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Volumn 85, Issue 1, 2000, Pages 118-121

Continuum field description of crack propagation

Author keywords

[No Author keywords available]

Indexed keywords

AMORPHOUS MATERIALS; BRITTLENESS; CONTINUUM MECHANICS; CRACK INITIATION; CRYSTAL DEFECTS; ELASTICITY; FRACTURE TOUGHNESS; MATHEMATICAL MODELS;

EID: 0034227516     PISSN: 00319007     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevLett.85.118     Document Type: Article
Times cited : (258)

References (35)
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    • note
    • We assume incompressibility condition (divv = 0).
  • 29
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    • 1 cannot be interpreted as the hydrostatic pressure due to thermal expansion. Although the temperature at the crack tip can be of the order of several hundred degrees, the thermal equilibrium is unlikely to be achieved at the crack tip; see, e.g., K. N. G. Fuller, P. G. Fox, and J. E. Field, Proc. R. Soc. London A 341, 537 (1975); J. A. Kallivayalil and A. T. Zender, Int. J. Fract. 66, 99 (1994).
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    • 1 cannot be interpreted as the hydrostatic pressure due to thermal expansion. Although the temperature at the crack tip can be of the order of several hundred degrees, the thermal equilibrium is unlikely to be achieved at the crack tip; see, e.g., K. N. G. Fuller, P. G. Fox, and J. E. Field, Proc. R. Soc. London A 341, 537 (1975); J. A. Kallivayalil and A. T. Zender, Int. J. Fract. 66, 99 (1994).
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    • note
    • The interaction with sound can be reduced by introducing additional damping term ∼u̇ to the right-hand side of Eq. (1).


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