Zhiyong Wu1,2,. , Donna Schwede1, Robert Vet2, John T

Slides:



Advertisements
Similar presentations
Parametrization of surface fluxes: Outline
Advertisements

PBL simulated from different PBL Schemes in WRF during DICE
Reading: Text, (p40-42, p49-60) Foken 2006 Key questions:
Development of Alternative Methods For Estimating Dry Deposition Velocity In CMAQ.
Globally distributed evapotranspiration using remote sensing and CEOP data Eric Wood, Matthew McCabe and Hongbo Su Princeton University.
ERS 482/682 Small Watershed Hydrology
Calculation of wildfire Plume Rise Bo Yan School of Earth and Atmospheric Sciences Georgia Institute of Technology.
Estimate of Mercury Emission from Natural Sources in East Asia Suraj K. Shetty 1 *, Che-Jen Lin 1, David G. Streets 2, Carey Jang 3, Thomas C. Ho 1 and.
Evaporation Theory Dennis Baldocchi Department of Environmental Science, Policy and Management University of California, Berkeley Shortcourse on ADAPTIVE.
Muntaseer Billah, Satoru Chatani and Kengo Sudo Department of Earth and Environmental Science Graduate School of Environmental Studies Nagoya University,
Gradient CORPORATION Vapor Intrusion Attenuation Factors (AFs) – Measured vs. EPA Defaults A Case Study Presented by Manu Sharma and Jennifer DeAscentis.
Lecture 10 Evapotranspiration (3)
Coupling of the Common Land Model (CLM) to RegCM in a Simulation over East Asia Allison Steiner, Bill Chameides, Bob Dickinson Georgia Institute of Technology.
Network for the support of European Policies on Air Pollution The assessment of European control measures and the effects of non-linearities.
50 Years of the Monin-Obukhov Similarity Theory Thomas Foken University of Bayreuth, Bayreuth, Germany.
Evaluation and Application of Air Quality Model System in Shanghai Qian Wang 1, Qingyan Fu 1, Yufei Zou 1, Yanmin Huang 1, Huxiong Cui 1, Junming Zhao.
4. Atmospheric chemical transport models 4.1 Introduction 4.2 Box model 4.3 Three dimensional atmospheric chemical transport model.
Rick Saylor 1, Barry Baker 1, Pius Lee 2, Daniel Tong 2,3, Li Pan 2 and Youhua Tang 2 1 National Oceanic and Atmospheric Administration Air Resources Laboratory.
PARTITIONING ET INTO E AND T USING CHAMBERS C. A. Garcia, D. I. Stannard, B. J. Andraski, M.J. Johnson.
A New Inter-Comparison of Three Global Monthly SSM/I Precipitation Datasets Matt Sapiano, Phil Arkin and Tom Smith Earth Systems Science Interdisciplinary.
An Exploration of Model Concentration Differences Between CMAQ and CAMx Brian Timin, Karen Wesson, Pat Dolwick, Norm Possiel, Sharon Phillips EPA/OAQPS.
1 Improving the parameterization of land-surface exchange in the GEOS-Chem Hg model Shaojie Song and Noelle Selin Massachusetts Institute of Technology.
Estimating background ozone in surface air over the United States with global 3-D models of tropospheric chemistry Description, Evaluation, and Results.
Robert W. Pinder, Alice B. Gilliland, Robert C. Gilliam, K. Wyat Appel Atmospheric Modeling Division, NOAA Air Resources Laboratory, in partnership with.
Georgia Institute of Technology SUPPORTING INTEX THROUGH INTEGRATED ANALYSIS OF SATELLITE AND SUB-ORBITAL MEASUREMENTS WITH GLOBAL AND REGIONAL 3-D MODELS:
EMEP WGSR, EMEP Progress on HMs, 2006  Review and evaluation of the MSCE-HM model (TFMM)  Atmospheric pollution in 2004 (emissions, monitoring.
A revised formulation of the COSMO surface-to-atmosphere transfer scheme Matthias Raschendorfer COSMO Offenbach 2009 Matthias Raschendorfer.
Updates to model algorithms and inputs for the Biogenic Emissions Inventory System (BEIS) model Jesse Bash, Kirk Baker, George Pouliot, Donna Schwede,
Yuqiang Zhang1, Owen R, Cooper2,3, J. Jason West1
Approach in developing PnET-BGC model inputs for Smoky Mountains
Impact of dissolved organic carbon (DOC) deposition on soil solution DOC Intern(ation)al data evaluation Arne Verstraeten ICP Forests combined Expert Panel.
Land Use in Regional Climate Modeling
Upper Rio Grande R Basin
ADAGIO (Atmospheric Deposition Analysis Generated by optimal Interpolation from Observations): Project plans and status A.S. Cole1, A. Robichaud2, M.D.
Meteorological drivers of surface ozone biases in the Southeast US
Tanya L. Spero1, Megan S. Mallard1, Stephany M
Lecture 10 Evapotranspiration (3)
Remote Sensing ET Algorithm— Remote Evapotranspiration Calculation (RET) Junming Wang,
EVAPORATION.
3-PG The Use of Physiological Principles in Predicting Forest Growth
in the Neversink River Basin, New York
Statistical Methods for Model Evaluation – Moving Beyond the Comparison of Matched Observations and Output for Model Grid Cells Kristen M. Foley1, Jenise.
“Consolidation of the Surface-to-Atmosphere Transfer-scheme: ConSAT
A Performance Evaluation of Lightning-NO Algorithms in CMAQ
Colin Michel1, C. Amelynck3, M. Aubinet1, A. Bachy1, P. Delaplace2, A
Ashok Luhar, Matthew Woodhouse, Ian Galbally 5 September 2017
Mark A. Bourassa and Qi Shi
Peter Zoogman, Daniel Jacob
Nitrogen Deposition: Measurement Techniques and Field Studies
The application of an atmospheric boundary layer to evaluate truck aerodynamics in CFD “A solution for a real-world engineering problem” Ir. Niek van.
Vegetation and Energy Balance.
Impact on Recent North American Air Quality Forecasts of Replacing a Retrospective U.S. Emissions Inventory with a Projected Inventory Michael Moran1,
Impact of GOES Enhanced WRF Fields on Air Quality Model Performance
Using CMAQ to Interpolate Among CASTNET Measurements
Development and Evaluation of a Forward Snow Microwave Emission Model
Integration of NCAR DART-EnKF to NCAR-ATEC multi-model, multi-physics and mutli- perturbantion ensemble-RTFDDA (E-4DWX) forecasting system Linlin Pan 1,
Shiliang Wu1 Loretta J. Mickley1, Daniel J
Development of a New Parameterization for Below-Cloud Scavenging of Size-Resolved Particles by Rain and Snow Xihong Wang1, Leiming Zhang2, and Michael.
Meteorology & Air Pollution Dr. Wesam Al Madhoun
JEHN-YIH JUANG, Donna Schwede, and Jon Pleim
Alexey Gusev, Victor Shatalov, Olga Rozovskaya, Nadejda Vulyh
REGIONAL AND LOCAL-SCALE EVALUATION OF 2002 MM5 METEOROLOGICAL FIELDS FOR VARIOUS AIR QUALITY MODELING APPLICATIONS Pat Dolwick*, U.S. EPA, RTP, NC, USA.
Topic 3: Meteorology and data filtering
Uncertainties of heavy metal pollution assessment
The EuroDelta inter-comparison, Phase I Variability of model responses
Multi-scale approach to HM and POP modelling
Jielun Sun NCAR Earth System Laboratory
Oleg Travnikov EMEP/MSC-E
Atmospheric modelling of HMs Sensitivity study
Update on specifying boundary conditions for regional-scale air quality models Mike Barna, NPS-ARD RTOWG call 9/10/19.
Presentation transcript:

Evaluation and intercomparison of five major dry deposition algorithms in North America Zhiyong Wu1,2,*, Donna Schwede1, Robert Vet2, John T. Walker1, Mike Shaw2, Ralf Staebler2, Leiming Zhang2 1US EPA; 2Environment and Climate Change Canada *ORISE Fellow; wu.zhiyong@epa.gov 16th Annual CMAS Conference – Oct. 25, 2017

Outline Background and Objectives Description of dry deposition models and measured Vd dataset Evaluation and inter-comparison of five models Conclusions

Background The inferential method is commonly used in dry deposition monitoring networks and atmospheric chemical transport models (CTMs). Different dry deposition algorithms are used in monitoring networks and models: CAPMoN & GEM-MACH: Zhang et al. (2003) CASTNET: Meyers et al. (1998) EMEP: Simpson et al. (2003) WRF-Chem & GEOS-Chem: Wesely (1989) CMAQ: Pleim and Ran (2011) …

CAPMoN vs CASTNET Similar concentration Very different Vd Schwede et al.(2011), AE

A comparison of inferential models across the NitroEurope network (UK) (Canada) (Europe) (Holland) Flechard et al. (2011), ACP Differences between models reach a factor 2–3 and are often greater than differences between monitoring sites.

Objectives The objectives of this study are: to evaluate and inter-compare the dry deposition algorithms used in US and Canada to quantify the magnitudes of model uncertainties to explore the dominant factors causing the discrepancies.

The five dry deposition models One-big-leaf framework the Zhang et al. (2003) scheme used in the Canadian Air and Precipitation Monitoring Network (CAPMoN) and several Canadian and American air quality models (termed as ZHANG) the Noah land surface model coupled with a photosynthesis-based Gas Exchange Model (Niyogi et al., 2009; Wu et al., 2012) (termed as Noah- GEM) the dry deposition module of the Community Multiscale Air Quality (CMAQ) model version 5.0.2 (Pleim and Ran, 2011) (termed as C5DRY) the dry deposition module of WRF-Chem which employs the widely-used Wesely (1989) scheme (termed as WESELY) The multi-layer model used in the US Clean Air Status and Trends Network (CASTNET) based on Meyers et al. (1998)(termed as MLM) Multi-layer framework

Measurements of O3 and SO2 dry depositions at Borden Forest Wu et al. (2016), EP Vegetation Type: 100-year old mixed forest Canopy Height: 22 m Peak Leaf Area Index: 4.6 m2 m-2 Observation: 6 levels of O3 and SO2 concentrations Period : May 2008 - April 2013 Modified gradient method: Wu et al. (2015), ACP

Measured Vd(O3) and Vd(SO2) at Borden Forest Wu et al.(2016), EP

Evaluation and inter-comparison of five models All models produced lower Vd values than measured for O3 in summer and SO2 in summer and winter; There was not a consistent tendency in the models to over- or underpredict for O3 in winter. Differences in mean Vd values between models were on the order of a factor of 2.

Air resistances (Ra & Rb) Monin-Obukhov Similarity Theory (MOST) based (WESELY, Noah-GEM, C5DRY & ZHANG) or where u* is friction velocity, ψh the stability correction function, Sc the Schmidt number, Pr Prandtl number for air (0.72), Dθ thermal diffusivity, and Dc molecular diffusivity of a specific gas. Wind based: (MLM) where a is a constant depending on stability, u mean wind speed, σɵ standard deviation of the wind direction, α constant depending on gas species, δ characteristic leaf dimension.

Vd,max = 1 / (Ra+Rb) MOST type MOST type Wind type Wind type MLM produced larger Ra and Rb than the MOST-based approaches (WESELY, Noah-GEM, C5DRY & ZHANG).

The contribution of atmospheric resistances to the total resistances of O3 and SO2 was generally small (5-15% in this study). With reduced Ra in MLM, mean Vd only increased by about 10%. The main causes of the differences in Vd across the models is mainly due to the differences in the calculated Rc.

Jarvis-style Rs scheme: 1/Rc = 1/Rs + 1/Rns Surface uptake = Stomatal uptake + Non-stomatal uptake Stomatal resistance (Rs) formulations Jarvis-style Rs scheme: (C5DRY, ZHANG & MLM) (WESELY) Ball-Berry Rs scheme: (Noah-GEM)

Stomatal conductance (Gs,x) = 1 / Rs,H2O × (Dx/DH2O) Rs,min=100 s/m Rs,min=150 s/m Rs,min=200s/m The Penman-Monteith method: Here are the modeled Rs for water vapor. Rs for the O3 or SO2 is scaled by the molecular diffusitivity ratio. Because the MLM model calculates Rs at many layers, it is not easy to input Rs as one value to compare with the other models. Rs by MLM is not shown here. Also I calculated Rs using the inverse of the penman-monteith method which is based on the measurements of water vapor flux. This method works well in summer when the water vapor flux is dominately from plants evaportranspiration.It is the black line with filled circles. As we see, the Rs by Zhang is slightly higher than that from the Penman-Monteith method. Both Jarvis-style and Ball-Berry-style schemes can produce a reasonable Rs if the main environmental factors are included and the key parameters are proper prescribed. The Rs by the Jarvis-style scheme is very sensitive to the prescribed value of Rs,min. However, this parameter is mainly derived from empirical fits to field measurements and suffers from large uncertainties.

The mean Vd for O3 and SO2 in ZHANG increased by 14% and 12%, respectively, if rs,min was reduced by 25%. Similar for the other Javis-type models. Large discrepancies still exist in Vd between ZHANG and the observations, which can be further attributed to the non-stomatal parameterization (Rns) of the model.

Non-stomatal conductance (Gns) = 1 / Rns leaf cuticle ground Non-stomatal conductance (Gns) = 1 / Rns Some model (e.g., ZHANG, Noah-GEM) Rns estimates showed significant diurnal variations, while others do not. New measurements from chamber and field studies are needed to better understand processes influencing Rns.

Conclusions and Recommendations The models performed better in summer than in winter with correlation coefficients for hourly Vd between models and measurements being approximately 0.6 and 0.3, respectively. All models produced lower Vd values than measured for O3 in summer and SO2 in summer and winter. There was not a consistent tendency in the models to over- or underpredict for O3 in winter. Differences in mean Vd values of O3 and SO2 between models were on the order of a factor of 2. Model differences were mainly due to different surface resistance parameterizations for stomatal and non-stomatal uptake pathways. Although it cannot be concluded which algorithm is most accurate, it is recommended that users of inferential dry deposition models consider an uncertainty factor of 2 or use ensemble modeling results for ecosystem assessment analysis.

Thank you! Any questions ? Thank you. I am happy to take any question. That is a good question!

Additional Slides