Journal of Applied Polymer Science · 2007 · 28 citations · 37 references
EngineeringNanostructured PolymerPolymer NanocompositesChemistryIsothermal Crystallization KineticsNeat PttPolymersPure PttPolymer MaterialIsothermal CrystallizationTrimethylene TerephthalatePolymer ChemistryMaterials SciencePolymer BlendPolymer MeltMechanical PropertiesNanomaterialsPolymer ScienceNanocomposite
Abstract The isothermal crystallization and subsequent melting behavior of poly(trimethylene terephthalate) (PTT) composites filled with nano‐CaCO 3 were investigated at designated temperatures with differential scanning calorimetry. The Avrami equation was used to fit the isothermal crystallization. The Avrami exponents were determined to be 2–3 for the neat PTT and PTT/CaCO 3 composites. The particles of nano‐CaCO 3 , acting as nucleating agents in the composites, accelerated the crystallization rate, with the half‐time of crystallization decreasing or the growth rate constant (involving both nucleation and growth rate parameters) increasing. The crystallization activation energy calculated from the Arrhenius formula was reduced as the nano‐CaCO 3 content increased from 0 to 2%, and this suggested that nano‐CaCO 3 made the molecular chains of PTT easier to crystallize during the isothermal crystallization process. Subsequent melting scans of the isothermally crystallized composites exhibited triple or double melting endotherms: the greater the content was of nano‐CaCO 3 , the lower the temperature was of the melting peak. The degree of crystallization deduced from the melt enthalpy of composites with the proper concentration of nano‐CaCO 3 was higher than that of pure PTT, but it was lower when the nano‐CaCO 3 concentration was more than 2%. The transmission electron microscopy pictures suggested that the dispersion state of nano‐CaCO 3 particles in the polymer matrix was even when its concentration was no more than 2%, whereas some agglomeration occurred when its concentration was 4%. Polarized microscopy pictures showed that much smaller or less perfect crystals formed in the composites because of the interaction between the molecular chains and nano‐CaCO 3 particles. © 2007 Wiley Periodicals, Inc. J Appl Polym Sci, 2007
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Kinetics of Phase Change. I General Theory
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