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BEHAVIOR AND MECHANISM OF HOT WORK-HARDENING FOR 316L STAINLESS STEEL |
SONG Renbo1); XIANG Jianying1); HOU Dongpo1); REN Peidong2) |
1 School of Materials Science and Engineering; University of Science and Technology Beijing; Beijing 100083
2 Technological Center of Jiuquan Iron $\&$ Steel Co. Ltd.; Jiayuguan 735100 |
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Cite this article:
SONG Renbo XIANG Jianying HOU Dongpo REN Peidong. BEHAVIOR AND MECHANISM OF HOT WORK-HARDENING FOR 316L STAINLESS STEEL. Acta Metall Sin, 2010, 46(1): 57-61.
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Abstract The characteristics of hot work-hardening for 316L stainless steel have been systematically studied through high temperature compression tests on the Gleeble-1500 thermal simulation testing machine. According to Ludwik true stress-strain model, the experimental data has been regressed by using nonlinear fitting method, and the $n$ value in Ludwik model, a comprehensive index which reflects the competitive result between work-hardening and softening, has been calculated with Crussard-Jaoul method. The dynamic recrystallization and twinning were observed by OM and TEM. The experiments reveal that 316L stainless steel is easy to work-hardening during hot deformation, and deformation rate can effect nC-J-ε curves and variation law; There is no peak stress on its true stress-strain curves, but partial dynamic recrystallization has occurred during hot working process. This incomplete softening mechanism can't counteract the effect of hot work-hardening, so the true stress-strain curves still rise with deformation increasing; In addition, twinning occurred during hot working is one of the major mechanisms of hot work-hardening.
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Received: 10 July 2009
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