Application of Aeolus Winds

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Presentation transcript:

Application of Aeolus Winds Ad.Stoffelen@knmi.nl Gert-Jan Marseille, KNMI Harald Schyberg, Met No

Overview High vertical resolution radiosonde clouds and implications for Aeolus measurements Theoretical tool for testing all the things we fancy so much in data assimilation: thinning, QC, bias, correlated error

LIPAS - Aeolus wind simulation 1 orbit on 1/1/2007 true zonal wind (UKMO) CALIPSO CALIPSO backscatter UKMO u-wind true HLOS wind (Mie channel) true HLOS wind (Rayleigh channel) 30 18

110 mJ Aeolus BM/CM HLOS winds HLOS wind (Rayleigh) HLOS wind (Mie) 30 18 true BM CM CM more noisy but larger coverage

HLOS wind statistics; 1 month LIPAS QC: SNR too low 1000 1500 BM 110 mJ, 50 km CM 110 mJ, 85 km CM 80 mJ , 85 km CM 80 mJ, 250 km mission requirement 110  80 mJ reduced Rayleigh coverage

Hi-res radiosonde and Aeolus Radiosondes provide high-resolution vertical variability Houchi et al. (2010) studied wind and shear Extended now with cloud vertical variability (and aerosol) Radiosondes also provide T and p Zhang et al. (2010) applied to De Bilt for 2007

Hi-res radiosonde shear Tropical tropopause shear in ECMWF model strongly variable in 2006 Houchi et al. 2010 RAOB RAOB ECMWF ECMWF

Cloud layer statistics 1/3 of cloud layers are thinner than 400m Such layers cause non-uniform backscatter and extinction Mean backscatter height will be uncertain Wind and wind shear will be biased De Bilt, NL, 2007

Centre-of-Gravity (COG) w(z) is the signal strength inside the Aeolus bin as a function of altitude z COG 1. Particle-free bin Analytical calculation (no T,p dependence) Using LIPAS and (T,p) from hi-res radiosondes 2. Bins including cloud/aerosol layer Analytical Using LIPAS and (T,p, cloud, aerosol) from hi-res RAOB

Particle free bin – analytical Rayleigh height assignment error is height dependent (currently a constant correction factor of 0.47 is used in L2Bp) Typical atmosphere Stratosphere, 2 km Rayleigh bin, wind-shear 0.01 s-1 H=40 m ~ 0.4 ms-1 bias Biases exceed mission requirement in more extreme scenes (tropopause jet stream, PBL) if height assignment error is not corrected height assignment error as function of Rayleigh channel bin size 2 km 1.5 km 1 km

(T,p) from radiosonde database analytical radiosonde (T,P) mean and stddev 1 year radiosonde data over De Bilt => (T,p) => m(z) => w(z) => COG Height assignment errors are slightly larger than from analytical expressions Not very sensitive to T,p errors and predictable Use AUXMET to correct for Rayleigh channel height assignment errors in L2B optical properties code

RMSE wind error (systematic) Mie Rayleigh Rayleigh HLOS insensitive to z c can be obtained from Aeolus optics Mie H sensitive to z cloud layer z  bin Results largely confirmed for LIPAS applied to the radiosonde database

Aeolus data assimilation Single obs. Experiment Over the English channel 500 hPa analysis increment Aeolus continuous mode observation separated by 86 km Aeolus burst-mode observation separated by 200 km (< B length scale) Background error length scale ~ 400 km Courtesy: Andras Horanyi (ECMWF)

Representativeness error From ODB ECMWF T1279 0.8 m/s on ASCAT 12.5 km wind Upper troposphere: 2.1 m/s on aircraft components Along-track accumulation reduces the representativeness error Accumulation length of observations such that the resulting spectrum matches the model spectrum: (1) Upper troposphere: aircraft accumulation along 100-150 km track (2) Ocean surface: ASCAT accumulation along 85-100 km track Log variance vs wave number Aeolus representativeness error negligible for ~ 100 km along-track accumulation

1D theoretical tool Usual meteorological analysis equations Fully solved 1D = horizontal Horizontal characteristics from ECMWF and HARMONIE model and (LIPAS) Aeolus observations Introduction of bias, correlation, averaging, thinning and misspecification

Effect of accumulation distance on analysis quality Assume obs error  1/SQRT(accumulation length) Longer accumulation  more accuracy, but fewer samples Example: 60N background statistics, continous 110 mJ, 500hPa (Rayleigh channel average obs error data from LIPAS ) Obs errors assumed uncorrelated Representativeness error not included 16

Correlated representativeness error 60N background statistics, continous 80 mJ, 500hPa (Rayleigh channel average obs error data from LIPAS ), 2/3 B bandwidth Representativness error variances based on assuming global model effective resolution 7*Dx (112 km) Triangular O correlation structure with half basis of 112 km Much lower analysis quality Optimal accumulation length is now about the effective model resolution 17

Conclusions theoretical tool Latitudinal dependence From BM  CM increases impact substantially From 110 mJ  80 mJ reduces impact substantially (CM 80 mJ ~ BM 110 mJ) Aeolus impact is maximum around 250 hPa Aeolus impact is maximum in the Tropics Impact is maximized for ~85 km accumulation length

Main conclusions theoretical tool Observation error correlation up to 0.1-0.15 not very detrimental Correlation of 0.1 corresponds to an increase of random error of 0.2 m/s Correlation of 0.38 corresponds to an increase of random error of 0.7 m/s Biases > 0.5 m/s are detrimental Negative impact for biases exceeding 1 m/s Impact of non-optimal B-matrix is substantial ESA VHAMP, TN8

Summary Hi-res radiosondes are very useful for Aeolus simulation A theoretical data assimilation tool can be useful to comprehend data assimilation system characteristics