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Thixoforming : Semi-solid Metal Processing

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350j 9 Rheocasting of Aluminium Alloys and Thixocasting of Steels<br />

Table 9.7 Diffusion coefficients, [46].<br />

Element<br />

Mg 1.49 · 10 5<br />

Si 1.38 · 10 5<br />

Ti 1.12 · 10 1<br />

Solid aluminium Liquid aluminium<br />

D0 (m 2 s 1 ) Q (kJ mol 1 ) D0 (m 2 s 1 ) Q (kJ mol 1 )<br />

120.5 1.49 · 10 5<br />

117.6 1.34 · 10 7<br />

260.0 9.90 · 10 5<br />

71.6 0.34<br />

30.0 7.11<br />

36.3 0.10<br />

Content (%)<br />

taken into account during the simulations, averaged over the simulation domain, as<br />

described recently [48].<br />

The grain density was evaluated from micrographs by image analysis. Samples<br />

were taken from the edge and the middle of each billet, etched (Barker method) and<br />

analysed metallographically. A total of 50 pictures (five per sample) were analysed in<br />

respect of the number of globules, and an average grain density of 77 mm 2 was<br />

found (SD ¼ 2.61 mm 2 ). The average spacing of the globules was 114 mm. This<br />

globule density does not represent the seed density directly after pouring, because the<br />

dissolution of small grains due to Oswald ripening was not considered. As a starting<br />

parameter for the simulation, this was accurate enough, especially as in the<br />

simulation only stable grains were considered.<br />

The MICRESS simulations were carried out on a 500 500 mm calculation<br />

domain. Twenty seeds are needed to achieve an average globulitic spacing as<br />

determined from the experimental results.<br />

In order to determine the boundaries of the globular–equiaxed transition from the<br />

simulations, a series of simulations with varying heat flux rate and seed density were<br />

carried out. The heat flux rate was varied from the experimentally determined<br />

0.94–10.0 J s 1 and the grain density from 5 to 40 grains per calculation domain.<br />

The seeds were set at random locations in the calculation domain.<br />

To analyse the results, a shape factor (F) for the simulated grains was calculated by<br />

the following equation [47]:<br />

F ¼ U<br />

ð9:1Þ<br />

4pA<br />

where U is the circumference and A the area of a grain.<br />

For F ¼ 1 all grains are circular and for F > 1 the grains exhibit an increasingly<br />

complex shape. Due to the influence on the viscosity, the shape factor should be

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