Sublimation rate and the mass-transfer coefficient for snow sublimation

Abstract Sublimation of snow is a fundamental process that affects the crystal structure of snow, and is important for ice core interpretation, remote sensing, snow hydrology and chemical processes in snow. Prior investigations have inferred the sublimation rate from energy, isotopic, or mass-balance calculations using field data. Consequently, these studies were unable to control many of the environmental parameters which determine sublimation rate (e.g. temperature, relative humidity, snow microstructure). We present sublimation rate measurements on snow samples in the laboratory, where we have controlled many of these parameters simultaneously. Results show that the air stream exiting the snow sample is typically saturated under a wide range of sample temperature and air-flow rate, within measurement precision. This result supports theoretical work on single ice grains which found that there is no energy barrier to be overcome during sublimation, and suggests that snow sublimation is limited by vapor diffusion into pore spaces, rather than sublimation at crystal faces. Undersaturation may be possible in large pore spaces (i.e. surface- or depth-hoar layers) with relatively high air-flow rates. We use these data to place bounds on the mass-transfer coefficient for snow as a linear function of Reynolds number, and find that h m  = 0.566 Re  + 0.075.

[1]  B. J. Mason,et al.  The evaporation of ice spheres and ice crystals , 1966 .

[2]  M. Albert Effects of snow and firn ventilation on sublimation rates , 2002, Annals of Glaciology.

[3]  P. Grootes,et al.  Isotopic diffusion in cold snow and firn , 1985 .

[4]  J. Freitag,et al.  A new method for predicting transport properties of polar firn with respect to gases on the pore-space scale , 2002, Annals of Glaciology.

[5]  S. Déry,et al.  Large‐scale mass balance effects of blowing snow and surface sublimation , 2002 .

[6]  W. Massman A review of the molecular diffusivities of H2O, CO2, CH4, CO, O3, SO2, NH3, N2O, NO, and NO2 in air O2 and N2 near STP , 1998 .

[7]  Matthew Sturm,et al.  Vapor transport, grain growth and depth-hoar development in the subarctic snow , 1997 .

[8]  U. Schotterer,et al.  Influence of sublimation on stable isotope records recovered from high-altitude glaciers in the tropical Andes , 2001 .

[9]  M. Broeke,et al.  The Surface Energy Balance of Antarctic Snow and Blue Ice , 1995 .

[10]  M. Sakly,et al.  Sublimation de la glace sous convection forcee. Determination du coefficient global de transfert de masse , 1989 .

[11]  Wolfgang Wagner,et al.  International Equations for the Pressure Along the Melting and Along the Sublimation Curve of Ordinary Water Substance , 1994 .

[12]  Frédéric Flin,et al.  The temperature-gradient metamorphism of snow: vapour diffusion model and application to tomographic images , 2008, Annals of Glaciology.

[13]  J. Wettlaufer,et al.  Growth-melt asymmetry in crystals and twelve-sided snowflakes. , 2006, Physical review letters.

[14]  K. Steffen,et al.  Sublimation on the Greenland Ice Sheet from automated weather station observations , 2001 .

[15]  E. C. Morris A simple frost-point humidity generator , 1997 .

[16]  G. Mann,et al.  An Intercomparison Among Four Models Of Blowing Snow , 2000 .

[17]  Y. Fujii,et al.  The role of sublimation and condensation in the formation of ice sheet surface at Mizuho Station, Antarctica , 1982 .

[18]  M. Albert,et al.  Thermal effects due to air flow and vapor transport in dry snow , 1992, Journal of Glaciology.