1968
DOI: 10.1016/0022-0248(68)90017-1
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Stability of the needle crystal

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Cited by 32 publications
(8 citation statements)
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“…Already during the later 1960s, it was hypothesised that morphological stability rather than extremum growth was the key element in modelling dendrite tip behaviour. Kotler and Tiller [62] concluded, ' … a true time-dependent perturbation analysis is vital to the development of a … detailed theory of dendritic growth'. Oldfield, a Ph.D. student of Tiller, undertook the first numerical simulations of dendrites in the mid-1960s.…”
Section: Marginal Stabilitymentioning
confidence: 99%
“…Already during the later 1960s, it was hypothesised that morphological stability rather than extremum growth was the key element in modelling dendrite tip behaviour. Kotler and Tiller [62] concluded, ' … a true time-dependent perturbation analysis is vital to the development of a … detailed theory of dendritic growth'. Oldfield, a Ph.D. student of Tiller, undertook the first numerical simulations of dendrites in the mid-1960s.…”
Section: Marginal Stabilitymentioning
confidence: 99%
“…Once a planar solid-liquid interface has become unstable, the theoretical description of the solidification process becomes more difficult as the geometry of the developing protrusions has to be taken into account. A number of models have been presented for the growth of single needle-shaped crystals (Ivantsov, 1947;Kotler & Tiller, 1968) and for a cellular growth morphology (Boiling & Tiller, i960). As mentioned above, the needle-or tongue-like protrusions tend to become unstable themselves such that perturbations, particularly in the 'shoulder' region, result in the formation of side-branches and dendritic structures (cf.…”
Section: Non-planar Growth Of Icementioning
confidence: 99%
“…The occurrence of sidebranches can be attributed to the diffusive (Mullins and Sekerka) instability. According to Mullins and Sekerka [10], a planar solid-liquid interface is morphologically unstable against infinitesimal small perturbation if the wavelength of the perturbation l is larger than the characteristic stability length l s of system defined as l s ¼ 2pðd 0 lÞ 1=2 , where l is the diffusion length, which is given by l ¼ 2Du À1 for planar interface advancing with the growth velocity u. Kotler and Tiller [11] have performed one of the first analytic investigations of the dendrite sidebranch evolution. They applied the Mullins and Sekerka-type perturbation analysis to steady-state paraboloid of revolution, and showed that such a body is unstable against evolution of repetitive rings.…”
Section: Introductionmentioning
confidence: 99%