SEARCH · Search PubMed

Results for “MD 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.

SourceResearch connectionFrom yearThrough year

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

At least 919 records · Page 51Linked to original sources

PubMed2006

Molecular dynamics simulation of the P2Y14 receptor. Ligand docking and identification of a putative binding site of the distal hexose moiety.

A rhodopsin-based homology model of the P2Y14 receptor was inserted into a phospholipid bilayer and refined by molecular dynamics (MD) simulation. The binding modes of several known agonists, namely UDP-glucose and its analogues, were proposed using automatic molecular docking combined with Monte Carlo Multiple Minimum calculations. Compared to other P2Y receptors, the P2Y14 receptor has an atypical binding mode of the nucleobase, ribose, and phosphate moieties. The diphosphate moiety interacts with only one cationic residue, namely Lys171 of EL2, while in other P2Y receptor subtypes three Arg or Lys residues interact with the phosphate chain. Two other conserved cationic residues, namely Arg253 (6.55) and Lys277 (7.35) of the P2Y14 receptor together with two anionic residues (Glu166 and Glu174, located in EL2), are likely involved in interactions with the distal hexose moiety.

Binding Sites↗

PubMed2003

Hydration of hydroxypyrrole influences binding of ImHpPyPy-beta-Dp polyamide to DNA.

Ligands which are able to recognize DNA sequence specifically are of fundamental interest as transcription controlling drugs. Recently a polyamide ligand was developed (ImHpPyPy-beta-Dp) which differentiates in a dimeric arrangement between all four possible base pair steps in the minor groove. This is a landmark for the design of DNA binding drugs because it was believed that such a recognition could only be possible in the major groove of DNA. Although the OH groups of the hydroxypyrrole (Hp) moieties of the ligands are responsible for this sequence discrimination, experiments showed that this OH group also reduces the absolute binding constant. We performed a free energy calculation by means of thermodynamic integration in order to find out the influence of this single hydroxyl on DNA binding. In our simulation, we found that the hydroxyl group reduces binding by about 1.3 kcal/mol, which is in excellent agreement with the experimentally determined value of 1.2 kcal/mol. In further MD simulations, the structural reasons for this reduction was estimated. The results of these simulations qualitatively agree with the X-ray structures, but in contrast, in the simulations both (ImHpPyPy-beta-Dp and ImPyPyPy-beta-Dp) ligand-DNA (d(CCAGTACTGG)(2)) complexes exhibit only slight structural differences. This is consistent with a recently published second pair of similar polyamide DNA crystal structures. Thus, we believe that the explanations resulting from the X-ray structures must be modified. We attribute the large structural differences between the two polyamide DNA complexes to a buffer molecule which binds only in the case of the ImHpPyPy-beta-Dp-DNA complex at the region of interest. We propose that the differential hydration of both ligands in the unbound state is responsible for the reduction of the binding constant. Additionally, we suggest an indirect readout of DNA, because of a lengthening of the Watson-Crick base pairs, which possibly contributes to the differentiation between T.A, A.T from G.C, C.G base pairs.

Computer Simulation↗

PubMed2006

Detailed structures and mechanism of polymer solvation.

In the present study, we simulated a model system, PE in biphenyl, to gain the insight into the detailed solvation structures and the molecular mechanism of polymer chain solvation. Using atomistic molecular dynamics (MD) simulation, it was found that when the biphenyl is far from PE chain or in the bulk, the dihedral angle of the two rings in the solvent molecule are approximately 32 degrees. But, the dihedral angel is about 27 degrees when the biphenyls are very close to the PE chain. In the first solvation shell, the orientation angle of the biphenyl long axis to the chain segment backbone was found to be enhanced around two values: approximately 0 and approximately 60 degrees. The detailed solvation structures found here include all dyad conformations (TT, TG, TG', GT, GG, GG', G'T, G'G, and G'G') and vary as a function of the distance between PE chain and biphenyls in the first solvation shell. The closer the the solvent molecule to the PE segment, the higher the TT conformation fraction response is. The other dyad conformations such as TG, GG', etc. undergo different decreases, respectively. This study shows that the solvation even in the Theta condition makes the overall size expansion or the chain stretched. Such a cooperative change was examined here and found not due to generating or losing a conformational state but due to a change in conformational distribution. This change occurs in the middle location of the chain instead of the chain end locations.

Journal Article↗

PubMed2002

Factors governing loss and rescue of DNA binding upon single and double mutations in the p53 core domain.

The mutation of R273-->H in the p53 core domain (p53-CD) is one of the most common mutations found in human cancers. Although the 273H p53-CD retains the wild-type conformation and stability, it lacks sequence-specific DNA binding, a transactivation function and growth suppression. However, mutating T284-->R in the 273H p53-CD restores the DNA binding affinity, and transactivation and tumour suppressor functions. Since X-ray/NMR structures of DNA-free or DNA-bound mutant p53-CD molecules are unavailable, the factors governing the loss and rescue of sequence-specific DNA binding in the 273H and 273H+284R p53-CD, respectively, are unclear. Hence, we have carried out molecular dynamics (MD) simulations of the wild-type, single mutant and double mutant p53-CD, free and DNA bound, in the presence of explicit water molecules. Based on the MD structures, the DNA-binding free energy of each p53 molecule has been computed and decomposed into component energies and contributions from the interface residues. The wild-type and mutant p53-CD MD structures were found to be consistent with the antibody-binding, X-ray and NMR data. The predicted DNA binding affinity and specificity of both mutant p53-CDs were also in accord with experimental data. The non-detectable DNA binding of the 273H p53-CD is due mainly to the disruption of a hydrogen-bonding network involving R273, D281 and R280, leading to a loss of major groove binding by R280 and K120. The restoration of DNA binding affinity and specificity of the 273H+284R p53-CD is due mainly to the introduction of another DNA-binding site at position 284, leading to a recovery of major groove binding by R280 and K120. The important role of water molecules and the DNA major groove conformation as well as implications for structure-based linker rescue of the 273H p53-CD DNA-binding affinity are discussed.

DNA↗

PubMed2002

Insights into the structure and dynamics of the dinuclear zinc beta-lactamase site from Bacteroides fragilis.

Herein, we report quantum chemical calculations and molecular dynamics (MD) simulations of the dinuclear form of the Bacteroides fragilis zinc beta-lactamase. We studied four different configurations which differ in the protonation state of the Asp103 residue and in the presence or absence of a Zn1-OH-Zn2 bridge. The flexibility of the Zn1-OH-Zn2 bridge was studied by means of quantum mechanical (QM) calculations on cluster models while the relative stabilities of the different configurations were estimated from QM linear scaling calculations on the enzyme. Contacts between important residues (Cys104, Asp69, Lys185, etc.), the solvation of the zinc ions, and the conformation of the active site beta-hairpin loop were characterized by the MD analyses. The influence of the buried sodium ion close to the Zn2 position was investigated by carrying out a secondary simulation where the sodium ion was replaced with an internal water molecule. The comparative structural analyses among the different MD trajectories augmented with energetic calculations have demonstrated that the B. fragilis protein efficiently binds the internal Na(+) ion observed crystallographically. Moreover, we found that when Asp103 is unprotonated, a rigid Zn1-OH-Zn2 bridge results, while for neutral Asp103, a fluctuating Zn1-Zn2 distance was possible via the breaking and formation of the Zn1-OH-Zn2 bridge. The mechanistic implications of these observations are discussed in detail.

Aspartic Acid↗

PubMed2002

Conformation of a trimannoside bound to mannose-binding protein by nuclear magnetic resonance and molecular dynamics simulations.

A model of the carbohydrate recognition domain of the serum form of mannose-binding protein (MBP) from rat complexed with methyl 3,6-di-O-(alpha-D-mannopyranosyl)-alpha-D-mannopyranoside is presented. Allowed conformations for the bound sugar were derived from simulated annealing protocols incorporating distance restraints computed from transferred NOESY spectra. The resulting sugar conformations were then modeled into the MBP binding site, and these models of the complex were refined using molecular dynamics (MD) simulations in the presence of solvent water. These studies indicate that only one of the two major conformations of the alpha(1-->6) linkage found in solution is significantly populated in the bound state (omega = 60 degrees ), whereas the alpha(1-->3) linkage samples at least two states, similar to its behavior in free solution. The bound conformation allows direct hydrogen bonds to form between the sugar and K182 of MBP, in addition to other water-mediated hydrogen bonds. Estimates of binding constants of candidate complexes based on changes in solvent-accessible surface areas upon binding support the NMR and MD results. These estimates further suggest that the enthalpic gains of the additional sugar-MBP interactions in a trisaccharide as opposed to a monosaccharide are offset by entropic penalties, offering an explanation for previous binding data.

Animals↗

PubMed2006

Molecular dynamics simulations of lithium alkyl carbonates.

A quantum chemistry-based many-body polarizable force field has been developed for two model solid-electrolyte interphase (SEI) components: dilithium ethylene dicarbonate (Li(2)EDC) and lithium methyl carbonate (LiMC). Molecular dynamics (MD) simulations of amorphous Li(2)EDC and LiMC were performed at temperatures from 393 to 600 K. Simulations reveal that Li(+) is coordinated by approximately 4.6 oxygen atoms from -COO(-) groups coming from different alkyl carbonate molecules. Charge transport in Li(2)EDC was found to be almost entirely due to Li(+). The temperature dependence of the ionic conductivity of the SEI model compounds Li(2)EDC and LiMC was found to be significantly stronger than that of liquid electrolytes (e.g., ethylene carbonate + LiTFSI), yielding extrapolated conductivities of the Li(2)EDC on order of 10(-10) S/cm at -30 degrees C.

Journal Article↗

PubMed2005

Multiscale modeling of lipids and lipid bilayers.

A multiscale modeling approach is applied for simulations of lipids and lipid assemblies on mesoscale. First, molecular dynamics simulation of initially disordered system of lipid molecules in water within all-atomic model was carried out. On the next stage, structural data obtained from the molecular dynamics (MD) simulation were used to build a coarse-grained (ten sites) lipid model, with effective interaction potentials computed by the inverse Monte Carlo method. Finally, several simulations of the coarse-grained model on longer length- and time-scale were performed, both within Monte Carlo and molecular dynamics simulations: a periodical sample of lipid molecules ordered in bilayer, a free sheet of such bilayer without periodic boundary conditions, formation of vesicle from a plain membrane, process of self-assembly of lipids randomly dispersed in volume. It was shown that the coarse-grained model, developed exclusively from all-atomic simulation data, reproduces well all the basic features of lipids in water solution.

Computer Simulation↗

PubMed2002

Secondary structural studies of bovine caseins: structure and temperature dependence of beta-casein phosphopeptide (1-25) as analyzed by circular dichroism, FTIR spectroscopy, and analytical ultracentrifugation.

The defining structural feature of all of the caseins is their common phosphorylation sequence. In milk, these phosphoserine residues combine with inorganic calcium and phosphate to form colloidal complexes. In addition, nutritional benefits have been ascribed to the phosphopeptides from casein. To obtain a molecular basis for the functional, chemical, and biochemical properties of these casein peptides, the secondary structure of the phosphopeptide of bovine beta-casein (1-25) was reexamined using Fourier transform infrared (FTIR) and circular dichroism (CD) spectroscopies. Both methods predict secondary structures for the peptide which include polyproline II elements as well as beta-extended sheet and turn-like elements. These structural elements were highly stable from 5 degrees to 70 degrees C. Reexamination of previously published 1H NMR data using chemical shift indices suggests structures in accord with the CD and FTIR data. Dephosphorylation showed little or no secondary structural changes, as monitored by CD and FTIR, but the modified peptide demonstrated pronounced self-association. The polymers formed were not highly temperature sensitive, but were pressure sensitive as judged by analytical ultracentrifugation at selected rotor speeds. Molecular dynamics (MD) simulations demonstrated relatively large volume changes for the dephosphorylated peptide, in accord with the pressure dependent aggregation observed in the analytical ultracentrifuge data. In contrast the native peptide in MD remained relatively rigid. The physical properties of the peptide suggest how phosphorylation can alter its biochemical and physiological properties.

Amino Acid Sequence↗

PubMed2006

Transmembrane helix packing of ErbB/Neu receptor in membrane environment: a molecular dynamics study.

Dimerization or oligomerization of the ErbB/Neu receptors are necessary but not sufficient for initiation of receptor signaling. The two intracellular domains must be properly oriented for the juxtaposition of the kinase domains allowing trans-phosphorylation. This suggests that the transmembrane (TM) domain acts as a guide for defining the proper orientation of the intracellular domains. Two structural models, with the two helices either in left-handed or in right-handed coiling have been proposed as the TM domain structure of the active receptor. Because experimental data do not distinguish clearly helix-helix packing, molecular dynamics (MD) simulations are used to investigate the energetic factors that drive Neu TM-TM interactions of the wild and the oncogenic receptor (Val664/Glu mutation) in DMPC or in POPC environments. MD results indicate that helix-lipid interactions in the bilayer core are extremely similar in the two environments and raise the role of the juxtamembrane residues in helix insertion and helix-helix packing. The TM domain shows a greater propensity to adopt a left-handed structure in DMPC, with helices in optimal position for strong inter-helical Hbonds induced by the Glu mutation. In POPC, the right-handed structure is preferentially formed with the participation of water in inter-helical Hbonds. The two structural arrangements of the Neu(TM) helices both with GG4 residue motif in close contact at the interface are permissible in the membrane environment. According to the hypothesis of a monomer-dimer equilibrium of the proteins it is likely that the bilayer imposes structural constraints that favor dimerization-competent structure responsible of the proper topology necessary for receptor activation.

Cell Membrane↗

PubMed1999

Conformational flexibility in calcitonin: the dynamic properties of human and salmon calcitonin in solution.

We have studied the dynamic properties of human (h) and salmon (s) calcitonin (CT) in solution. For both hormones, distance geometry in torsion-angle space has been used to generate three-dimensional structures consistent with NMR data obtained in sodium dodecyl sulfate micelles. For sCT and hCT we used, respectively, 356 and 275 interproton distances together with hydrogen-bonds as restraints. To better characterize their flexibility and dynamic properties two fully unrestrained 1100-ps molecular dynamics (MD) simulations in methanol were performed on the lowest-energy structures of both hormones. Statistical analyses of average geometric parameters and of their fluctuations performed in the last 1000 ps of the MD run show typical helical values for residues 9-19 of sCT during the whole trajectory. For hCT a shorter helix was observed involving residues 13-21, with a constant helical region in the range 13-19. Angular order parameters S(phi) and S(psi) indicate that hCT exhibits a higher flexibility, distributed along the whole chain, including the helix, while the only flexible amino acid residues in sCT connect three well-defined domains. Finally, our study shows that simulated annealing in torsion-angle space can efficiently be extended to NMR-based three-dimensional structure calculations of helical polypeptides. Furthermore, provided that a sufficient number of NMR restraints describes the system, the method allows the detection of equilibria in solution. This identification occurs through the generation of 'spurious' high-energy structures, which, for right-handed alpha-helices, are likely to be represented by left-handed alpha-helices.

Amino Acid Sequence↗

PubMed2007

Protein dynamics from X-ray crystallography: anisotropic, global motion in diffuse scattering patterns.

Understanding X-ray crystallographic diffuse scattering is likely to improve our comprehension of equilibrium collective protein dynamics. Here, using molecular dynamics (MD) simulation, a detailed analysis is performed of the origins of diffuse scattering in crystalline Staphylococcal nuclease, for which the complete diffuse scattering pattern has been determined experimentally. The hydrogen-atom contribution and the scattering range over which the scattering can be considered to be a sum of solvent and protein scattering are determined. Two models of correlated protein motion are investigated by calculating the model-derived diffuse scattering and comparing with the scattering calculated directly from MD trajectories. In one model, previously used in diffuse scattering interpretation, the atomic displacement correlations decay isotropically with increasing separation. Model correlation lengths are obtained by refining the model scattering against the simulation-derived scattering pattern, and are found to be significantly different from those correlation lengths derived directly from the MD trajectories. Furthermore, the convergence between the model-derived and MD-derived scattering is poor. The second model, in which the displacement correlations are calculated from the principal components of the MD trajectories, is capable of fully reproducing the MD-derived diffuse scattering if the approximately 50% lowest-frequency modes are included. However, a small number ( approximately 10) of lowest-frequency and largest-amplitude modes dominates the diffuse scattering and thus the correlated protein motions. A detailed analysis of the principal components is performed. In particular, the effective free energy profile associated with each principle mode is analyzed and the eigenfrequency and damping coefficient computed using a model of Brownian dynamics. Those collective modes with effective frequencies below approximately 0.5 THz, including those that determine the diffuse scattering, are overdamped.

Anisotropy↗

PubMed2000

Molecular dynamics simulations of a beta-hairpin fragment of protein G: balance between side-chain and backbone forces.

How is the native structure encoded in the amino acid sequence? For the traditional backbone centric view, the dominant forces are hydrogen bonds (backbone) and phi-psi propensity. The role of hydrophobicity is non-specific. For the side-chain centric view, the dominant force of protein folding is hydrophobicity. In order to understand the balance between backbone and side-chain forces, we have studied the contributions of three components of a beta-hairpin peptide: turn, backbone hydrogen bonding and side-chain interactions, of a 16-residue fragment of protein G. The peptide folds rapidly and cooperatively to a conformation with a defined secondary structure and a packed hydrophobic cluster of aromatic side-chains. Our strategy is to observe the structural stability of the beta-hairpin under systematic perturbations of the turn region, backbone hydrogen bonds and the hydrophobic core formed by the side-chains, respectively. In our molecular dynamics simulations, the peptides are solvated. with explicit water molecules, and an all-atom force field (CFF91) is used. Starting from the original peptide (G41EWTYDDATKTFTVTE56), we carried out the following MD simulations. (1) unfolding at 350 K; (2) forcing the distance between the C(alpha) atoms of ASP47 and LYS50 to be 8 A; (3) deleting two turn residues (Ala48 and Thr49) to form a beta-sheet complex of two short peptides, GEWTYDD and KTFTVTE; (4) four hydrophobic residues (W43, Y45, F52 and T53) are replaced by a glycine residue step-by-step; and (5) most importantly, four amide hydrogen atoms (T44, D46, T53, and T55, which are crucial for backbone hydrogen bonding), are substituted by fluorine atoms. The fluorination not only makes it impossible to form attractive hydrogen bonding between the two beta-hairpin strands, but also introduces a repulsive force between the two strands due to the negative charges on the fluorine and oxygen atoms. Throughout all simulations, we observe that backbone hydrogen bonds are very sensitive to the perturbations and are easily broken. In contrast, the hydrophobic core survives most perturbations. In the decisive test of fluorination, the fluorinated peptide remains folded under our simulation conditions (5 ns, 278 K). Hydrophobic interactions keep the peptide folded, even with a repulsive force between the beta-strands. Thus, our results strongly support a side-chain centric view for protein folding.

Amino Acid Sequence↗

PubMed2004

Structure, dynamics and interaction with kinase targets: computer simulations of calmodulin.

Calmodulin (CaM) is a small protein involved in calcium signaling; among the targets of CaM are a number of kinases, including myosin light chain kinases (MLCK), various CaM-dependent kinases and phosphorylase kinase. We present results of molecular dynamics (MD) simulations of 4-ns length for calmodulin in its three functional forms: calcium-free, calcium-loaded, and in complex with both calcium and a target peptide, a fragment of the smooth muscle MLCK. The simulations included explicit water under realistic conditions of constant temperature and pressure, the presence of counterions and Ewald summation of electrostatic forces. Our simulation results present a more complete description of calmodulin structure, dynamics and interactions in solution than previously available. The results agree with a wide range of experimental data, including X-ray, nuclear magnetic resonance (NMR), fluorescence, cross-linking, mutagenesis and thermodynamics. Additionally, we are able to draw interesting conclusions about microscopic properties related to the protein's biological activity. First, in accord with fluorescence data, we find that calcium-free and calcium-loaded calmodulin exhibit significant structural flexibility. Our simulations indicate that these motions may be described as rigid-body translations and rotations of the N- and C-terminal domains occurring on a nanosecond time scale. Our second conclusion deals with the standard model of calmodulin action, which is that calcium binding leads to solvent exposure of hydrophobic patches in the two globular domains, which thus become ready to interact with the target. Surprisingly, the simulation results are inconsistent with the activation model when the standard definitions of the hydrophobic patches are used, based on hydrophobic clefts found in the X-ray structure of calcium-loaded calmodulin. We find that both experimental and simulation results are consistent with the activation model after a redefinition of the hydrophobic patches as those residues which are actually involved in peptide binding in the experimental structure of the calmodulin-peptide complex. The third conclusion is that the calmodulin-peptide interactions in the complex are very strong and are dominated by hydrophobic effects. Using quasi-harmonic entropy calculations, we find that these strong interactions induce a significant conformational strain in the protein and peptide. This destabilizing entropic contribution leads to a moderate overall binding free energy in the complex. Our results provide interesting insights into calmodulin binding to its kinase targets. The flexibility of the protein may explain the fact that CaM is able to bind many different targets. The large loss of conformational entropy upon CaM:peptide binding cancels the entropy gain due to hydrophobic interactions. This explains why the observed entropic contribution to the binding free energy is small and positive, and not large and negative as expected for a complex with such extensive hydrophobic contacts.

Animals↗

PubMed2001

Calculation of NMR-relaxation parameters for flexible molecules from molecular dynamics simulations.

Comparatively small molecules such as peptides can show a high internal mobility with transitions between several conformational minima and sometimes coupling between rotational and internal degrees of freedom. In those cases the interpretation of NMR relaxation data is difficult and the use of standard methods for structure determination is questionable. On the other hand, in the case of those system sizes, the timescale of both rotational and internal motions is accessible by molecular dynamics (MD) simulations using explicit solvent. Thus a comparison of distance averages ([r(-6)](-1/6) or [r(-3)](1/3)) over the MD trajectory with NOE (or ROE) derived distances is no longer necessary, the (back)calculation of the complete spectra becomes possible. In the present study we use two 200 ns trajectories of a heptapeptide of beta-amino acids in methanol at two different temperatures to obtain theoretical ROESY spectra by calculating the exact spectral densities for the interproton vectors and the full relaxation matrix. Those data are then compared with the experimental ones. This analysis permits to test some of the assumptions and approximations that generally have to be made to interpret NMR spectra, and to make a more reliable prediction of the conformational equilibrium that leads to the experimental spectrum.

Computer Simulation↗

PubMed2005

Study of the Villin headpiece folding dynamics by combining coarse-grained Monte Carlo evolution and all-atom molecular dynamics.

The folding mechanism of the Villin headpiece (HP36) is studied by means of a novel approach which entails an initial coarse-grained Monte Carlo (MC) scheme followed by all-atom molecular dynamics (MD) simulations in explicit solvent. The MC evolution occurs in a simplified free-energy landscape and allows an efficient selection of marginally-compact structures which are taken as viable initial conformations for the MD. The coarse-grained MC structural representation is connected to the one with atomic resolution through a "fine-graining" reconstruction algorithm. This two-stage strategy is used to select and follow the dynamics of seven different unrelated conformations of HP36. In a notable case the MD trajectory rapidly evolves towards the folded state, yielding a typical root-mean-square deviation (RMSD) of the core region of only 2.4 A from the closest NMR model (the typical RMSD over the whole structure being 4.0 A). The analysis of the various MC-MD trajectories provides valuable insight into the details of the folding and mis-folding mechanisms and particularly about the delicate influence of local and nonlocal interactions in steering the folding process.

Algorithms↗

PubMed2005

Molecular dynamics simulations of retinal in rhodopsin: from the dark-adapted state towards lumirhodopsin.

The formation of photointermediates and conformational changes observed in the retinal chromophore of bilayer-embedded rhodopsin during the early steps of the protein activation have been studied by molecular dynamics (MD) simulation. In particular, the lysine-bound retinal has been examined, focusing on its conformation in the dark-adapted state (10 ns) and on the early steps after the isomerization of the 11-cis bond to trans (up to 10 ns). The parametrization for the chromophore is based on a recent quantum study [Sugihara, M., Buss, V., Entel, P., Elstner, M., and Frauenheim, T. (2002) Biochemistry 41, 15259-15266] and shows good conformational agreement with recent experimental results. The isomerization, induced by switching the function governing the dihedral angle for the C11=C12 bond, was repeated with several different starting conformations. From the repeated simulations, it is shown that the retinal model exhibits a conserved activation pattern. The conformational changes are sequential and propagate outward from the C11=C12 bond, starting with isomerization of the C11=C12 bond, then a rotation of methyl group C20, and followed by increased fluctuations at the beta-ionone ring. The dynamics of these changes suggest that they are linked with photointermediates observed by spectroscopy. The exact moment when these events occur after the isomerization is modulated by the starting conformation, suggesting that retinal isomerizes through multiple pathways that are slightly different. The amplitudes of the structural fluctuations observed for the protein in the dark-adapted state and after isomerization of the retinal are similar, suggesting a subtle mechanism for the transmission of information from the chromophore to the protein.

Adaptation, Physiological↗

PubMed2005

Role of lipid charge in organization of water/lipid bilayer interface: insights via computer simulations.

Anionic unsaturated lipid bilayers represent suitable model systems that mimic real cell membranes: they are fluid and possess a negative surface charge. Understanding of detailed molecular organization of water-lipid interfaces in such systems may provide an important insight into the mechanisms of proteins' binding to membranes. Molecular dynamics (MD) of full-atom hydrated lipid bilayers is one of the most powerful tools to address this problem in silico. Unfortunately, wide application of computational methods for such systems is limited by serious technical problems. They are mainly related to correct treatment of long-range electrostatic effects. In this study a physically reliable model of an anionic unsaturated bilayer of 1,2-dioleoyl-sn-glycero-3-phosphoserine (DOPS) was elaborated and subjected to long-term MD simulations. Electrostatic interactions were treated with two different algorithms: spherical cutoff function and particle-mesh Ewald summation (PME). To understand the role of lipid charge in the system behavior, similar calculations were also carried out for zwitterionic bilayer composed of 1,2-dioleoyl-sn-glycero-3-phosphocholine (DOPC). It was shown that, for the charged DOPS bilayer, the PME protocol performs much better than the cutoff scheme. In the last case a number of artifacts in the structural organization of the bilayer were observed. All of them were attributed to inadequate treatment of electrostatic interactions of lipid headgroups with counterions. Electrostatic properties, along with structural and dynamic parameters, of both lipid bilayers were investigated. Comparative analysis of the MD data reveals that the water-lipid interface of the DOPC bilayer is looser than that for DOPS. This makes possible deeper penetration of water molecules inside the zwitterionic (DOPC) bilayer, where they strongly interact with carbonyls of lipids. This can lead to thickening of the membrane interface in zwitterionic as compared to negatively charged bilayers.

Computer Simulation↗