1974
DOI: 10.1080/14786437408213555
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Ductile versus brittle behaviour of crystals

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Cited by 1,527 publications
(418 citation statements)
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“…[42,43,82] The premise of this model is that near-crack-tip stress (and local stress intensity) is modeled by coupling a small array of dislocations, spaced in equilibrium with the crack tip elastic stress field, and including Rice-Thompson dislocation emission. [86] These dislocations shield the singular-elastic stress at the crack tip. Surrounding-tip plasticity is represented by a superdislocation located at the centroid of the highly strained continuum plastic zone, and related to stress intensity.…”
Section: E Threshold For Heacmentioning
confidence: 99%
“…[42,43,82] The premise of this model is that near-crack-tip stress (and local stress intensity) is modeled by coupling a small array of dislocations, spaced in equilibrium with the crack tip elastic stress field, and including Rice-Thompson dislocation emission. [86] These dislocations shield the singular-elastic stress at the crack tip. Surrounding-tip plasticity is represented by a superdislocation located at the centroid of the highly strained continuum plastic zone, and related to stress intensity.…”
Section: E Threshold For Heacmentioning
confidence: 99%
“…These together suggest that the 0.27 MPa m 1/2 stress intensity above in fact may not even be suciently high to emit the ®rst dislocation. This is further reinforced by Rice and Thomson's [35] original calculation of the local stress intensity, k Ie , for dislocation emission in copper. This value is given as 0.32 MPa m 1/2 .…”
Section: Superlayer Induced Film Decohesionmentioning
confidence: 97%
“…But quantification of the rôle of n has so far been lacking. For polycrystalline metals, quantitative analyses [18,19] following Pugh [12] consider the stress state at a crack tip and the local conditions for spontaneous emission of dislocations. In metallic glasses, in contrast, plasticity is mediated by the shear bands.…”
Section: Introductionmentioning
confidence: 99%