Diagnosis of background errors for radiances and other observable quantities in a variational data assimilation scheme, and the explanation of a case of poor convergence

In any statistical data assimilation scheme the ratio between the observation and background errors fundamentally determines the weight given to the observations. The observation errors are specified directly in terms of the observable quantities. In variational data assimilation schemes these can include satellite-measured radiances as well as conventional observations. The background errors, on the other hand, are specified in terms of those quantities that lead to a compact formulation of the background term (the Jb of the variational analysis), viz. balanced vorticity, unbalanced temperature, divergence and surface pressure, and specific humidity. It is not obvious how the magnitudes of these background errors can be compared with the various observation errors. Within the variational analysis, the background errors are implied in terms of observed quantities, i.e. not normally computed explicitly. They depend, in general, on the Jb formulation and on the observation operators. In the case of radiance observations this involves the Jacobian of the radiative-transfer model which, in turn, depends on the atmospheric state. By applying the observation operators of a variational data assimilation scheme to a set of random vectors, drawn from a population whose probability density function is given by the assumed background-error covariance matrix, we obtain grid-point fields of background-error standard deviations for any observed quantity. These are valuable for diagnosing the response of the data assimilation system to observational data, and for tuning the specified observation and background errors in general. The calculated error standard deviations can be compared with those obtained from studies of innovation statistics (i.e. observed departures from the background). The technique has been applied to a range of observable quantities, including the radiance data from both the infrared and microwave instruments of the TIROS operational vertical sounder (TOVS). We used the results for some of the higher-peaking channels to verify that the specified background errors in the recently introduced 50-level version of the ECMWF model are also reasonable in the upper stratosphere, where there are few conventional data. We also found that the operational background errors for humidity were set unrealistically large in some dry subtropical areas. A case of poor convergence of the variational analysis was found to be due to unrealistically high background errors in terms of one of the humidity-sensitive radiance channels (the Meteosat water-vapour channel, similar to TOVS channel 12). Excessively large ratios between background and observation errors locally led to larger than normal eigenvalues of the analysis Hessian—thus increasing the condition number of the minimization problem, with an associated decrease in the rate of convergence of the minimization. The mis-specification of background errors was confined to relatively small areas in the subtropics, but it affected the minimization globally.

[1]  Jean-Noël Thépaut,et al.  Variational inversion of simulated TOVS radiances using the adjoint technique , 1990 .

[2]  C. Rodgers,et al.  Retrieval of atmospheric temperature and composition from remote measurements of thermal radiation , 1976 .

[3]  J. Mahfouf,et al.  The ecmwf operational implementation of four‐dimensional variational assimilation. III: Experimental results and diagnostics with operational configuration , 2000 .

[4]  Philippe Courtier,et al.  The ECMWF implementation of three-dimensional variational assimilation ( 3 D-Var ) . 111 : Experimental results , 2006 .

[5]  P. Courtier,et al.  A strategy for operational implementation of 4D‐Var, using an incremental approach , 1994 .

[6]  Pierre Gauthier,et al.  Chaos and quadri-dimensional data assimilation: a study based on the Lorenz model , 1992 .

[7]  John Derber,et al.  The use of TOVS level‐1b radiances in the NCEP SSI analysis system , 2000 .

[8]  John Derber,et al.  The Use of TOVS Cloud-Cleared Radiances in the NCEP SSI Analysis System , 1998 .

[9]  Philippe Courtier,et al.  Four‐Dimensional Assimilation In the Presence of Baroclinic Instability , 1992 .

[10]  M. Matricardi,et al.  An improved fast radiative transfer model for assimilation of satellite radiance observations , 1999 .

[11]  P. Courtier,et al.  The ECMWF implementation of three‐dimensional variational assimilation (3D‐Var). I: Formulation , 1998 .

[12]  Andrew C. Lorenc,et al.  Analysis methods for numerical weather prediction , 1986 .

[13]  Roger Daley,et al.  Estimating the Wind Field from Chemical Constituent Observations: Experiments with a One-Dimensional Extended Kalman Filter , 1995 .

[14]  Philippe Courtier,et al.  Use of cloud‐cleared radiances in three/four‐dimensional variational data assimilation , 1994 .

[15]  P. Courtier,et al.  The ECMWF implementation of three‐dimensional variational assimilation (3D‐Var). II: Structure functions , 1998 .

[16]  A. Hollingsworth,et al.  The statistical structure of short-range forecast errors as determined from radiosonde data Part II: The covariance of height and wind errors , 1986 .

[17]  John Derber,et al.  The National Meteorological Center's spectral-statistical interpolation analysis system , 1992 .

[18]  Claude Lemaréchal,et al.  Some numerical experiments with variable-storage quasi-Newton algorithms , 1989, Math. Program..

[19]  J. Derber,et al.  A reformulation of the background error covariance in the ECMWF global data assimilation system , 1999 .

[20]  A. Lorenc Optimal nonlinear objective analysis , 1988 .

[21]  Anthony Hollingsworth,et al.  The statistical structure of short-range forecast errors as determined from radiosonde data , 1986 .

[22]  A. Lorenc A Global Three-Dimensional Multivariate Statistical Interpolation Scheme , 1981 .