The heat-stretching process of acrylic fiber on Turbo Stapler has been analyzed by investigating the temperature dependence of the load-elongation properties of that fiber and by building a modelesque theory of heat-transmission process in the heat-stretching zone of Turbo Stapler-with the following results:
(1) The temperature dependence of the load-elongation properties of acrylic fiber is expressible thus: -log
e; ε=6.00-0.509w-0.0334θ ……(1) where ε=elongation w=load (g) θ=temperature (°C)
(2) The temperature of tow in any position in the heat-stretching zone is expressible thus: (a) heat exchanger model θ
x; =Θ-(Θ-θ
o; )exp(-2.68x) ……(2) where θ
x; =temperature of tow at position
x (°C) Θ=temperature of heating plate (°C) θ
o; =initial temperature of tow (°C)
x=distance from entrance to heating plate (m) (b) radiation model 100
4/2T
p;
3={(tan
-1φ
x; -tan
-1φ
0; )+(tan
-1φ
x; -tanh
-φ
0; )}=0.5384x ……(3) where
Tp; =temperature of heating plate (°k)
To; =initial temperature of tow (°k)
Tx; =temperature of tow at position x (°k) φ
x; =
Tx; /Tp; φ
o; =
To; /Tp; x=distance from entrance to heating plate (m)
(3) The load needed to stretch tow is obtainable as follows: w=6.00+log
e; ε-0.0334θ
l; /0.509 where
w=load needed to stretch 3d single fiber (g) ε=stretching ratio (fixed according to gearing) θ
l; =temperature of tow at the exit of heating plate (°C) (obtainable from formula (2) or (3)) The relation between the temperature of heating plates and the load needed to stretch tow is a straight line within the condition of practical use.
(4) The elongation of tow at any position in the heat-stretching zone, with Turbo Stapler under any condition, is obtainable by connecting the results of formulas (1), (2) and (3).
View full abstract