2001
DOI: 10.1016/s0022-0248(01)01318-5
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Numerical 3D study of FZ growth: dependence on growth parameters and melt instability

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Cited by 18 publications
(12 citation statements)
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“…50 For Re ¼ 0 and Ma ¼ 30, the eigenmodes A 2 (critical), B 2 , C 1 , C 2 , D 2 are stationary so that the angular phase velocity of the eigenmode is zero. The complex-conjugate pair A 1 , B 1 is associated with a non-zero frequency and corresponds to two traveling waves propagating with angular phase velocities of 19.9 at Ma ¼ 35.2 in the positive and negative azimuthal directions, respectively.…”
Section: Energy Analysismentioning
confidence: 99%
“…50 For Re ¼ 0 and Ma ¼ 30, the eigenmodes A 2 (critical), B 2 , C 1 , C 2 , D 2 are stationary so that the angular phase velocity of the eigenmode is zero. The complex-conjugate pair A 1 , B 1 is associated with a non-zero frequency and corresponds to two traveling waves propagating with angular phase velocities of 19.9 at Ma ¼ 35.2 in the positive and negative azimuthal directions, respectively.…”
Section: Energy Analysismentioning
confidence: 99%
“…Several 3D simulations were reported as well [8], but the phase boundaries were not taken into account. Recently, a 3D simulation of time-dependent melt convection was carried out by Ratnieks et al [9] based on a zone shape from their 2D selfconsistent model [7]. The coupling of timedependent convection with the growth rate was also reported, where back melting due to oscillatory rotational flow was illustrated.…”
Section: Introductionmentioning
confidence: 99%
“…Two codes specialized for crystal-growth modelling are FEMAG [40] and CrysVUN [41]. Examples of crystal-growth modelling performed using popular general-purpose codes can be found in [58] (CFX4), [65] (FIDAP), [66] (FLUENT), and [67] (CFD-ACE). It is not necessary for users to completely understand the numerical methods used in these codes, but a general understanding will greatly facilitate their correct use.…”
Section: Computer-aided Analysismentioning
confidence: 99%