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Flow-induced crystallization of polypropylene STW progress, 21th of september 2011 Tim van Erp , Gerrit Peters. overview. non-isothermal, multi-phase crystallization effects of cooling rate effects of pressure flow-induced (non-isothermal, multi-phase) crystallization experimental part
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Flow-induced crystallization of polypropyleneSTW progress, 21th of september 2011Tim van Erp, Gerrit Peters
overview • non-isothermal, multi-phase crystallization • effects of cooling rate • effects of pressure • flow-induced (non-isothermal, multi-phase) crystallization • experimental part • modeling part; discussion on parameters processing structure properties
PVT apparatus A = Outer pistonB = Inner rotating piston C = SampleD = Teflon sealing ring E = Cooling channelsF = Cooling channelsG = Thermocouples
processing protocol: FIC experiments Annealing 10 min @ 250°C Compressed air cooling @ ~1°C/s Isobaric mode Pressures: 100 – 500 – 900 – 1200 bar Short term shearing of ts = 1s Shear rates: 3 - 10 – 30 – 100 – 180 s-1 ∆T = Tm(p) – Tshear = 30 - 60°C
analysis PVT data normalizedspecific volume dimensionlesstransition temperature
analysis PVT data Deborah number (‘strength of flow’) WLF Temperature shift Pressure shift normalizedspecific volume dimensionlesstransition temperature Shear temperature
dimensionless transition temperature dimensionlesstransition temperature
flow regimes under non-isothermal conditions from spherulitic morphology to oriented structures
flow regimes under non-isothermal conditions saturation in crystallization temperature
overview • non-isothermal, multi-phase crystallization • effects of cooling rate • effects of pressure • flow-induced (non-isothermal, multi-phase) crystallization • experimental part • modeling part • quiescent crystallization • flow-inducedcrystallization
quiescent crystallization space filling Schneider rate equations Avrami equation nucleation density individualgrowth rate ‘number’ ‘radius’ ‘surface’ ‘undisturbed volume’ ‘real volume’
flow-induced crystallization model total nucleation density (flow-induced) nucleation rate shish length (L) growth rate equations Avrami equation for ‘length’ ‘surface’ ‘undisturbed volume’ ‘real volume’
flow-induced crystallization model total nucleation density (flow-induced) nucleation rate shish length (L) growth rate equations Avrami equation for ‘length’ ‘surface’ ‘undisturbed volume’ ‘real volume’ experiment model
flow-induced crystallization model total nucleation density (flow-induced) nucleation rate shish length (L) growth rate equations Avrami equation very laborious and inaccurate work F. Custódio, PhD Thesis, 2008
FIC regimes total nucleation density (flow-induced) nucleation rate shish length (L) growth Avrami equation
prediction of FIC regimes Mismatch between experimental results and model in oriented regime
parameters gn and gl plane equation scaling parameter aT, aPrheological shift factors gn and gl arbitrary function of T and p?
critical stretch shish length (L) growth
critical stretch new definition for critical stretch criterium?
critical stretch new definition for critical stretch criterium?
prediction of FIC regimes Good agreement between experimental results and model
conclusions • characterization of flow enhanced (point-like) nucleation regime over wide range of processing conditions • characterization of FIC of oriented structures regime over wide range of processing conditions • extended dilatometry (PVT) proven to be a powerfull tool in characterizing flow induced crystallization