Multiscale Kain-Fritsch Scheme: Formulations and Tests

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Presentation transcript:

Multiscale Kain-Fritsch Scheme: Formulations and Tests US EPA Multiscale Kain-Fritsch Scheme: Formulations and Tests   Kiran Alapaty1, John S. Kain2, Jerold A. Herwehe1, O. Russell Bullock Jr. 1, Megan S. Mallard3, Tanya L. Spero 1, and Christopher G. Nolte1  1National Exposure Research Laboratory, U.S. Environmental Protection Agency, Research Triangle Park, NC 2National Severe Storms Laboratory, National Oceanic Atmospheric Administration, Norman, Oklahoma   3Institute for Environment, University of North Carolina, Chapel Hill, NC

Forewords… Kain-Fritsch Convection Parameterization is the most widely used scheme in: Global Models & Regional Models Europe, Asia, and US KF scheme is designed for ~25 km grids no scale dependency This research is geared to benefit climate simulations – based on GCM and LES modeling studies A small step forward to achieve scale independency improving climate simulations Evaluation results were presented by Jerry Herwehe (Pls see his poster) Any improvements that we make will help a large number of researchers and communities

US EPA Our Broad Objective… Develop credible regional climate projections for use in air quality, ecosystems, and human health research studies at the US EPA.

Impacts of introducing KF Cloud-Radiation Interactions US EPA Impacts of introducing KF Cloud-Radiation Interactions Surface Precipitation for Southeast U.S.A. at 36 km grids in the WRF model Climate Branch at EPA is developing regional climate data sets for use with ecosystem and human exposure studies. Credibility of regional climate data is very important for our exposure studies and thus improved the WRF regional climate simulations by incorporating cloud-radiation interactions increasing the credibility of climate simulations. With this we can have confidence in our future climate projections using this improved model. Wet bias from Kain-Fritsch convection scheme is largely eliminated at 36 km grids Alapaty et al., 2012, GRL; Herwehe et al., 2014, JGR

Regional Climate Simulations US EPA Regional Climate Simulations (12 km grid spacing) using the WRF model Climate Branch at EPA is developing regional climate data sets for use with ecosystem and human exposure studies. Credibility of regional climate data is very important for our exposure studies and thus improved the WRF regional climate simulations by incorporating cloud-radiation interactions increasing the credibility of climate simulations. With this we can have confidence in our future climate projections using this improved model.

Weather Research & Forecasting (WRF) US EPA Weather Research & Forecasting (WRF) Model V3.6.1 for 12 km climate simulations Kain-Fritsch (KF) convective parameterization RRTMG SW and LW radiation WSM6 microphysics (plus 2 other) YSU PBL Revised Monin-Obukhov surface layer Noah LSM Mild analysis nudging of free atmosphere u-v wind components, temperature : 5.0E-5 s-1 moisture: 5.0E-6 s-1 NCEP-DOE AMIP-II reanalysis (R-2) 1.875° data DX = 12 km – JJA 2006 simulations 12 km grids, 3.5 m simulation, physics, inputs, fdda, mpe, prism, cfsr, etc…

Wet Bias with the KF scheme US EPA Observations for Precipitation from Two Different Sources Wet Bias with the KF scheme WRF 3.6b over-predicted surface Precipitation even with KF-Radiation Interactions

---------------------------------------------------- US EPA Which moist physics should restore stability to the atmosphere? KF = Kain Fritsch E = Explicit/Resolved KF scheme SHOULD gradually drop out ---------------------------------------------------- Warm periods KF & E schemes Warm & Cool periods E scheme Grid Resolution ~36 km ……… ………. ~1 km As resolution increases, a CPS should drop out smoothly such that as resolution increases, the influence of a CPS should decrease and almost cease at deep cloud resolving grid resolutions One way to gradually dropout the KF is to control its ability to stabilize the atmosphere and help to moisten the environment

Dependence of cloud fraction on “Resolution” using a CRM (warm season) Arakawa & Schubert (1974)  at any grid resolution up to cloud resolving grids MSKF Scheme b parameter Alapaty et al. (2013) Arakawa & Wu (2013) Dependence of cloud fraction on “Resolution” using a CRM (warm season) 25 km Cloud Fraction

Sub-Cloud layer length scale = ZLCL US EPA Bulk Approach: Cloud layer length scale = H Cloud layer velocity scale: WCL Sub-Cloud layer length scale = ZLCL Sub-cloud layer velocity scale: WSb 1:10 size Pbl:clouds UNKNOWNS: WCL AND WSb From Kiran’s notes

KF parameters that control surface precipitation Developing Multiscale Kain-Fritsch Scheme to Transition Across Grid Spacing KF parameters that control surface precipitation (0) KF Cloud-Radiation interactions (NEW) (1) Adjustment timescale (τ) (NEW) (2) Minimum Entrainment (relax 2 km radius constraint) (NEW) (3) Fallout RATE in Autoconversion (UPDATED) (4) Stabilizing Capacity (UPDATED) (5) Eliminate “double” counting of precipitation (NEW) (6) Vertical momentum impacts: Impacts on grid-scale W using KF mass fluxes (NEW) (7) New Trigger function suitable for high-resolution grids (under development) (NEW) Green = scale- dependent parameters KF scheme is real good at 25 km grid spacing ! Probable parameters that influence the estimation of surface precipitation in the KF scheme: these parameters need some scale dependency so that the KF scheme becomes something called a scale-independent (scale-aware) CP scheme

GCM study of Bechtold et al. (2008) What is the Adjustment Timescale (t ) for Cumulus Clouds (both Deep & Shallow)? It is the time needed to restore stability to the atmosphere Why is t important? In air pollution modeling it can influence photolysis rates & sulphate aerosol produced via oxidation of SO2 in Clouds In NWP & climate models it determines duration of convective heating & drying, precipitation, and radiative fluxes In KF scheme t =U/dx (0.5h to 1h) GCM study of Bechtold et al. (2008)

Estimation of Cloud Velocity Scale, WCL : for Shallow Cumulus Clouds: From Grant & Lock (2004) LES studies and BOMEX observations Now, for Deep Cumulus Clouds… Bullock et al. MWR revision From Arakawa & Schubert (1974), Cloud Work Function per unit cloud base mass flux: BOMEX = Barbados Oceanographic and Meteorological EXperiment e.g, Old Grell scheme where When h = 1, then Using the relation or 13 13 13

Based on Cloud Work Function ….. Shallow Cumulus Clouds Based on LES & Obs Gran & Lock 2004 Irony: Reveals gap Between Shallow and Deep Cumulus Cloud modelers Deep Cumulus Clouds Russ Bullock’s formulation Based on Cloud Work Function Bullock et al. 2014 in review

Two formulations for Convective Adjustment Timescale (Bullock et al Two formulations for Convective Adjustment Timescale (Bullock et al., Alapaty et al.) W* does not exist in SBL but convective clouds do exist; also, over water/oceans W* is at best small +ve number (i.e, small SHF). So, new formulation works for land or water – continental clouds due to heating or large-scale forcing over land/water like in monsoon environments 14

Developing Multiscale KF to Transition Across Grid Spacing: (1) New Adjustment Timescale, t OLD t =U/dx (0.5h to 1h) NEW 1616 Bullock et al. Alapaty et al. JJA 2006 KF Precipitation Differences (NEW - OLD)

Hurricane Katrina: August 28-31, 2005 RCM added value! Observations Dynamic Tau Version Standard KF Version Hurricane Katrina inland rainfall totals dramatically improved with US EPA science updates. (Bullock et al., MWR in review)

Adapting KF to Transition Across Grid Spacing: (2) Entrainment 4 km grids KF clouds NEW OLD Efficiency (C1= Tokioka parameter = 0.03) (actually 0.025, Tokioka 1988) GCM studies: Kang et al. (2009); Kim et al. (2011): Max and Min values of Tokioka parameter are based on GCM works  Larger C1 (Tokioka)  Grid-scale Precip KF precip LES Studies: Stevens and Bretherton (1999): Dependency of entrainment with horizontal grid resolution for Shallow Cumulus  Entrainment increases as grid spacing decreases

US EPA Developing Multiscale KF to Transition Across Grid Spacing: (2) New Entrainment OLD NEW JJA 2006 KF Precipitation Differences (NEW - OLD)

No microphysics (in most of the CPS) Cpe  Tuning Parameter ( s-1) Developing Multiscale KF to Transition Across Grid Spacing: (3) New Fallout Efficiency No microphysics (in most of the CPS) Cpe  Tuning Parameter ( s-1) GCMs: Kim & Kang (2011) : Cpe = 0.02 RCMs: WRF, Cpe = 0.03 NRCM, Cpe = 0.01 OLD NEW NRCM = NCAR Regional Climate Model; Chris Nolte is helping me on aerosols On going work: replace this Equation with a 2-moment microphysics scheme  AMS 2015 (Chris Nolte)

Developing Multiscale KF to Transition Across Grid Spacing: (3) New Fallout Efficiency JJA 2006 KF Precipitation Differences (NEW - OLD)

More improvements expected Developing Multi-Scale KF to Transition Across Grid Spacing: (4) Stabilizing Capacity Developing Multi-Scale KF to Transition Across Grid Spacing: (5) “Double” counting Developing Multi-Scale KF to Transition Across Grid Spacing: (6) Linear Mixing of Wkf Developing Multi-Scale KF to Transition Across Grid Spacing: (7) New Trigger Function for high resolution under development More improvements expected

12 km WRF JJA simulations with MSKF Accumulated Surface Precipitation Generalized dynTau …………………………………………… Bullock’s dynTau ……………………………………………

KF - RAd mskf Observation Accumulated JJA 2006 Precipitation US EPA June-August 2006 WRF MSKF Precipitation KF - RAd mskf

9 km and 3 km MSKF simulations: WRF 3.3.1 -- Forecast mode: Yue et al., in review 1800 UTC 29 – 0000 UTC 30 July 2010 9 KM grids 1800 UTC 29 – 0000 UTC 30 July 2010 3 KM grids

1 km MSKF simulations for Eastern North Carolina WRF 3.3.1 -- Forecast mode: Sims et al. Surface shortwave by the WSM6, WSM6+MSKF, and Satellite clouds on June 29, 2012 at 1700 UTC using 1 km grids. GOES Imagery

SUMMARY Several New formulations within the Kain-Fritsch (KF) scheme were tested using 12 km, 9 km, 3 and 1 km grids In general : Results are positive for all these grid spacings For the eastern US our 12 km 3-month simulations indicate: Each of the science updates reduces precipitation bias while new adjustment timescale & entrainment formulations are big contributors Surface stats are encouraging (See Jerry Herwehe’s poster) Slight dry bias exists in some western regions of the domain. Last item (new trigger) is being worked out for further improvements

Additional Material

Adapting KF to Transition Across Grid Spacing: (2) Entrainment: EFFICIENCY vs EFFICACY TWP-ICE Darwin, Australia, DOE ARM – SCAM5 test for 2006 monsoon

Area Averaged Monthly Variation of Surface Temperature & Precipitatoin US EPA Area Averaged Monthly Variation of Surface Temperature & Precipitatoin Temperature Bias (Model – CFSR) Precipitation Bias (Model – NARR)