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14). In this case the sample (which was provided by F. E. Buresch) was also loaded slowly in order to generate stable crack growth. The observed relative change in sound velocity as measured by time-of-flight and V{z) tech­ niques varies from sample to sample, but the average change in sound velocity is always larger than the measurement accuracy discussed above. This can easily be understood because each time v where e is the strain and A is the appropriate acousto-elastic constant which has been mea­ sured recently for skimming longitudinal and shear waves in A1 2 0 3 [12] up to strains of about 10" 3 .

Advanced Ceramics II, Elsevier, London, 1987, p. 45. 2 F. E. Buresch, Materialprufung, 29 (1987) 261. 3 R. Knehans and R. Steinbrech, Fortschritts. Ber. Deutsch. Keram. , 1 (1985) 59. 4 E. Babilon, F. E. Buresch, G. Kleist and H. Nickel, in E. ), Proc. Euro. Conf. of Fracture 7, Budapest, 1988, EMAS, Warley, 1988, p. 552. 5 R. Knehans and R. Steinbrech, /. Mater. , 1 (1982)327. 6 J. M. Rowe, J. Kushibiki, M. G. Somekh and G. A. D. Briggs, Philos. Trans. R. Soc. London, Ser. A, 320 (1986) 201.

A. Crosbie, R. J. Dewhurst, A. D. W. McKie and S. B. Palmer, IEEE Trans, Ultrason. Ferroelectr. Freq. Control, 33 (1986) 462. 2 P. Cielo, F. Nadeau and M. Lamontagne, Ultrasonics, 23 (1985)55. 3 P. Cielo, C. K. Jen and X. Maldague, Can. J. , 64 (1986)1324. 4 J. P. Monchalin, Rev. Sci. , 56 (1985) 543. 5 A. Sarrafzadeh-Khoee and J. C. , Rev. Sci. , 57(1986)2321. 6 S. R. J. Brueck, T. F. Deutsch and D. E. Oates, Appl. Phys. , 43 (1983) 157. 7 D. A. Hutchins, F. Hauser and T. Goetz, IEEE Trans. Ultrason.

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