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Understanding Chain Folding Morphology of Semicrystalline Polymers Based on Rod-Coil Multiblocks Model

Abstract

We employ rod-coil multiblocks molecular chain model to investigate the chain folding behavior, which is a significant characteristic in semicrystalline polymers, by using the method of the self-consistent field theory (SCFT). Polymer chains with different conformations in crystalline and amorphous regions are described by rigid rod chains and flexible Gaussian chains, respectively. At present, we concentrate on the thermodynamic behaviors of polymer semi-crystals after the formation of initial lamellar crystals. A new mechanism for lamellar thickening is proposed to realize that the end of lamellar thickening depends on the crystallinity degree. In other words, it is impossible for lamellae to develop into extended-chain crystals by means of lamellar thickening if crystallinity is limited to a certain degree. We further discuss the competition between crystalline and amorphous regions and its influence on the crystallization behaviors such as the formation of double lamellae, chain tilt, the density anomalies and adjacent re-entry. The synergistic influences of driving force of crystallization, interfacial energy and crystallinity degree on the chain folding behavior are also investigated when the density anomalies in amorphous regions are excluded out. Our model demonstrates advantages in accurately describing the mesoscopic layered structures of semicrystalline polymers based upon microscopic chain model and provides at least a semi-quantitative thermodynamic picture for the chain folding.

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Publication details

The article was accepted on 10 Oct 2017 and first published on 10 Oct 2017


Article type: Paper
DOI: 10.1039/C7SM01892D
Citation: Soft Matter, 2017, Accepted Manuscript
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    Understanding Chain Folding Morphology of Semicrystalline Polymers Based on Rod-Coil Multiblocks Model

    F. Q. Liu, T. Sun, P. Tang, H. Zhang and F. Qiu, Soft Matter, 2017, Accepted Manuscript , DOI: 10.1039/C7SM01892D

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