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Published byPearl Edwards Modified over 8 years ago
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Our experiences with EnKF assimilation of high-res radar observations collected in the 5 June 2009 Vortex 2 tornadic supercell. Jim Marquis, Yvette Richardson, Paul Markowski, David Dowell, Josh Wurman, Karen Kosiba, Paul Robinson Photo by Sean Waugh
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Goals of EnKF analysis Increase availability of 3-D kinematic and thermodynamic data (dual-Doppler and in situ obs are spatially/temporally limited). Courtesy of Paul Markowski
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Goals of EnKF analysis We want a set of smoothly evolving EnKF analyses (i.e., We are not using EnKF to initialize a forecast). Analyze roles that mesocyclone-scale processes play in tornadogenesis, maintenance, and decay: - trajectory analysis, - circulation/vorticity budgets, - mid-upper level features.
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Model Specifics WRF-ARW 3.2.1: -Δx,y = 500 m, 80m < Δz < 2km, [120 x 80 x 20] km 3 -LFO microphysics, -open lateral BCs, -no surface fluxes, no radiation, flat terrain. Homogeneous environment :
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DA Specifics DART: – Ensemble adjustment filter, – 50 members, – Localization: Gaspari-Cohn, W = 0 @ r = 6 km – Ensemble initiation: 10 randomly placed warm bubbles at model t 0 for each member – Ensemble spread maintained with: Additive noise added to T, Td, U, V every 5 min where radar reflectivity is > 25 dBZ, (Dowell and Wicker 2009) Perturbations smoothed to 4 km (horiz), 2 km (vert) scales
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Courtesy www.vortex2.org σ 2 obs = (2 m/s) 2 Radar velocities assimilated every 2 minutes OBAN: Cressman weighting 500 m horizontal grid spacing (for 500m-model grid experiment) data along conical slices Experiment timeline “synthetic Data”
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Thinning the amount of observations assimilated: Unthinned50% assim’ed 25% assim’ed Model grid Radar vel. ob. Y X No thinning done in vertical direction shown today; though, experiments show poor storm structure when low-level elevation angles are neglected.
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θρθρ dBZ ζ W > 0 Z = 0.5 km AGL (Note: these experiments conducted with 2-km model grid) (K) X Y 50% assimilated 25% assimilated unthinned Y
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ζ radars Dual-Doppler EnKF W m/s Z = 400 m AGL Dual-Doppler – EnKF (ensemble mean) kinematics comparison (DOW6 & DOW7) X (km) Y (km)
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Model errors/idealized conditions require DA for a good storm. Storm structure with/without radar assimilation: Top row: Series of EnKF (Ens. Mean) analyses. Bottom row: Single member forecasted forward from 2157 (no DA). ζ Z = 150 m X (km) Y (km)
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ζ Ensemble mean analyses – temperature fields Z = 50 m (Note: these experiments conducted with 1-km model grid)
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ζ Z = 50 m Mob. Mesonets
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ζ Z = 50 m Mob. Mesonets
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MM obs – EnKF outflow comparison θ’ (K) ζ Low-level w max trace: dBZ MM obs: Not great, particularly in far left FF Better overall, but still disagreement in FF Decent, but still disagreement in FF Warmth (lasts 1-2analysis times) - Seems to disagree With few available MM obs Pretty good decent ok MM’s only just getting into storm, but so far - not good My < 1 sentence impression of the agreement of MM obs and each EnKF analysis Z = 50 m Sequence of EnKF analyses of theta’ and MM obs (valid +/- 1 min from EnKF analysis) overlayed: ζ Z = 50 m
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Mesocyclone buoyancy (function of height & time) Circulation and radial motion (function of radius & time) Periods of tornado lifecycle Pre-tornadic T-genesis Intensification Maturity Weakening Time (UTC) Inbound 0 m/s Outbound Positively buoyant Negatively buoyant
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Trajectories (storm-rel.) calculated from ens. mean analyses W (z = 200m) Ring (radius = 1 km) of 20 parcels centered on peak ζ at z = 200 m; integrated forward in time from 4 times θρθρ ‘ (K) Most parcels rising into updraft Some parcels rising into updraft Few/no parcels rising into updraft No parcels rising into updraft
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θρθρ ‘ (K) Pre-tornadic T-genesis Intensification Maturity Weakening Comparison across model grid resolutions
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RMSI Total Spread Consistency Ratio
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θ’ (K) Low-level w max trace: MM obs: ζ
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Summary EnKF Kinematic Analyses: -Compare well with dual-Doppler fields of similar scale. -Storm-scale structure robust with different model scale. More details come with finer model grid res. EnKF Thermo Analyses: -Mixed success with comparisons to MM in situ obs (where available). -500-m model grid seems verify with MM obs best in mesocyclone area (partially due to more details captured?) -Seemingly random, possibly unphysical(?) anomalies appear more prominently with finer model resolution.
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Questions 1)Different way to maintain ensemble spread (adaptive methods)? 2)How else can we determine plausibility of analyses (kinematic and thermodynamic)? -Forcing terms along parcel trajectories? 3)More rigorous methods for optimizing scales/amounts of observations (compared to model resolution)?
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Acknowledgements The EnKF experiments were performed using NCAR CISL supercomputing facilities with the Data Assimilation Research Testbed (DART) and WRF-ARW software. Thank you to Glen Romine, Lou Wicker, Dan Dawson, Chris Snyder, and Nancy Collins for advice/help. Thanks to all VORTEX2 crew for their dedication while collecting data on 5 June 2009. This research is funded by NSF grants: NSF-AGS-0801035, NSF- AGS-0801041. The DOW radars are NSF Lower Atmospheric Observing Facilities supported by NSF-AGS-0734001.
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