Physical structure of elastic “hard” fibers
Physical structure of elastic “hard” fibers
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DOI:
10.1080/00222347008217135
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发表时间:
1970-12
期刊:
影响因子:
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通讯作者:
G. R. Quynn;H. Brody;E. S. Sobering;K. K. Park-K.;L. Foley;D. H. Noethe;W. Whitney;R. Pritchart;A. M. Seiminki;D. Hutchison;L. H. Wagner;J. Sumit;K. Sakaku;R. Karneluisson
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文献类型:
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作者:
G. R. Quynn;H. Brody;E. S. Sobering;K. K. Park-K.;L. Foley;D. H. Noethe;W. Whitney;R. Pritchart;A. M. Seiminki;D. Hutchison;L. H. Wagner;J. Sumit;K. Sakaku;R. Karneluisson
It has been found [11 that polypropylene, poly-3-methylbutene-1 and some of its 1-olefin copolymers, and the acetal copolymer Celcon, under conditions of high stress during crystallization from the melt, can be formed into highly crystalline, macroscopic fibers which display an unusually high degree of length recovery from extension (for example, 97% recovery from 100% extension with polypropylene fiber). Some of these materials have been described in patents [la-f], but their physical structure has not been clarified. Early in 1965 this laboratory undertook a comprehensive investigation of the physical properties of this unusual class of materials. Of all high polymer solids previously known, only elastomers of low crystallinity exhibit high elasticity, ie, the ability to retract rapidly and nearly completely from high extensions. We have now found a new class of elastic polymeric solids of high crystallinity that undergo large elastic deformations due to a specific morphology. In our laboratory these materials are referred to as elastic “hard” structures. We have also found [lc] that elastic hard fibers undergo on stretching a marked, mainly reversible, reduction in apparent density, eg, a halving of the unstretched density at 110% extension with certain polypropylene fiber specimens. High-pressure mercury porosimetry confirms microscopic measurements of relative den-sity and indicate that accessible, submicroscopic voids are formed within the fiber on stretching; porosimetry and other measurements indicate that the majority of this void space is readily accessible to gases and liquids. It consists of size units ranging in linear dimensions from several thousand Angstroms downward, the range depending mainly on the amount of extension. Brunauer-Emmet-Tellen gas adsorption measurements likewise indicate a very large increase on stretching of accessible surface area. Electron-microscopic replicas of the surfaces of elastic fibers and films show close-packed lamellae with their normals predominately parallel to the fiber or film extrusion direction. On stretching the elastic materials parallel to the extrusion direction the lamellae tilt and splay apart, creating gaps or crevasses which are believed