4.7 Article

Radiative forcing of the direct aerosol effect from AeroCom Phase II simulations

Journal

ATMOSPHERIC CHEMISTRY AND PHYSICS
Volume 13, Issue 4, Pages 1853-1877

Publisher

COPERNICUS GESELLSCHAFT MBH
DOI: 10.5194/acp-13-1853-2013

Keywords

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Funding

  1. US Department of Energy, Office of Science, Scientific Discovery through Advanced Computing (SciDAC) Program
  2. Office of Science Earth System Modeling Program
  3. National Science Foundation
  4. DOE by Battelle Memorial Institute [DE-AC06- 76RLO 1830]
  5. FP6 project EUCAARI [34684]
  6. Research Council of Norway through the EarthClim project [207711/E10]
  7. Research Council of Norway through the NOTUR/NorStore project
  8. Norwegian Space Centre through PM-VRAE
  9. EU project PEGASOS
  10. EU project ACCESS
  11. National Basic Research Program of China [2011CB403405]
  12. US NSF [AGS-0942106]
  13. NASA [NNX11AQ72G]
  14. NASA-MAP [NNX09AK32G]
  15. Joint DECC/Defra Met Office Hadley Centre Climate Programme [GA01101]
  16. Research Council of Norway through the SLAC project
  17. EU-project ECLIPSE
  18. Natural Environment Research Council [NE/G006148/1] Funding Source: researchfish
  19. Directorate For Geosciences [0946739] Funding Source: National Science Foundation
  20. Div Atmospheric & Geospace Sciences [0942106] Funding Source: National Science Foundation
  21. NERC [NE/G006148/1] Funding Source: UKRI

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We report on the AeroCom Phase II direct aerosol effect (DAE) experiment where 16 detailed global aerosol models have been used to simulate the changes in the aerosol distribution over the industrial era. All 16 models have estimated the radiative forcing (RF) of the anthropogenic DAE, and have taken into account anthropogenic sulphate, black carbon (BC) and organic aerosols (OA) from fossil fuel, biofuel, and biomass burning emissions. In addition several models have simulated the DAE of anthropogenic nitrate and anthropogenic influenced secondary organic aerosols (SOA). The model simulated all-sky RF of the DAE from total anthropogenic aerosols has a range from -0.58 to -0.02 Wm(-2), with a mean of -0.27 Wm(-2) for the 16 models. Several models did not include nitrate or SOA and modifying the estimate by accounting for this with information from the other AeroCom models reduces the range and slightly strengthens the mean. Modifying the model estimates for missing aerosol components and for the time period 1750 to 2010 results in a mean RF for the DAE of -0.35 Wm(-2). Compared to AeroCom Phase I (Schulz et al., 2006) we find very similar spreads in both total DAE and aerosol component RF. However, the RF of the total DAE is stronger negative and RF from BC from fossil fuel and biofuel emissions are stronger positive in the present study than in the previous AeroCom study. We find a tendency for models having a strong (positive) BC RF to also have strong (negative) sulphate or OA RF. This relationship leads to smaller uncertainty in the total RF of the DAE compared to the RF of the sum of the individual aerosol components. The spread in results for the individual aerosol components is substantial, and can be divided into diversities in burden, mass extinction coefficient (MEC), and normalized RF with respect to AOD. We find that these three factors give similar contributions to the spread in results.

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