Abstract

Abstract. Atmospheric black carbon (BC) is a leading climate warming agent, yet uncertainties on the global direct radiative forcing (DRF) remain large. Here we expand a global model simulation (GEOS-Chem) of BC to include the absorption enhancement associated with BC coating and separately treat both the aging and physical properties of fossil-fuel and biomass-burning BC. In addition we develop a global simulation of brown carbon (BrC) from both secondary (aromatic) and primary (biomass burning and biofuel) sources. The global mean lifetime of BC in this simulation (4.4 days) is substantially lower compared to the AeroCom I model means (7.3 days), and as a result, this model captures both the mass concentrations measured in near-source airborne field campaigns (ARCTAS, EUCAARI) and surface sites within 30%, and in remote regions (HIPPO) within a factor of 2. We show that the new BC optical properties together with the inclusion of BrC reduces the model bias in absorption aerosol optical depth (AAOD) at multiple wavelengths by more than 50% at AERONET sites worldwide. However our improved model still underestimates AAOD by a factor of 1.4 to 2.8 regionally, with the largest underestimates in regions influenced by fire. Using the RRTMG model integrated with GEOS-Chem we estimate that the all-sky top-of-atmosphere DRF of BC is +0.13 Wm−2 (0.08 Wm−2 from anthropogenic sources and 0.05 Wm−2 from biomass burning). If we scale our model to match AERONET AAOD observations we estimate the DRF of BC is +0.21 Wm−2, with an additional +0.11 Wm−2 of warming from BrC. Uncertainties in size, optical properties, observations, and emissions suggest an overall uncertainty in BC DRF of −80%/+140%. Our estimates are at the lower end of the 0.2–1.0 Wm−2 range from previous studies, and substantially less than the +0.6 Wm−2 DRF estimated in the IPCC 5th Assessment Report. We suggest that the DRF of BC has previously been overestimated due to the overestimation of the BC lifetime (including the effect on the vertical profile) and the incorrect attribution of BrC absorption to BC.

Highlights

  • Black carbon aerosol (BC), which is produced from incomplete combustion, is an important component of atmospheric particulate matter (PM)

  • The integrated effect of mass concentration and optical properties can be described by the aerosol optical depth (AOD), single scattering albedo (SSA), absorption aerosol optical depth (AAOD) and asymmetry factor, which are the basis for calculating direct radiative forcing (DRF) in models

  • We use the Goddard Earth Observing System (GEOS)-Chem global chemical transport model integrated with online RRTMG radiation transfer model (GCRT) to investigate the mass concentrations, optical properties and radiative effect of black carbon (BC)

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Summary

Introduction

Black carbon aerosol (BC), which is produced from incomplete combustion, is an important component of atmospheric particulate matter (PM). The AR5 estimate is based on two studies: the multimodel assessment from AeroCom II (Aerosol Comparisons between Observations and Models) by Myhre et al (2013) (+0.23 Wm−2 from fossil and biofuel emissions), and the substantially higher forcing estimate of the Bond et al (2013) assessment, which incorporates an observationally weighted scaling of previous modeling estimates (+0.51 Wm−2 from fossil and biofuel emissions, +0.2 Wm−2 from biomass burning) This difference of more than a factor of 2 highlights both the uncertainty in BC DRF and the potential for a substantial underestimation of BC absorption in the current generation of global models. The integrated effect of mass concentration and optical properties can be described by the aerosol optical depth (AOD), single scattering albedo (SSA), absorption aerosol optical depth (AAOD) and asymmetry factor, which are the basis for calculating DRF in models.

The standard GC-RT model
Updated aging mechanism for BC
Updated BC properties for optical calculation
Treatment of brown carbon
Aircraft and surface concentration measurements
AERONET measurements
Comparing simulated BC mass concentrations to observations
Near-source measurements
Comparing simulated and AERONET regional AAOD
DRE and DRF in GC-RT
Uncertainties
Findings
Conclusions and implications
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