TY - JOUR
T1 - Strain induced martensite formation characteristics of austenite stainless steel during various loading conditions
AU - Okayasu, M.
AU - Fukui, H.
AU - Ohfuji, H.
AU - Shiraishi, T.
PY - 2014/3
Y1 - 2014/3
N2 - The strain induced martensitic transformation (SMT) of the austenite stainless steel (SUS 304) under cyclic loading and static loading was investigated directly using electron backscattered diffraction. Two different SMT characteristics are observed, which are attributed to the differences of plastic and twinning deformation. The maximum cyclic stress has a strong influence on the SMT. The total area fraction of the Fe-α' phase increases significantly when the maximum cyclic load is >80% σUTS. In other words, the SMT is apparently absent when the samples are loaded with less than σmax=70% σUTS, although such samples are fractured completely. Moreover, there is a clear R ratio effect on the SMT. For example, the loading condition R=-1 gives rise to a strong SMT compared to R=0·1 due to the more severe strain caused by the compressive stress. In contrast, no clear frequency effect (1 versus 30 Hz) on the SMT is detected, which may be attributed to the same maximum cyclic stress. Like the SMT characteristics under cyclic loading, the proportion of Fe-α' phase shows no clear increase until the sample is loaded statically to a tensile stress <70% σUTS.
AB - The strain induced martensitic transformation (SMT) of the austenite stainless steel (SUS 304) under cyclic loading and static loading was investigated directly using electron backscattered diffraction. Two different SMT characteristics are observed, which are attributed to the differences of plastic and twinning deformation. The maximum cyclic stress has a strong influence on the SMT. The total area fraction of the Fe-α' phase increases significantly when the maximum cyclic load is >80% σUTS. In other words, the SMT is apparently absent when the samples are loaded with less than σmax=70% σUTS, although such samples are fractured completely. Moreover, there is a clear R ratio effect on the SMT. For example, the loading condition R=-1 gives rise to a strong SMT compared to R=0·1 due to the more severe strain caused by the compressive stress. In contrast, no clear frequency effect (1 versus 30 Hz) on the SMT is detected, which may be attributed to the same maximum cyclic stress. Like the SMT characteristics under cyclic loading, the proportion of Fe-α' phase shows no clear increase until the sample is loaded statically to a tensile stress <70% σUTS.
KW - Cyclic loading
KW - Plastic deformation
KW - Stainless steel
KW - Static loading
KW - Strain induced martensitic transformation
KW - Twin deformation
UR - http://www.scopus.com/inward/record.url?scp=84893298456&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=84893298456&partnerID=8YFLogxK
U2 - 10.1179/1743284713Y.0000000353
DO - 10.1179/1743284713Y.0000000353
M3 - Article
AN - SCOPUS:84893298456
SN - 0267-0836
VL - 30
SP - 301
EP - 308
JO - Materials Science and Technology
JF - Materials Science and Technology
IS - 3
ER -