Search results for "Phase Transition"

showing 10 items of 1281 documents

Microfluidic Synthesis of Actuating Microparticles from a Thiol-Ene Based Main-Chain Liquid Crystalline Elastomer.

2016

In this article the microfluidic synthesis of strongly actuating particles on the basis of a liquid crystalline main-chain elastomer is presented. The synthesis is carried out in a capillary-based co-flow microreactor by photo-initiated thiol-ene click chemistry of a liquid crystalline monomer mixture. These microparticles exhibit a deformation from a spherical to a rod-like shape during the thermal-initiated phase transition of the liquid crystalline elastomer (LCE) at which the particles’ aspect ratio is almost doubled. Repeated contraction cycles confirm the complete reversibility of the particles’ actuation properties. The transition temperature of the LCE, the temperature range of the …

Phase transitionMaterials sciencePolymers and PlasticsCapillary actionMicrofluidicsmicrofluidicsoft actuator02 engineering and technologycontinuous flow synthesis010402 general chemistryElastomer01 natural sciencesArticlestimuli-responsivelcsh:QD241-441Physics::Fluid Dynamicschemistry.chemical_compoundphoto polymerizationlcsh:Organic chemistryLiquid crystalliquid crystalComposite materialmicrofluidic; microparticles; liquid crystal; stimuli-responsive; soft actuator; thiol-ene; liquid crystalline elastomer; photo polymerization; continuous flow synthesismicroparticlesthiol-eneGeneral ChemistryAtmospheric temperature range021001 nanoscience & nanotechnology0104 chemical sciencesCondensed Matter::Soft Condensed MatterMonomerchemistryliquid crystalline elastomerMicroreactor0210 nano-technologyPolymers
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ABC and BAC triblock copolymers - morphological engineering by variation of the block sequence

1997

Different morphologies and phase transitions of ternary triblock copolymers with different block sequences (ABC and BAC) are discussed qualitatively. The interplay between interfacial energies and elastic energies of the different blocks leads to various morphologies and enhances or prevents mixing of different blocks, depending on composition and topology.

Phase transitionMaterials sciencePolymers and PlasticsChemical physicsBlock (programming)Organic ChemistryPolymer chemistryMaterials ChemistryCopolymerSequence (biology)Condensed Matter PhysicsTernary operationTopology (chemistry)Macromolecular Symposia
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Dielectric properties of 0.4Na0.5Bi0.5TiO3–(0.6-x)SrTiO3–xPbTiO3 solid solutions

2014

Abstract In this paper we present our measurements of the linear and nonlinear dielectric permittivity of 0.4 Na 0.5 Bi 0.5 TiO 3 – ( 0.6 - x ) SrTiO 3 – xPbTiO 3 solid solutions (x = 0, 0.05, 0.1, 0.15). The dielectric anomaly increases in the system with respect to the concentration of lead, showing that interactions between dipolar entities are modified. The system exhibits dipolar-glass-like behaviour at low values of x ( 0 ⩽ x 0.1 ). Relaxor behaviour emerges in the sample where x = 0.1 . Furthermore, a spontaneous first-order phase transition from relaxor to normal ferroelectric is observed at x ⩾ 0.15 . A few peculiar dispersion regions are observed in the ferroelectric phase, which …

Phase transitionMaterials sciencePolymers and PlasticsCondensed matter physicsMetals and AlloysDielectricFerroelectricityElectronic Optical and Magnetic MaterialsCondensed Matter::Materials SciencePhase (matter)Ceramics and CompositesRelaxation (physics)Phase diagramSolid solutionCole–Cole equationActa Materialia
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Orientation and Dynamics of ZnO Nanorod Liquid Crystals in Electric Fields.

2010

ZnO nanorod polymer hybrids (i.e., ZnO nanorods coated with a block copolymer with a short anchor block (dopamine) and a longer solubilizing block of polystyrene (PS)) form liquid crystalline (LC) phases if they are dispersed at high concentration e.g., in a PS oligomer matrix. Due to the high mobility of the low T(g)-matrix the nanorod polymer hybrids show a switching behavior under an applied AC electric field. Hence, the orientation of the nanorod mesogens can be changed from planar (parallel to the substrate) to homeotropic (perpendicular) in full analogy to the switching of low molecular liquid crystals in an electric field. Dielectric measurements show that such a switching is mainly …

Phase transitionMaterials sciencePolymers and PlasticsHomeotropic alignmentDielectricpolystyrenesemiconducting nanorodspressureliquid crystalsLiquid crystalElectric fieldnanostructuresPolymer chemistryMaterials Chemistryarraysnanoparticle polymer compositespolymerschemistry.chemical_classificationbehaviorbusiness.industryOrganic ChemistryPolymermatrixelectric fieldblock copolymersDipolechemistryOptoelectronicsNanorodphasesbusinesscharge-transportMacromolecular rapid communications
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Can Hyperbranched Polymers Entangle? Effect of Hydrogen Bonding on Entanglement Transition and Thermorheological Properties of Hyperbranched Polyglyc…

2016

Melt rheology and thermal phase transition of a series of hyperbranched polyglycerol samples (hbPG) (DB ≈ 60%) in a broad molecular weight range (Mn = 600–440 000 g/mol) were investigated and correlated to both molecular weight and nature of the end group (hydroxyl vs permethylated and trimethylsilylated). The well-characterized and defined flexible polyethers are particularly suitable to shed light on the linear viscoelastic behavior with respect to (i) hyperbranched topology and (ii) hydrogen bond interactions, particularly in comparison to the perfectly linear polyglycerol counterparts studied recently [Osterwinter, C.; Macromolecules 2015, 48, 119−130]. We present a detailed examination…

Phase transitionMaterials sciencePolymers and PlasticsHydrogen bondOrganic ChemistryThermodynamics02 engineering and technology010402 general chemistry021001 nanoscience & nanotechnology01 natural sciencesViscoelasticity0104 chemical sciencesInorganic ChemistryEnd-groupRheologyPolymer chemistryMaterials ChemistryMolecule0210 nano-technologyTopology (chemistry)MacromoleculeMacromolecules
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Dimesogenic ferroelectric polysiloxanes

1994

Dimesogenic polysiloxane [Si(Me) 2 O] m [Si(Me)(R)O] n (R= (CH 2 ) 3 CH(COO[CH 2 ] 11 OPhPhOCOPh(NO 2 )OC * H(Me)C 6 H 13 ) 2 are synthesized by hydrosilylation. The phase transition temperaturs are determined and the ferroelectric properties are investigated

Phase transitionMaterials sciencePolymers and PlasticsHydrosilylationTransition temperatureOrganic ChemistryBiphenyl derivativesFerroelectricitychemistry.chemical_compoundchemistryLiquid crystalPolymer chemistryMaterials ChemistrySide chainMacromolecular Rapid Communications
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Monodomain Liquid Crystal Main Chain Elastomers by Photocrosslinking

2007

A new synthetic strategy for the preparation of macroscopically oriented smectic main chain liquid crystal elastomers (MC-LCE) by the photocrosslinking of laterally functionalized polyesters is presented. X-ray measurements proved the formation of the monodomain and allowed a quantitative determination of the order parameter. The thermo-actuation of our material at the phase transition from the liquid-crystalline to the isotropic phase was demonstrated by temperature dependent measurements of the sample length, showing a fully reversible shape change of � 40%. Mechanical measurements showed that the sample can be stretched by up to 60% along the smectic layer normal without any reorientatio…

Phase transitionMaterials sciencePolymers and PlasticsOrganic ChemistryIsotropyThermodynamicsContext (language use)ElastomerPolyesterLiquid crystalPhase (matter)Polymer chemistryMaterials ChemistryStress relaxationMacromolecular Rapid Communications
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Nanosized shape-changing colloids from liquid crystalline elastomers.

2010

A method to prepare shape-changing nanospheres from liquid crystalline elastomers is reported. The nanosized colloids are prepared by a miniemulsion process. During this process, colloids are prepared from a liquid crystalline (LC) main-chain polyester and subsequently crosslinked into a nanometer-sized LC elastomer. The ability of these LC elastomers to change their shape at the phase transition temperature from the smectic A to the isotropic phase was detected by temperature-dependent transmission electron microscopy. The phase transition-induced shape change leads to strongly shape anisotropic nanosized elastomer particles.

Phase transitionMaterials sciencePolymers and PlasticsPolyestersdigestive oral and skin physiologyOrganic ChemistryNanoparticleElastomerLiquid CrystalsMiniemulsionPolyesterChemical engineeringElastomersTransmission electron microscopyPhase (matter)Polymer chemistryMaterials ChemistryNanoparticlessense organsParticle sizeColloidsParticle SizeMacromolecular rapid communications
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Investigation of Solid-Liquid Phase Transition for Sn-54wt%In Alloy by Positron Anihilation Spectroscopy

1995

The peak coincidence counting rate F(T) was measured for Sn-54wt%In alloy at the temperature range from room temperature to 400°C. It was observed that for both heating and cooling run, F(Τ) parameter changes . in the liquid phase. These changes were related to disintegration of SnII microcrystals. From a simple trapping model the defect disintegration enthalpy, H1,, was calculated. For heating and cooling run, the value of H1 was 0.53 ± 0.03 eV and 0.67 ± 0.07 eV, respectively. For well-annealed and cold rolled samples we find only one component, equal 200 ps, in the lifetime spectrum. PACS numbers: 64.70.Dv, 61.72.Cc, 78.70.Bj.

Phase transitionMaterials sciencePositronEnthalpyAlloyengineeringGeneral Physics and AstronomyCoincidence countingTrappingAtmospheric temperature rangeAtomic physicsengineering.materialSpectroscopyActa Physica Polonica A
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Polymorphism of praseodymium orthovanadate under high pressure

2021

Zircon-type $\mathrm{PrV}{\mathrm{O}}_{4}$ has been studied at high pressures and room temperature by means of synchrotron powder x-ray diffraction. At room temperature, we observed the previously known zircon-to-monazite phase transition at 5.5(4) GPa and a second phase transition from monazite to a monoclinic structure at 12.7(8) GPa, which we identified as a $\mathrm{PbW}{\mathrm{O}}_{4}$-III-type phase. This conclusion is supported by our ab initio calculations, which also predict a scheelite-type phase to be stable at high pressure. Motivated by this finding, we subjected zircon-type $\mathrm{PrV}{\mathrm{O}}_{4}$ samples to high pressure (7 GPa) and temperature (600, 800, and 1000 \if…

Phase transitionMaterials sciencePraseodymiumchemistry.chemical_elementKinetic energyPhysics::GeophysicsCondensed Matter::Materials Sciencechemistry.chemical_compoundCrystallographychemistryAb initio quantum chemistry methodsScheelitePhase (matter)MetastabilityMonoclinic crystal systemPhysical Review B
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