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199 mathematical modeling of mold-filling and solidification - Acta ...

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<strong>Acta</strong> Metallurgica Slovaca, 15, 2009, 3 (<strong>199</strong> - 207) 206<br />

where T l <strong>and</strong> T s are the liquidus <strong>and</strong> the solidus temperatures (K), respectively. Another widely<br />

used expression is the Scheil equation, which assumes uniform solute concentration in the liquid<br />

but no diffusion in the solid [23]:<br />

−1/1−k ⎛ T<br />

o<br />

m − T ⎞<br />

f s = 1 − ⎜ ⎟<br />

Tm<br />

T<br />

⎝ − l ⎠<br />

(12)<br />

where T m is the melting point <strong>of</strong> the solvent metal (K),<strong>and</strong> k o is the equilibrium partition<br />

coefficient <strong>of</strong> the alloy.<br />

Eq. (10) defines the heat flux [3] which is released during liquid cooling <strong>and</strong><br />

<strong>solidification</strong>. In classical models, the heat generated after <strong>solidification</strong> is assumed to be zero,<br />

i.e., for T< T s , Q & = 0. However, experimental investigations showed that lattice defects <strong>and</strong><br />

vacancies are condensed in the already solidified part <strong>of</strong> the crystal <strong>and</strong> the enthalpy <strong>of</strong> the solid<br />

increases <strong>and</strong> thus the latent heat will decrease. Based on this fact, another way to represent the<br />

change <strong>of</strong> the solid fraction during <strong>solidification</strong> can be written as [3]:<br />

2<br />

⎡ π ( T − T ) ⎤<br />

( T − T ) + ( Ts<br />

− T )(1 − cos<br />

l<br />

l<br />

l ⎢ ⎥<br />

π<br />

⎣ 2( Ts<br />

− Tl<br />

)<br />

f =<br />

⎦<br />

s<br />

( Tl<br />

− Ts<br />

)(( 1−<br />

2 / π )<br />

(13)<br />

Combining Eqs. (7), (9) <strong>and</strong> (10), the new unsteady state heat conduction equation<br />

can be expressed in the form [4; 23]:<br />

∂ ( ρ c´<br />

T )<br />

= ∇.( k∇<br />

T)<br />

∂ t<br />

(14)<br />

At the range <strong>of</strong> temperatures where <strong>solidification</strong> occurs for binary metallic alloys, the<br />

physical properties will be evaluated taking into account the amount <strong>of</strong> liquid <strong>and</strong> solid that<br />

coexists in equilibrium at each temperature, as shown by Eqs. (9), (10) <strong>and</strong> (14).<br />

3. Conclusions<br />

A comprehensive theoretical basis regarding equations <strong>of</strong> fluid mechanics <strong>and</strong> heat<br />

flow has been shown. Like other CFD problems, the momentum equation, the continuity<br />

equation, <strong>and</strong> the energy equation are the partial differential equations that are essential in the<br />

numerical analysis <strong>of</strong> the casting process. The moving boundary liquid metal/air is modeled<br />

using the VOF method to trace the free surface in <strong>mold</strong> <strong>filling</strong> processes. The latent heat release<br />

during the unsteady <strong>solidification</strong> phenomenon is taken into account as a source term in the<br />

energy equation. The implementation <strong>of</strong> such equations is aimed to furnish important<br />

information such as <strong>filling</strong> dynamics <strong>and</strong> the thermal field along the casting process.<br />

Acknowledgements<br />

The authors acknowledge financial support provided by CNPq (The Brazilian<br />

Research Council), FAPESP (The Scientific Research Foundation <strong>of</strong> the State <strong>of</strong> São Paulo,<br />

Brazil) <strong>and</strong> CAPES - Coordenação de Aperfeiçoamento de Pessoal de Nível Superior.

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