Search results for "soft"

showing 10 items of 9809 documents

Origin of the low-frequency plateau and the light-scattering slow mode in semidilute poly(ethylene glycol) solutions

2019

A low-frequency plateau is often found in the rheological spectra of various kinds of semidilute solutions of polymers and other colloids; also, many such solutions have been reported to show slow-modes in their dynamic light scattering autocorrelation functions. Both these observations may lead to the hypothesis of weak associative network structures built by the dissolved polymer chains or colloidal building blocks. To challenge this hypothesis, we conduct a series of comparative studies on semidilute solutions of poly(ethylene glycol) by using classical rheology as well as passive microrheology based on dynamic light scattering, along with structural studies using static light scattering…

chemistry.chemical_classificationMicrorheologyMaterials scienceScatteringRheometer02 engineering and technologyGeneral ChemistryPolymer010402 general chemistry021001 nanoscience & nanotechnologyCondensed Matter PhysicsPlateau (mathematics)01 natural sciencesLight scattering0104 chemical sciencesCondensed Matter::Soft Condensed MatterchemistryDynamic light scatteringChemical physicsStatic light scattering0210 nano-technologySoft Matter
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1988

Phase diagrams were calculated for flowing solutions of polystyrene in trans-decahydronaphthalene assuming that the energy (Es) stored in the sheared state has to be added to the Gibbs energy of mixing; Es is computed from viscometric data (flow curves). The resulting phase diagrams exhibit two maxima in most of the cases instead of only one for the stagnant solutions. A comparison with experimental data (Part 1) shows that the calculated demixing behaviour agrees well for moderate shear rates and concentrations of the polymer. Deviations in the semidilute region, particularly for higher values, are a consequence of the fact that so far no reliable theoretical relation has been given for th…

chemistry.chemical_classificationMineralogyThermodynamicsPolymerGibbs free energyPhysics::Fluid DynamicsCondensed Matter::Soft Condensed Mattersymbols.namesakechemistry.chemical_compoundShear (geology)chemistryPolymer chemistryStored energysymbolsPolystyreneMaximaDissolutionPhase diagramDie Makromolekulare Chemie
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Structure and morphology of liquid-crystalline polymers

2007

Liquid-crystalline phases are characterized by structures intermediate between a three-dimensionally ordered crystal and a disordered fluid. Polymers with liquid-crystalline structures can be obtained from specific monomers containing mesogenic groups with a tendency to form liquid-crystalline phases. These mesogenic groups are either incorporated into the main chain or attached to a chain as side groups. In both cases liquid-crystalline structures, and also enantiotropic liquid-crystalline phases, have been reported. Smectic polymers are characterized by layered structures with long-range order in the direction of the layer normal and two-dimensional short-range order within the layers. Th…

chemistry.chemical_classificationMorphology (linguistics)Materials scienceMesogenGeneral EngineeringPolymerMicroscopic scaleCondensed Matter::Soft Condensed MatterCrystalchemistry.chemical_compoundCrystallographyMonomerchemistryLiquid crystalLayer (electronics)Journal of Polymer Science: Polymer Symposia
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Calculation of the Phase Behavior of Lipids

1998

The self-assembly of monoacyl lipids in solution is studied employing a model in which the lipid's hydrocarbon tail is described within the Rotational Isomeric State framework and is attached to a simple hydrophilic head. Mean-field theory is employed, and the necessary partition function of a single lipid is obtained via a partial enumeration over a large sample of molecular conformations. The influence of the lipid architecture on the transition between the lamellar and inverted-hexagonal phases is calculated, and qualitative agreement with experiment is found.

chemistry.chemical_classificationPartition function (quantum field theory)Quantitative Biology::BiomoleculesStatistical Mechanics (cond-mat.stat-mech)010304 chemical physicsChemistryFOS: Physical sciencesThermodynamics02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesMolecular conformationLarge sampleQuantitative Biology::Subcellular ProcessesCondensed Matter::Soft Condensed MatterHydrocarbonPhase (matter)0103 physical sciencesLamellar structurelipids (amino acids peptides and proteins)Lipid bilayer phase behavior0210 nano-technologyCondensed Matter - Statistical Mechanics
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Influence of polymer flexibility on nanoparticle dynamics in semidilute solutions

2018

The hierarchical structure and dynamics of polymer solutions control the transport of nanoparticles (NPs) through them. Here, we perform multi-particle collision dynamics simulations of solutions of semiflexible polymer chains with tunable persistence length lp to investigate the effect of chain stiffness on NP transport. The NPs exhibit two distinct dynamical regimes - subdiffusion on short time scales and diffusion on long time scales. The long-time NP diffusivities are compared with predictions from the Stokes-Einstein relation (SER), mode-coupling theory (MCT), and a recent polymer coupling theory (PCT). Increasing deviations from the SER as the polymer chains become more rigid (i.e. as…

chemistry.chemical_classificationPersistence lengthCouplingQuantitative Biology::BiomoleculesFlexibility (anatomy)Materials scienceDiffusionStiffnessNanoparticle02 engineering and technologyGeneral ChemistryVolume viscosityPolymer010402 general chemistry021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciences0104 chemical sciencesCondensed Matter::Soft Condensed Mattermedicine.anatomical_structurechemistryChemical physicsmedicinemedicine.symptom0210 nano-technologySoft Matter
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Mapping onto ideal chains overestimates self-entanglements in polymer melts

2017

In polymer physics it is typically assumed that excluded volume interactions are effectively screened in polymer melts. Hence, chains could be described by an effective random walk without excluded volume interactions. In this letter, we show that this mapping is problematic by analyzing the occurrence of knots, their spectrum and sizes in polymer melts, corresponding random walks and chains in dilute solution. The effective random walk severely overrates the occurrence of knots and their complexity, particularly when compared to melts of flexible chains, indicating that non-trivial effects due to remnants of self-avoidance still play a significant role for the chain lengths considered in t…

chemistry.chemical_classificationPersistence lengthMaterials sciencePolymers and PlasticsOrganic ChemistrySegment lengthFOS: Physical sciences02 engineering and technologyPolymerCondensed Matter - Soft Condensed Matter021001 nanoscience & nanotechnologyRandom walk01 natural sciencesInorganic ChemistryCondensed Matter::Soft Condensed Mattersurgical procedures operativeKnot (unit)stomatognathic systemchemistryChemical physics0103 physical sciencesMaterials ChemistrySoft Condensed Matter (cond-mat.soft)010306 general physics0210 nano-technology
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Standard Definitions of Persistence Length Do Not Describe the Local “Intrinsic” Stiffness of Real Polymer Chains

2010

On the basis of extensive Monte Carlo simulations of lattice models for linear chains under good and Θ solvents conditions, and for bottle-brush polymers under good solvent conditions, different me...

chemistry.chemical_classificationPersistence lengthPhysics::Biological PhysicsQuantitative Biology::BiomoleculesPolymers and PlasticsOrganic ChemistryMonte Carlo methodStiffnessPolymerCondensed Matter::Soft Condensed MatterInorganic ChemistrychemistryLattice (order)Materials ChemistrymedicineStatistical physicsPhysics::Chemical Physicsmedicine.symptomWorm-like chainMacromolecules
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Structure of bottle brush polymers on surfaces: weak versus strong adsorption.

2011

Large-scale Monte Carlo simulations are presented for a coarse-grained model of cylindrical molecular brushes adsorbed on a flat structureless substrate, varying both the chain length N of the side chains and the backbone chain length N(b). For the case of good solvent conditions, both the cases of weak adsorption (only 10 to 15% of the monomers being bound to the surface) and strong adsorption (~40% of the monomers being bound to the surface, forcing the bottle brush into an almost 2D conformation) are studied. We focus on the scaling of the total linear dimensions of the cylindrical brush with both chain lengths N and N(b), demonstrating a crossover from rod-like behavior (for not very la…

chemistry.chemical_classificationPersistence lengthQuantitative Biology::BiomoleculesChemistryMonte Carlo methodBrushBackbone chainPolymerSurfaces Coatings and Filmslaw.inventionCondensed Matter::Soft Condensed Matterchemistry.chemical_compoundAdsorptionChemical physicslawPolymer chemistryMaterials ChemistrySide chainPhysical and Theoretical ChemistryScalingThe journal of physical chemistry. B
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Phase Separation of Colloid Polymer Mixtures Under Confinement

2013

Colloid polymer mixtures exhibit vapor-liquid like and liquid-solid like phase transitions in bulk suspensions, and are well-suited model systems to explore confinement effects on these phase transitions. Static aspects of these phenomena are studied by large-scale Monte Carlo simulations, including novel “ensemble switch” methods to estimate excess free energies due to confining walls. The kinetics of phase separation is investigated by a Molecular Dynamics method, where hydrodynamic effects due to the solvent are included via the multiparticle collision dynamics method.

chemistry.chemical_classificationPhase transitionComputer scienceMonte Carlo methodKineticsPolymerCondensed Matter::Soft Condensed MatterSolventContact angleColloidMolecular dynamicschemistryChemical physicsPhase (matter)Thermodynamic limit
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Orientational ordering transitions of semiflexible polymers in thin films: A Monte Carlo simulation

2011

Athermal solutions (from dilute to concentrated) of semiflexible macromolecules confined in a film of thickness D between two hard walls are studied by means of grand-canonical lattice Monte Carlo simulation using the bond fluctuation model. This system exhibits two phase transitions as a function of the thickness of the film and polymer volume fraction. One of them is the bulk isotropic-nematic first-order transition, which ends in a critical point on decreasing the film thickness. The chemical potential at this transition decreases with decreasing film thickness ("capillary nematization"). The other transition is a continuous (or very weakly first-order) transition in the layers adjacent …

chemistry.chemical_classificationPhase transitionMaterials scienceCondensed matter physicsCapillary actionMonte Carlo method02 engineering and technologyPolymer021001 nanoscience & nanotechnology01 natural sciencesCondensed Matter::Soft Condensed MatterchemistryLiquid crystalCritical point (thermodynamics)0103 physical sciencesVolume fractionThin film010306 general physics0210 nano-technologyPhysical Review E
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