2013
DOI: 10.5194/gmdd-6-4531-2013
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Atmospheric inverse modeling with known physical bounds: an example from trace gas emissions

Abstract: Many inverse problems in the atmospheric sciences involve parameters with known physical constraints. Examples include non-negativity (e.g., emissions of some urban air pollutants) or upward limits implied by reaction or solubility constants. However, probabilistic inverse modeling approaches based on Gaussian assumptions cannot incorporate such bounds and thus often produce unrealistic results. The atmospheric literature lacks consensus on the best means to overcome this problem, and existing atmospheric stud… Show more

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Cited by 2 publications
(3 citation statements)
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References 52 publications
(11 reference statements)
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“…Previous inversion studies have used a range of strategies to prevent unrealistic negative fluxes, including lognormal data transformations, Lagrange multipliers, and Markov chain Monte Carlo methods (Ganesan et al, ; Miller et al, ). We experimented here with a nonnegativity enforcement algorithm that started with the standard posterior solution but then iteratively corrected the whole field for negative fluxes using Lagrange multipliers and the bounded, limited‐memory Broyden‐Fletcher‐Goldfarb‐Shanno approach (Byrd et al, ).…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…Previous inversion studies have used a range of strategies to prevent unrealistic negative fluxes, including lognormal data transformations, Lagrange multipliers, and Markov chain Monte Carlo methods (Ganesan et al, ; Miller et al, ). We experimented here with a nonnegativity enforcement algorithm that started with the standard posterior solution but then iteratively corrected the whole field for negative fluxes using Lagrange multipliers and the bounded, limited‐memory Broyden‐Fletcher‐Goldfarb‐Shanno approach (Byrd et al, ).…”
Section: Discussionmentioning
confidence: 99%
“…We experimented here with a nonnegativity enforcement algorithm that started with the standard posterior solution but then iteratively corrected the whole field for negative fluxes using Lagrange multipliers and the bounded, limited‐memory Broyden‐Fletcher‐Goldfarb‐Shanno approach (Byrd et al, ). In principle, the iterative solution should have conserved mass, with any removal of negative fluxes accompanied by weaker positive fluxes elsewhere (Miller et al, ). In practice, the nonnegativity algorithm was very slow to converge and led to an overall net increase in N 2 O emissions of about 0.3–0.4 Tg N/yr over the CT‐L domain.…”
Section: Discussionmentioning
confidence: 99%
“…Following Jeong et al (), we use the Just Another Gibbs Sampler system (Plummer, ) and the R statistical language (https://cran.r-project.org/) to build Markov chain Monte Carlo (MCMC) samplers for the posterior distribution in equation . The individual probability distributions in equation are described in supporting information Text S1 and convergence and accuracy of MCMC samples (50,000 samples for each parameter) are described in Text S3 (Gelman et al, ; Gelman & Hill, ; Gelman & Rubin, ; Kass et al, ; Korner‐Nievergelt et al, ; Kruschke, ; Michalak, ; Miller et al, ; Rasmussen & Williams, ).…”
Section: Methodsmentioning
confidence: 99%