TY - JOUR
T1 - EFFECTS OF CONVECTION ON PHYSICAL VAPOR TRANSPORT OF HG2CL2 IN THE PRESENCE OF KR - PART I: UNDER MICROGRAVITY ENVIRONMENTS
AU - Lee, Yong Keun
PY - 2013/2
Y1 - 2013/2
N2 - Special attention in the role of convection in vapor crystal growth has been paid since some single crystals under microgravity environments less than 1 g0 exhibits a diffusive-convection mode and much uniformity in front of the crystal regions than a normal gravity acceleration of 1 g0. The total molar fluxes show asymmetrical patterns in interfacial distribution, which indicates the occurrence of either one single or more than one convective cell. As the gravitational level decreases form 1 g0 down to 1.0 × 10−4 g0, the intensity of convection, indicative of the maximum molar fluxes, is reduced significantly for ΔT = 30 K and 90 K. The total molar fluxes decay first order exponentially with the partial pressure of component B, PB (Torr) for 20 Torr ≤ PB ≤ 300 Torr, and two gravity accelerations of gy = 1 g0 and 0.1 g0.
AB - Special attention in the role of convection in vapor crystal growth has been paid since some single crystals under microgravity environments less than 1 g0 exhibits a diffusive-convection mode and much uniformity in front of the crystal regions than a normal gravity acceleration of 1 g0. The total molar fluxes show asymmetrical patterns in interfacial distribution, which indicates the occurrence of either one single or more than one convective cell. As the gravitational level decreases form 1 g0 down to 1.0 × 10−4 g0, the intensity of convection, indicative of the maximum molar fluxes, is reduced significantly for ΔT = 30 K and 90 K. The total molar fluxes decay first order exponentially with the partial pressure of component B, PB (Torr) for 20 Torr ≤ PB ≤ 300 Torr, and two gravity accelerations of gy = 1 g0 and 0.1 g0.
U2 - 10.6111/JKCGCT.2013.23.1.020
DO - 10.6111/JKCGCT.2013.23.1.020
M3 - Article
SN - 1225-1429
VL - 23
SP - 20
EP - 26
JO - 한국결정성장학회지
JF - 한국결정성장학회지
IS - 1
ER -