1967
DOI: 10.1080/14786436708229253
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Climb kinetics of dislocation loops in aluminium

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Cited by 107 publications
(19 citation statements)
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“…This transition is similar to the NC case in which there was a switch from full dislocations to partial dislocations as the grain size decreased below a critical value [47][48][49][50][51]. For Ni NWs with an SF energy between $0.128 and 0.24 J/m [52,53] and a shear modulus of 93.2 GPa [46], the critical grain size ranged from $11 to 22 nm. When considering the twin thickness as the grain size, it is reasonable that only partial dislocations were observed when the TT was less than 6.5 nm.…”
Section: Discussionmentioning
confidence: 63%
“…This transition is similar to the NC case in which there was a switch from full dislocations to partial dislocations as the grain size decreased below a critical value [47][48][49][50][51]. For Ni NWs with an SF energy between $0.128 and 0.24 J/m [52,53] and a shear modulus of 93.2 GPa [46], the critical grain size ranged from $11 to 22 nm. When considering the twin thickness as the grain size, it is reasonable that only partial dislocations were observed when the TT was less than 6.5 nm.…”
Section: Discussionmentioning
confidence: 63%
“…35,36 In these experiments, the chemical stress remains close to zero because the surfaces are efficient sinks for vacancies. The driving mechanical force iŝ T R zc, whereT is the dislocation line tension, R is the average loop radius, and c is the stacking fault energy.…”
Section: Comparison With Experimental Resultsmentioning
confidence: 81%
“…The fact that double layer loops form at all suggests that the energy of the resulting extrinsic fault is less than twice the intrinsic fault energy. This has been confirmed by comparative annealing experiments on faulted and unfaulted loops in aluminium (Dobson and Smallman 1966) which show that the intrinsic fault energy is about 130 erg cm-2 while the extrinsic fault energy is about 170 erg cm-' (Dobson et al 1967, Kritzinger er a1 1969.…”
Section: Aluminiummentioning
confidence: 77%
“…Considering first the results from dislocation loops, most of the shrinkage experiments have been directed towards a determination of stacking fault energies following the early experiments by Edington and Smallman (1 965). It has been shown that the shrinkage of dislocation loops in aluminium foils is diffusion controlled (Dobson et al 1967). For large loops (loop radius r greater than half the foil thickness) it is appropriate to solve the diffusion equations for cylindrical symmetry and the rate of shrinkage for extrinsically faulted (drldt),, and perfect loops (dr/dtb are given by Dobson and Smallman (1966) and…”
Section: Measurement Of Self Diffusion Parametersmentioning
confidence: 99%