Before discussing the oxidation behavior of Ni-Al alloys, it is necessary to review the high-temperature oxidation behavior of pure nickel and pure aluminum. Atkinson et al. [13] conducted isotopic oxidation experiments on pure nickel, and the results showed that after the oxidation, the outer layer of the oxide film was formed by the outward diffusion of Ni, while the inner layer was formed by the inward diffusion of oxygen. The situation of the Ni-Al alloys studied in this article is similar, that is, the outer layer of NiO is formed by the outward diffusion of Ni, and the NiO in the inner layer of NiO + NiAl2O4 is formed by the inward diffusion of oxygen. Due to the slow growth rate of the oxide film on pure aluminum and the thin thickness of the oxide film, it is difficult to conduct labeling experiments. However, a large number of experimental results [14–16] tend to support the dominance of oxygen inward transport. The situation of the Ni-Al alloys studied in this article is similar, that is, Al2O3 layer in the innermost layer of scales and the internal oxidation zone is formed by oxygen inward diffusion.
The Δ G values of the oxidation of nickel and aluminum at different temperatures calculated by the HSC software are shown in Fig. 8. At 900℃, the Δ G values of the oxidation of nickel and aluminum are − 63.9 kJ and − 207.7 kJ, respectively.
Therefore, based on the Vant Hoff isotherm equation, the minimum oxygen pressure required for the oxidation of nickel and aluminum can be calculated by the change of Gibbs free energy of the reaction. Since the activity of solid substances is 1, the equation can be written as:
When ΔG = 0 kJ, the reaction is in equilibrium, and the equation can change to:
From this, it can be calculated that the minimum oxygen pressure required for the oxidation of nickel and aluminum is 1.4×10− 3 Pa and 5.6×10− 10 Pa, respectively. Due to the extremely low oxygen pressure required for the oxidation of Al, Al2O3 can form as an internal oxidation zone below the scales/alloy interface (with an oxygen pressure of 1.4×10− 3 Pa).
Schematic diagram of scales grown on Ni-Al alloys under 0.1 MPa pure O2 at 900℃ is shown in Fig. 9. Internal oxidation of Ni-9Al, Ni-10Al, and Ni-11Al are illustrated in Fig. 9a. It can be seen that when Ni-Al alloys oxidize, Ni diffuses outward to form a NiO layer on the surface of the alloy, and new oxides form on the outer side of the NiO layer. Meanwhile, due to the inward diffusion of oxygen, NiO also forms inside the alloys until the oxygen pressure drops below 1.4×10− 3 Pa. Similarly, because the oxidation of Al is dominated by the oxygen inward transfer, Al2O3 is generated below the alloy interface until the oxygen pressure drops below 5.6×10− 10 Pa. It is worth noting that due to the presence of concentration gradient and the lower system energy after oxidation, the Al element inside the alloy diffuses outward and oxidizes at the oxygen pressure of 5.6×10− 10 Pa, resulting in the enrichment of Al2O3 at this oxygen pressure, followed by the formation of a relatively continuous Al2O3 layer.
Single external oxidation of Ni-13Al and Ni-14Al are illustrated in Fig. 9b. Compared with internal oxidation, the main feature of single external oxidation of Ni-Al alloy is the absence of internal oxidation zone of Al2O3. This is due to the increased Al content in the alloy, resulting in the formation of a protective Al2O3 layer at an oxygen pressure greater than 1.4×10− 3 Pa. The formation of a dense Al2O3 layer causes a sudden drop of oxygen pressure lower than 5.6×10− 10 Pa. An oxygen pressure zone higher than 5.6×10− 10 Pa and lower than 1.4×10− 3 Pa like Fig. 9a does not exist, so internal oxidation of Al cannot happen. The alloys of Ni-13Al and Ni-14Al achieve a transition from internal oxidation to external oxidation due to the increase of Al content. In the near future, further research will be conducted on the specific process and mechanism of Ni-Al alloy's transition from transient oxidation to steady-state oxidation.