ELDORA TPARC/TCS08 Dataset
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1 ELDORA TPARC/TCS08 Dataset Wen-Chau Lee and Michael M. Bell NCAR NCAR/NPS
2 NRL-P3 ELectra DOppler RAdar 3. cm, 1.8 beam, 38.7 db Gain Antennas & Tx 40 kw Peak Power PRF in 4:5 ratio (6 m/s NV in TPARC) Scan rate up to 144 /s (87 /s in TPARC) Complex chirp w/4 (3 in TPARC) Freq. ~500 m along track resolution in TPARC Unambig. Range ~75 km (Convective) TOGA COARE (93),VORTEX 95, FASTEX (97), LAKEICE (97/98), MAP (99), IHOP (0), CRYSTAL- FACE (0), BAMEX (03), RAINEX (05), TCS- 08/TPARC (08) ELDORA Airborne Doppler Radar
3 ELDORA Data Fields
4 CAPPI Movies Bonus Dataset
5 Dataset Summary Velocity data appears very good throughout project INS Navigation corrections were stable Aft Reflectivity is low from RF16 RF1, reduced sensitivity in cloudy & clear air 165 GB dataset ready, on CODIAC soon Dorade sweep files in ~00 MB 10-minute tar files (netcdf translator available) Navigation correction factors (cfac files)
6
7 Problems in Raw Data 1. Earth surface is tilted.. Earth surface is not stationary. 3. Earth surface moves at different speeds. Testud et al 1995
8 ELDORA Navigation Corrections Accurate knowledge of the aircraft orientation and radar beam pointing angle is essential to airborne Doppler analysis Lee et al, 1994; Testud et al, 1995; Georgis et al, 000; Bosart et al, 00
9 Definitions of INS Attitude Angles Meteorological coordinates-positive clockwise Drift is the angle between track and heading (T=HD), a positive drift angle is defined as the track is more clockwise than the heading Pitch is the angle that the aircraft longitudinal axis makes with the horizontal plane, nose up is positive pitch Roll is the angle that the wings make with the horizontal plane, right wing down is positive Through these three sequential rotation, X is transformed into X a
10 Uncertainties in INS and Antenna Pointing Angles Measurement/Instrument Errors: Horizontal velocity (V H ): ± m s -1 Drift angle (α): ± 1 Aircraft vertical velocity (W): ± 0.15 m s -1 Pitch angle (β): ± 0.05 Tilt angle (θ): ± 0.05 Roll/spin angle (φ): ± 0.05 Systematic errors (e.g., mounting errors) in the order of 1 may exist
11 Spherical Trigonometry and Radial Velocity V r = usin(a z )cos(el) vcos(a z )cos(el) (w w t )sin(el) V g V a cos A z sinθ sinelsinβ = coselcosβ sinel= sinθ sinβ cosθ cosβ cosφ cosψ= cosα cosβ sinθ cosα sinβ cosθ cosφ sinα cosθ sinφ α: drift β: pitch φ: spin/rotation θ: tilt Ψ: π/-track-relative tilt A z : azimuth EL: elevation
12 Velocity Error Analysis Estimated aircraft ground speed (V Ge ): V = V cos Ψ W sin EL Ge H = ( V H V o cos λ )(cosα cos β sinθ cosα sin β cosθ cosφ sinα cosθ sinφ) W (sinθ sin β cosθ cos β sinφ) Measured aircraft ground speed by the radar (V G ): δv G : the velocity of the ground gate after removing ground speed δv G = V G = δ ( V = δw δθv V H V cos Ψ W cosθ cosφ V H H Ge sinα cosθ cosφ δβv (cosα sinθ sinα cosθ sinφ) δv = A B 1 sinφ B o sin EL) H (sinα sinθ cosα cosθ sinφ) cosφ (cosα cosθ sinα sinθ sinφ) δθ H cosα cosθ cosφ H
13 Range Error Analysis R N G G H = sin EL Rε δr tan EL δr: gate spacing R R : actual distance to the ground ε: beam width R G = H cosφ = sin EL H = sinθ sin β cosθ cos β cosφ R R ΔR R Ge = sinθ sin β e e H e cosθ e cos β cosφ e e
14 Range Error Analysis (Continue) δr G : difference between the actual distance to the ground and estimates from aircraft altitude and elevation angles of a radar beam R R δr R G Ge = = R R G G = δr R δh ( H G Ge ΔR tanθ δβ cosφ tanθδθ tanθδφ) cos φ( R R R Ge ) ΔR = H tanθ δβ cosθ Hδφ sinφ cosθ δh H tanθδθ ΔR cosφ cos φ cosθ = C D sinφ D cosφ E cos φ 1
15
16 Moving Ocean Surface If the ground is not stationary, then we match in situ wind with near aircraft dual- Doppler wind if there are scatterers near the aircraft (BLW correction) Use to refine ground speed and drift
17 Reverse Headings
18
19 TPARC/TCS08 Corrections Ground speed, Tilt error determined from reverse headings, drift from project average
20 Basic Analysis Process
21 1. *Translate the raw ELDORA field format data into DORADE sweep files. *Calculate navigation correction factors (cfac files) for each flight 3. Fine-tune navigation corrections for each leg of data 4. Edit the data to remove ground echo, noise, clutter, and radar side-lobes, as well as velocity unfolding. 5. Interpolate and/or Synthesize multiple data files to get 3-dimensional wind field and derived quantities.
22 Raw Data
23 Edited Data
24 Typhoon Hagupit
25 Typhoon Hagupit
26 Hagupit Pre-genesis
27 Multi-Doppler Synthesis V r = u sin(a)cos(e) vcos(a)cos(e) (w w t )sin(e) sin a cos e sinacosacos e sinacosesine u sinacosacos e cos a cos e cosacosesine v = sinacosesine cosacosesine sin e w w t V r sinacose V r cosacose V r sine Hildebrand et al 1996
28 Doppler Synthesis Approaches Forward Local (Sprint/Reorder & Cedric) Empirical Interpolation of V r (Distance weighted averaging), then local synthesis Forward Global (Gamache, Raymond & Carrillo*) Empirical Interpolation, then global synthesis Reverse Global (Gao et al. 1999/004, Bell) Interpolation from grid to radar space during cost function minimization
29 Forward Local synthesis Conventional using reorder/cedric Quasi-horizontal assumption Resolve horizontal velocities then integrate continuity equation vertically to obtain vertical velocities Limited to elevation angle less than 45 deg Difficult to resolve storm top when storm is close to the radar
30 Problems with Radial Velocity Interpolation and Averaging Big issue for airborne synthesis and Reorder Also a problem for ground-based platforms near the radar Solutions: Use more, small chunks Include full az/elev info Avoid it
31 3-D Variational Formulation (Gamache 1997, Reasor et al 009): Solve two or more radial velocity equations and mass continuity equation simultaneously. B B ijk K k J j I i k n ijk k ijk k ijk k ijk k ijk k ijk k ijk k ijk k ijk k ijk k ijk k ijk k ijk k ijk k ijk k ijk k ijk k ijk k K k J j I i n ijk k K k J j I i n ijkl ml Tml ml ijk ml ml ijk ml ml ijk rml L l K k J j I i k m n n n n n n n n w w J z y w z x w y x w z y v z x v y x v z y v z x u y x u z w y w x w z v y v x v z u y u x u J V J v w v u V J J J J J J J F δ α φ φ φ θ φ θ λ λ λ λ λ λ ) ( ) ( ) sin sin cos sin cos cos ( } { = = = = = = = = = = = = = = = = = = r L
32 TCVAR (Bell 009) Can combine radar, dropsonde, and flight level data Low noise via cubic interpolations and spectral derivatives Tunable error specifications and filtering a q(r,z) = rv,ψ,h, q v, { }
33 Raymond & Carrillo
34 Advantages / Disadvantages Error Propagation Memory/C PU Diagnostics Multiple Data Sources Anisotropic Filtering Extra Balance Constraints Forward Local Vertical Low/Fast Established Difficult Possible Difficult Forward Global Horizontal & Vertical High/Slo w Complex Possible Difficult Possible Reverse Global (Bell) BG Error Covariance Low/Slo w Moderate Yes Yes Possible Multiple analysis techniques are a good thing!
35 Automatic Editing for Data Assimilation and New Users Still work in progress Fuzzy logic echo classification system under development Soloii scripts available now for light (80%) to heavy (99%) artifact removal In between is most difficult
36 Automatically Edited (80%)
37 Automatically Edited (99%)
38 Manually Edited Data
39 Summary Data quality is good with exception of aft reflectivity later in project. Radar data is ready, on CODIAC soon CAPPI movies will be available soon also A variety of software tools are available for viewing, editing, and processing New users welcome! Come talk to us about how you could use ELDORA data
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