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Folkert Boersma

Folkert Boersma. Reducing errors in using tropospheric NO 2 columns observed from space. Blond et al. (2007). SCIAMACHY. EMEP. Main use of satellite observations: estimating emissions of NO x. What is so uncertain about emissions? quantities locations times trends.

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Folkert Boersma

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  1. Folkert Boersma Reducing errors in using tropospheric NO2 columns observed from space

  2. Blond et al. (2007) SCIAMACHY EMEP Main use of satellite observations: estimating emissions of NOx • What is so uncertain about emissions? • quantities • locations • times • trends But we can see the NOx sources from space chem= 4-24 hrs Emissions

  3. Satellite observations • Pros • sensitivity to lower troposphere • improving horizontal resolution • global coverage • Cons • daytime only • column only • clouds • sensitivity to forward model parameters assumptions

  4. Retrieval method

  5. Retrieval method • 3-step procedure • obtain slant column along average light path • separate stratospheric and tropospheric contributions • convert tropospheric slant column in vertical column In equation: Ns, Ns,st, Mtr are all error sources

  6. Retrieval method aerosols surface pressure

  7. ‘State-of-science’ van Noije et al., ACP, 6, 2943-2979, 2006

  8. Systematic differences van Noije et al., ACP, 6, 2943-2979, 2006

  9. Stratospheric column Accounting for zonal variability or not? 41.5°N E. J. Bucsela – NASA GSFC Model information Reference Sector

  10. Stratospheric column Without correction errors up to 11015 molec.cm-2 March 1997

  11. Stratospheric column • Alternative: limb-nadir matching • Limb observes zonal variability • Stratospheric column estimate may introduce offsets from limb-technique Courtesy of E. J. Bucsela – NASA GSFC A. Richter et al.– IUP Bremen

  12. Stratospheric column • In summary • Reference sector method questionable • Assimilation & nadir-limb correct known systematic errors • Assimilation self-consistent; uncertainty ~0.2×1015 • Validation needed • - SAOZ network (sunrise, sunset) • Brewer direct sun (Cede et al.) in unpolluted areas

  13. Air mass factor Retrieval method Tropospheric air mass factor Mtr- Computed with radiative transfer model and stored in tables Mtr = f(xa,b) xa = a priori tropospheric NO2 prf b = forward model parameters - cloud fraction - cloud pressure - surface albedo - aerosols ( - viewing geometry)

  14. Air mass factor errors A priori profile • Large range in sensitivities between 200 & 1000 hPa, especially in the BL • Low sensitivity in lower troposphere for dark surfaces • Clear pixel, albedo = 0.02 • Clear pixel, albedo = 0.15 • Cloudy pixel with fcl = 1.0, pcl = 800 hPa Eskes and Boersma, ACP, 3, 1285-1291, 2003

  15. Air mass factor errors A priori profile from CTMs • Shapes reasonably captured by CTMs • Effect of model assumptions on BL mixing lead to errors <10-15% • Models are coarse relative to latest retrievals Martin et al., JGR, 109, D24307, 2004

  16. Jun-Aug 2004 SCIAMACHY NO2 MOZART-2 AMF Air mass factor errors Effect of choice of CTM on retrieval MOZART-2 (2°2°) vs. WRF-CHEM (0.2°0.2°) A. Heckel et al. (IUP Bremen)

  17. Jun-Aug 2004 SCIAMACHY NO2 WRF-Chem AMF Air mass factor errors Effect of choice of CTM on retrieval Effect ~10% A. Heckel et al. (IUP Bremen)

  18. Air mass factor sensitivities M = wMcl+ (1-w)Mcr Cloud fraction Boersma et al., JGR, 109, D04311, 2004 Cloud pressure Albedo

  19. AMF errors – surface albedo M = M/asf asf asf = 0.02 (GOME-TOMS) (%)

  20. AMF errors – cloud fraction M = M/fcl fcl fcl = 0.05 (FRESCO) (%)

  21. AMF errors – cloud pressure M = M/pcl pcl pcl = 50.0 (FRESCO) (%)

  22. Martin et al., JGR, 108, 4537, 2003 Air mass factor errors - aerosols • If NO2 present, then also aerosol • Aerosols affect radiative transfer dep. on particle type

  23. Indirect correction through M=wMcl+(1-w)Mcr Direct correction Air mass factor errors - aerosols • Aerosols affect radiative transfer • Cloud fraction sensitive to aerosols ( = +1.0  fcl +0.01)

  24. Air mass factor errors – surface pressure • Surface pressure from CTMs (2°× 3°) • Strong differences with hi-res surface pressures GOME SCIAMACHY Schaub et al., ACPD, 2007

  25. Error top-10 • Cloud fraction errors ~30% • Surface albedo ~15% + resolution effect? • Vertical profile ~10% + resolution effect? • Aerosols ~10%? More research needed • Cloud pressure ~5% • Surface pressure depends on orography

  26. Is there a recipe for reducing all these errors? 1. Better estimates of forward model parameters A good example: surface pressures (Schaub et al.) What should be done: - a validation/improvement of surface albedo databases - a validation/improvement of cloud retrievals - investigate effects aerosols on (cloud) retrievals - validation vertical profiles - higher spatial resolution (sfc. albedo, pressure, profile)

  27. Is there a recipe for reducing all these errors? 2. How do we know if better forward model parameters improve retrievals? We need an extensive, unambiguous and well-accessible validation database Testbed for retrieval improvements: - in situ aircraft NO2 (Heland, ICARTT, INTEX) - surface columns (SAOZ, Brewer, (MAX)DOAS) - in situ profiles (Schaub/Brunner) - surface NO2 (regionally)

  28. Is there a recipe for reducing all these errors? • 3. Towards a common algorithm/reduced errors? • Difficult! • Without testbed, verification of improvements is hard • Improvements for one algorithm may deteriorate other algorithms, depending on retrieval assumptions • Improved model parameters may work for some regions and some seasons, but not for others

  29. Is there a recipe for reducing all these errors? • 3. Towards a common algorithm/reduced errors? • Worth the try! • Systematic differences can be reduced (emission estimates) • Requires ‘scientific will’ – enormous task • Collection of validation set • Flexible algorithms digesting various model parameters • Intercomparison leading to recommendations • Fits purpose ACCENT/TROPOSAT

  30. Advantage common algorithm – an example

  31. Advantage common algorithm – an example Advantage common algorithm – an example SCIAMACHY OMI Concurrent measurements of tropospheric NO2 from OMI and SCIAMACHY Folkert Boersma, Daniel Jacob, Henk Eskes, Rob Pinder, Jun Wang, and Ronald van der A Folkert Boersma

  32. OMI and SCIAMACHY NO2 • GOME and SCIAMACHY overpass at similar times (10:30 and 10:00) • OMI and SCIAMACHY overpass at different times (13:30 and 10:00) • Consistent retrieval algorithms • NO2 has a relatively short lifetime (4-24 hours) • NOx has diurnal cycle in source and loss terms • Can we observe fast photochemistry and changes in emissions from space? QUESTION:

  33. Collocated, cloud-free (rcl<50%) measurements at 0.5°0.5°

  34. Ratio SCIAMACHY:OMI over source regions

  35. Diurnal variation of NO2 columns NNO2: NO2 column (t): NO2:NOx ratio E(t): NOx emissions k(t) : rate constant NNOx: NOx column  E rate constant k(t) applies to conversion of NOx to HNO3 NO2+OH+M  HNO3+M k

  36. GEOS-Chem Relative decrease in NO2 column from 10:00 to 13:30 pm Observed GEOS-Chem US: -16% -28% EU: -6% -13% China: -26% -22%

  37. 2003 2005 Biomass burning mainly in afternoon 2001 2002 2004 Relative increase in NO2 column from 10am to 1:30 pm Jun Wang Observed GEOS-Chem Africa: +48% +16% Indon.: +60% +10% Brazil: +54% +13%

  38. tm4no2a-omi, v0.9.3.4

  39. tm4no2a-omi, v0.9.3.4

  40. tm4no2a-omi, v0.9.3.4

  41. Lambert-Beer in space: Retrieval method Now you can think of the Lambert-Beer law: • Well controlled environment • Observe direct beam • Light path well defined • Attenuation measure for absorption yobs= ylamp· e-  =  · l • Poorly controlled environment • Observe scattered radiation • Light path complex – air mass factor needed • Attenuation measure for absorption and scattering • Satellite observes both yobsand ylamp • Retrieved: slant column

  42. Retrieval method • What is the air mass factor (AMF)? • represents the relative length of the light path, • converts the slant into a vertical column • M = Ns/Nv • Computed with radiative transfer model • AMF depends on a priori knowledge of atmospheric state • Cloud fraction • Cloud height • Vertical distribution NO2 • Surface albedo

  43. Air mass factor errors A priori profile from CTMs • Profile shape error affects air-mass factor • few NO2 profile shape measurements • simple approach: • Temporal variability in TM3 is a measure for shape error • Different mixing schemes

  44. Air mass factor errors

  45. Saturday Sunday

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