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8/18/2019 Evaluacion de Radiacion y Microfisica en Zonas Polares
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Evaluation of WRF Radiation and MicrophysicsParameterizations for use in the Polar Regions
Mark W. Seefeldt
Michael Tice
Department of Engineering – Physics – SystemsProvidence College
Cooperative Institute for Research in Environmental Sciences (CIRES)
University of Colorado at Boulder
Atmospheric Model Parameterizations in the Polar Regions WorkshopBoulder, CO – July 12, 2012
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Outline
• Objective / Motivation
• WRF General Configuration
• Radiation Parameterizations
• Microphysics Parameterizations
• Observations for Evaluation
• Statistical Comparisons• WRF 3.0 Physics Evaluation (2009)
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Objective
• The preferred physics parameterizations in the
polar regions is still under debate and evaluation
• e purpose o s s u y s o eva ua e a su e oradiation and microphysics parameterizations for
the use of the WRF model in the polar regions
• The anticipated outcome is the identification of abest-use combination of microphysics and radiation
• A secondary goal is the elimination of several of the
physics parameterizations as viable options
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WRF in the Polar Regions
• Atmospheric models have been found to have difficulty inreproducing representative conditions in the polar regions
(Wyser et al. 2008)
e pro ems are genera y re a e o e a mosp er c p ys cs
cloud processes
radiation
processes
PBL and surface fluxes
sea ice / icecovered land
WRF-ARW Version 3
Modeling SystemUser’s Guide
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WRF Physics Parameterizations
• There are seven general WRF physics
parameterizations:
– ra a on – s or wave ra_ w_p ys cs – radiation – longwave (ra_sw_physics)
– microphysics (mp_physics)
– cumulus (cu_physics)
– boundar la er bl_ bl_ h sics
– surface layer (sf_sfclay_physics)
– land surface model (sf_surface_physics)
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WRF Physics Parameterizations• The performance of a given physics parameterization is often
related to the associated parameterizations
•
The most complete way to identify the preferred physicsparameterizations is to evaluate different physics combinations
WRF Tutorial
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WRF Physics Evaluation – Summary
• This study will focus on the performance of the
radiation and microphysics parameterizations
• e s u y w compare s mu a ons anobservations for two locations:
Barrow, Alaska Summit, Greenland
• The month-long climate simulations will be evaluated
against observations of meteorology (surface and
upper- eve , c ou s, an ra at on• A statistical evaluation will be completed with the
results providing a ranking of the preferred
parameterizations
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WRF Physics Evaluation – General Configuration
• WRF-ARW v3.4 (released April, 2012)
• month-long climate simulations:
- - ,
• simulations for four different months covering different seasonal
and radiation forcing conditions:
October 2011, January 2012, April 2012, July 2012• Initial and lateral boundary conditions: ERA-Interim
• Fractional sea ice: NSIDC Near Real-Time DMSP SSMI
• Domains: outer – 50 km, inner – 10 km (one-way nesting)• Vertical: 40 levels with a 50 mb top
• Timestep : 50 km – 300 s, 10 km – 60 s
• Post-processing: CF NetCDF files using wrfout_to_cf.nclhttp://foehn.colorado.edu/wrfout_to_cf/
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WRF Physics Evaluation – Domains
• Two domains: Barrow – Alaska, Summit Camp – Greenland
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WRF Physics Evaluation – Non-Varying Physics
General Physics:
•Land surface model (sf_surface_physics): Noah LSM (2)
•Surface Layer (sf_sfclay_physics): Eta (2)•Boundary layer (bl_pbl_physics): MYJ (2)
•Cumulus (cu_physics): Grell-Devenyi (3)
•Fractional Sea Ice (fractional_seaice = 1)
•SST Updates (sst_update = 1 – uses wrflowinp_d0n)
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WRF Physics – Radiation Parameterizations
• Limit the shortwave (ra_sw_physics) and longwave(ra_lw_physics) radiation parameterizations to paired selections
• Four selected radiation combinations (LW / SW):
– o ar w_ -sw_ – CAM / CAM (lw_3-sw_3)
– RRTMG / RRTMG (lw_4-sw_4)
– New Goddard / New Goddard (lw_5-sw_5)
• RRTM / Goddard was selected because of its use in past WRF
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WRF Physics – Radiation Parameterizations
To be evaluated:• RRTM / Goddard (lw_1-sw_2)
• CAM / CAM (lw_3-sw_3)
• RRTMG / RRTMG (lw_4-sw_4)• New Goddard / New Goddard (lw_5-sw_5)
Eliminated:
• Dudhia (1) shortwave scheme was not selected based on poor
• Fu-Liou Gu (7/7) was not selected as it is a new scheme with no
particular known strengths for the polar regions
• GFDL (99/99) was not chosen as it is old and being phased out
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WRF Physics – Microphysics Parameterizations
• Eliminate the warm-rain and 3-phase parameterizations: – Kessler (1)
– WRF Single-Moment 3-class (3)
NCEP models:
– Eta (5) / (95)
• Eliminate the WRF double-moment parameterizations:
– WRF Double-Moment 5-class (14)
– WRF Double-Moment 6-class (16)
• m nate severe storm ocuse parameter zat ons:
– NSSL 2-moment (17, 18)
• Eliminate the 7-class paratmerization:
– Milbrandt-Yau Double-Moment 7-class (9)
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WRF Physics – Microphysics Parameterizations
To be evaluated – seven
microphysics parameterizations:•Lin et al. (2)
•WRF Single-Moment 5-class (4)
•WRF Single-Moment 6-class (6)•Goddard (7)
•New Thompson (8)
•Morrison Double-Moment (10)
•Stony Brook University (Lin) (13)
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WRF Physics Evaluation – Simulations Summary
Summary of simulations:• Two domains (Barrow, AK and Summit Camp)
– evaluating the 50 km and the 10 km domains separately
• Four months (October 2011, January, April, July 2012)• Four radiation parameterization combinations
• Seven microphysics parameterizations
Total number of simulations:
x x x = s mu at ons
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WRF Physics Evaluation – Observations
• Reviewed the available the data from the International ArcticSystems for Observing the Atmosphere (IASOA) observatories
http://iasoa.org/
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WRF Physics Evaluation – Observations
Barrow, Alaska – 71.323 N, 156.609 W, 11 m asl:http://www.esrl.noaa.gov/gmd/obop/brw/
Summit, Greenland – 72.580 N, 38.48 W, 3238 m asl:
http://www.geosummit.org/
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WRF Physics Evaluation – Observations
Evaluating WRF using observations from Barrow and Summit:• surface meteorology (temperature, pressure, dew point /
mixing ratio, wind speed)
• upper-a r meteoro ogy temperature, e g t, pressure,moisture)
• surface radiation (downwelling longwave, downwelling
shortwave)• radar and microwave (IWP, LWP)
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WRF Physics – Statistical Comparisons
• Monthly time series plots comparing WRF simulations toobservations will be created
• Statistical measures of bias, RMSE, and correlation will be
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WRF Physics – Statistical Comparisons
• The statistical performance for each radiation and microphysics
combination will be evaluated for each month and each domain
• The rankings of the statistical comparisons will be used todetermine preferred radiation and microphysics parameterizations
• Evaluation of the time series plots can be conducted to dig
further into the statistical comparisons
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WRF 3.0 Physics Evaluation (ca. 2009)• Goal: identify preferred radiation and microphysics parameterizations
– radiation – 5 combinations (lw-sw): RRTM-Dudhia,
RRTM-Goddard, RRTM-CAM, CAM-Goddard, CAM-CAM
– microphysics – 6 schemes:Lin, WSM5, WSM6, Goddard, Thompson, Morrison
• Observations:
– Barrow – Baseline Surface Radiation Network – SHEBA – Surface-Met Tower, Cloud Radiation
, , , ,
liquid water path (SHEBA), ice water path (SHEBA)
• Evaluate: over different months: January, March, May, June
• Evaluate: 10 km domain versus 50 km domain
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WRF 3.0 Physics Evaluation (ca. 2009)• The WRF results are compared against observations from the SHEBA met tower
and Barrow – Baseline Surface Radiation Network
observations:
-longwave downward-shortwave downward-2 m temperature-surface pressure
SHEBA only:-LWP-IWP
Statistics are calculatedto objectively evaluatethe performance of themodel in comparison to
the observations.
Correlation, Bias (WRF – obs), Root Mean Square Error (RMSE)
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WRF 3.0 Physics Evaluation (ca. 2009)• The statistics of each sensor for each physics configuration, location, month, and
model domain are aggregated together in a list
Note: The values for all 30 physics configurations and the different sensors have been
removed for display.
Each sensor statistic for each physicsconfiguration is ranked by performance (1-30)
The average rank and standarddeviation is calculated for each sensor
h l
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WRF 3.0 Physics Evaluation (ca. 2009)• The average of the three primary sensors (2 m temperature, shortwave downward,
and longwave downward) is calculated for each domain and location
Note: The values for Barrow have been removed to simplify the display.
WRF 3 0 Ph i E l i ( 2009)
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WRF 3.0 Physics Evaluation (ca. 2009)• The average rank for each physics configuration is calculated across the different
domains, months, and locations.
• The physics parameterizations are sorted by the average rank, from best to worst
WRF 3 0 3 S (T SW LW) R ki
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WRF 3.0 – 3 Sensor (T, SW, LW) Rankings• The CAM-CAM (3-3) radiation combination shows
consistently the best performance (4 of top 8)
• The Goddard (7) microphysics is a strong showing with the
top 3 performances
• Overall, the CAM-Goddard (3-2) and RRTM-CAM (1-3)radiation schemes perform well
• The RRTM-Dudhia (1-1) and RRTM-Goddard radiationcombinations do not do well
• The Lin (2) and Morrison (10) microphysics schemes do very poorly, no matter the radiation combination
WRF 3 0 5 S (T SW LW IWP LWP)
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WRF 3.0 – 5 Sensor(T, SW, LW, IWP, LWP)• The CAM-CAM (3-3) radiation continues to perform well
(5 of top 11)
• The Goddard (7) and Lin microphysics does well followed
by the WSM5 (4) and WSM6 (6)
• The RRTM-CAM (1-3) radiation performs fair, but all otherthan CAM-CAM have a mixture of results
• The Morrison (10) microphysics scheme continues to dooorl
RRTM Goddard (1 2) Morrison (10) May 1998
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RRTM – Goddard (1-2), Morrison (10) – May 1998
CAM CAM (3 3) Goddard (7) May 1998
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CAM – CAM (3-3), Goddard (7) – May 1998
Sh t d L R di ti R ki
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Shortwave and Longwave Radiation Rankings• The CAM SW (3) consistently does very well
with the SW rankings (top 8)
• The Goddard SW (2) does moderate withSW rankings
• The Dudhia SW (1) performs very poorly with the SW sensor
• The CAM LW (3) does well, but not
spectacular with LW rankings• The RRTM LW (1) does well when matched
with Dudhia SW (1) but not Goddard SW orCAM SW (3)
• The CAM-CAM (3-3) radiation combinationprovides the best results
Liq id Water Path and Ice Water Path Rankings
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Liquid Water Path and Ice Water Path Rankings• The Goddard (7) and Thompson (8) show
consistently good performance with LWP(6 of top 7)
• The Lin (2) and Morrison (10) do poorly w
• The Lin (2) and Morrison (10) do very well with IWP
• The Goddard does poorly with IWP
• Overall, using LWP and IWP is suspect asthe model results showed limited success(i.e. LWP in January)
WRF 3 0 Physics Evaluation (ca 2009) Summary
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WRF 3.0 Physics Evaluation (ca. 2009) - Summary
• The CAM-CAM (3-3) radiation combination consistentlyperforms with the best results in nearly every ranking and
categorization
e - - an - o ar - per orms
reasonable, but not as good as CAM-CAM
• The results for the microphysics is not as clear and will requirefurther analysis
• The Goddard (7) microphysics scheme could be classified as
strongest, but with some questions
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Mark Seefeldt [email protected]