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 1,333 records · Page 74Linked to original sources
PubMed2001

Spectroscopic and molecular dynamics simulation studies of the interaction of insulin with glucose.

The interaction between monomeric insulin and monosaccharides has been investigated through circular dichroism, fluorescence spectroscopy and two dimensional nuclear magnetic resonance. CD spectra indicate that D-glucose interacts with monomeric insulin whereas D-galactose, D-mannose and 2-deoxy-D-glucose have a lower effect. Fluorescence emission was quenched at sugar concentrations of 5-10 mM. Titration with the different sugars produces a quenching of the tyrosine spectrum from which a binding free energy value for the insulin-sugar complexes has been evaluated. Transfer nuclear Overhauser enhancement NMR experiments indicate the existence of dipolar interactions at short interatomic distances between C-1 proton of D-glucose in the beta form and the monomeric insulin. Further, NMR total correlation spectra experiments revealed that the hormone is in the monomeric form and that upon addition of glucose no aggregation occurs. The interaction does not involve relevant changes in the secondary structure of insulin suggesting that the interaction occur at the side chain level. Molecular dynamics simulations and modeling studies, based on the dynamic fluctuations of potential binding moiety sidechains, argued from results of NMR spectroscopy, provide additional informations to locate the putative binding sites of D-glucose to insulin.

Binding Sites↗
PubMed2004

Molecular dynamics simulations of Guanine quadruplex loops: advances and force field limitations.

A computational analysis of d(GGGGTTTTGGGG)(2) guanine quadruplexes containing either lateral or diagonal four-thymidine loops was carried out using molecular dynamics (MD) simulations in explicit solvent, locally enhanced sampling (LES) simulations, systematic conformational search, and free energy molecular-mechanics, Poisson Boltzmann, surface area (MM-PBSA) calculations with explicit inclusion of structural monovalent cations. The study provides, within the approximations of the applied all-atom additive force field, a qualitatively complete analysis of the available loop conformational space. The results are independent of the starting structures. Major conformational transitions not seen in conventional MD simulations are observed when LES is applied. The favored LES structures consistently provide lower free energies (as estimated by molecular-mechanics, Poisson Boltzmann, surface area) than other structures. Unfortunately, the predicted optimal structure for the diagonal loop arrangement differs substantially from the atomic resolution experiments. This result is attributed to force field deficiencies, such as the potential misbalance between solute-cation and solvent-cation terms. The MD simulations are unable to maintain the stable coordination of the monovalent cations inside the diagonal loops as reported in a recent x-ray study. The optimal diagonal and lateral loop arrangements appear to be close in energy although a proper inclusion of the loop monovalent cations could stabilize the diagonal architecture.

Computer Simulation↗
PubMed1995

Molecular dynamics simulations of excimer forming (+)-anti-BPDE-DNA adducts in aqueous solution.

The chemical carcinogen (+)-anti BPDE preferentially binds covalently to the guanine base in the minor groove of DNA. Fluorescence spectroscopic studies have shown that the BPDE molecules bound to DNA can interact in their photo-excited state giving strong excimer fluorescence when bound to poly(dGdC).poly(dGdC). It was suggested that the formation of such excited state complexes is most probable when the two (+)-anti-BPDE bind to guanines of adjacent base pairs on the two different strands of the DNA. In the present work a model for such an excimer forming DNA-BPDE double adduct system has been constructed and shown to be stable over a 300 ps molecular dynamics simulation in a water box. The model is a d(CG)3.d(CG)3 molecule with two BPDE molecules bound to the guanines at the 4th position on each strand, located in the minor groove and each oriented towards the 5' end of the modified strand, respectively. The results of 300 ps MD simulation show that the two BPDE chromophores exhibited on the average a relative geometry favourable for excimer formation. The local structure at the adduct position was considerably distorted and the helix axis was bent. The modified bases were found to be paired through a stable single non-Watson Crick type of hydrogen bond.

7,8-Dihydro-7,8-dihydroxybenzo(a)pyrene 9,10-oxide↗
PubMed2005

Time series analysis of ion dynamics in glassy ionic conductors obtained by a molecular dynamics simulation.

We present several characteristics of ionic motion in glassy ionic conductors brought out by time series analysis of molecular dynamics (MD) simulation data. Time series analysis of data obtained by MD simulation can provide crucial information to describe, understand and predict the dynamics in many systems. The data have been treated by the singular spectrum analysis (SSA), which is a method to extract information from noisy short time series and thus provide insight into the unknown or partially unknown dynamics of the underlying system that generated the time series. Phase-space plot reconstructed using the principal components of SSA exhibited complex but clear structures, suggesting the deterministic nature of the dynamics.

Journal Article↗
PubMed2003

Molecular dynamics simulations of peptides and proteins with a continuum electrostatic model based on screened Coulomb potentials.

A continuum electrostatics approach for molecular dynamics (MD) simulations of macromolecules is presented and analyzed for its performance on a peptide and a globular protein. The approach incorporates the screened Coulomb potential (SCP) continuum model of electrostatics, which was reported earlier. The model was validated in a broad set of tests some of which were based on Monte Carlo simulations that included single amino acids, peptides, and proteins. The implementation for large-scale MD simulations presented in this article is based on a pairwise potential that makes the electrostatic model suitable for fast analytical calculation of forces. To assess the suitability of the approach, a preliminary validation is conducted, which consists of (i) a 3-ns MD simulation of the immunoglobulin-binding domain of streptococcal protein G, a 56-residue globular protein and (ii) a 3-ns simulation of Dynorphin, a biological peptide of 17 amino acids. In both cases, the results are compared with those obtained from MD simulations using explicit water (EW) molecules in an all-atom representation. The initial structure of Dynorphin was assumed to be an alpha-helix between residues 1 and 9 as suggested from NMR measurements in micelles. The results obtained in the MD simulations show that the helical structure collapses early in the simulation, a behavior observed in the EW simulation and consistent with spectroscopic data that suggest that the peptide may adopt mainly an extended conformation in water. The dynamics of protein G calculated with the SCP implicit solvent model (SCP-ISM) reveals a stable structure that conserves all the elements of secondary structure throughout the entire simulation time. The average structures calculated from the trajectories with the implicit and explicit solvent models had a cRMSD of 1.1 A, whereas each average structure had a cRMSD of about 0.8A with respect to the X-ray structure. The main conformational differences of the average structures with respect to the crystal structure occur in the loop involving residues 8-14. Despite the overall similarity of the simulated dynamics with EW and SCP models, fluctuations of side-chains are larger when the implicit solvent is used, especially in solvent exposed side-chains. The MD simulation of Dynorphin was extended to 40 ns to study its behavior in an aqueous environment. This long simulation showed that the peptide has a tendency to form an alpha-helical structure in water, but the stabilization free energy is too weak, resulting in frequent interconversions between random and helical conformations during the simulation time. The results reported here suggest that the SCP implicit solvent model is adequate to describe electrostatic effects in MD simulation of both peptides and proteins using the same set of parameters. It is suggested that the present approach could form the basis for the development of a reliable and general continuum approach for use in molecular biology, and directions are outlined for attaining this long-term goal.

Amino Acid Sequence↗
PubMed2004

Potential energy surfaces and dynamics of Ni2+ ion aqueous solution: molecular dynamics simulation of the electronic absorption spectrum.

We develop a model effective Hamiltonian for describing the electronic structures of first-row transition metals in aqueous solutions using a quasidegenerate perturbation theory. All the states consisting of 3d(n) electronic configurations are determined by diagonalizing a small effective Hamiltonian matrix, where various intermolecular interaction terms such as the electrostatic, polarization, exchange, charge transfer, and three-body interactions are effectively incorporated. This model Hamiltonian is applied to constructing the ground and triplet excited states potential energy functions of Ni(2+) in aqueous solution, based on the ab initio multiconfiguration quasidegenerate perturbation theory calculations. We perform molecular dynamics simulation calculations for the ground state of Ni(2+) aqueous solution to calculate the electronic absorption spectral shape as well as the ground state properties. Agreement between the simulation and experimental spectra is satisfactory, indicating that the present model can well describe the Ni(2+) excited state potential surfaces in aqueous solution.

Journal Article↗
PubMed1999

A molecular dynamics simulation study of the solvent isotope effect on copper plastocyanin.

The effect of heavy water on the structure and dynamics of copper plastocyanin as well as on some aspects of the solvent dynamics at the protein-solvent interfacial region have been investigated by molecular dynamics simulation. The simulated system has been analyzed in terms of the atomic root mean square deviation and fluctuations, intraprotein H-bond pattern, dynamical cross-correlation map and the results have been compared with those previously obtained for plastocyanin in H2O (Ciocchetti et al. Biophys. Chem. 69 (1997), 185-198). The simulated plastocyanin structure in the two solvents, averaging 1 ns, is very similar along the beta-structure regions, while the most significant differences are registered, analogous to the turns and the regions likely involved in the electron transfer pathway. Moreover, plastocyanin in D2O shows an increase in the number of both the intraprotein H-bonds and the residues involved in correlated motions. An analysis of the protein-solvent coupling evidenced that D2O makes the H-bond formation more difficult with the solvent molecules for positively charged and polar residues, while an opposite trend is observed for negatively charged residues. On the other hand, the frequency of exchange of the solvent molecules involved in the protein-solvent H-bond formation is significantly depressed in D2O. The results are discussed also in connection with protein functionality and briefly with some experimental results connected with the thermostability of proteins in D2O.

Journal Article↗
PubMed2002

Role of hydrophilic and hydrophobic contacts in folding of the second beta-hairpin fragment of protein G: molecular dynamics simulation studies of an all-atom model.

Predicting the folding mechanism of the second beta-hairpin fragment of the Ig-binding domain B of streptococcal protein G is unexpectedly challenging for simplified reduced models because the models developed so far indicated a different folding mechanism from what was suggested from high-temperature unfolding and equilibrium free-energy surface analysis based on established all-atom empirical force fields in explicit or implicit solvent. This happened despite the use of empirical residue-based interactions, multibody hydrophobic interactions, and inclusions of hydrogen bonding effects in the simplified models. This article employs a recently developed all-atom (except nonpolar hydrogens) model interacting with simple square-well potentials to fold the peptide fragment by molecular dynamics simulation methods. In this study, 193 out of 200 trajectories are folded at two reduced temperatures (3.5 and 3.7) close to the transition temperature T* approximately 4.0. Each simulation takes <7 h of CPU time on a Pentium 800-MHz PC. Folding of the new all-atom model is found to be initiated by collapse before the formation of main-chain hydrogen bonds. This verifies the mechanism proposed from previous all-atom unfolding and equilibrium simulations. The new model further predicts that the collapse is initiated by two nucleation contacts (a hydrophilic contact between D46 and T49 and a hydrophobic contact between Y45 and F52), in agreement with recent NMR measurements. The results suggest that atomic packing and native contact interactions play a dominant role in folding mechanism.

Amino Acids↗
PubMed1992

Solution structure of a DNA octamer containing the Pribnow box via restrained molecular dynamics simulation with distance and torsion angle constraints derived from two-dimensional nuclear magnetic resonance spectral fitting.

The DNA octamer [d(GTATAATG].[(CATATTAC)], containing the prokaryotic upstream consensus recognition sequence, has been examined via proton homonuclear two-dimensional nuclear Overhauser effect (2D NOE) and double-quantum-filtered correlation (2QF-COSY) spectra. All proton resonances, except those of H5' and H5" protons, were assigned. A temperature dependence study of one-dimensional nuclear magnetic resonance (NMR) spectra, rotating frame 2D NOE spectroscopy (ROESY), and T1 rho measurements revealed an exchange process that apparently is global in scope. Work at lower temperatures enabled a determination of structural constraints that could be employed in determination of a time-averaged structure. Simulations of the 2QF-COSY cross-peaks were compared with experimental data, establishing scalar coupling constant ranges of the individual sugar ring protons and hence pucker parameters for individual deoxyribose rings. The rings exhibit a dynamic equilibrium of N and S-type conformers with 80 to 100% populations of the latter. A program for iterative complete relaxation matrix analysis of 2D NOE spectral intensities, MARDIGRAS, was employed to give interproton distances for each mixing time. According to the accuracy of the distance determination, upper and lower distance bounds were chosen. The distance bounds define the size of a flat-well potential function term, incorporated into the AMBER force-field, which was employed for restrained molecular dynamics calculations. Torsion angle constraints in the form of a flat-well potential were also constructed from the analysis of the sugar pucker data. Several restrained molecular dynamics runs of 25 picoseconds were performed, utilizing 184 experimental distance constraints and 80 torsion angle constraints; three different starting structures were used: energy minimized A-DNA, B-DNA, and wrinkled D-DNA, another member of the B-DNA family. Convergence to similar structures obtained with root-mean-square deviations between resulting structures of 0.37 to 0.92 A for the central hexamer of the octamer. The average structure from the nine different molecular dynamics runs was subjected to final restrained energy minimization. The resulting final structure was in good agreement with the structures derived from different molecular dynamics runs and exhibited a substantial improvement in the 2D NOE sixth-root residual index in comparison with the starting structures. An approximation of the structure in the terminal base-pairs, which displayed experimental evidence of fraying, was made by maintaining the structure of the inner four base-pairs and performing molecular dynamics simulations with the experimental structural constraints observed for the termini.(ABSTRACT TRUNCATED AT 400 WORDS)

Base Sequence↗
PubMed1997

Selectin-ligand interactions revealed by molecular dynamics simulation in solution.

Through a computer modeling and simulation technique, we investigated the binding mode of a complex of E-selectin-GSC-150, which is a novel selectin blocker. GSC-150 is the 3'-sulfated Lewis X derivative with a long, branched alkyl chain. Initial attempts to construct a model for E-selectin-GSC-150 complex were performed based on a previously reported model of E-selectin-sialyl Lewis X (sLex) complex [Kogan, T.P.; Revelle, B.M.; Tapp, S.; Scott, D.; Beck, P.J.J. Biol. Chem. 1995, 270, 14047-14055]. In our model, the carbohydrate portion of GSC-150 interacted with the protein in a similar manner as that of sLex reported previously. Interestingly, each of the branched alkyl chains extended on the surface of E-selectin and interacted with two different hydrophobic portions. One of these hydrophobic portions consists of Tyr44, Pro46, and Tyr48. Another portion forms a shallow cavity, and it consists of Ala9, Leu114, and the alkyl moieties of the side chains of Lys111, Lys112, and Lys113. A subsequent 200-ps molecular dynamics simulation in solution revealed that the interactions involved in the sugar portion of the ligand were relatively weak, whereas the hydrophobic interactions involved in the branched alkyl chains were fairly stable in solution. These results suggest that the branched alkyl chain serves as an "anchor" for the tight binding of GSC-150 on the surface of E-Selectin. This is the first attempt to evaluate the dynamics of E-Selectin-ligand interactions in solution, and it sheds light on the nature of ligand recognition by selectins.

Carbohydrate Sequence↗
PubMed2004

The hydrophobic effect: molecular dynamics simulations of water confined between extended hydrophobic and hydrophilic surfaces.

Structural and dynamic properties of water confined between two parallel, extended, either hydrophobic or hydrophilic crystalline surfaces of n-alkane C(36)H(74) or n-alcohol C(35)H(71)OH, are studied by molecular dynamics simulations. Electron density profiles, directly compared with corresponding experimental data from x-ray reflectivity measurements, reveal a uniform weak de-wetting characteristic for the extended hydrophobic surface, while the hydrophilic surface is weakly wetted. These microscopic data are consistent with macroscopic contact angle measurements. Specific water orientation is present at both surfaces. The ordering is characteristically different between the surfaces and of longer range at the hydrophilic surface. Furthermore, the dynamic properties of water are different at the two surfaces and different from the bulk behavior. In particular, at the hydrophobic surface, time-correlation functions reveal that water molecules have characteristic diffusive behavior and orientational ordering due to the lack of hydrogen bonding interactions with the surface. These observations suggest that the altered dynamical properties of water in contact with extended hydrophobic surfaces together with a partial drying of the surfaces are more indicative of the hydrophobic effect than structural ordering, which we suggest to be independent of surface topology.

Journal Article↗
PubMed2002

Influence of the environment in the conformation of alpha-helices studied by protein database search and molecular dynamics simulations.

The influence of the solvent on the main-chain conformation (phi and Psi dihedral angles) of alpha-helices has been studied by complementary approaches. A first approach consisted in surveying crystal structures of both soluble and membrane proteins. The residues of analysis were further classified as exposed to either the water (polar solvent) or the lipid (apolar solvent) environment or buried to the core of the protein (intermediate polarity). The statistical results show that the more polar the environment, the lower the value of phi(i) and the higher the value of Psi(i) are. The intrahelical hydrogen bond distance increases in water-exposed residues due to the additional hydrogen bond between the peptide carbonyl oxygen and the aqueous environment. A second approach involved nanosecond molecular dynamics simulations of poly-Ala alpha-helices in environments of different polarity: water to mimic hydrophilic environments that can form hydrogen bonds with the peptide carbonyl oxygen and methane to mimic hydrophobic environments without this hydrogen bond capabilities. These simulations reproduce similar effects in phi and Psi angles and intrahelical hydrogen bond distance and angle as observed in the protein survey analysis. The magnitude of the intrahelical hydrogen bond in the methane environment is stronger than in the water environment, suggesting that alpha-helices in membrane-embedded proteins are less flexible than in soluble proteins. There is a remarkable coincidence between the phi and Psi angles obtained in the analysis of residues exposed to the lipid in membrane proteins and the results from computer simulations in methane, which suggests that this simulation protocol properly mimic the lipidic cell membrane and reproduce several structural characteristics of membrane-embedded proteins. Finally, we have compared the phi and Psi torsional angles of Pro kinks in membrane protein crystal structures and in computer simulations.

Biophysical Phenomena↗
PubMed2005

Molecular dynamics simulations of unsaturated lipid bilayers: effects of varying the numbers of double bonds.

The importance of unsaturated, and especially polyunsaturated phosphatidylcholine molecules for the functional properties of biological membranes is widely accepted. Here, the effects of unsaturation on the nanosecond-scale structural and dynamic properties of the phosphatidylcholine bilayer were elucidated by performance of multinanosecond molecular dynamics simulations of all-atom bilayer models. Bilayers of dipalmitoylphosphatidylcholine and its mono-, di-, and tetraunsaturated counterparts were simulated, containing, respectively, oleoyl, linoleoyl, or arachidonoyl chains in the sn-2 position. Analysis of the simulations focused on comparison of the structural properties, especially the ordering of the chains in the membranes. Although the results suggest some problems in the CHARMM force field of the lipids when applied in a constant pressure ensemble, the features appearing in the ordering of the unsaturated chains are consistent with the behaviour known from (2)H NMR experiments. The rigidity of the double bonds is compensated by the flexibility of skew state single bonds juxtaposed with double bonds. The presence of double bonds in the sn-2 chains considerably reduces the order parameters of the CH bonds. Moreover, the double bond region of tetraunsaturated chains is shown to span all the way from the bilayer centre to the head group region.

1,2-Dipalmitoylphosphatidylcholine↗
PubMed1995

Molecular dynamics simulations of protein unfolding and limited refolding: characterization of partially unfolded states of ubiquitin in 60% methanol and in water.

Extensive experimental data are available on the native, partially and fully unfolded states of ubiquitin. Two and three-dimensional NMR experiments of a partially unfolded form of the protein in 60% methanol indicate that approximately one-half of the molecule contains disrupted but native-like structure while the other half is unstructured and/or contains non-native structure. In contrast, the interpretation of hydrogen-exchange data have led to the conclusion that this state is native-like. Thus, there are discrepancies between the experimental studies, or interpretations based on the data. We compare the results of molecular dynamics simulations, under varying conditions, with the experimental results. The simulations extend past 0.5 ns and include explicit solvent molecules: either pure water or 60% methanol. To begin with, ubiquitin was thermally denatured in water (at 498 K). Two particular structures, or "aliquots", during the unfolding process were selected for further study (60 and 198 ps). These structures were then simulated separately in water and 60% methanol at a lower and experimentally meaningful temperature (335 K). The conformations generated from the structure extracted later in the simulation contained significant amounts of non-native structure in the presence of methanol while satisfying both the NMR and hydrogen exchange data. In fact, clearly non-native regions of the structure yielded the desired protection from hydrogen exchange. In contrast, an earlier, more native-like, intermediate did not do as well at predicting the hydrogen-exchange behavior and was inconsistent with the NMR data. These data suggest that the results and interpretations using the different experimental techniques can be reconciled by a single state. This finding also brings into question the practice of interpreting protection to hydrogen exchange in terms of native secondary and tertiary structure, especially when one has weak patterns and low protection factors. When the partially unfolded states were placed in pure water, the protein collapsed and began to refold. Therefore, the desired solvent-dependent properties were observed: the partially unfolded conformations with increased exposure of hydrophobic residues remained expanded in methanol but collapsed in water as the non-polar groups minimized their exposure to solvent.

Amino Acid Sequence↗
PubMed2004

"Cooperativity blockage" in the mixed alkali effect as revealed by molecular-dynamics simulations of alkali metasilicate glass.

The relaxation dynamics of a complex interacting system can be drastically changed when mixing with another component having different dynamics. In this work, we elucidate the effect of the less mobile guest ions on the dynamics of the more mobile host ions in mixed alkali glasses by molecular-dynamics (MD) simulations. One MD simulation was carried out on lithium metasilicate glass with the guest ions created by freezing some randomly chosen lithium ions at their initial locations at 700 K. A remarkable slowing down of the dynamics of the majority mobile Li ions was observed both in the self-part of the density-density correlation function, Fs(k,t), and in the mean-squared displacements. On the other hand, there is no significant change in the structure. The motion of the Li ions in the unadulterated Li metasilicate glass is dynamically heterogeneous. In the present work, the fast and slow ions were divided into two groups. The number of fast ions, which shows faster dynamics (Levy flight) facilitated by cooperative jumps, decreases considerably when small amount of Li ions are frozen. Consequently there is a large overall reduction of the mobility of the Li ions. The result is also in accordance with the experimental finding in mixed alkali silicate glasses that the most dramatic reduction of ionic conductivity occurs in the dilute foreign alkali limit. Similar suppression of the cooperative jumps is observed in the MD simulation data of mixed alkali system, LiKSiO3. Naturally, the effect found here is appropriately described as "cooperativity blockage." Slowing down of the motion of Li ions also was observed when a small number of oxygen atoms chosen at random were frozen. The effect is smaller than the case of freezing some the Li ions, but it is not negligible. The cooperativity blockage is also implemented by confining the Li metasilicate glass inside two parallel walls formed by freezing Li ions in the same metasilicate glass. Molecular-dynamics simulations were performed on the dynamics of the Li ions in the confined glass. Slowing down of the dynamics is largest near the wall and decreases monotonically with distance away from the wall.

Journal Article↗
PubMed2005

Molecular dynamics simulations of the periplasmic ferric-hydroxamate binding protein FhuD.

FhuD is a periplasmic binding protein (PBP) that, under iron-limiting conditions, transports various hydroxamate-type siderophores from the outer membrane receptor (FhuA) to the inner membrane ATP-binding cassette transporter (FhuBC). Unlike many other PBPs, FhuD possesses two independently folded domains that are connected by an alpha-helix rather than two or three central beta-strands. Crystal structures of FhuD with and without bound gallichrome have provided some insight into the mechanism of siderophore binding as well as suggested a potential mechanism for FhuD binding to FhuB. Since the alpha-helix connecting the two domains imposes greater rigidity on the structure relative to the beta-strands in other 'classical' PBPs, these structures reveal no large conformational change upon binding a hydroxamate-type siderophore. Therefore, it is difficult to explain how the inner membrane transporter FhuB can distinguish between ferrichrome-bound and ferrichrome-free FhuD. In the current study, we have employed a 30 ns molecular dynamics simulation of FhuD with its bound siderophore removed to explore the dynamic behavior of FhuD in the substrate-free state. The MD simulation suggests that FhuD is somewhat dynamic with a C-terminal domain closure of 6 degrees upon release of its siderophore. This relatively large motion suggests differences that would allow FhuB to distinguish between ferrichrome-bound and ferrichrome-free FhuD.

Amino Acid Sequence↗
PubMed2003

The quaternary structure of the Saccharomyces cerevisiae succinate dehydrogenase. Homology modeling, cofactor docking, and molecular dynamics simulation studies.

Succinate dehydrogenases and fumarate reductases are complex mitochondrial or bacterial respiratory chain proteins with remarkably similar structures and functions. Succinate dehydrogenase oxidizes succinate and reduces ubiquinone using a flavin adenine dinucleotide cofactor and iron-sulfur clusters to transport electrons. A model of the quaternary structure of the tetrameric Saccharomyces cerevisiae succinate dehydrogenase was constructed based on the crystal structures of the Escherichia coli succinate dehydrogenase, the E. coli fumarate reductase, and the Wolinella succinogenes fumarate reductase. One FAD and three iron-sulfur clusters were docked into the Sdh1p and Sdh2p catalytic dimer. One b-type heme and two ubiquinone or inhibitor analog molecules were docked into the Sdh3p and Sdh4p membrane dimer. The model is consistent with numerous experimental observations. The calculated free energies of inhibitor binding are in excellent agreement with the experimentally determined inhibitory constants. Functionally important residues identified by mutagenesis of the SDH3 and SDH4 genes are located near the two proposed quinone-binding sites, which are separated by the heme. The proximal quinone-binding site, located nearest the catalytic dimer, has a considerably more polar environment than the distal site. Alternative low energy conformations of the membrane subunits were explored in a molecular dynamics simulation of the dimer embedded in a phospholipid bilayer. The simulation offers insight into why Sdh4p Cys-78 may be serving as the second axial ligand for the heme instead of a histidine residue. We discuss the possible roles of heme and of the two quinone-binding sites in electron transport.

Amino Acid Sequence↗
PubMed1999

Rotational viscosity in a nematic liquid crystal: a theoretical treatment and molecular dynamics simulation.

The rotational viscosity coefficient gamma(1) of 4-n-pentyl-4(')-cyanobiphenyl in the nematic phase is investigated by combination of existing statistical-mechanical approaches (SMAs), based on a rotational diffusion model and computer simulation technique. The SMAs rest on a model in which it is assumed that the reorientation of an individual molecule is a stochastic Brownian motion in a certain potential of mean torque. According to the SMAs, gamma(1) is found to be a function of temperature, density, rotational diffusion coefficient, and a number of order parameters (OPs). The diffusion coefficient and the OPs were obtained from an analysis of a trajectory generated in a molecular dynamics simulation using realistic atom-atom interactions. In addition, a set of experimentally determined diffusion coefficients and OPs was used for evaluation of gamma(1). Reasonable agreement between calculated and experimental values of gamma(1) is obtained. It is shown that near the clearing point gamma(1) is proportional to (-)P22, where (-)P2 is the second-rank OP. This limiting value of gamma(1) is in agreement with mean-field theory.

Journal Article↗