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Thixoforming : Semi-solid Metal Processing

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66j 3 Material Aspects of Steel <strong>Thixoforming</strong><br />

the warm transformation, diffusion annealing at temperatures beneath the <strong>solid</strong>us<br />

(1150–1200 C) is necessary. The holding times here are strongly dependent on the<br />

component dimensions [58, 59].<br />

Calculations concerning the disintegration, segregation and element contents of<br />

steels with 1%C and 1.5% Cr during <strong>solid</strong>ification show segregation fractions of<br />

Is(Cr) ¼ 3 4. The segregation fraction is calculated according to Equation 3.10 from<br />

the maximum and minimum carbon contents:<br />

IsðCrÞ ¼ cmax=cmin ð3:10Þ<br />

The segregation fraction increases with rising C content up to maximum 1.5%<br />

carbon and decreases again above this critical value, due to the beginning of carbide<br />

formation. As soon as the carbon content at which carbides can form has been<br />

reached, further addition leads to premature development of eutectic with less<br />

chromium content during <strong>solid</strong>ification. Therefore, the segregation fraction of the<br />

element chromium decreases, so that no development of eutectic carbides results for<br />

steel 100Cr6 [60].<br />

For steel 100Cr6, furthermore, the risk exists that at temperatures from 1140 to<br />

1160 C the material becomes overheated and the grain boundary areas start to<br />

melt [59]. The reason for this is the local enrichment with chromium and carbon in<br />

the surroundings of dissolved, ledeburitic carbide grains, because relatively high<br />

chromium and carbon contents remain in their surroundings after their dissolution<br />

(Figure 3.14) [61].<br />

Important process-relevant material characteristics of the steel 100Cr6 such as<br />

heat-transmission coefficient, dilation coefficient, heat capacity and thermal conductivity<br />

from room temperature up to fusion heat are currently determined by<br />

means of basic experiments. Furthermore, flow curves in the partial liquid state were<br />

established with case-compression experiments [4, 50].<br />

Figure 3.14 Pseudo-binary phase diagram for the Fe–Cr–C system.

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