Spatial distributions of (a) cloud-liquid mass density (g m-3 ) and (b) cloud-ice mass density (g m-3 ) over the west-east direction and at 15 km in the north-south direction. They are obtained at 13:30 LST 20 March. 

Spatial distributions of (a) cloud-liquid mass density (g m-3 ) and (b) cloud-ice mass density (g m-3 ) over the west-east direction and at 15 km in the north-south direction. They are obtained at 13:30 LST 20 March. 

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This study examines mechanisms which control heavy snowfalls in the eastern coast of Korea. Previous observational studies have indicated that heavy snowfalls are caused by the advection of cold and dry air over the warm ocean off the eastern coast. Previous studies have not considered the effects of surface heat fluxes on heavy snowfalls. It is li...

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... b show the snapshots of cloud-liquid and cloud-ice mass concentration (g m -3 ), re- spectively, in the control run. These snapshots are obtained over the west-east direction and at 15 km in the north-south direction. They are at 13:30 LST which is the time of the maximum snowfall rate and hence, represent clouds at their mature stage. As seen in Fig. 6, clouds are typically cumulus clouds which are trapped in the PBL whose tops are around 1.6 km. The cores of these clouds occupy a portion of the domain and thus cause the inhomogeneous distribution of cloud properties such as cloud mass. In both Figs. 6a and b, the cores are defined as areas which have hydrometeor mix- ing ratios ...
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... of the maximum snowfall rate and hence, represent clouds at their mature stage. As seen in Fig. 6, clouds are typically cumulus clouds which are trapped in the PBL whose tops are around 1.6 km. The cores of these clouds occupy a portion of the domain and thus cause the inhomogeneous distribution of cloud properties such as cloud mass. In both Figs. 6a and b, the cores are defined as areas which have hydrometeor mix- ing ratios above ~0.03 g m -3 . In Fig. 6b, there are significant non-zero cloud-ice mixing ratios between the cores. How- ever, in Fig. 6a, there are no significant cloud-liquid mixing ratios between the cores. Lower density of cloud-ice particles than that of cloud-liquid ...
Context 3
... are typically cumulus clouds which are trapped in the PBL whose tops are around 1.6 km. The cores of these clouds occupy a portion of the domain and thus cause the inhomogeneous distribution of cloud properties such as cloud mass. In both Figs. 6a and b, the cores are defined as areas which have hydrometeor mix- ing ratios above ~0.03 g m -3 . In Fig. 6b, there are significant non-zero cloud-ice mixing ratios between the cores. How- ever, in Fig. 6a, there are no significant cloud-liquid mixing ratios between the cores. Lower density of cloud-ice particles than that of cloud-liquid particles enables more efficient de- trainment of cloud-ice particles from cores to places between them ...
Context 4
... of these clouds occupy a portion of the domain and thus cause the inhomogeneous distribution of cloud properties such as cloud mass. In both Figs. 6a and b, the cores are defined as areas which have hydrometeor mix- ing ratios above ~0.03 g m -3 . In Fig. 6b, there are significant non-zero cloud-ice mixing ratios between the cores. How- ever, in Fig. 6a, there are no significant cloud-liquid mixing ratios between the cores. Lower density of cloud-ice particles than that of cloud-liquid particles enables more efficient de- trainment of cloud-ice particles from cores to places between them than that of cloud-liquid particles. In addition, the ba- sic thermodynamics indicates that the ...

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