Ci. Hung et al., TRANSIENT NATURAL-CONVECTION AND CONJUGATE HEAT-TRANSFER IN A CRYSTAL-GROWTH DEVICE, International journal of heat and mass transfer, 38(4), 1995, pp. 701-712
In crystal growth devices, in order to control the growth defects and
compositional homogeneity of the crystal, a thorough understanding of
the heat transfer characteristics is required. In this effort, the com
bined natural convection and conjugate heat transfer in an axisymmetri
c configuration representative of the container used in float zone dev
ices are numerically simulated. The geometry adopted contains two conc
entric cylinders, the inner one representing the crystal within which
heat conduction takes place, and the outer one being the container wal
l; between them is the domain of a height-to-width ratio of 40, filled
with encapsulated argon gas. The main parameters varied in this study
are Rayleigh number (Ra) and heating location. Substantial refinement
in grid size, from 61 x 81 to 201 x 301 nodes, has been exercised to
assess the numerical accuracy of the solutions. For Ra = 1.25 x 10(4),
steady-state solutions exist regardless of the heating location. For
Rn = 1.25 x 10(5), on the other hand, persistently oscillatory convect
ive patterns appear, exhibiting both co-rotating (buoyancy-induced) ce
lls and contra-rotating (shear-induced) cells. Consequently, the overa
ll heat transfer rates fluctuate in time. The heat transfer fluctuatio
n in the heated region is not as strong as in other regions; however,
the magnitudes of the heat flux there are strongly influenced by the h
eating location, indicating that, in order to maintain a uniform therm
al environment, the power level of the heat source needs to be adaptiv
ely adjusted according to the heating location. This challenge to the
design and operation of the materials processing equipment can be met
with the aid of knowledge gained from numerical simulations.