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Properties of amorphous and crystallizable hydrocarbon polymers. I. Melt rheology of fractions of linear polyethylene
154
Citations
23
References
1979
Year
Crystallizable Hydrocarbon PolymersEngineeringLinear PolyethyleneChemistrySoft MatterIntrinsic ViscositiesAmorphous MaterialsPolymersPolymer MaterialMolecular ThermodynamicsPolymer ProcessingPolymer PhysicRheologyMelt RheologyPlateau Modulus GPolymer ChemistryMaterials ScienceLinear Polyethylene FractionsPhysical ChemistryPlasticityPolymer MeltPolymer SciencePolymer CharacterizationPolymer PropertyPolymer Modeling
Abstract The dynamic moduli G′ (ω) and G″ (ω) for two groups of linear polyethylene fractions (reported M w / M n < 1.2) were measured in the melt state using the eccentric rotating disk method. Values of zero shear viscosity η 0 were obtained and compared with published results on similar fractions. Molecular weight data were converted to a common basis through intrinsic viscosities in trichlorobenzene (TCB) at 135°C. With recent data on M w (light scattering) vs. [η] TCB , for linear polyethylene, the relationship at 190°C, η 0 = 3.40 × 10 −14 ( M w ) 3.60 , was obtained. The flow activation energy E a was 6.4 kcal ( T = 140–195°C). The plateau modulus G at 190°C was determined from the area under the loss modulus peak in one high‐molecular‐weight sample. The value obtained, G = 1.5 8 × 10 7 dyn/cm 2 , corresponds to an apparent molecular weight between entanglements of 1850. The storage compliance J′ (ω) becomes anomalously large at low frequencies. The recoverable compliance J could not be determined for any of the fractions.
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