Defect and Material Mechanics
DOI: 10.1007/978-1-4020-6929-1_9
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Distributed dislocation approach for cracks in couple-stress elasticity: shear modes

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Cited by 9 publications
(27 citation statements)
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“…. The same ratio was also obtained by Sternberg and Muki (1967) for the mode I problem and by Gourgiotis and Georgiadis (2007) for the mode II problem in couple-stress elasticity. Of course, from the physical point of view, the case    is of no interest since the characteristic length is a small quantity.…”
Section: Reduction Of the Crack Problem To A System Of Singular Integsupporting
confidence: 71%
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“…. The same ratio was also obtained by Sternberg and Muki (1967) for the mode I problem and by Gourgiotis and Georgiadis (2007) for the mode II problem in couple-stress elasticity. Of course, from the physical point of view, the case    is of no interest since the characteristic length is a small quantity.…”
Section: Reduction Of the Crack Problem To A System Of Singular Integsupporting
confidence: 71%
“…However, this is not the case in couple-stress elasticity because a discrete climb dislocation produces both normal stresses yy σ and couple-stresses yz m along the dislocation line 0  y . Therefore, it is not possible to satisfy both (41a) and (41b) It is noteworthy that in the mode II crack problem of couple-stress elasticity studied by the present authors (Gourgiotis and Georgiadis, 2007), only a distribution of glide dislocations was indeed sufficient to generate the requisite shear stress yx σ along the crack-faces. This is because a discrete glide dislocation produces neither normal stresses yy σ nor couple-stresses yz m along the crack-line 0  y…”
Section: The Corrective Solutionmentioning
confidence: 74%
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“…It is observed that the couple stress decays rapidly as the distance from the crack-tip increases. Also, it is interesting to note that m xz is bounded at the crack-tip, as in the stationary crack case (Huang et al, 1997;Gourgiotis and Georgiadis, 2007). In particular, the couple-stress m xz takes a finite negative value at the crack tip then increases to a bounded positive maximum, and diminishes monotonically to zero for X >> ℓ, thus recovering the classical solution of linear elasticity.…”
Section: Analytical Representation Of Displacements Stresses and Coumentioning
confidence: 85%