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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Colby, Ralph H.
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Publications (6/6 displayed)
- 2021Rheological response of entangled isotactic polypropylene melts in strong shear flowscitations
- 2020Flow-induced crystallization of poly(ether ether ketone)citations
- 2020Determination of intrinsic viscosity of native cellulose solutions in ionic liquidscitations
- 2020Shear Flow-Induced Crystallization of Poly(ether ether ketone)citations
- 2019Solvent-non-solvent rapid-injection for preparing nanostructured materials from micelles to hydrogelscitations
- 2016Brittle fracture in associative polymers: the case of ionomer meltscitations
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article
Flow-induced crystallization of poly(ether ether ketone)
Abstract
<p>When a semicrystalline polymer melt is processed in intense flow, the nucleation rate can be accelerated and the resultant morphology is transformed to anisotropic structures. These cumulative changes to the crystallization process are referred to as flow-induced crystallization (FIC). In this study, shear flow-induced crystal formations of poly(ether ether ketone) (PEEK) are investigated after applying a short-term shear (γ' = 20 s<sup>-1</sup> and t<sub>s</sub> < 230 s) via rheology and ex situ small-angle X-ray scattering (SAXS) and wide-angle X-ray scattering (WAXS). Using rheology, three types of dynamic response are monitored during FIC: no flow effect, nucleation acceleration, and instant crystal growth without crystallization induction time. Ex situ SAXS is employed with sheared PEEK disks to evaluate the flow-induced lamellar structure and orientation. The short-term shear changes the fraction and degree of lamellar stack orientation, whereas the lamellar structure is barely affected by shear, in terms of the long spacing (L* = 14.6 nm), linear crystallinity (χ<sub>c</sub> = 0.34), and crystalline and amorphous layer thicknesses (L<sub>c</sub> = 5.0 nm and L<sub>a</sub> = 9.6 nm). Ex situ WAXS patterns indicate that PEEK chains (c-axis) are aligned in the shear direction within crystalline domains.</p>