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Thixoforming : Semi-solid Metal Processing

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homogeneous microstructure and no difference concerning the microstructure was<br />

observed between samples from the edge and centre.<br />

Using a simple modulating valve, the cooling air flow could be altered. With<br />

different lever positions, varying cooling times were achieved. Retrospectively the<br />

heat transfer was determined from measured cooling curves. Eight experiments were<br />

performed. In experiment number 8 the highest cooling rate was achieved by water<br />

cooling. From the middle between the edge and centre of the cast billets, samples<br />

were taken and image analysed, as for the preliminary experiments with MICRESS<br />

simulation.<br />

The results of the image analyses (with the software package IBAS) are given in<br />

Table 9.8. The change in the microstructure with different cooling rates is illustrated<br />

in Figure 9.40. Furthermore, this figure shows the measured frequency distributions<br />

to illustrate the effect of the cooling rates on the microstructures. A transition from a<br />

globular to a dendritic grain shape becomes apparent. Moreover, the microstructure<br />

formed is much finer with higher cooling rates (see Figure 9.40, where the measured<br />

grain amount is plotted against the cooling rate). Because a mixed microstructure<br />

forms during the transition a from globular to a dendritic shape, no clear borderline<br />

could be set; the change from globular to dendritic microstructure is fluent.<br />

To estimate nevertheless the highest possible cooling rate to achieve a useful<br />

globular microstructure, the measured and simulated shape factors were plotted<br />

against the cooling rate (Figure 9.40). For an easier depiction, the reciprocal of the<br />

shape factor from Equation 9.1 was used. As expected, the shape factor decreases with<br />

an increase in cooling rate. The reading points could be approximated by a linear<br />

Table 9.8 Results of the validation experiments for the MICRESS simulations.<br />

Parameter<br />

Experiment No.<br />

1 2 3 4 5 6 7 8<br />

9.4 Rheoroutej353<br />

Average starting temperature a ( C) 607.0 603.5 606.0 608.5 608.0 607.3 607.4 606.7<br />

End temperature a ( C) 585.0 585.0 585.0 585.0 585.0 585.0 585.0 585.0<br />

Cooling duration (s) 335.5 245.5 143.0 147.5 138.5 100.0 83.0 48.0<br />

Cooling duration extrapolated<br />

(613–585 C) (s)<br />

427 372 191 176 169 126 104 62<br />

Cooling rate (K s 1 ) 0.066 0.075 0.147 0.159 0.166 0.223 0.270 0.452<br />

Grain density d (mm 1 ) 72 88 99 104 90 120 120 170<br />

Grain density b,c (mm 1 ) 57 67 76 73 59 82 85 86<br />

Omitted portion c<br />

0.09 0.12 0.12 0.22 0.22 0.25 0.24 0.43<br />

Solid fraction d (%) 54.79 53.94 53.45 54.98 54.62 52.62 50.89 49.63<br />

Averaged shape factor d<br />

0.79 0.76 0.78 0.71 0.69 0.72 0.72 0.63<br />

Average grain diameter d (mm) 81.37 75.52 69.45 68.03 69.57 62.89 61.87 50.93<br />

a Linear cooling condition.<br />

b Without edge-truncated grains.<br />

c Only grains with area 1500 mm 2 .<br />

d Determined using image analysis software; because of ripening effects during quenching, the<br />

measurements may differ from the real microstructure at the quenching temperature, but this effect<br />

is negligible.

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