On the kinetics of polymer crystallization in opposite-nozzle flow

Citation
H. Janeschitz-kriegl et al., On the kinetics of polymer crystallization in opposite-nozzle flow, RHEOL ACT, 40(3), 2001, pp. 248-255
Citations number
18
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
RHEOLOGICA ACTA
ISSN journal
00354511 → ACNP
Volume
40
Issue
3
Year of publication
2001
Pages
248 - 255
Database
ISI
SICI code
0035-4511(200105)40:3<248:OTKOPC>2.0.ZU;2-1
Abstract
The present work was encouraged by the successes obtained previously in thi s laboratory with short-term shearing experiments on slightly undercooled m elts of i-PP: post-shearing lamellar growth on (inconspicuous) thread-like precursors. For the present purpose (evaluation of the influence of extensi onal flow) the pioneering work by Mackley and Keller is taken as the point of departure. Our own machine of the same type has been adapted for creep e xperiments (adjustment to steady flow in fractions of the time needed in th e original machine). The range of extension rates, where a transition takes place from a mere multiplication of the number of nuclei to the induction of highly oriented structures, appears to be quite narrow in undercooled i- PP melts. In the range of high extension rates (congruent to 50 s(-1)) the critical time for the formation of an oriented structure could not be measu red because of its shortness (less than 0.2 s). It turns out that the flow pattern in the opposite-nozzle machine is far from ideal. A proposal had to be made for a redesign. In spite of the preliminary nature of some of our results, several interesting insights should not be "bottled up". First of all, there is the usefulness of creep flow (because of its fast transition into steady state, after an almost instantaneous compliance). Secondly, the re is the quite unexpected ineffectiveness of lower stretching rates for th e formation of oriented structures. Thirdly, there is the overwhelming infl uence of a change of the geometry: the provisional introduction of trumpet- shaped (nearly hyperbolic) entrance regions to the nozzles caused a remarka ble broadening of the birefringent zone, which was previously observed as a very thin "string" connecting the nozzles. Finally, the almost certain use fulness of the revised machine for other (sometimes purely theological) pur poses, e.g., for steady-state flow birefringence measurements in extensiona l flow should be mentioned.