Microphysics Schemes
W.-K. Tao
- S. Lang, J. Chern, T. Matsui, X. Li, T. Iguchi, D. Wu
NASA Goddard Space Flight Center
1/30 + 1
Microphysics Schemes W.-K. Tao S. Lang , J. Chern, T. Matsui, X. Li, - - PowerPoint PPT Presentation
Microphysics Schemes W.-K. Tao S. Lang , J. Chern, T. Matsui, X. Li, T. Iguchi, D. Wu NASA Goddard Space Flight Center All microphysical schemes have their own set of unique assumptions and capabilities. It is critical therefore to sample and
1/30 + 1
2
4
Tao, W.-K., D. Wu, S. Lang, J. Chern, C. Peters-Lidard, A. Fridlind, and T. Matsui, 2016: High-resolution NU-WRF model simulations of MC3E, deep convective-precipitation systems: Comparisons between Goddard microphysics schemes and observations, J. Geophys. Res., 121, 1278-1306. doi:10.1002/2015JD023986.
5
6
Bin Scheme is used to correct the overestimation
density and fall speed of graupel in bulk scheme
By assuming exp. rain DSD, bulk scheme artificially increases #s
bin
7
Bin model improvements:
dependent ice particles collection efficiencies;
production terms when snow aggregates or ice crystals collect cloud droplets.
Ice particle collection efficiency
Li, X., W.-K. Tao, T. Matsui, C. Liu and H. Masunaga, 2010: Improving spectral bin microphysical scheme using TRMM satellite observations. Quart. J. Roy. Meteor. Soc. 136, 382–399.
8
Ground-based Radar Space-based Radar Microwave (TB)
Dolan, B., T. Matsui, A. A. Matthews, S. A. Rutledge, W. Xu, W.-K. Tao, T. Iguchi, V. Chandrasekar , 2016: Multi-sensor Radar Observations and Size-Resolving Cloud Modeling Analysis of the 25 April 2011 MC3E Convective Case, (to be submitted to MWR)
9
10
11
12
13 Wu/Tao et al. (2015)
2015-12-03 00:00 UTC 2015-12-03 15:00 UTC
4ICE Morrison WSM6
14
15
Major characteristics of Goddard 4-ICE scheme and three two-moment schemes (RAMS, JP Chen and Morrison). The similarities and differences between these schemes are shown.
16
17/30
Tao, W.-K., J. Simpson, S. Lang, M. McCumber, R. Adler and R. Penc, 1990: An algorithm to estimate the heating budget from vertical hydrometeor profiles. J. Appl. Meteor., 29, 1232-1244.
18
Tao, W.-K., Y. N. Takayabu, S. E. Lang, W. Olson, S. Shige, A. Hou, G. M. Skofronick-Jackson, X. Jiang, K.-M. Lau, T. Krishnamurti, D. Waliser, C. Zhang, R. Johnson, R. Houze, P. Ciesielski, M. Grecu, S. Hagos, R. Kakar, N. Nakamura, S. Braun, and A. Bhardwaj, 2016: TRMM Latent Heating Retrieval: Applications and Comparisons with Field Campaigns and Large-Scale Analyses, Amer. Meteor. Soc. Meteorological Monographs - Multi-scale Convection-Coupled Systems in the Tropics, 56, Chapter 2, doi: 10.1175/AMSMONOGRAPHS-D-15-0013.1
LH QR Edd y Q1
Purple: Simulated Q1 Green: Observed Q1
LH: Latent Heat - phase change of water
Eddy - heat transport by cloud dynamics
QR: Radiation
19
20
21
Northern Array Southern Array
CSH (PR): 6.56 mm/day, 43% stratiform TRMM 3B42: 6.6 mm/day Q2 budget: 5.5 mm/day CSH (PR): 8.43 mm/day. 45% stratiform TRMM 3B42: 6.3 mm/day Gauge network: 7.2 mm/day
22
Lx P Ptop
base
1
Po is surface rainfall So is surface sensitive flux TRMM Derived Rainfall
23
02/23/2016 JPST
24
25
03/16/2014 18:00 UTC 02/17/2015 03:00 UTC 02/21/2015 18:00 UTC NEXRAD NEXRAD NEXRAD NU-WRF NU-WRF NU-WRF
26
27
28
29
30/30
For high resolution runs (18,6 and 2 km): Different parameterization schemes seem no impact on diurnal variation (intensity and timing) For low resolution runs (30 and 18 km): Weaker precipitation and do not predict the afternoon rainfall well For medium resolution run (18, 6 or 30,10 km): Similar to those high resolution runs
+1
4