Search results for "transition"

showing 10 items of 3988 documents

Nucleotide, Nucleoside, Purine, Pyrimidine, Pteridine

1952

Die Organe erwachsener Tiere enthalten zumeist mehr Ribonucleotide als Desoxyribonucleotide (Tabelle 159). Der Quotient RN : DRN ist in fetalen Geweben kleiner als in erwachsenen. J. Geschwind und C. H. Li fanden ihn in der fetalen Rattenleber zu 0,9, in der Leber neugeborener Ratten zu 1,9 und in der Leber 40 Tage alter Ratten zu 2,8.

chemistry.chemical_classificationPyrimidine analogueTransition (genetics)chemistryPurine/pyrimidinePyrimidine metabolismmedicinePurine nucleoside phosphorylaseNucleotideMolecular biologyNucleosidePteridinemedicine.drug
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Monte carlo simulation of the glass transition of polymer melts

2007

The bond fluctuation model of polymer melts is presented as a reasonable compromise between simulation efficiency and realistic chemical detail. It is shown that inclusion of a potential energy that depends on the length of the effective bonds connecting the effective monomers easily creates a conflict between configurational entropy of dense packing and the energetic tendency of the bonds to stretch. This competition leads to a glass transition of the model, which very well describes many features of real systems.

chemistry.chemical_classificationQuantitative Biology::BiomoleculesMaterials scienceMonte Carlo methodConfiguration entropyThermodynamicsPolymerPotential energyCondensed Matter::Soft Condensed Matterchemistry.chemical_compoundMonomerchemistryGlass transitionSupercoolingBond fluctuation model
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Monte Carlo simulation studies of the interfaces between polymeric and other solids as models for fiber-matrix interactions in advanced composite mat…

1996

As a coarse-grained model for dense amorphous polymer systems interacting with solid walls (i.e., the fiber surface in a composite), the bond fluctuation model of flexible polymer chains confined between two repulsive surfaces is studied by extensive Monte Carlo simulations. Choosing a potential for the length of an effective bond that favors rather long bonds, the full temperature region from ordinary polymer melts down to the glass transition is accessible. It is shown that in the supercooled state near the glass transition an “interphase” forms near the walls, where the structure of the melt is influenced by the surface. This “interphase” already shows up in static properties, but also h…

chemistry.chemical_classificationQuantitative Biology::BiomoleculesMaterials sciencePolymers and PlasticsOrganic ChemistryMonte Carlo methodMineralogyPolymerCondensed Matter PhysicsGyrationAmorphous solidCondensed Matter::Soft Condensed MatterInorganic ChemistrychemistryChemical physicsMaterials ChemistryRadius of gyrationSupercoolingGlass transitionConfined spaceMacromolecular Theory and Simulations
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Polymer-specific effects of bulk relaxation and stringlike correlated motion in the dynamics of a supercooled polymer melt

2003

We analyze dynamical heterogeneities in a simulated “bead-spring” model of a nonentangled, supercooled polymer melt. We explore the importance of chain connectivity on the spatially heterogeneous motion of the monomers. We find that when monomers move, they tend to follow each other in one-dimensional paths, forming strings as previously reported in atomic liquids and colloidal suspensions. The mean string length is largest at a time close to the peak time of the mean cluster size of mobile monomers. This maximum string length increases, roughly in an exponential fashion, on cooling toward the critical temperature TMCT of the mode-coupling theory, but generally remains small, although large…

chemistry.chemical_classificationQuantitative Biology::BiomoleculesMaterials scienceScatteringGeneral Physics and Astronomy02 engineering and technologyPolymer021001 nanoscience & nanotechnology01 natural sciencesExponential functionCondensed Matter::Soft Condensed MatterCrystallographychemistry.chemical_compoundMonomerchemistryChain (algebraic topology)Chemical physics0103 physical sciencesRelaxation (physics)Physical and Theoretical Chemistry010306 general physics0210 nano-technologySupercoolingGlass transitionThe Journal of Chemical Physics
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A Unified Theory of Liquid-Liquid Demixing and Polymer Formation Kinetics

2009

Sickle hemoglobin is a natural hemoglobin mutation with a hydrophobic replacement of a charged aminoacid on the molecular surface. This leads to aggregation into rigid helical structures (“polymerization”), the underlying cause of sickle cell disease. It has also been shown that polymerization occurs in close correspondence with the phase transition of liquid-liquid demixing , or with the critically diverging fluctuations of local concentration occurring in its proximity. Due to this correspondence, polymerization kinetics remarkably appear to exhibit, with respect to demixing temperature, the same universal scaling features shown by amplitudes and lifetimes of fluctuations occurring in pro…

chemistry.chemical_classificationQuantitative Biology::BiomoleculesPhase transitionChemistryKineticsBiophysicsPolymerLight scatteringlaw.inventionCrystallographyPolymerizationlawChemical physicsCrystallizationUnified field theoryScalingBiophysical Journal
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Simulation of Copolymer Bottle-Brushes

2007

The structure of bottle-brush polymers with a rigid backbone and flexible side chains is studied in three dimensions, varying the grafting density, the side chain length, and the solvent quality. Some preliminary results of theoretical scaling considerations for one-component bottle-brush polymers in a good solvent are compared with Monte Carlo simulations of a simple lattice model. For the simulations a variant of the pruned-enriched Rosenbluth method (PERM) allowing for simultaneous growth of all side chains in the Monte Carlo sampling is employed. For a symmetrical binary (A,B) bottle-brush polymer, where two types (A,B) of flexible side chains are grafted with one chain end to the backb…

chemistry.chemical_classificationQuantitative Biology::BiomoleculesPhase transitionLattice model (finance)Polymers and PlasticsOrganic ChemistryMonte Carlo methodPolymerCondensed Matter PhysicsCondensed Matter::Soft Condensed MatterchemistryMean field theoryChemical physicsMaterials ChemistrySide chainCylinderStatistical physicsScalingMacromolecular Symposia
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Simulations of phase transitions in macromolecular systems

2002

Abstract The study of phase transitions in concentrated solutions and melts of flexible or stiff polymers is a computational challenge for computer simulations, since already a single polymer coil exhibits nontrivial structure from the scale of a chemical bond (1 A) to the coil radius (100 A), and for the simulation of collective phenomena huge simulation boxes containing many polymers are required. A strategy to deal with this problem is the use of highly coarse-grained models on a lattice, such as the bond fluctuation model. Several studies employing such models will be briefly reviewed, e.g.: temperature-driven isotropic-nematic phase transition in concentrated solutions of semiflexible …

chemistry.chemical_classificationQuantitative Biology::BiomoleculesPhase transitionMaterials scienceComputer simulationMonte Carlo methodGeneral Physics and AstronomyPolymerCondensed Matter::Soft Condensed MatterchemistryChemical bondHardware and ArchitectureChemical physicsLattice (order)Polymer blendStatistical physicsScalingComputer Physics Communications
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1986

Covalently crosslinked liquid crystalline networks with elastic properties were prepared in isotropic solution from linear liquid crystalline polymers. As linear precursors for the networks were used: (i) polymers with the mesogenic groups in the side groups (polyacrylates and polymethacrylates), (ii) polymers with the mesogenic groups in the main chain (polymalonates) and (iii) polymers with the mesogenic groups in main chain and side groups (“combined liquid crystalline polymers”). In all crosslinked polymers the liquid crystalline phases of the linear polymers are retained. For low degrees of crosslinking (≤2 mol-%) the phase transition temperatures remain nearly unchanged. These elastom…

chemistry.chemical_classificationQuantitative Biology::BiomoleculesPhase transitionMaterials scienceMesogenPolymerElastomerCondensed Matter::Soft Condensed MatterChain (algebraic topology)chemistryLiquid crystalCovalent bondPolymer chemistryPendant groupDie Makromolekulare Chemie
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Phase transitions of single polymer chains and of polymer solutions: insights from Monte Carlo simulations

2008

The statistical mechanics of flexible and semiflexible macromolecules is distinct from that of small molecule systems, since the thermodynamic limit can also be approached when the number of (effective) monomers of a single chain (realizable by a polymer solution in the dilute limit) is approaching infinity. One can introduce effective attractive interactions into a simulation model for a single chain such that a swollen coil contracts when the temperature is reduced, until excluded volume interactions are effectively canceled by attractive forces, and the chain conformation becomes almost Gaussian at the theta point. This state corresponds to a tricritical point, as the renormalization gro…

chemistry.chemical_classificationQuantitative Biology::BiomoleculesPhase transitionMonte Carlo methodThermodynamicsStatistical mechanicsPolymerCondensed Matter PhysicsCondensed Matter::Soft Condensed MatterTricritical pointchemistryPhase (matter)Thermodynamic limitExcluded volumeGeneral Materials ScienceJournal of Physics: Condensed Matter
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Competition between liquid-crystalline ordering and glassy freezing in melts of semiflexible polymers: A monte carlo simulation

1999

We present results of a Monte Carlo simulation of dense melts of semiflexible polymers using the bond-fluctuation model. The chosen Hamiltonian increases the chain stiffness upon cooling which in turn leads to glass-transition like freezing of the polymer mobility. Employing an efficient simulation algorithm, which is able to equilibrate the simulated systems to lower temperature than the Rouse-type algorithm showing the glassy freezing, we are able to observe an isotropic-nematic phase transition. This transition lies above the glass transition temperature one would extrapolate from the observed freezing behavior.

chemistry.chemical_classificationQuantitative Biology::BiomoleculesPhase transitionPolymers and PlasticsChemistryLiquid crystallineOrganic ChemistryMonte Carlo methodThermodynamicsStiffnessPolymerCondensed Matter PhysicsCondensed Matter::Soft Condensed Mattersymbols.namesakeSimulation algorithmMaterials Chemistrymedicinesymbolsmedicine.symptomHamiltonian (quantum mechanics)Glass transitionMacromolecular Symposia
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