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Volumn 59, Issue 12, 1999, Pages 8232-8236

Peierls-nabarro model of interfacial misfit dislocation: an analytic solution

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EID: 0344835548     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.59.8232     Document Type: Article
Times cited : (52)

References (49)
  • 6
    • 0000247290 scopus 로고
    • North-Holland, Amsterdam F. R. N. Nabarro
    • J. W. Matthews, in Dislocations in Solids, edited by F. R. N. Nabarro (North-Holland, Amsterdam, 1979), Vol. 2, p. 461.
    • (1979) Dislocations in Solids , vol.2 , pp. 461
    • Matthews, J.W.1
  • 7
    • 85037892656 scopus 로고    scopus 로고
    • F. S. Shien and S. L. Sass, in Metal-Ceramic Interfaces, ibid., p. 258; Y. Ishida, J.-Y. Wang, T. Suga, and S. Tanaka, in Metal-Ceramic Interfaces, edited by M. Rühle, A. G. Evans, M. F. Ashby, and J. P. Hirth (Pergamon Press, Oxford, 1990), p. 234;
    • Y. Ishida, J.-Y. Wang, T. Suga, and S. Tanaka, in Metal-Ceramic Interfaces, edited by M. Rühle, A. G. Evans, M. F. Ashby, and J. P. Hirth (Pergamon Press, Oxford, 1990), p. 234;F. S. Shien and S. L. Sass, in Metal-Ceramic Interfaces, ibid., p. 258;
  • 37
    • 0025421834 scopus 로고
    • (Formula presented) (Formula presented) and (Formula presented) for plane strain. The derivation of expression (3) can refer to Z. Suo and J. W. Hutchinson, Int. J. Fract. 43, 1 (1990).
    • (1990) Int. J. Fract. , vol.43 , pp. 1
    • Suo, Z.1    Hutchinson, J.W.2
  • 38
    • 85037882608 scopus 로고    scopus 로고
    • J. P. Hirth and J. Lothe, Theory of Dislocations, 2nd ed. (Wiley, New York, 1982), p. 732.
    • J. P. Hirth and J. Lothe, Theory of Dislocations, 2nd ed. (Wiley, New York, 1982), p. 732.
  • 47
    • 85037902126 scopus 로고    scopus 로고
    • The linear behavior of (Formula presented) vs (Formula presented) must break down in all cases as R approaches (Formula presented) due to the interaction of dislocations. Here, we choose R in range of (Formula presented) because (Formula presented) occupies more than (Formula presented) of total elastic energy (Formula presented) when (Formula presented)
    • The linear behavior of (Formula presented) vs (Formula presented) must break down in all cases as R approaches (Formula presented) due to the interaction of dislocations. Here, we choose R in range of (Formula presented) because (Formula presented) occupies more than (Formula presented) of total elastic energy (Formula presented) when (Formula presented)


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