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Thixoforming : Semi-solid Metal Processing

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212j 6 Modelling the Flow Behaviour of <strong>Semi</strong>-<strong>solid</strong> <strong>Metal</strong> Alloys<br />

Figure 6.46 Simulation results in the container after 553 s:<br />

(a) temperature, K, (b) <strong>solid</strong> fraction, (c) grain density, m 3 ,<br />

(d) grain size, mm, (e) solute concentration, wt%, (f) liquid<br />

velocity, m s 1 , after 93 s.<br />

sudden rise at about 0.6 s as a result of the high supercooling that occurred when the<br />

hot liquid metal reached CP1 and CP2. It fluctuates afterwards as a result of latent<br />

heat release, flow drift and grain transport. The slight decrease in cooling rate at CP1<br />

as per Figure 6.47a results in gradual reduction in grain production rate and n<br />

(Figure 6.47b).<br />

The values of T, f S and n were tracked in the container and the results (Figure 6.48)<br />

manifested the role of the container in this process. The cooling curves in<br />

Figure 6.48a show a relatively higher temperature at the container top compared<br />

with the bottom and the difference diminishes as time proceeds. These results agree<br />

with the experiments of B€unck [47]. The grain size (Figure 6.48b) exhibits a<br />

continuous increase due to temperature losses and grain growth. The grain density<br />

reaches a steady state value of 4.39 10 10 m 3 after complete filling of container at<br />

about 5 s, where the cooling rate is slower and the expected undercooling is much<br />

lower. If the grain density in the container is compared with the outgoing one from<br />

the channel (Figure 6.47b), the former was found to have 1.0 10 10 m 3 more grains.<br />

This means that further nucleation took place during container filling, where its<br />

initial temperature was 60 C.

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