2004
DOI: 10.1016/j.msea.2003.10.049
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The mechanism for spontaneous grain refinement in undercooled pure Cu melts

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Cited by 43 publications
(33 citation statements)
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“…At a well defined undercooling, ΔT * = 140-150 K, Walker observed an abrupt transition from a coarse columnar grain structure to a fine equiaxed structure, with a reduction in grain size of at least one order of magnitude. Similar behavior was found in Co, with a value for ΔT * of ≈180 K. This effect has subsequently been identified in other pure metals [2][3][4] and in a range of alloy systems [5][6][7][8][9][10][11][12][13][14], in which a more complex evolutionary sequence is often observed as the undercooling is increased. At low undercooling an initially columnar growth pattern is observed which gives way to an equiaxed grain structure as the undercooling is increased beyond a critical value, ΔT 1 *…”
Section: Introductionsupporting
confidence: 68%
“…At a well defined undercooling, ΔT * = 140-150 K, Walker observed an abrupt transition from a coarse columnar grain structure to a fine equiaxed structure, with a reduction in grain size of at least one order of magnitude. Similar behavior was found in Co, with a value for ΔT * of ≈180 K. This effect has subsequently been identified in other pure metals [2][3][4] and in a range of alloy systems [5][6][7][8][9][10][11][12][13][14], in which a more complex evolutionary sequence is often observed as the undercooling is increased. At low undercooling an initially columnar growth pattern is observed which gives way to an equiaxed grain structure as the undercooling is increased beyond a critical value, ΔT 1 *…”
Section: Introductionsupporting
confidence: 68%
“…Their model is further supported by experimental observations of a 'trapped-in' seaweed-like structure in samples of highly undercooled pure Cu [18].…”
Section: Introductionmentioning
confidence: 56%
“…However, although there is plentiful evidence of an initial decrease in microstructural length scale in the low undercooling region, it has proved almost impossible to make a continuous extension of such an analysis into the high undercooling regime where the presence of a local minimum might be inferred. Even for systems where a single dendritic phase exists over the whole undercooling range, such as Ni-Cu [39] or Cu-O [44], the intervention of remelting and/or recrystallisation effects such as spontaneous grain refinement [43,45,46] make the estimation of the original tip radius during dendritic growth impossible. Given that the local minimum in the tip radius moves to lower undercooling as the Lewis number is increasing we consider, on the balance of probabilities, that at higher Lewis numbers than those studied here it may still be the case that a local maximum in the tip radius will be observed.…”
Section: Resultsmentioning
confidence: 99%