Part II: Implementation of a New Snow Parameterization EXPLICIT FORECASTS OF WINTER PRECIPITATION USING AN IMPROVED BULK MICROPHYSICS SCHEME Thompson G.,

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Part II: Implementation of a New Snow Parameterization EXPLICIT FORECASTS OF WINTER PRECIPITATION USING AN IMPROVED BULK MICROPHYSICS SCHEME Thompson G., P. R. Field, R. M. Rasmussen, and W. D. Hall, 2008: Explicit Forecasts of Winter Precipitation Using an Improved Bulk Microphysics Scheme. Part II: Implementation of a New Snow Parameterization. Mon. Wea. Rev., 136,

Outline Introduction Introduction Snow distribution assumptions Snow distribution assumptions 1.Bulk snow density 2.Particle size distribution (PSD) Results of sensitivity experiments Results of sensitivity experiments 1.Sensitive experiment design 2.Results a)Shallow/warm cloud system b)Deep/cold cloud system Discussion Discussion 1.Snow geometry 2.PSD diagnostic method 3.PSD shape

INTRODUCTION

Introduction In designing this new scheme, the objectives were: In designing this new scheme, the objectives were: 1)to improve quantitative precipitation forecasts (QPFs), 2)to improve forecasts of water phase at the surface and aloft (particularly the aircraft icing), 3)to incorporate recent microphysical observation from various field projects, and 4)to fulfill the requirements of real-time modeling needs in terms of speed.

Introduction New features specific to this version compared to that described in Part I description include a generalized gamma distribution shape for each hydrometeor species; a generalized gamma distribution shape for each hydrometeor species; a y-intercept of rain that depend on the rain mixing ratio and whether an apparent source is melted ice; a y-intercept of rain that depend on the rain mixing ratio and whether an apparent source is melted ice; a y-intercept of graupel that depend on the graupel mixing ratio; a y-intercept of graupel that depend on the graupel mixing ratio; a more accurate saturation adjustment scheme; a more accurate saturation adjustment scheme; a variable gamma distribution shape parameter for cloud water based on observations; a variable gamma distribution shape parameter for cloud water based on observations; a lookup table for freezing of water drops; a lookup table for freezing of water drops; a lookup table for transferring cloud ice into the snow category; a lookup table for transferring cloud ice into the snow category; Improved vapor deposition, sublimation, and evaporation; Improved vapor deposition, sublimation, and evaporation; Variable collection efficiency for rain-, snow-, and graupel- collecting cloud droplets; and Variable collection efficiency for rain-, snow-, and graupel- collecting cloud droplets; and Improved rain-collecting snow and graupel. Improved rain-collecting snow and graupel.

Outline Introduction Introduction Snow distribution assumptions Snow distribution assumptions 1.Bulk snow density 2.Particle size distribution (PSD) Results of sensitivity experiments Results of sensitivity experiments 1.Sensitive experiment design 2.Results a)Shallow/warm cloud system b)Deep/cold cloud system Discussion Discussion 1.Snow geometry 2.PSD diagnostic method 3.PSD shape

SNOW DISTRIBUTION ASSUMPTIONS

Bulk Snow Density Spherical, constant density Nonspherical, variable density

Snow Size Distribution Reisner et al. (1998) Thompson et al. (2004) Thompson et al. (2008)

Snow Distribution Assumptions Field et al. (2005)

Black dot : bin model Red + : observation Gray line : PSD this study used

Outline Introduction Introduction Snow distribution assumptions Snow distribution assumptions 1.Bulk snow density 2.Particle size distribution (PSD) Results of sensitivity experiments Results of sensitivity experiments 1.Sensitive experiment design 2.Results a)Shallow/warm cloud system b)Deep/cold cloud system Discussion Discussion 1.Snow geometry 2.PSD diagnostic method 3.PSD shape

RESULTS OF SENSITIVITY EXPERIMENTS

Cloud Top Temperature (CTT) = C

Experiment design and results Slight more 66% more twice 7% less 15 % increased 2/3 Exp3 produced the most snow and least supercooled liquid water (SLW) a) Shallow/warm cloud system (CTT=-13 o C)

CTL Exp1 Exp2 Exp3 Cloud water SnowRain Contour Frequency versus Altitude Diagrams (CFADs) the assumed nonspherical snow, namely CTL and Exp1, produced more SLW and less snow than the assumed spherical snow. the assumed nonspherical snow, namely CTL and Exp1, produced more SLW and less snow than the assumed spherical snow. the two growth processes are controlled by the particle number and surface area the two growth processes are controlled by the particle number and surface area In under 30 min, the snow amount in Exp2 was nearly 50 times that in Exp1 and further accelerated as riming growth commenced. In under 30 min, the snow amount in Exp2 was nearly 50 times that in Exp1 and further accelerated as riming growth commenced. For a given snow mixing ration, the mass-weighted mean size of snow in Exp2 was larger than Exp1 For a given snow mixing ration, the mass-weighted mean size of snow in Exp2 was larger than Exp1

Experiment design and results 42% more b) Deep/cold cloud system (CTT=-60 o C) 6% more 30% less

CTL Exp1 Exp2 Exp3 Cloud water SnowRain Contour Frequency versus Altitude Diagrams (CFADs) The large amount of snow in Control above the inversion was due to the more numerous small particles, the more numerous small particles were responsible for both reduced sedimentation and increased vapor depositional growth The large amount of snow in Control above the inversion was due to the more numerous small particles, the more numerous small particles were responsible for both reduced sedimentation and increased vapor depositional growth In contract the shallow cloud, the relatively high constant-density, spherical snow of Exp2 was less efficient in removing SLW, which is why Exp2 had larger amounts of cloud water and less snow than Exp1. In contract the shallow cloud, the relatively high constant-density, spherical snow of Exp2 was less efficient in removing SLW, which is why Exp2 had larger amounts of cloud water and less snow than Exp1.

The larger snowflakes were then responsible for more efficient riming in the liquid cloud

Outline Introduction Introduction Snow distribution assumptions Snow distribution assumptions 1.Bulk snow density 2.Particle size distribution (PSD) Results of sensitivity experiments Results of sensitivity experiments 1.Sensitive experiment design 2.Results a)Shallow/warm cloud system b)Deep/cold cloud system Discussion Discussion 1.Snow geometry 2.PSD diagnostic method 3.PSD shape

DISCUSSION

Snow geometry

PSD diagnostic method temperature snow content For this work, it defined the PSD by employing both temperature and snow content using orders of magnitude observed PSDs than are found in either of the other references. Field et al. (2005) Houze et al. (1979) Sekhon and Srivastava (1970)

PSD shape

With God all things are possible. -Matthew 19:26 THE END

PSD shape CTL produced the least saturation with respect to ice whereas Exp3 produced the highest saturation and producing cloud water The CTL experiment produced minimal liquid cloud between 0 o and -10 o C, Exp1 produced only slightly more cloud water to higher altitudes around hPa Exp3 are not consistent with observations at all, with liquid cloud reaching above the altitude of T=-20 o C CTL Exp1 Exp3Exp2