2004
DOI: 10.1016/j.jallcom.2004.02.053
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Thermodynamic modeling of oxidation of Al–Cr–Ni alloys

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Cited by 70 publications
(36 citation statements)
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“…The Raman peak at 981 cm -1 wavenumber is due to the symmetric stretching mode, whilst the Raman peak at 1051 cm -1 is as a result of the asymmetric stretching mode [30]. A broad peak at approximately 840cm -1 wavenumber is believed to be due to molecular vibrations of SO 4 2-ions. Co 3 O 4 was detected on the surface of the two Co-containing alloys, Alloy P420 and Alloy P421.…”
Section: Raman Analysismentioning
confidence: 98%
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“…The Raman peak at 981 cm -1 wavenumber is due to the symmetric stretching mode, whilst the Raman peak at 1051 cm -1 is as a result of the asymmetric stretching mode [30]. A broad peak at approximately 840cm -1 wavenumber is believed to be due to molecular vibrations of SO 4 2-ions. Co 3 O 4 was detected on the surface of the two Co-containing alloys, Alloy P420 and Alloy P421.…”
Section: Raman Analysismentioning
confidence: 98%
“…Two prominent peaks that are similar to all the investigated alloys occur within the 1026-1032cm -1 and 1048-1062cm -1 ranges. The peaks were assigned to molecular vibrations of SO 4 2-ions. Sulphates form prints in the 900-1250cm -1 and 570-680 cm -1 range.…”
Section: Raman Analysismentioning
confidence: 99%
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“…1 The excellent oxidation stability of the stainless steel is closely related to the formation of the thermodynamically stable oxide layer, restraining the diffusion of the metal atoms from the matrix and slowing the oxidation rate. [2][3][4] As the common oxide layers, the Cr 2 O 3 -based protective scale can prevent stainless steels from oxidizing in hightemperature applications. However, such scale will be destroyed under water-steam environment when the service temperature is higher than 650 C because of the formation of volatile Cr x (OH) y species, thus losing its protective role and causing the failure of the stainless steels.…”
Section: Introductionmentioning
confidence: 99%