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HANSER Hanser Publishers, Munich • Hanser Gardner Publications ...

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Table 3.1 Coefficients of Heat Penetration of Mold Material and Resin [8]<br />

Material<br />

Beryllium copper (BeCu 25)<br />

Unalloyed steel (C45W3)<br />

Chromium steel (X40Crl3)<br />

Polyethylene (HDPE)<br />

Polystyrene (PS)<br />

The approximate values for steel are<br />

A =50W/(m-K)<br />

p =7850kg/m 3<br />

c = 0.485 kj/(kg <strong>•</strong> K)<br />

The coefficient of heat penetration b<br />

3.3 Heat Conduction with Dissipation<br />

The power created by the tangential forces in the control volume of the fluid flow is<br />

denoted as dissipation [9]. In shear flow the rate of energy dissipation per unit volume is<br />

equal to the product of shear force and shear rate [ 10]. The power due to dissipation [11]<br />

therefore is:<br />

From the power law we get<br />

For a Newtonian fluid with n - 1 we obtain<br />

Coefficient of heat penetration b<br />

Ws 05 Hi 2 KT 1<br />

17.2 <strong>•</strong> 10 3<br />

13.8 <strong>•</strong> 10 3<br />

11.7- 10 3<br />

0.99 <strong>•</strong> 10 3<br />

0.57 <strong>•</strong> 10 3<br />

(3.46)<br />

(3.47)<br />

(3.48)<br />

The applicable differential equation for a melt flow between two plates, where the upper<br />

plate is moving with a velocity Ux (Figure 2.4) and the lower plate is stationary [11] is<br />

(3.49)

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