1977
DOI: 10.1002/apmc.1977.050580105
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Blends aus Polyvinylchlorid und chloriertem Polyäthylen. II. Morphologie von Blends aus Polyvinylchlorid und chloriertem Polyäthylen

Abstract: ZUSAMMENFASSUNG:Blends aus Polyvinylchlorid (PVC) und chloriertem Polyathylen (CPE) bilden ein schlagzahes Zweiphasensystem, welches bisher elektronenmikroskopisch nicht untersucht werden konnte. Durch ein neues chemisches Kontrastierungsverfahren wird die Abbildung des Zweiphasensystems im Elektronenmikroskop moglich. Aus den Morphologieuntersuchungen geht hervor, daB zu Beginn der Schmelzverarbeitung des Blends PVCSekundarkorner (5&200 pm) durch die Weichphase in Primarkorner (0,l-1 pm) separiert werden. Dur… Show more

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Cited by 19 publications
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“…The discrepancy between experimental data and theoretical prediction is obvious. Even if one realizes that equation [3] describes the melting point depression experienced by an infinitely large crystal of CH 2 segments in equilibrium with a melt having the mol fraction XcHcl of CHCl-groups and that in reality the melting of rather small crystals has to be described, there remains still a large discrepancy. The theory may be adjusted for the melting of small crystals introducing a size-and surface free energy depending term following the arguments of Eby and Sanchez (16) T~=T °_l-~xcHcl I.Oc.AH °]" [4] Here G is the surface free energy of the top and bottom surfaces of crystal lamellae of the thickness I and the density G. As one realizes from equation [4] this results in a parallel shift of the Flory-line (at constant l) to a new position marked F' in figure 1 assuming that neither l nor…”
Section: The Melting Behavior Of the Copolymersmentioning
confidence: 92%
“…The discrepancy between experimental data and theoretical prediction is obvious. Even if one realizes that equation [3] describes the melting point depression experienced by an infinitely large crystal of CH 2 segments in equilibrium with a melt having the mol fraction XcHcl of CHCl-groups and that in reality the melting of rather small crystals has to be described, there remains still a large discrepancy. The theory may be adjusted for the melting of small crystals introducing a size-and surface free energy depending term following the arguments of Eby and Sanchez (16) T~=T °_l-~xcHcl I.Oc.AH °]" [4] Here G is the surface free energy of the top and bottom surfaces of crystal lamellae of the thickness I and the density G. As one realizes from equation [4] this results in a parallel shift of the Flory-line (at constant l) to a new position marked F' in figure 1 assuming that neither l nor…”
Section: The Melting Behavior Of the Copolymersmentioning
confidence: 92%