Abstract
Ni-30Cr alloy samples were oxidized at temperatures between 500 and 900 °C to investigate the link between the evolution of the microstructure and the chemical composition in the alloy substrate beneath a growing chromia layer. Before oxidation, a layer of ultrafine grains was observed between the surface and a thick lamellar layer. This structure was replaced by some larger recrystallized grains after oxidation. The growth kinetics of the recrystallized grains was described by a parabolic law with a kinetic constant following an Arrhenius law from 500 to 700 °C. For samples oxidized at 800 and 900 °C, all Cr profiles showed a gradient close to the shape predicted by Wagner models. In the samples oxidized between 500 and 700 °C, many Cr profiles showed a two-step shape, with the smaller Cr fraction in the step closer to the alloy/oxide interface. By considering a fast diffusion accelerated by grain boundaries in the zone of recrystallized grains, the two-step shape can be simulated by numerical resolution of diffusion problem.
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Acknowledgements
The authors would like to thank the advice of Kévin Ginestar for oxidation tests and SEM observation, Florence Robaut for SEM-FIB preparation and Thomas Demonchaux for TEM-EDX analysis.
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Appendix: Table of variables
Appendix: Table of variables
Variable | Unit | Description |
---|---|---|
\({d}_{\mathrm{g}}\) and \({d}_{\mathrm{g},0}\) | cm | Grain diameters at time \(t\) and at the initial time |
\(D\) and \({D}_{0}\) | cm−2.s−1 | Diffusion coefficient of Ni or Cr in volume, in dislocations or in grain boundaries and its pre-exponential factor |
\(\widetilde{D}\) | cm−2.s−1 | Interdiffusion coefficient in volume or in grain boundaries or apparent interdiffusion coefficient |
\(e\) | cm | Thickness of the oxide layer |
\({E}_{\mathrm{a}}\) | J.mol−1 | Activation energy |
\(f\) | dimensionless | Volume fraction of dislocations or grain boundaries |
\({J}_{\mathrm{Cr},\mathrm{i}}\) | mol.cm−2.s−1 | Flux of Cr at the alloy/oxide interface |
\({k}_{\mathrm{d}}\) | cm3.s−1 | Kinetic constant for recovery |
\(k\), \({k}_{\mathrm{p}}\) and \({k}_{\mathrm{c}}\) | cm−2.s−1 | Parabolic kinetic constants for grain growth, oxidation and recession processes, respectively |
\(n\) | dimensionless | Exponent of the kinetic law |
\({N}_{\mathrm{Cr}}\) | at% | Molar fraction of Cr at the depth \(x\), at the interface or in the bulk |
\(s\) | dimensionless | Segregation factor |
\(t\) | s | Time |
\(T\) | K | Temperature |
\({V}_{\mathrm{m}}\) | cm3.mol−1 | Molar volumes of the Ni-30Cr alloy or the Cr2O3 oxide |
\(x\) and \({\Delta x}_{\mathrm{m}}\) | cm | Depth in the alloy from the alloy/oxide interface and recession depth, respectively |
\(\delta\) | cm | Grain boundary width |
\({\lambda }_{\mathrm{vol}}\) | cm | Characteristic length of volume diffusion |
\({\rho }_{\mathrm{d}}\) and \({\rho }_{\mathrm{d},0}\) | cm−2 | Density of dislocations at time \(t\) and at the initial time |
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Huang, X., Martinelli, L., Bosonnet, S. et al. Chromium Depletion in a Ni-30Cr Alloy During High-Temperature Oxidation. High Temperature Corrosion of mater. 100, 745–773 (2023). https://doi.org/10.1007/s11085-023-10198-8
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DOI: https://doi.org/10.1007/s11085-023-10198-8