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Heat transfer during dry spinning of fibers
Authors:Siu Yuen Fok and Richard G Griskey
Institution:(1) Department of Chemical Engineering, Virginia Polytechnic Institute, 24061 Blacksburg, Virginia, USA;(2) Present address: Chemistry Department, Clarkson College of Technology, Potsdam, New York, USA
Abstract:Summary Heat transfer to fibers formed in dry spinning has been subjected to fundamental analysis. Solutions of the equation of energy have been derived and tested with experimental data. Results were deemed satisfactory in view of the accuracy of the experimental data. The present work is believed to yield a good representation of the heat transfer in the dry spinning process.Nomenclature h heat transfer coefficient, cal/cm2 °C sec - k thermal conductivity, cal/cm °C sec - r radial distance, cm - t time, sec - Z axial distance, cm - A surface area, cm2 - A n 
$$(T_0  - T)(a_n \pi )^{\tfrac{1}{2}} \frac{{\sin {\text{ }}a_n }}{{a_n^2 }} - \frac{{\cos {\text{ }}a_n }}{{a_n }};$$
or n-th root of 
$${\text{tan }}a = \frac{{ak}}{{k + h}}$$
- A 0 energy required for solvent evaporation, cal/sec cm3 - C p specific heat cal/gm °C - J 0 Bessel function of first kind, order zero - J 1 Bessel function of first kind, order one - J 2 Bessel function of first kind, order two - N k/(R 2 rgrC p V) - Q volumetric flow rate cm3/sec - R outside radius, cm - T point temperature, °C - T S surface temperature °C - T 0 initial fiber temperature °C - T infin ambient air temperature, °C - 
$$\bar T$$
average fiber temperature, °C - 
$$\bar T$$
1 average fiber temperature of preceding segment, °C - V average fiber velocity relative to air strean, cm/sec - V r radial velocity component, cm/sec - V z axial velocity components, cm/sec - V theta theta direction velocity component cm/sec - W weight of solvent evaporated in a given fiber segment, gms - agr n a solution of the equation J 0(X)=0 - lambda heat of vaporization of solvent, cal/gm - theta theta dimension - phgr r/R - rgr density, gms/cc
Keywords:
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