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Frontiers of Chemical Science and Engineering

ISSN 2095-0179

ISSN 2095-0187(Online)

CN 11-5981/TQ

Postal Subscription Code 80-969

2018 Impact Factor: 2.809

Front Chem Eng Chin    2009, Vol. 3 Issue (1) : 26-32    https://doi.org/10.1007/s11705-009-0002-2
RESEARCH ARTICLE
Lamellar thickness transition of melt-crystallized polybuten-1 tetragonal phase: configurational change in chain folding directions
Motoi YAMASHITA()
College of pharmaceutical Sciences, Ritsumeikan University, 1-1-1 Noji-higashi, Kusatsu, Shiga 525-8577, Japan
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Abstract

Lamellar crystal thickness lc of isotactic polybutene-1 (it-PB1) have been investigated for crystallization in the melt over a wide range of crystallization temperature T from 40°C to 90°C by small angle X-ray scattering experiments and density measurements. The crystal thickness lc demonstrates two linear dependences on inverse supercooling and a transition from one dependence to the other has been observed around T = 65°C. Each of the two dependences obeys the nucleation theory in the high and low supercooling ranges, respectively. Chain folding free energy q determined from the low supercooling range is larger than that determined from the high supercooling range. Possible mechanisms for the transition are discussed taking account of entropy of chain folding directions.

Keywords isotactic polybutene-1      tetragonal phase      crystal thickness      melt growth      chain folding      small angle X-ray scattering      nucleation theory      end surface free energy     
Corresponding Author(s): YAMASHITA Motoi,Email:motoi-y@fc.ritsumei.ac.jp   
Issue Date: 05 March 2009
 Cite this article:   
Motoi YAMASHITA. Lamellar thickness transition of melt-crystallized polybuten-1 tetragonal phase: configurational change in chain folding directions[J]. Front Chem Eng Chin, 2009, 3(1): 26-32.
 URL:  
https://academic.hep.com.cn/fcse/EN/10.1007/s11705-009-0002-2
https://academic.hep.com.cn/fcse/EN/Y2009/V3/I1/26
Fig.1  WAXD profiles of -PB1 crystallized at 40°C, 65°C and 90°C plotted against the modulus of the scattering vector . ( = 4πsin, is half the scattering angle, is the wave length used. The diffraction intensity data were taken from Ref. [].) The profiles for samples as crystallized and aged are plotted. Peaks shown in the plots of the as crystallized samples are indexed with 200, 220, 213 reflections of the tetragonal phase. The peaks exhibited in the plots of the aged samples are indexed with 110, 300, 220 reflections of the trigonal phase
Fig.2  Crystallinity plotted against crystallization temperature (The crystallinity data were taken from Ref. [] )
Fig.3  Lamellar crystal thickness and the first-order long period as functions of crystallization temperature . (The data were taken from Ref. [].) The and values are 171 ? and 334 ?, respectively, at 85°C. These values are roughly in agreement with the values of the as crystallized tetragonal crystals reported by Fu et al., = 150 ? and = 300 ? []
Fig.4  Lamellar crystal thickness as a function of the inverse supercooling, (Taken from Ref. [] )
Fig.5  (a) Chain folding directions on facetted crystal growth front. Since chain re-entrant sites are restricted to the 2 neighboring stems along the (100) growth front, there are only two combinations of chain folding-in and chain folding-out directions shown as A and B. A schematic illustration of possible chain re-entrant sites in facetted crystals seen from the crystalline -axis is shown in the inset. (b) Chain folding on kinetically roughened growth front. Since the growth front is rough, chain re-entrant sites can be neighboring 8 stems. Chain can fold-in from neighboring 8 stems and can fold-out into neighboring 7 stems. The number of possible combinations of chain folding-in and folding-out directions is 8×7=56. A schematic illustration of possible chain re-entrant sites in kinetically roughened crystals seen from the crystalline -axis is shown in the inset
Fig.6  Schematic illustrations of chain re-entrant sites (a) in kinetically roughened crystals and (b) in facetted crystals seen from the crystalline -axis when a chain re-entry can skip a stem. Non-adjacent sites are indicated by shadowed regions
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