Chapter 1 deals with the diameters of twisted filament yarns. Chapter 2 discusses the structures of twisted filament yarn.
In chapter 1 the authors conclude that:
Given the number
n of twist turns per meter, yarn shrinkage ε
y and yarn count
D denier, diamete
R of twisted viscose yarn can be expressed by the following equation:
R=
R0/
K√1-ε
y where
R0 is an assumed diameter when the yarn is assumed to be filled with fibers. and is a constant value for a given yarn.
K is expressed as follows:
K=0.693+0.00122
D+0.000055
n-(
n/150)
-2.25ε
y This empirical formula is applicable in calculating the diameters of viscose and bemberg twisted yarns.
In chapter 2 the authors reach the following conclusions:
The structure of a twisted filament yarn deviates from an ideal helical form. The deviation may be explained thus: (1) As the filaments increase in number, so the deviation becomes greater; (2) the finer the yarn count, the less the deviation; (3) the greater the yarn tension during twisting, the smaller the deviation; (4) the smaller the coefficient of friction between filaments, the greater the deviation; (5) the shape of the cross section of a filament apparently has a bearing on the degree of deviation; (6) the higher the yarn contraction rate, the greater the deviation.
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