HANSER Hanser Publishers, Munich • Hanser Gardner Publications ...
HANSER Hanser Publishers, Munich • Hanser Gardner Publications ...
HANSER Hanser Publishers, Munich • Hanser Gardner Publications ...
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Temperature T<br />
Figure 5.41 Representation of temperature correction for latent heat [22]<br />
heat conduction. The numerical solution of Equation 3.31 using the correction introduced<br />
by GLOOR [22] was given in [25] on the basis of the method of differences after SCHMIDT<br />
[24]. A computer program for this solution is presented in [3]. The time interval used in<br />
this method is<br />
where<br />
Enthalpy<br />
(5.88)<br />
At = time interval<br />
Ax = thickness of a layer<br />
M = number of layers, into which the slab is devided, beginning from the mid plane of<br />
the slab (Figure 5.42)<br />
The mold temperature and the thermodynamic properties of the polymer are assumed<br />
to be constant during the cooling process. The temperature at which the latent heat is<br />
evolved, and the temperature correction W1 (Figure 5.41) are obtained from the enthalpy<br />
diagram as suggested by GLOOR [22]. An arbitrary difference of about 6 0 C is assigned<br />
between the temperature of latent heat release at the mid plane and the temperature at<br />
the outer surface of the slab.<br />
Figure 5.42 Nomenclature for numerical solution of non-steady state conduction in a slab [25]<br />
s