1. The Importance of Atmospheric Variability for Data Requirements, Data Assimilation, Forecast Errors, OSSEs and Verification Rod Frehlich and Robert Sharman University of Colorado, Boulder RAP/NCAR Boulder Funded by NSF (Lydia Gates) and FAA/AWRP

2. In Situ Aircraft Data Highest resolution data Many flights provide robust statistical description (GASP, MOZAIC) Reference for “truth”

3. Spatial Spectra Robust description in troposphere Power law scaling Valid almost everywhere

4. Structure Functions Alternate spatial statistic Interpretation is simple (no aliasing) Also has power law scaling Structure functions (and spectra) from model output are filtered Corrections possible by comparisons with in situ data Produce local estimates of turbulence defined by ε or C T 2 over LxL domain

5. RUC20 Analysis RUC20 model structure function In situ “truth” from GASP data Effective spatial filter (3Δ) determined by agreement with theory

6. UKMO 0.5 o Global Model Effective spatial filter (5Δ) larger than RUC The s 2 scaling implies only linear spatial variations of the field

7. DEFINITION OF TRUTH For forecast error, truth is defined by the spatial filter of the model numerics For the initial field (analysis) truth should have the same definition for consistency Measurement error What are optimal numerics?

8. Observation Sampling Error Truth is the average of the variable x over the LxL effective grid cell Total observation error Instrument error =  x Sampling error =  x The instrument sampling pattern and turbulence determines the sampling error

9. Sampling Error for Velocity and Temperature Rawinsonde in center of square effective grid cell of length L

10. UKMO Global Model Rawinsonde in center of grid cell Large variations in sampling error Dominant component of total observation error in high turbulence regions Very accurate observations in low turbulence regions

11. Optimal Data Assimilation Optimal assimilation requires estimation of total observation error covariance Requires calculation of instrument error which may depend on local turbulence (profiler, coherent Doppler lidar) Requires climatology of turbulence Correct calculation of analysis error

12. Adaptive Data Assimilation Assume locally homogeneous turbulence around analysis point r forecast observations

13. Optimal Analysis Error Analysis error depends on forecast error and effective observation error forecast error effective observation error (local turbulence)

14. Analysis Error for 0.5 o Global Model Instrument error is 0.5 m/s Large reduction in analysis error for  b =3 m/s

15. Implications for OSSE’s Synthetic data requires local estimates of turbulence and climatology Optimal data assimilation using local estimates of turbulence Improved background error covariance based on improved analysis Resolve fundamental issues of observation error statistics (coverage vs accuracy) Determine effects of sampling error (rawinsonde vs lidar)

16. Implications for NWP Models Include realistic variations in observation error in initial conditions of ensemble forecasts Determine contribution of forecast error from sampling error Include climatology of sampling error in performance metrics

17. Future Work Determine global climatology and universal scaling of small scale turbulence Calculate total observation error for critical data (rawinsonde, ACARS, profiler, lidar) Determine optimal model numerics Determine optimal data assimilation, OSSE’s, model parameterization, and ensemble forecasts Coordinate all the tasks since they are iterative

18. Estimates of Small Scale Turbulence Calculate structure functions locally over LxL square Determine best-fit to empirical model Estimate in situ turbulence level and ε ε 1/3

19. Climatology of Small Scale Turbulence Probability Density Function (PDF) of ε Good fit to the Log Normal model Parameters of Log Normal model depends on domain size L Consistent with large Reynolds number turbulence

20. Scaling Laws for Log Normal Parameters Power law scaling for the mean and standard deviation of log ε Consistent with high Reynolds number turbulence