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Creep-Resistant Steels. Z-phase, inaccurate data. Can only break even at absolute zero. Thermodynamics. Cannot win, can only break even. Cannot reach absolute zero. Goal. Increase as far as is possible, the maximum temperature in the cycle i.e. better materials & engineering.
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Can only break even at absolute zero Thermodynamics Cannot win, can only break even Cannot reach absolute zero
Goal Increase as far as is possible, the maximum temperature in the cycle i.e. better materials & engineering
b a time = t+∆t time = t
Coarsening diffusion r r 2 1 flux a q q concentration aq c r aq 1 c r 2 distance
-6 10 -7 10 -8 10 -9 10 2 3 4 5 6 7 8 9 10 10 10 10 10 10 10 10 10 10 4 2 0 2 3 4 5 6 7 8 9 10 10 10 10 10 10 10 10 10 10 1/3 Mean radius / m 1/2 Time / s -3 Number density 18 10 m Time / s Fujita & Bhadeshia, 2000
1 10 0 10 -1 10 -2 10 1 2 3 4 10 10 10 10 Data from Abe, 1999 Fe-9Cr-W alloys 0W 1W 2W 4W M_23C_6 size / µm Time at 600 °C / h
0.03 0.02 0.01 0.00 0 1 2 3 4 5 M_23 C_6 Mole fraction of phase Laves phase Tungsten / wt%
Multicomponent coarsening Venugopalan & Kirkaldy, 1978
1.8e-19 1.7e-19 1.6e-19 1.5e-19 0 1 2 3 4 5 Coarsening accelerated by tungsten -1 chromium alone 2 Effective diffusivity / m s multicomponent Tungsten / wt%
Multiphase coarsening ? Laves concentration in ferrite q q distance
650 oC Cole & Bhadeshia, 2002