Search results for "Simulation"

showing 10 items of 5095 documents

Monte Carlo and molecular dynamics simulation of the glass transition of polymers

1998

Two coarse-grained models for polymer chains in dense glass-forming polymer melts are studied by computer simulation: the bond-fluctuation model on a simple cubic lattice, where a bond-length potential favors long bonds, is treated by dynamic Monte Carlo methods, and a bead-spring model in the continuum with a Lennard-Jones potential between the beads is treated by Molecular Dynamics. While the dynamics of both models differ for short length scales and associated time scales, on mesoscopic spatial and temporal scales both models behave similarly. In particular, the mode coupling theory of the glass transition can be used to interpret the slowing down of the undercooled polymer melt. For the…

chemistry.chemical_classificationMesoscopic physicsComputer simulationChemistryMonte Carlo methodFOS: Physical sciencesDisordered Systems and Neural Networks (cond-mat.dis-nn)PolymerCondensed Matter - Soft Condensed MatterCondensed Matter - Disordered Systems and Neural NetworksCondensed Matter PhysicsCondensed Matter::Soft Condensed MatterMolecular dynamicsMode couplingSoft Condensed Matter (cond-mat.soft)Entropy (information theory)General Materials ScienceStatistical physicsGlass transition
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Electrospray ion mobility mass spectrometry of positively charged sodium bis[2-ethythexyl)sulfosuccinate aggregates.

2014

Collision cross-sections (CCS) of positively singly and multiply charged aggregates of the surfactant sodium bis(2-ethylhexyl)sulfosuccinate (AOTNa) in the gas phase have been measured by quadrupole ion mobility time-of-flight mass spectrometry. Calibration of the observed drift times to the CCS of the AOTNa non-covalent aggregates was achieved by collecting, under the same experimental conditions, the drift times of a range of singly and multiply charged polyalanine peptides whose CCS had been obtained by conventional ion mobility spectrometry. Together with an obvious increase of the aggregate cross-section with the aggregation number, it was found that the aggregate cross-section increa…

chemistry.chemical_classificationModels MolecularElectrosprayRange (particle radiation)Dioctyl Sulfosuccinic AcidSpectrometry Mass Electrospray IonizationAggregation numberIon-mobility spectrometrySodiumStatic ElectricityAnalytical chemistrychemistry.chemical_elementIon mobility surfactants AOT collision cross section mass spectrometry supramolecular aggregatesGeneral MedicineMass spectrometryAtomic and Molecular Physics and OpticsIonchemistryModels ChemicalComputer SimulationCounterionSpectroscopyEuropean journal of mass spectrometry (Chichester, England)
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The dynamic orientation of membrane-bound peptides: bridging simulations and experiments.

2007

AbstractThe structural organization in a peptide/membrane supramolecular complex is best described by knowledge of the peptide orientation plus its time-dependent and spatial fluctuations. The static orientation, defined by the peptide tilt and a rotation about its molecular axis, is accessible through a number of spectroscopic methods. However, peptide dynamics, although relevant to understand the functionality of these systems, remains largely unexplored. Here, we describe the orientation and dynamics of Trp-flanked and Lys-flanked hydrophobic peptides in a lipid bilayer from molecular dynamics simulations. A novel view is revealed, where collective nontrivial distributions of time-evolvi…

chemistry.chemical_classificationModels MolecularMembranesProtein ConformationLipid BilayersBiophysicsSupramolecular chemistryAnchoringMembrane ProteinsPeptideOrientation (graph theory)CrystallographyMolecular dynamicsMembraneProtein structurechemistryModels ChemicalChemical physicsComputer SimulationLipid bilayerDimyristoylphosphatidylcholinePeptidesBiophysical journal
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Self-Assembling of Peptide/Membrane Complexes by Atomistic Molecular Dynamics Simulations

2007

Abstract Model biological membranes consisting of peptide/lipid-bilayer complexes can nowadays be studied by classical molecular dynamics (MD) simulations at atomic detail. In most cases, the simulation starts with an assumed state of a peptide in a preformed bilayer, from which equilibrium configurations are difficult to obtain due to a relatively slow molecular diffusion. As an alternative, we propose an extension of reported work on the self-organization of unordered lipids into bilayers, consisting of including a peptide molecule in the initial random configuration to obtain a membrane-bound peptide simultaneous to the formation of the lipid bilayer. This strategy takes advantage of the…

chemistry.chemical_classificationModels MolecularMolecular diffusionMembranesChemistryMacromolecular SubstancesMembrane FluidityBilayerLipid BilayersMolecular ConformationBiophysicsPeptideBiological membraneTransmembrane proteinMolecular dynamicsCrystallographyMembraneModels ChemicalQuantum TheoryComputer SimulationLipid bilayerPeptidesPhospholipidsBiophysical Journal
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Numerical model for composite material with polymer matrix reinforced by carbon nanotubes

2008

Due to the high stiffness and strength, as well as their ability to act as conductors, carbon nanotubes are under intense investigation as fillers in polymeric materials. The nature of the carbon nanotube/polymer bonding and the curvature of the carbon nanotubes within the polymer have arisen as particular factors in the efficacy of the carbon nanotubes to actually provide any enhanced stiffness or strength to the nanocomposite. Here the effects of carbon nanotube curvature and interface interaction with the matrix on the nanocomposite stiffness are investigated using nanomechanical analysis. In particular, the effects of poor bonding and thus poor shear lag load transfer to the carbon nano…

chemistry.chemical_classificationNanocompositeMaterials scienceMechanical EngineeringCarbon nanotube actuatorsComposite numbertechnology industry and agricultureMechanical properties of carbon nanotubesmacromolecular substancesPolymerCarbon nanotubeCondensed Matter::Mesoscopic Systems and Quantum Hall EffectCondensed Matter PhysicsCarbon Nanotube Numerical Simulations Composite Materials Nanotechnology.law.inventionCarbon nanotube metal matrix compositesSettore ING-IND/14 - Progettazione Meccanica E Costruzione Di MacchineCondensed Matter::Materials ScienceCarbon nanobudchemistryMechanics of MaterialslawComposite materialMeccanica
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Highly Defined, Colloid‐Like Ionic Clusters in Solution

2012

Many societal challenges at the beginning of the 21st century lead to an apparent and growing need for functional materials and novel ways of materials synthesis and assembly. Rising to the challenge, the utilization of small, self-assembling building blocks for the bottom-up construction of new types of polymers and nanostructures has enjoyed increasing popularity among materials researchers in the recent past. Supramolecular materials like foldamers, surface films, nanoparticles, etc. are created by exploiting noncovalent forces [1] leading to an ordered arrangement of nanoscale building blocks. [2] In the search for new polymers based on noncovalent molecular forces, we are motivated by …

chemistry.chemical_classificationNanostructureChemistrySupramolecular chemistryNanoparticleIonic bondingdynamic light scatteringNanotechnologyself-assemblyGeneral ChemistryPolymerCommunicationsmolecular dynamicsnanoscale electrostaticsMonte Carlo simulationsSupramolecular polymersMolecular dynamicsSelf-assemblyChemistryOpen
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Phase transitions in polymeric systems: A challenge for Monte Carlo simulation

1995

Polymers are more difficult to simulate than small molecule systems, due to the large size of random polymer coils (and their slow relaxation, that is observed when dynamic simulation algorithms are used). However, variation of the chain length N of a flexible polymer chain provides a very useful additional control parameter, allowing stringent tests of theories, and new physical phenomena may emerge. As an example of these concepts, critical phenomena in polymer mixtures are described. It is shown that unmixing of symmetrical mixtures ( N A = N B = N ) is described by an equation for the critical temperature T c ( N ) = aN + b rather than T c ∝ N as claimed by some theories. While for fini…

chemistry.chemical_classificationNuclear and High Energy PhysicsPhase transitionCritical phenomenaMonte Carlo methodCrossoverPolymerAtomic and Molecular Physics and OpticsDynamic simulationchemistryLattice (order)Statistical physicsScalingMathematicsNuclear Physics B - Proceedings Supplements
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Third virial coefficient for 4-arm and 6-arm star polymers

2008

We discuss the computation of the third virial coefficient in polymer systems, focusing on an additional contribution absent in the case of monoatomic fluids. We determine the interpenetration ratio and several quantities that involve the third virial coefficient for star polymers with 4 and 6 arms in the good-solvent regime, in the limit of a large degree of polymerization.

chemistry.chemical_classificationPhysicsMonatomic gasStatistical Mechanics (cond-mat.stat-mech)Polymers and PlasticsOrganic ChemistryMonte Carlo methodFOS: Physical sciencesThermodynamicsPolymerStatistical mechanicsDegree of polymerizationCondensed Matter - Soft Condensed MatterCondensed Matter Physicsmonte carlo simulations; star polymers; statistical mechanics; statistical thermodynamics; virial expansionInorganic ChemistrychemistryVirial coefficientMaterials ChemistryVirial expansionSoft Condensed Matter (cond-mat.soft)Limit (mathematics)Condensed Matter - Statistical Mechanics
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"Dormant" secondary metal-alkyl complexes are not omnipresent.

2006

This theoretical study was inspired by the perpetual debate over the so-called “dormancy” of the active sites in propylene polymerization, i.e., a drop in their activity after a regioerror (2,1-insertion), which was reported to occur in many (although not all) catalytic systems. To explore the range of possible situations, we have selected two homogeneous systems of fundamentally different structure: an octahedral system of C 2 symmetry with a tetradentate O N N O ligand and a bridged indenyl catalyst. This choice was not accidental; it is in these two systems where the experimentalists cannot reach a consensus about dormancy. Our density-functional theory calculations explain why in certa…

chemistry.chemical_classificationPolymerization Special FeatureEngineeringMultidisciplinaryPrimary (chemistry)Ligandbusiness.industryCatalysischemistryOctahedronPolymerizationComputational chemistryDormancySolvent effectsbusinessAlkylSimulationProceedings of the National Academy of Sciences of the United States of America
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Polymer chains confined into tubes with attractive walls: A Monte Carlo simulation

1994

A bead-spring off-lattice model of a polymer chain with repulsive interactions among repeating units confined into straight tubes of various cross sections, DT2, is studied by Monte Carlo simulation. We are also varying the chain length from N = 16 to 128 and the strength of a short-range attractive interaction between the repeating units and the walls of the tube. Longitudinal and perpendicular static linear dimensions of the chains are analyzed, as well as the density profile of repeating units across the tube. These data are interpreted in terms of scaling concepts describing the crossover between three-dimensional and quasi-one-dimensional chain conformations and the adsorption transiti…

chemistry.chemical_classificationPolymers and Plastics530 PhysicsOrganic ChemistryMonte Carlo methodRelaxation (NMR)Polymer530 PhysikCondensed Matter PhysicsMolecular physicsInorganic ChemistrychemistryChain (algebraic topology)Materials ChemistryPerpendicularRadius of gyrationConfined spaceScalingSimulationMacromolecular Theory and Simulations
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