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the effect of carbon content of the mechanical properties - McMaster ...

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M.A.Sc. Thesis – E. E. Yang <strong>McMaster</strong> – Materials Science & Engineering<br />

The local stresses in austenite and ε-martensite were also examined as a function<br />

<strong>of</strong> <strong>the</strong> global strain as seen in Figure 6.9. The ε-martensite local stress was above <strong>the</strong><br />

austenite phase indicating <strong>the</strong> ε-martensite was loaded more heavily. The difference<br />

between <strong>the</strong> model and <strong>the</strong> two phases was seen to be less at low levels <strong>of</strong> strain and<br />

increased slightly with strain before reaching constant proportions.<br />

Figure 6.9 Iso-Work Model Local Stress – Global Strain <strong>of</strong> 0.2C Alloy<br />

Global strain in <strong>the</strong> 0.2C alloy and <strong>the</strong> local strains in <strong>the</strong> two phases from<br />

Equation 6.6 were also plotted in Figure 6.10 to show <strong>the</strong> relative contributions <strong>of</strong> each<br />

phase to strain partitioning. Both austenite and ε-martensite were strained equally at low<br />

strains before austenite began contributing more to <strong>the</strong> global strain. This indicated <strong>the</strong><br />

austenite as a s<strong>of</strong>ter phase compared to <strong>the</strong> ε-martensite and <strong>the</strong> difference was seen to<br />

increase with global strain.<br />

local/global stress<br />

1400<br />

1200<br />

1000<br />

800<br />

600<br />

400<br />

200<br />

0.2C alloy<br />

Austenite<br />

martensite<br />

0<br />

0.00 0.05 0.10 0.15 0.20 0.25 0.30 0.35 0.40<br />

global strain<br />

116

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