Cycling Variational Assimilation of Remotely Sensed Observations for Simulations of Hurricane Katrina S.-H. Chen1 E. Lim2, W.-C. Lee3, C. Davis2, M. Bell3, Q. Xiao2, H.-C. Lin2, G. Holland2 Land, Air, and Water Resources, University of California, Davis, CA, USA 2 Mesoscale and Microscale Meteorology Division/NCAR, Boulder, CO, USA 3 Earth Observing Laboratory/NCAR, Boulder, CO, USA 1 Introduction Results and Discussion 1000 990 SLP (hPa) 1000 950 990 980 940 970 0 6 12 960 18 Time (h) 24 30 36 950 940 (b) 920 OBS ALL_2h NORAD 910 900 0 6 CNTL ALL_3h 12 ▲ Fig. 4: 300-mb geopotential height and wind vectors from (a) AVN reanalysis, (b) EXP1 ALL_3h, (c) EXP2 ALL_2h, and (c) EXP3 06h at 18Z 26 August 2005. ALL RAD 18 24 Time (h) 30 36 1000 990 SLP (hPa) 980 970 (c) 960 OBS 03h 09h 00h 06h 12h Observations 0 6 12 18 Time (h) 24 30 36 (c) (c) ▲ Fig. 3: Simulated tracks from (a) EXP1, (b) EXP2, and (3) EXP3. Assimilated data CNTL CNTL ALL ALL GTS + Sat + hourly Radar ALL_2h ALL_2h GTS + Sat + 2-hly Radar ALL_3h ALL_3h GTS + Sat + 3-hly Radar NORAD NORAD RAD RAD (c) 1000 (d) 50 65 990 980 970 980 980 OBS OBS CNTL CNTL ALL ALL ALL_2h ALL_2h ALL_3h ALL_3h RAD RAD NORAD NORAD 970 970 960 960 950 950 66 12 12 960 OBS CNTL ALL ALL_2h ALL_3h RAD NORAD 950 940 930 920 910 940 940 00 980 18 24 18 24 Time (h) Time (h) 30 30 36 36 970 960 OBS 03h 09h 950 00h 06h 12h 0 6 12 18 Time (h) 24 30 36 40 35 30 25 OBS CNTL ALL ALL_2h ALL_3h RAD NORAD 940 900 45 20 0 6 12 18 Time (h) 24 30 36 0 6 12 18 Time (h) 24 30 36 CNTL ALL ALL_2h 55 ALL_3h RAD 50 NORAD 60 45 40 35 30 55 24 30 36 06h 09h 12h 6 12 35 30 20 18 Time (h) 03h 40 20 12 00h 45 25 6 OBS 50 25 0 (f) 65 OBS 60 10-m Maximum wind (m/s) 990 990 (e) 0 18 Time (h) 24 30 36 ▲ Fig. 5: Simulated minimum sea level pressure (a-c) and maximum 10-m wind speed (d-f). Experiment Design EXP1 EXP2 (25/18Z-26/00Z) (26/00Z-26/06Z) 1000 SLP (hPa) ▲ Fig. 2: (a) The positions of Katrina with respected to Miami radar, R, and the coverage of (b) QuikSCAT and (c) Special Sensor Microwave/Imager (SSM/I) satellite data from 18Z 25 August to 00Z 26 August, 2005 used in this study. The blue dot at the tip of Florida is Katrina’s position at 0000 UTC 26 August, 2005. (b) 990 SLP(hPa) (hPa) SLP ▲ Fig. 1: (a) Best track positions, (b) observations (pts) and best track (line) maximum sustained surface wind speed, and (c) pressure observations (pts) and best track (line) minimum central pressure for Hurricane Katrina, 23-30 August 2005. (Courtesy of National Hurricane Center) 1000 1000 (a) 10-m Maximum wind (m/s) (b) SLP (hPa) (a) The simulated storms from EXP1 moved too slowly and meandered over southern Florida. No improvement was made for simulated tracks after the use of any observation (Fig. 3a). This is because the upper-level anticyclone did not intrude southward into the northern Gulf of Mexico (Fig. 4a vs. 4b). The results were greatly improved when the model started 6 h later (i.e., EXP2; Fig. 3b), in particular with the assimilation of observations. The error was ~50 km throughout the simulation period. The location of the upper-level anticyclone was comparable with that from AVN reanalysis (Fig. 4a vs. 4c). Simulated tracks from EXP3 were slightly deflected southward (Fig. 3c) because the upper-level anticyclone intruded slightly too far south (Fig. 4a vs. 4d). However, these tracks were much better than those from EXP1, which started data cycling with the same first guess at 1800 UTC 25 August 2005. Results from EXP1-3 further illustrate that the improvement to the simulated track was contributed by GTS data and/or satellite data from 0000 UTC to 0600 UTC August 26. 10-m Maximum wind (m/s) 930 940 (b) (d) OBS CNTL ALL ALL_2h ALL_3h RAD NORAD 970 950 (a) (c) (b) (a) 960 SLP (hPa) Tropical cyclones (TCs) at landfall are one of the most dangerous natural disasters. Accurate TC data analysis and forecasts are crucial for the protection of life and property. Despite recent progress in TC track forecasting, intensity forecasting remains unsatisfactory primarily due to complicated processes at multiple scales, including cloud-scale moist convection interacting with hurricane large-scale environmental flows. To gain understanding of TC multi-scale processes and thus improve forecasts of the rapid intensification or weakening of TCs, it is important to observe both the small-scale inner-core structure and the large-scale environmental flows that have a profound impact on TC evolution. Unfortunately, TC forecasting over the ocean remains a big challenge, especially during the period of most rapid intensification and weakening, because of the lack of in-situ observations. Consequently, specification of the model initial condition must rely on remotely-sensed techniques to retrieve the critical parameters over both the inner-core and the vast area covered by TCs. This study assimilated different scale observations from radar, satellite, and conventional instruments and assessed the impact of these data on Hurricane Katrina (2005) simulations during one of its rapid intensification periods (see the magenta lined box in Fig. 1) using the high-resolution Weather Research and Forecasting (WRF) model. (a) 980 No data GTS + Sat GTS + hourly Radar EXP3 (25/18Z-26/06Z) Assimilated data 00h Sat + 25/18Z Radar 03h GTS + Sat + 25/18Z & 25/21Z Radar 06h GTS + Sat + 25/18Z, 25/21Z & 26/00Z Radar 09h GTS + Sat + 3-hly Radar until 26/03Z 12h GTS + Sat + 3-hly Radar until 26/06Z Three sets of experiments, EXP1-3, with various initial times and data cycling periods were conducted. The data cycling periods, which were applied to the coarsest three domains, were 1800 UTC August 25 to 0000 UTC August 26 (6 h), 0000 UTC to 0600 UTC August 26 (6 h), and 1800 UTC August 25 to 0600 UTC August 26 (12 h) for EXP1-3, respectively. The different observations assimilated for each experiment are shown in Table 1. The first two sets (i.e. EXP1 and EXP2) evaluated the impact of assimilating different observations on Katrina simulations, while the last one (EXP3) examined the influence of different assimilation periods for radar data. In EXP3, satellite and conventional data were assimilated whenever data were available during the whole 12-h cycling period, but radar data were assimilated only every three hours over different time periods (i.e., 0h, 3h, 6h, 9h, and 12h). Thirty-six hour model integrations were then performed on all four domains after the data cycling. Katrina was not only extremely intense but also exceptionally large. Unfortunately, the simulated Katrina was smaller than observed for all experiments conducted here (figure not shown). Results from EXP1 show that the assimilation of radar and conventional data had a positive impact on simulated storm intensities during the first 24 hours. The influence of satellite data was also positive, though less significant, but was able to extend over the whole 36-h simulation (Figs. 5a and 5d) since the coverage of satellite data was much larger than that of radar. Results from EXP2 show great improvement in both simulated storm intensities (Figs. 5b and 5e) and tracks after the use of observations. Finally, EXP1-3 (Fig. 5) indicated that the assimilation of radar data at an interval of every three hours for a 6-h time period is optimal. Summary Simulated Katrina was smaller than the observed size. The assimilation of observations improved simulated storm intensity for all three experiments and improved simulated storm track for EXP2 and EXP3. Radar data influenced the first 24 hours of simulations, while the influence of satellite data lasted longer, but was less significant. EXP3 confirmed that observations from 0000 UTC to 0600 UTC Aug 26 played a key role in improving simulated tracks. Doppler radar data assimilation mainly contributed to the improvement of simulated hurricane intensity, in particular during the early time period of simulations The assimilation of radar data at an interval of every three hours for a 6-h time period is close to an optimal setting.