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By Weder R., Exner P. (eds.)
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Example text
METAL BEHAVIOR 49 [14] Z. Marciniak and J. 1. [15] K. Yoshida, K. Yoshii, H. Komorida and K. 1. [16] K. Yoshida, H. Hayashi, K. Miyauchi, Y. Yamamoto and K. Abe, Proc. 8th Biennial Congress IDDRG, Gothenburg, (1972), 258. [17] K. Yoshida, H. Takechi, S. Kuriyama and H. Hayashi, Proc. Biennial Congress IDDRG, ASM, Ann Arbor, (1976), 151. [18] A. K. Ghosh and J. V. , 167. [19] K. Yoshida and K. Miyauchi, Sci. Papers Inst. of Physical and Chemical Research (Tokyo), 60 (1966) 5; Proc. , Liege, (1966) Communication V.
72-74. 56 P. B. MELLOR, A. PARMAR was assumed together with the Levy-Mises flow rule. Although this was known to be theoretically incorrect it was a device often adopted in pre-computer days to obtain strain distributions which were not inconsistent with expected boundary conditions and with experiment. Hill showed that the generalized strain could with little error be taken to be equal to the circumferential strain in the flange. He found that the positions of the particles in the deforming flange showed little dependence on the stress-strain properties of the material, but that there were greater differences in the thickness with the general tendency of work-hardening to reduce the variation in thickness across the annulus at any moment.
Sato, Proc. Int. Conf. Sci. Tech. Iron and Steel, Tokyo, (1971) 837. [10] T. Kobayashi, K. Murata, H. Ishigaki, T. Abe and R. , 841. [11] H. Josselin, M. Tong-Cuong and R. , 845. [12] T. Matsuoka, C. Sudo and M. , 809. [13] For example, M. J. Painter and R. Pearce, Proc. ; S. S. 1; T. Kobayashi, H. Ishigaki and T. 1. METAL BEHAVIOR 49 [14] Z. Marciniak and J. 1. [15] K. Yoshida, K. Yoshii, H. Komorida and K. 1. [16] K. Yoshida, H. Hayashi, K. Miyauchi, Y. Yamamoto and K. Abe, Proc. 8th Biennial Congress IDDRG, Gothenburg, (1972), 258.