By K. Tanaka, S. Kodama and T. Goto (Eds.)
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Extra resources for X-ray Diffraction Studies on the Deformation and Fracture of Solids
9] P. Predecki, A. S. Barret, Adv. X-Ray Analysis, 31, 231-243 (1988).  K. Tanaka, Y. Yamamoto, N. Mine, K. Suzuki and H. Nakagawa, Trans. Japan Soc. Mech. , 56, 402-410 (1990).  V. Hauk and H. Kockelmann, Z. , 68, 719-724 (1977).  E. Kröner, Z. Physik, 151, 504-518 (1958). T. Wu, Int. J. , 2, 1-8 (1966).  T. Mura, Micromechanics of Defect in Solids, pp. 430-433 Martinus Nijhoff, Dordrecht, The Netherlands (1987).  S. Endo and K. Kawata, Trans. Japan Soc. Mech. , A43, 1620-1628 (1977).
Ikeuchi and H. Fujiwara, J. Soc. Mater. Sei. Japan, 31, 547 (1982) (in Japanese).  V. Hauk and E. Macherauch, Adv. in X-Ray Anal, 27, 81 (1984).  Y. Ikeuchi and H. Fujiwara, J. Soc. Mater. Sei. Japan, 32, 271 (1983) (in Japanese). 46 YASUKAZU IKEUCHI ET AL.  Y. Ikeuchi and H. Fujiwara, Proc. 27th Japan Cong. Mater. , p. 153 (1984).  Y. Ikeuchi and H. Fujiwara, Residual Stresses in Science and Technology, E. Macherauch and V. , DGM Informationsgesellschaft Verlag, 1, 523 (1987). Influence of Microstress on X-ray Residual Stress Analysis TAKAO HANABUSA and HARUO FUJIWARA Faculty of Engineering, Tokushima University, 2-1 Minamijosanjima-cho, Tokushima 770, Japan ABSTRACT The criterion of triaxiality in X-ray residual stress analysis is studied in relation to the wavelength of microstress distribution and relaxation of relevant stress components in a near-surface layer.
It can be seen that the matrix thermal stress behavior shown in Fig. 12 is qualitatively the same as that of the fiber FP/Al composite shown in Fig. 10, while there is a quantitative difference in the matrix stresses, probably because of the difference of flow stresses in the matrix. Length measurements of the composite for each state A and N showed that the composite length was reproducible in each stress state, and that the composite in matrix stress state N was longer by 9Ό μτη (0Ό30% in strain) than that in state A .