Chain structure and entanglement
It is shown that the entanglement junction may be modeled as a binary hooking contact of Kuhn nodes between two chains. The entanglement behavior is thus determined by chain tortuosity and given by Nv = (1/β)C ∞α, where Nv is the number of real or virtual skeletal bonds in an entanglement strand, C∞...
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Veröffentlicht in: | Journal of polymer science. Part B, Polymer physics Polymer physics, 1989-03, Vol.27 (4), p.723-741 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | It is shown that the entanglement junction may be modeled as a binary hooking contact of Kuhn nodes between two chains. The entanglement behavior is thus determined by chain tortuosity and given by Nv = (1/β)C ∞α, where Nv is the number of real or virtual skeletal bonds in an entanglement strand, C∞ is the characteristic ratio, α = 2 is the number of hooks involved at an entanglement junction, and β = 1/3 is the fraction of binary hooking configurations out of all possible configurations at a binary nodal contact. In other words, we have Nv = 3C ∞2, which is verified experimentally for 44 polymers, covering a wide variety of skeletal, pendant, and stereoisomeric (tacticity) structures. Since C∞ may be estimated by group additivity, the present equation may be used to predict the entanglement behavior from chemical structure. |
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ISSN: | 0887-6266 1099-0488 |
DOI: | 10.1002/polb.1989.090270401 |