Evan Kodra Introduction: Auroop Ganguly 08/2013

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SDS Lab Overview + Physics-guided statistical approach to uncertainty quantification from climate model ensembles Evan Kodra Introduction: Auroop Ganguly 08/2013

Postdocs: Poulomi Ganguli - drought characterization and prediction Rachindra Mawagaledara - regional climate modeling David Wang oceanography and climate physics Professor Auroop Ganguly Research Assistant Babak Fard computer science PhD Candidates: Debasish Das climate extremes data mining Evan Kodra extremes uncertainty quantification Devashish Kumar non linear dynamics and natural hazards Saeed Zabet Hydrological data analysis

Selected SDS Lab Members Research 2009 2011 2012 Persistence of cold extremes under climate change Increasing intensity and uncertainty in heatwaves Ghosh et al. 2012 Ganguly et al. 2009 Kodra et al. 2011 Increasing spatial variability in Indian rainfall extremes

Now: Putting a bunch of ideas together Opportunity to use known physics, statistical models, and observed data to quantify (and reduce??) uncertainty in rainfall extremes Pall et al. 2007 Tebaldi et al. 2004 & 2005 O Gorman et al. 2009 Fasullo and Trenberth 2012 Hall and Qu 2006 Min et al. 2011

Physics Infused Statistical Uncertainty Quantification What processes dictate rainfall extremes? Vertical wind velocity Horizontal moisture convergence Moist adiabatic temperature lapse rate Saturation vapor pressure Local mean air temperature when extremes occur Modeled and measured well Modeled and measured less well Idea: weight ESMs by which ones get the link between temperature and rainfall extremes right let the unknown and unmeasured fall into uncertainty terms

lncc(t = 0:30, h = 1) 0 10 20 30 40 50 Physics Infused Statistical Uncertainty Quantification Measuring ESM reliability: realism in portraying adherence to Clausius-Clapeyron Scaling h=1 h=-0.5 h=0.5 The original August-Roche- Magnus approximation to the CC A log transformation 0 5 10 15 20 25 30 Time Example deviations from the August-Roche-Magnus, where h=1 is the original August-Roche- Magnus. intercept slope error A statistical mechanism to encapsulate a basic physical process and the rest falling into an error term A (potentially generalized) linear regression relationship with some unknown parameters that can be mapped back to nonlinear deviations from CC scaling

% Change in Seasonal Maxima (1950-1999 2050-2099) 0.15 0.05 0.05 0.10 0.15 0.3 0.2 0.1 0.0 0.1 0.00 0.05 0.10 0.15 0.05 0.05 0.10 0.15 0.20 But will this link tell us anything useful? We might want something like this In CONUS Observations: Processes that dictate rainfall extremes differ across seasons Pearson s ρ (seasonal maxima rainfall total, same day average temperature, 1915-2011) SON, tau=0.35 DJF, tau= 0.30 Which ESMs capture these patterns? And do they say something different about thee future? 0.5 0.6 0.7 0.8 0.50 0.55 0.60 0.65 0.70 MAM, tau=0.10 JJA, tau= 0.12 Hints that this approach might be useful in constraining uncertainty Variability by region Variability by season Host of additional considerations 0.55 0.65 0.75 0.85 0.2 0.3 0.4 0.5 0.6 Spatial PDF Overlap [0,1]

lncc(t = 0:30, h = 1) 0 10 20 30 40 50 Applying the idea in a UQ Framework ln[h r ] μ r l r + (δ r )X r ln[h j,r ] μ j,r l r + (δ j,r +δ r )X r ln[p j,r H j,r ] μ j,r l r + {(δ j,r + δ r )Y r - β[(δ j,r +δ r ) X r ]} GLMs for location parameters in a GEV or GPD model to be updated in a recursive MCMC algorithm Use concepts of skill and consensus (e.g. Tebaldi et al. 2004 and Smith et al. 2009) Weight assignment: f (δ r, δ j,r, δ j,r ) Weights should decay as GCMs fall further from true nature of adherence to real CC scaling described by δ r (but not necessarily from theoretical CC scaling) h=1 h=-0.5 h=0.5 0 5 10 15 20 25 30 Time H k,r H j,r P j,r H j,r X r, Y r δ Historical observation from dataset k at location r Historical simulation from ESM j at location r Projection from GCM j at location r, conditioned on GCM j s historical simulation Historical temperature and future at location r (in reality uncertain) Regression coefficients relating X r and Y r to central tendency of log transformed rainfall extremes.

Thank you PhD Committee Auroop Ganguly (NEU) Climate & Data Science Snigdhansu Chatterjee (UMN) Statistics Albert-László Barabási (NEU) Network Science John Drake (UTK, previously lead climate modeler at ORNL) Climate Modeling Jerome Hajjar (NEU) Structures Ferdi Hellweger (NEU) - Hydrology

References Fasullo, J. T., and K. E. Trenberth (2012), A less cloudy future: The role of subtropical subsidence in climate sensitivity, science, 338(6108), 792 794. Ganguly, A. R., K. Steinhaeuser, D. J. Erickson, M. Branstetter, E. S. Parish, N. Singh, J. B. Drake, and L. Buja (2009), Higher trends but larger uncertainty and geographic variability in 21st century temperature and heat waves, Proc. Natl. Acad. Sci., 106(37), 15555 15559. Ghosh, S., D. Das, S.-C. Kao, and A. R. Ganguly (2011), Lack of uniform trends but increasing spatial variability in observed Indian rainfall extremes, Nat. Clim. Change, 2(2), 86 91. Hall, A., and X. Qu (2006), Using the current seasonal cycle to constrain snow albedo feedback in future climate change, Geophys. Res. Lett., 33(3). [online] Available from: http://onlinelibrary.wiley.com/doi/10.1029/2005gl025127/full (Accessed 15 August 2013) Kodra, E., K. Steinhaeuser, and A. R. Ganguly (2011), Persisting cold extremes under 21st-century warming scenarios, Geophys. Res. Lett., 38(8). [online] Available from: http://onlinelibrary.wiley.com/doi/10.1029/2011gl047103/full (Accessed 28 June 2013) Kodra, E., Ganguly, A.R., (2013), Asymmetric projected changes of hot versus cold temperature extremes under climate change. In review Min, S.-K., X. Zhang, F. W. Zwiers, and G. C. Hegerl (2011), Human contribution to more-intense precipitation extremes, Nature, 470(7334), 378 381. O Gorman, P. A., and T. Schneider (2009), The physical basis for increases in precipitation extremes in simulations of 21st-century climate change, Proc. Natl. Acad. Sci., 106(35), 14773 14777. Pall, P., M. R. Allen, and D. A. Stone (2007), Testing the Clausius Clapeyron constraint on changes in extreme precipitation under CO2 warming, Clim. Dyn., 28(4), 351 363. Smith, R. L., C. Tebaldi, D. Nychka, and L. O. Mearns (2009), Bayesian modeling of uncertainty in ensembles of climate models, J. Am. Stat. Assoc., 104(485). [online] Available from: http://amstat.tandfonline.com/doi/full/10.1198/jasa.2009.0007 (Accessed 19 July 2013) Tebaldi, C., L. O. Mearns, D. Nychka, and R. L. Smith (2004), Regional probabilities of precipitation change: A Bayesian analysis of multimodel simulations, Geophys. Res. Lett., 31(24). [online] Available from: http://onlinelibrary.wiley.com/doi/10.1029/2004gl021276/full (Accessed 19 July 2013) Tebaldi, C., R. L. Smith, D. Nychka, and L. O. Mearns (2005), Quantifying uncertainty in projections of regional climate change: A Bayesian approach to the analysis of multimodel ensembles, J. Clim., 18(10), 1524 1540.

0 10 20 30 0.10 0.05 0.10 0.00 0.05 0.05 0.00 0.05 0.05 0.10 0.05 0.00 0.05 0.10 0.05 0.00 0.05 0.10 0.05 0.10 0.00 0.05 0.05 0.00 0.05 0.05 2013: Model-data driven insights a) Winter Minima nhex, winter minima Kodra et al. 2013 b) Winte EVT and resampling: Statistical tools for hypothesis testing Asymmetry measured as Δ in quantiles here a) Winter Minima 0.005 0.01 0.05 0.1 0.25 0.5 0.75 0.9 0.95 0.99 0.995 shex, winter minima c) Summer Minima PDF Quantiles b) Winte 0.005 0.01 d) Summ Almost unanimous that the global PDF will change asymmetrically especially for winter and minimum temperature based extremes 0.005 0.01 0.05 0.1 0.25 0.5 0.75 0.9 0.95 0.99 0.995 c) Summer Minima PDF Quantiles CMIP5 model ensemble generally projects larger changes in the highest than the lowest statistics of temperature extremes 0.005 0.01 0.05 0.1 0.25 0.5 0.75 0.9 0.95 0.99 0.995 PDF Quantiles Covariates describing asymmetry: season >> tail >> latitude band >> GCM variability 0.005 0.01 d) Summ 0.005 0.01