Austenitic stainless steels are an industrially important class of metals that have found use in a myriad of applications.* These metals are characterized by their inherent corrosion resistance and excellent strength and ductility. The latter properties arise from their face-centered cubic (FCC) crystal structure that results from the expansion of the austenite phase field transformation primarily due to large nickel additions and the increased sluggishness of the gamma to alpha phase caused by the large chromium and nickel additions [1]. The hardening in austenitic stainless steels is a combination of solution hardening, interstitial hardening (nitrogen and oxygen additions, in particular), precipitate hardening (MC carbides, where M is one of the metal alloy additions), and, after straining, hardening from the stored dislocation density.
VARIATION OF YIELD STRESS WITH TEMPERATURE AND STRAIN RATE IN ANNEALED MATERIALSBecause austenitic stainless steels are often used at cryogenic temperatures as well as temperatures well above room temperature (RT, where T/T m = 0.163), * Much of the content in this chapter was originally published in Reference 1. This chapter contains minor revisions and some new material (e.g., Section 11.5).* The strain rate for measurements reported in product bulletins is rarely specified. However, the capabilities of standard testing machines imply that these strain rates (usually constant cross head velocity rather than true strain rate) are in the range of 10 −4 -10 −2 s −1 .* Clauss reported in Reference 2 that these data are from U.S. Steel.