Science and Technology of Fibers and Related Materials: Proceedings of the Fiber Society 50th Anniversary Technical Conference Held in Princeton, New Jersey, August 19-23, 1990 |
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Page 326
That is , the deformation energy density at a material point P depends only on
values taken at P by the functions defining the initial and final configurations of
the body together with many of their derivatives . In the simplest class of problems
...
That is , the deformation energy density at a material point P depends only on
values taken at P by the functions defining the initial and final configurations of
the body together with many of their derivatives . In the simplest class of problems
...
Page 364
Carpet body is a relatively new term in the literature and deserves additional
explanation . Expert graders have long evaluated carpet body in new styles and
yarns based on the carpet sample resistance when compressed between their ...
Carpet body is a relatively new term in the literature and deserves additional
explanation . Expert graders have long evaluated carpet body in new styles and
yarns based on the carpet sample resistance when compressed between their ...
Page 368
The unique advantage of the high shrink blend lies in its ability to completely
avoid the appearance retention / body trade - off defined above for conventional
carpet yarns . Carpet body actually increases with increased post - heatset
plytwist ...
The unique advantage of the high shrink blend lies in its ability to completely
avoid the appearance retention / body trade - off defined above for conventional
carpet yarns . Carpet body actually increases with increased post - heatset
plytwist ...
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Contents
M | 33 |
Strain Rate Effects in Ultrastrong Polyethylene Fibers and Composites | 45 |
Morphology and Near Tm Behavior of High Performance Ultrahigh | 67 |
Copyright | |
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Common terms and phrases
amorphous analysis angle appearance Applied behavior bending blend body braided break calculated carpet cellulose compared composite compression constant cotton crystalline crystallization curve decrease deformation density dependence described determined developed diameter direction discussed distance distribution draw effect elastic energy experimental extension fabric factor failure fiber Figure filament finish force frictional function geometry given heat higher improved increase indicated initial length liquid load lower m/min material measured mechanical method modulus nylon observed obtained occurs orientation parameter polyester polymer present pressure problem produced properties range ratio reduced relative resistance sample scanning shape shear shown in Figure shows solution specimen speed spinning spun strain strength stress structure surface Table temperature tenacity tensile tension Text treated treatment twist unit untreated values variability yarn