the melt, and (iv). the alpha-relaxation time. The resulting T(c) values are found to agree within about 10%. In addition, the time dependent memory kernel is calculated from the MCT for the incoherent intermediate scattering function around T(c) and compared with the kernel obtained by inverting the molecular dynamics data for the corresponding correlator.

Journal Article↗

Orientation restraints in molecular dynamics simulations using time and ensemble averaging.

In this article we present methodology for simulating protein dynamics while imposing restraints derived from NMR measurements on partially ordered molecules. Such measurements may include residual dipolar couplings and chemical-shift anisotropies. We define a restraint potential for use in molecular dynamics and energy minimization. The presented potential is consistent with the simultaneously optimized molecular order tensor. Restraining can be performed with time and ensemble averaging. We performed a large number of molecular dynamics simulations of the histidine containing phosphocarrier protein with restraints on backbone N-H vector orientations derived from residual dipolar couplings. From these simulations it is evident that the use of time- or ensemble-averaged restraints is essential to leave the fluctuations of the restrained vectors unaffected. Without averaging the fluctuations of the restrained vectors are reduced significantly. This also has the effect of decreasing the apparent molecular order-parameter tensor.

Algorithms↗

Conformational analysis of a tetrasaccharide based on NMR spectroscopy and molecular dynamics simulations.

The conformational preference of the human milk oligosaccharide lacto-N-neotetraose, beta-d-Galp-(1 --> 4)-beta-d-GlcpNAc-(1 --> 3)-beta-d-Galp-(1 --> 4)-d-Glcp, has been analyzed using (1)H,(1)H T-ROESY and (1)H,(13)C trans-glycosidic J coupling experiments in isotropic solution and (1)H,(13)C residual dipolar couplings (RDCs) obtained in lyotropic liquid crystalline media. Molecular dynamics simulations of the tetrasaccharide with explicit water as the solvent revealed that two conformational states are significantly populated at the psi glycosidic torsion angle, defined by C(anomeric)-O-C-H, of the (1 --> 3)-linkage. Calculation of order parameters, related to the molecular shape, were based on the inertia tensor and fitting of experimental RDCs to different conformational states showed that psi(+) > 0 degrees is the major and psi(-) < 0 degrees is the minor conformation in solution, in complete agreement with a two-state analysis based on the T-ROESY data. Attention was also given to the effect of salt (200 mM NaCl) in the anisotropic medium, which was a ternary mixture of n-octyl-penta(ethylene glycol), n-octanol, and D(2)O.

Carbohydrate Sequence↗

Molecular basis for the Cu2+ binding-induced destabilization of beta2-microglobulin revealed by molecular dynamics simulation.

According to experimental data, binding of the Cu(2+) ions destabilizes the native state of beta2-microglobulin (beta2m). The partial unfolding of the protein was generally considered an early step toward fibril formation in dialysis-related amyloidosis. Recent NMR studies have suggested that the destabilization of the protein might be achieved through increased flexibility upon Cu(2+) binding. However, the molecular mechanism of destabilization due to Cu(2+), its role in amyloid formation, and the relative contributions of different potential copper-binding sites remain unclear. To elucidate the effect of ion ligation at atomic detail, a series of molecular dynamics simulations were carried out on apo- and Cu(2+)-beta2m systems in explicit aqueous solutions, with varying numbers of bound ions. Simulations at elevated temperatures (360 K) provide detailed pictures for the process of Cu(2+)-binding-induced destabilization of the native structure at the nanosecond timescale, which are in agreement with experiments. Conformational transitions toward partially unfolded states were observed in protein solutions containing bound copper ions at His-31 and His-51, which is marked by an increase in the protein vibrational entropy, with TDeltaS(vibr) ranging from 30 to 69 kcal/mol. The binding of Cu(2+) perturbs the secondary structure and the hydrogen bonding pattern disrupts the native hydrophobic contacts in the neighboring segments, which include the beta-strand D2 and part of the beta-strand E, B, and C and results in greater exposure of the D-E loop and the B-C loop to the water environment. Analysis of the MD trajectories suggests that the changes in the hydrophobic environment near the copper-binding sites lower the barrier of conformational transition and stabilize the more disordered conformation. The results also indicate that the binding of Cu(2+) at His-13 has little effect on the conformational stability, whereas the copper-binding site His-31, and to a lesser extent His-51, are primarily responsible for the observed changes in the protein conformation and dynamics.

Cations, Divalent↗

Steered molecular dynamics simulation of the Rieske subunit motion in the cytochrome bc(1) complex.

Crystallographic structures of the mitochondrial ubiquinol/cytochrome c oxidoreductase (cytochrome bc(1) complex) suggest that the mechanism of quinol oxidation by the bc(1) complex involves a substantial movement of the soluble head of the Rieske iron-sulfur protein (ISP) between reaction domains in cytochrome b and cytochrome c(1) subunits. In this paper we report the results of steered molecular dynamics simulations inducing, through an applied torque within 1 ns, a 56 degrees rotation of the soluble domain of ISP. For this purpose, a solvated structure of the bc(1) complex in a phospholipid bilayer (a total of 206,720 atoms) was constructed. A subset of 91,061 atoms was actually simulated with 45,131 moving atoms. Point charge distributions for the force field parametrization of heme groups and the Fe(2)S(2) cluster of the Rieske protein included in the simulated complex were determined. The simulations showed that rotation of the soluble domain of ISP is actually feasible. Several metastable conformations of the ISP during its rotation were identified and the interactions stabilizing the initial, final, and intermediate positions of the soluble head of the ISP domain were characterized. A pathway for proton conduction from the Q(o) site to the solvent via a water channel has been identified.

Animals↗

Molecular dynamics simulations of a pulmonary surfactant protein B peptide in a lipid monolayer.

Pulmonary surfactant is a complex mixture of lipids and proteins that lines the air/liquid interface of the alveolar hypophase and confers mechanical stability to the alveoli during the breathing process. The desire to formulate synthetic mixtures for low-cost prophylactic and therapeutic applications has motivated the study of the specific roles and interactions of the different components. All-atom molecular dynamics simulations were carried out on a model system composed of a monolayer of palmitic acid (PA) and a surfactant protein B peptide, SP-B(1-25). A detailed structural characterization as a function of the lipid monolayer specific area revealed that the peptide remains inserted in the monolayer up to values of specific area corresponding to an untilted condensed phase of the the pure palmitic acid monolayer. The system remains stable by altering the conformational order of both the anionic lipid monolayer and the peptide secondary structure. Two elements appear to be key for the constitution of this phase: an electrostatic interaction between the cationic peptide residues with the anionic headgroups, and an exclusion of the aromatic residues on the hydrophobic end of the peptide from the hydrophilic and aqueous regions.

Biomimetics↗

Investigation of possible structures of silicon nanotubes via density-functional tight-binding molecular dynamics simulations and ab initio calculations.

We show, computationally, that single-walled silicon nanotubes (SiNTs) can adopt a number of distorted tubular structures, representing respective local energy minima, depending on the theory used and the initial models adopted. In particular, "gearlike" structures containing alternating sp(3)-like and sp(2)-like silicon local configurations have been found to be the dominant structural form for SiNTs via density-functional tight-binding molecular dynamics simulations (followed by geometrical optimization using Hartree-Fock or density function theory) at moderate temperatures (below 100 K). The gearlike structures of SiNTs deviate considerably from, and are energetically more stable than, the smooth-walled tubes (the silicon analogues of single-walled carbon nanotubes). They are, however, energetically less favorable than the "string-bean-like" SiNT structures previously derived from semiempirical molecular orbital calculations. The energetics and the structures of gearlike SiNTs are shown to depend primarily on the diameter of the tube, irrespective of the type (zigzag, armchair, or chiral). In contrast, the energy gap is very sensitive to both the diameter and the type of the nanotube.

Journal Article↗

Molecular dynamics simulations of hydrophilic pores in lipid bilayers.

Hydrophilic pores are formed in peptide free lipid bilayers under mechanical stress. It has been proposed that the transport of ionic species across such membranes is largely determined by the existence of such meta-stable hydrophilic pores. To study the properties of these structures and understand the mechanism by which pore expansion leads to membrane rupture, a series of molecular dynamics simulations of a dipalmitoylphosphatidylcholine (DPPC) bilayer have been conducted. The system was simulated in two different states; first, as a bilayer containing a meta-stable pore and second, as an equilibrated bilayer without a pore. Surface tension in both cases was applied to study the formation and stability of hydrophilic pores inside the bilayers. It is observed that below a critical threshold tension of approximately 38 mN/m the pores are stabilized. The minimum radius at which a pore can be stabilized is 0.7 nm. Based on the critical threshold tension the line tension of the bilayer was estimated to be approximately 3 x 10(-11) N, in good agreement with experimental measurements. The flux of water molecules through these stabilized pores was analyzed, and the structure and size of the pores characterized. When the lateral pressure exceeds the threshold tension, the pores become unstable and start to expand causing the rupture of the membrane. In the simulations the mechanical threshold tension necessary to cause rupture of the membrane on a nanosecond timescale is much higher in the case of the equilibrated bilayers, as compared with membranes containing preexisting pores.

1,2-Dipalmitoylphosphatidylcholine↗

Interaction of the antimicrobial peptide cyclo(RRWWRF) with membranes by molecular dynamics simulations.

Antimicrobial peptides have gained a lot of interest in recent years due to their potential use as a new generation of antibiotics. It is believed that this type of relatively short, amphipathic, cationic peptide targets the bacterial membrane, and destroys the chemical gradients over the membrane via formation of stable or transient pores. Here we use the NMR structure of cyclo(RRWWRF) in a series of molecular dynamics simulations in membranes at various peptide/lipid ratios. We observe that the NMR structure of the peptide is still stable after 100 ns simulation. At a peptide/lipid ratio of 2:128, the membrane is only a little affected compared to a pure dipalmitoylphosphatidylcholine lipid membrane, but at a ratio of 12:128, the water-lipid interface becomes more fuzzy, the water molecules can reach deeper into the hydrophobic core, and the water penetration free-energy barrier changes. Moreover, we observe that the area per lipid decreases and the deuterium order parameters increase in the presence of the peptide. We suggest that the changes in the hydrophobic core, together with the changes in the headgroups, result in an imbalance of the membrane and that it is thus not an efficient hydrophobic barrier in the presence of the peptides, independent of pore formation.

1,2-Dipalmitoylphosphatidylcholine↗

The binding mode of progesterone to its receptor deduced from molecular dynamics simulations.

An unambiguous understanding of the binding mode of human progesterone to its receptor still eludes experimental search. According to the X-ray structure of the ligand-binding domain, only one (O3) of the two keto groups at the ligand ends (O3 and O20) should play a role. This result is in conflict with chemical intuition and the results of site-directed mutagenesis experiments. Herein, we report classical molecular dynamics simulations that reveal the dynamic nature of the binding in solution, elucidate the reasons why X-ray studies failed to determine the role of O20, and clarify the effects of the mutations. The predictive power of the force field is ensured by the consistent introduction of a first-principles representation of the ligand.

Binding Sites↗