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EnKF Localization Techniques and Balance 1 Steven J. Greybush, 1 Eugenia Kalnay, 2 Takemasa Miyoshi 1 University of Maryland, College Park, MD, U.S.A. 2 Numerical Prediction Division, Japan Meteorological Agency, Tokyo, Japan. Results from Assimilation of Gridded Observations
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EnKF Localization Techniques and Balance 1Steven J. Greybush, 1Eugenia Kalnay, 2Takemasa Miyoshi 1University of Maryland, College Park, MD, U.S.A. 2Numerical Prediction Division, Japan Meteorological Agency, Tokyo, Japan • Results from Assimilation of Gridded Observations • Assimilate 20 observations of h and v (randomly perturbed from the truth) at regular intervals along the domain; observe accuracy and balance of the analysis. • Localization • A modification of the covariance matrices in the Kalman gain formula that reduces the influence of distant regions. (Houtekamer and Mitchell, 2001) • Removes spurious long distance correlations due to sampling error of the model covariance from finite ensemble size. (Anderson, 2007) • Takes advantage of the ensemble's lower dimensionality in local regions. (Hunt et. al., 2007) • Ultimately creates a more accurate analysis (reduces RMSE). Localization Distance L=1000 km; Distance between Observations D = 500 km; Wavelength W = 2000 km Analysis Increments: Initial Waveforms: • Balance • Lorenc (2003) and Kepert (2006) argue that localization reduces the balance information encoded in the model covariance matrix. • Houtekamer and Mitchell (2005) noted balance issues when applying a localized EnKF to the Canadian GCM. • Imbalanced analyses project information onto inertial-gravity waves, which are filtered out (geostrophic adjustment, digital filtering, etc.), resulting in a loss of information and a suboptimal analysis. • Two Methods of Localization • Model Covariance Matrix Localization (B Localization) • Accomplished by taking a Schur product between the model covariance matrix and a matrix whose elements are dependent upon the distance between the corresponding grid points. (Hamill et al., 2001) • Model grid points that are far apart have zero error covariance. • Observation Covariance Matrix Localization (R Localization) • Observations that are far away from a grid point have infinite error. K = BHT(HBHT + R)-1 Analysis Imbalance: B Localization >> R Localization > No Localization Analysis RMS Error: B Localization < R Localization < No Localization • Results from Monte Carlo Simulations • Three scales in the problem: W = wavelength of solutions L = localization distance D = distance between observations • Explore the phase space of the three scales. • Obtain robust results by repeating each scenario 100x with random observation errors. L Bloc = B * exp(-(ri-rj)2 / 2L2) Rloc = R * exp(+(d)2 / 2L2) Constant D=500 km, W=2000 km, vary L: • Research Questions • How does localization introduce imbalance into an analysis? Can it be avoided? • How do the analyses produced by B-localization and R-localization EnKF compare in terms of accuracy (RMSE) and (geostrophic) balance? • Experimental Setup • Model • The shallow water equations in a rotating, inviscid fluid. • Variation only along the x-axis. • The variables of interest are h and v. • Linearize the equations, and apply a harmonic form to the solution. • Substituting into the governing equations, and assuming geostrophic balance, yields the following solutions for h and v: • Ensemble • Initially geostrophic waveform for truth and 2 ensemble members. • 101 Grid Points every 50 km along domain. Constant D=250 km, vary L and W: (warmer colors show greater imbalance) • Use ageostrophic wind as measure of imbalance. • vageo = v – g/f dh/dx • Localize the waveforms with L=1500 km. • |-dh/dx| increases while |v| decreases, disrupting the balance between the wind field and the mass field. (Lorenc 2003) Initial Ensemble and Truth • Conclusions • Both types of localization do introduce imbalance into analysis increments, especially for short localization distances. • R localization is significantly more balanced than B localization, but is slightly less accurate. • Future Work • Complement this study by comparing balance for B localization and R localization EnSQRT data assimilation on the SPEEDY GCM (Molteni, 2003), using realistic observation densities and locations. • Further investigate the mathematical properties of the two localization methods. Imbalance (Ageostrophic Wind) Localized Ensemble • Acknowledgements • Thanks to Kayo Ide and Jeff Anderson for their helpful comments and critiques of this project. WCRP/THORPEX WORKSHOP on 4D-VAR and ENSEMBLE KALMAN FILTER COMPARISONSBuenos Aires, Argentina; November 10-13, 2008