The face centered cubic (FCC) microstructure of austenitic stainless steel is enabled by the inclusion of
nickel (cite). Under normal atmospheric conditions, the
crystal structure of iron is body centered cubic (BCC), also known as alpha-iron or
ferrite. Above approximately 910 °C (1183 K), the crystal structure changes to FCC gamma-iron, or
austenite. By contrast, nickel maintains a FCC crystal structure regardless of temperature. Carbon atoms readily produce carbides from alloyed chromium, forming as precipitates within the metal. the formation of carbides can leech chromium from the Cr2O3 coating of the metal. When worked at cold temperatures or subjected to mechanical stresses beyond the yield point, austenitic steels will
work harden, as dislocations formed within the crystal structure compound upon one another. Additionally, misalignment of crystalline structures results in the formation of body-centered tetragonal (BCT)
martensite, a significantly harder crystal structure of steel. Above temperatures of approximately 480 °C (753 K), deformation becomes plastic as power-law creep occurs, with glide becoming predominant. The transition to climb-plus-glide power law creep is however not distinct, due to the temperature at which austenite forms; at this point, dynamic recrystallization of the metal begins, and creep of the material will accelerate as the steel rapidly becomes more malleable. As a result, these steels are usually not recommended for use above 700 °C for structural purposes, ==See also==