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Thixoforming : Semi-solid Metal Processing

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Figure 5.14 The density of 100Cr6. The dashed curve shows<br />

the density in the case when austenite is retained metastably<br />

below its stable range.<br />

X210CrW12, thus relieving the situation somewhat. The melting behaviour can be<br />

expected to be different from that of X210CrW12. It is unclear which sites are more<br />

preferred for nucleation of the liquid. The more probable are grain boundaries and<br />

non-metallic inclusions. The coarseness of the microstructure is probably controlled<br />

by the (austenite) grain size, which can be rather coarse, leading to large globules.<br />

Further nucleation of liquid droplets within the globules, in particular when they are<br />

large, may be possible by self-blocking remelting as described in Chapter 2 and by<br />

Kleiner et al. [22]. Reducing the austenite grain size appears to be an effective way to<br />

reach an acceptably small globule size with no or limited internal droplets [23].<br />

5.4<br />

Calculations for the High-speed Steel HS6-5-2<br />

5.4 Calculations for the High-speed Steel HS6-5-2j163<br />

So far, only a relatively small amount of work has concerned the high-speed steel<br />

HS6-5-2 (or any other high-speed steel). The physical metallurgy of this steel, as for<br />

other high-speed steels, is very complex, involving several different carbides. It also<br />

shows very strong microsegregation, making it difficult to produce using conventional<br />

casting. Here, semi-<strong>solid</strong> processing could open up new possibilities. A<br />

calculated temperature versus mass% C phase diagram is shown in Figure 5.15.<br />

The interesting phase field here is the one marked g þ MC þ M 6C. This shows the

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