Conclusions
-
(1)
According to the features of dynamic recovery for body-centered cubic metals, the mathematical expression of the stress-strain Curve describing its hot defermation is\(\sigma (\varepsilon ) = \sigma _s \cdot th^{1/2} \left( {\sqrt {\frac{{\mu bMZ}}{{\upsilon _0 }} \cdot \frac{\varepsilon }{\varepsilon }} } \right)\).
-
(2)
The stress-strain expression derived and the experimental result are very consistent.
Similar content being viewed by others
References
Roberts, W., Bergstrom, Y., The stress-strain behaviour of single crystals and polycrystals of face-centered cubic metals-A new dislocation treatment,Acta Metall., 1973, 21(3): 457.
Hallen, H. A., Theory of dynamic recovery in F. C. C.,Metals. Mater. Sci. Eng., 1985, 72(2): 119.
Liu Xiandong, Fang Hongsheng, Cheng Nanping, Dynamic recovery behaviour of mid-temperature austenite area in Low carbon manganese boronacium steel,Materials Science Progress (in Chinese), 1990, 4(4): 324.
Sakai, T., Dynamic recrystallization behaviour,Japanese Iron & Steel Association Symposium Test, 1979, 2: 19.
Sun Dongsheng, Yamane, T., Hirao, K., The dynamic restoration process during hot and tensile deformation of a17Cr ferritic stainless steel,J. Mater. Sci. Lett., 1993, 12: 1716.
Hirsch, P. B., Cambridge extended jogs in dislocations in F. C. C.,Metals. Philos. Mag., 1962, 73(1): 67.
Tarnura, T., Hot deformation behaviour and ausforming of austenite,Iron & Steel (in Chinese), 1985. 20(1): 64.
Author information
Authors and Affiliations
About this article
Cite this article
Sun, D., Li, M., Zou, Y. et al. A model for dynamic recovery of bcc structure. Chin.Sci.Bull. 42, 1211–1215 (1997). https://doi.org/10.1007/BF02882851
Received:
Issue Date:
DOI: https://doi.org/10.1007/BF02882851