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Chemical Source Inversion Using Assimilated Constituent Observations. Andrew Tangborn Global Modeling and Assimilation Office. How are data assimilation and chemical source inversion related?. 1. Underdetermined systems – fewer constraints than unknowns.
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Chemical Source Inversion Using Assimilated Constituent Observations Andrew Tangborn Global Modeling and Assimilation Office
How are data assimilation and chemical source inversion related? 1. Underdetermined systems – fewer constraints than unknowns. 2. Use Bayesian methods – require error statistics. 3. If errors are normally distributed and unbiased – optimal scheme results in weighted least squares estimate.
How are they different? 1. Different goals: state estimate vs. source estimate. 2. Use different errors: source errors vs. model and State errors.
Example: Kalman Filtering (KF) and Green’s function (GF) Inversion Inputs chemical tracer observations winds chemical source/sinks Initial state Error estimates
Algorithms KF: Kalman gain observation operator ca = cf + K(co – Hcf) observations analysis forecast
KF: Where K = PfHT (R+HPfHT)-1 is a weighted by obs error (R) and forecast error (HPfHT) covariances. The forecast error covariance Pf = MPaMT + Q is evolved in time from analysis error using the discretized model (winds) M and added model error Q
GF: Green’s function Inverse of source error cov. xinv = (GTXG+W)-1 (GTXco+Wz) Inverse of R obs first guess source inverted source G: calculated by running model forward using unit sources at each grid point.
Differences between KF and GF KF: Initial condition (analysis) used in forecast contains earlier observation information. GF: Initial condition does not explicitly contain observation data. KF: Uses model (wind) and observation errors. State errors are propagated in time. GF: Uses source and observation errors. State errors are never calculated.
Combing KF and GF • Carry out KF assimilation of tracer observations. • Use both the analysis and analysis error covariance as the observations and observation error in the GF co = ca X = (Pa)-1 • Now X contains information on model errors (including wind errors) and co is spread to all grid points through assimilation.
Numerical Experimentsadvection diffusion in 2p x 2p domainwith constant and random source errors Model source True Source
Tracer Fields True field Model solution Analysis field
Source InversionError Standard Deviation No Assimilation With assimilation
Conclusions • Data Assimilation can add information to source inversion. • Improvements likely come through improved and more complete error covariance information and spreading observation information to more grid points.