Computers in Materials Technology. Proceedings of the by T. Ericsson

By T. Ericsson

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Additional info for Computers in Materials Technology. Proceedings of the International Conference Held at the Institute of Technology, Linköping University, Sweden, June 4–5, 1980

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5. CIMT d _l 1 5 10 OBSERVED INFLECTION PT. (SIXTEENTHS) Comparison of predicted and observed i n f l e c t i o n points. 8640 - ~~~~* ^ ν ^ · 20 - 10 - · 1340 ·—-£—_·_ — - * J 1 3 1 1 16 -i -H ^ — - ? 4 I 4 5 ^^* oc I DATA - · 1541 1 1 24 1 - DEPTH (SIXTEENTHS) Fig. 6. Comparison of predicted and observed Jominy curves for non-boron heats. 16 24 DEPTH (SIXTEENTHS) Fig. 7. Comparison of predicted and observed Jominy curves for boron heats. 41 150 o 100 Lü O Û LU ÛC a. I 50l· 50 100 KSI -OBSERVED 150 Fig.

However, in CASIS, many non-linear empirical terms have been added so as to more accurately represent the alloy synergisms. S. g. Fig. , Fig. 4 ) . From the velocity and CCT start curves it is then possible to estimate the inflection point or half(3) hardness depth of the corresponding Jominy curvev ' . Fig. 5 shows a comparison of predictions and observations (as estimated for the published H-bands) for the Bethlehem set of 9 steels. CASIS combines calculations such as the foregoing with empirical, (3) carbon-dependent Jominy curve shapes to yield a general predictor^ '.

11 a after quenching. Fig. 10 Phase composition after quenching. DISCUSSION As pointed out above, the numerical instruments for the problem at hand seem to be well developed. More difficulties seem to be involved when it comes to the type of material properties needed (such as yield strengths and hardening constants for separate phases, and so on). From the numerical examples given above the author has learnt that especially the properties of the martensitic phase will affect the final results considerably.

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