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 128
The constant Ky is given by K ; = key cap - ) = A ' exp ( - AFT ) ( 1 ) where k is the
transmission coefficient assumed to be unity for temperatures much above
absolute zero , k is Boltzmann ' s constant , h is Plank ' s constant , T is absolute ...
The constant Ky is given by K ; = key cap - ) = A ' exp ( - AFT ) ( 1 ) where k is the
transmission coefficient assumed to be unity for temperatures much above
absolute zero , k is Boltzmann ' s constant , h is Plank ' s constant , T is absolute ...
Page 130
[ 4 ] , while describing the breakage phenomena in threads under constant load ,
introduced the concept of slippage of fibers ( or molecules for the microscopic
response ) as part of the mechanism of material failure . Accordingly , for
sufficiently ...
[ 4 ] , while describing the breakage phenomena in threads under constant load ,
introduced the concept of slippage of fibers ( or molecules for the microscopic
response ) as part of the mechanism of material failure . Accordingly , for
sufficiently ...
Page 265
The dynamic mechanical properties were measured at a constant frequency of 1
Hz and a constant oscillation amplitude of 0 . 3 mm ( peak - peak ) using a Du
Pont Instruments 983 dynamic mechanical analyzer interfaced to a 9900 Series ...
The dynamic mechanical properties were measured at a constant frequency of 1
Hz and a constant oscillation amplitude of 0 . 3 mm ( peak - peak ) using a Du
Pont Instruments 983 dynamic mechanical analyzer interfaced to a 9900 Series ...
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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