The Capacitance of Pristine Ice Crystals and Aggregate Snowflakes
The Capacitance of Pristine Ice Crystals and Aggregate Snowflakes
复制标题
原始冰晶和聚集雪花的电容
DOI:
10.1175/2007jas2315.1
复制
发表时间:
2006
影响因子:
3.1
通讯作者:
A. Illingworth
中科院分区:
文献类型:
--
作者:
C. Westbrook;R. Hogan;A. Illingworth
A new method of accurately calculating the capacitance of realistic ice particles is described: such values are key to accurate estimates of deposition and evaporation (sublimation) rates in numerical weather models. The trajectories of diffusing water molecules are directly sampled, using random ‘walkers’. By counting how many of these trajectories intersect the surface of the ice particle (which may be any shape) and how many escape outside a spherical boundary far from the particle, the capacitance of a number of model ice particle habits have been estimated, including hexagonal columns and plates, ‘scalene’ columns and plates, bullets, bullet-rosettes, dendrites, and realistic aggregate snowflakes. For ice particles with sharp edges and corners this method is an efficient and straightforward way ofsolving Laplace’s equation for the capacitance. Provided that a large enough number of random walkers are used to sample the particle geometry (∼ 10 4 ) the authors expect the calculated capacitances to be accurate to within ∼ 1%. The capacitance for our modelled aggregate snowflakes (C/Dmax = 0.25, normalised by the maximum dimension Dmax) is shown to be in close agreement with recent aircraft measurements of snowflake sublimation rates. This result shows that the capacitance of a sphere (C/Dmax = 0.5) which is commonly used in numerical models, overestimates the evaporation rate of snowflakes by a factor of two. The effect of vapor ‘screening’ by crystals growing in the vicinity of one another has also been investigated. The results clearly show that neighbouring crystals growing on a filament in cloud chamber experiments can strongly constrict the vapor supply to each other, and the resulting growth rate measurements may severely underestimate the rate for a single crystal in isolation (by a factor of 3 in our model setup).