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Institute of Environmental Physics and Remote SensingIUP/IFE-UB Physics/Electrical Engineering
Department 1
Andreas.Richter@iup.physik.uni-bremen.de
Institute of Environmental Physics and
Institute of Remote Sensing
University of Bremen
Tropospheric NO2 Height Determination
Andreas Richter, A. Hilboll, and J. P. Burrows
S5P Verification MeetingBremen, November 29, 2013
Andreas.Richter@iup.physik.uni-bremen.de2
Introduction
• Satellite observations provide nice global maps of tropospheric NO2
• Absolute values depend strongly on assumed vertical distribution• This information currently comes completely from a priori dataÞ Can‘t we do better than that?
Andreas.Richter@iup.physik.uni-bremen.de3
What triggered this study?
• Monthly GOME-2 tropospheric NO2 data are missing most of the large values
• These were removed by cloud filtering as aerosol was so thick that data were classified as partially cloudy
No cloud screening
Andreas.Richter@iup.physik.uni-bremen.de4
Is it only Aerosols?
• Even without cloud screening, there are data gaps over pollution hot spots on some days
• This is due to quality checking as these fits are poor
No Chisq. screening
Andreas.Richter@iup.physik.uni-bremen.de5
Why are the fits poorer at strong pollution?
• There are large and clearly structured residuals in fits over pollution hot spots
• This is not random noise!
• Comparison to NO2 cross-sections shows that scaling of NO2 should change over fitting window
Andreas.Richter@iup.physik.uni-bremen.de6
Wavelength dependence of Air Mass Factor
• For constant albedo, AMF of NO2 layer close to the surface increases with wavelength in a Rayleigh atmosphere
• For a surface layer, this can be a significant effect• With radiative transfer modelling and a formal inversion, this should
provide information on the altitude of the NO2
About +/- 20%
Andreas.Richter@iup.physik.uni-bremen.de7
Empirical Approach
• Take standard NO2 x-section
• Scale to increase amplitude with wavelength
• Orthogonalise to leave NO2 columns unchanged
When introduced in the fit, large residuals are fixed
Andreas.Richter@iup.physik.uni-bremen.de8
Results Empirical Approach
• The empirical NO2 AMF proxy is found over the pollution hotspot in China
• It is not found at other locations where the NO2 slant column is large
• There is some noise in the retrieval of the proxy
Andreas.Richter@iup.physik.uni-bremen.de9
Results Empirical Approach: OMI
• As for GOME-2 data, the empirical NO2 AMF proxy is found over the pollution hotspot in China
• There is more noise than in GOME-2 data• Problems with row anomaly
Andreas.Richter@iup.physik.uni-bremen.de10
Is there more than China?
• Fit is improved by AMF proxy everywhere over pollution hotspots
Andreas.Richter@iup.physik.uni-bremen.de11
Comparison to NO2 columns
• Overall pattern similar to NO2 map
• Differences in distributions of maxima
• Artefacts over water• noise
Andreas.Richter@iup.physik.uni-bremen.de12
Impact of Clouds
• On many days in winter, very large NO2 slant columns are observed over Europe and the US
• The NO2 AMF proxy picks up only very few of these signals
• This is linked to the fact that most of the events are related to cloudy scenes or snow on the surface, resulting in small wavelength dependence
Andreas.Richter@iup.physik.uni-bremen.de13
Sensitivity Study
• Ratio of AMF proxy and NO2 has strong dependence on NO2 layer height
• Dependence on albedo is small between 3% and 7%
Synthetic data:• Rayleigh atmosphere• Constant albedo• NO2 layer in different altitudes• DOAS fit on spectra• NO2 temperature dependence
corrected by using 2 NO2 x-sections• AMF proxy included
• Ratio of AMF proxy / NO2 to normalise signal
Andreas.Richter@iup.physik.uni-bremen.de14
Sensitivity Study: SZA
• Effect varies with SZA; larger effect at larger SZA• At large SZA, AMF proxy also found for elevated NO2
• Dependence on albedo is small between 3% and 7%
Andreas.Richter@iup.physik.uni-bremen.de15
Sensitivity Study: Bright Surfaces
Þ multiple scattering over bright surfaces is stronger at shorter wavelengths
Þ wavelength dependence of AMF is inverted
• Increasing albedo reduces effect as expected for reduced importance of Rayleigh scattering
• For large albedo (> 50%), negative fit factors are found for AMF proxy => wavelength dependence is inverted and only weakly dependent on altitude
Andreas.Richter@iup.physik.uni-bremen.de16
Impact of Aerosols and Clouds
Shielding
• Similar effect for both, AMF proxy and NO2 => will cancel in ratio
• Ratio will give layer height for cloud free part of pixel
Light path enhancement
• Light path enhancement in clouds / aerosols depends only weakly on wavelength
• Effect on NO2 but no effect on AMF proxy
• Ratio will no longer be representative of NO2 layer height
Andreas.Richter@iup.physik.uni-bremen.de17
Case Study Highveld
• NO2 plume from Highveld power plants can be tracked onto the ocean
• NO2 SC values increase downwind of the source
• AMF Proxy also has higher values within the plume, but– Is more narrow– Has largest values at beginning of plume, not at the end of it
Andreas.Richter@iup.physik.uni-bremen.de18
What about larger wavelength difference?
• Tropospheric signal much smaller in UV fit• Ratio between two fits depends on location (=> NO2 height)
• BUT: UV fit is noisy
Andreas.Richter@iup.physik.uni-bremen.de19
Summary
• A simple empirical pseudo-cross-section was used to detect and correct the AMF wavelength dependence of tropospheric NO2 in GOME-2 data
• Application improves NO2 fits over pollution hotspots under clear sky conditions
• As expected, the signature is not found over clouds and bright surfaces or in cases of large stratospheric NO2
• The results can at least give an indication for where an AMF for BL NO2 is appropriate
• Tests on synthetic data suggest that for good signal to noise, an effective NO2 layer height can be determined
• Using more separated wavelengths and applying a formal inversion including aerosol properties might provide more vertical information
• Application to more data also from OMI and S5P foreseenFunding by DLR Bonnunder Contract 50EE1247
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