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 138
( 13 ) over a large number of cycles is not feasible using the experimentally
observed values of By and Sp . Therefore , it is necessary to scale values of lo
and By very carefully to shift the domain to very small values of By and sufficiently
large ...
( 13 ) over a large number of cycles is not feasible using the experimentally
observed values of By and Sp . Therefore , it is necessary to scale values of lo
and By very carefully to shift the domain to very small values of By and sufficiently
large ...
Page 290
According to the equation shown in Figure 2 , the fractional surface coverage is
given by cos 0 a - cos 0 au * cos 0 ai – cos 0 au True changes in X result from
changes in cos 6 values as a result of chemical or physical loss ( evaporation ...
According to the equation shown in Figure 2 , the fractional surface coverage is
given by cos 0 a - cos 0 au * cos 0 ai – cos 0 au True changes in X result from
changes in cos 6 values as a result of chemical or physical loss ( evaporation ...
Page 380
The value of u decreases rapidly as the pressure level increases from the first to
the second level and then tends to level ... The values of n and C are obtained by
the method described earlier from the set of values of F / A and N / A . It was felt ...
The value of u decreases rapidly as the pressure level increases from the first to
the second level and then tends to level ... The values of n and C are obtained by
the method described earlier from the set of values of F / A and N / A . It was felt ...
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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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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