Direct aerosol forcing: Calculation from observables and sensitivities to inputs

Hong Guan, J. A. Ogren, Ernie R. Lewis, Allison McComiskey, Stephen E. Schwartz, B. Schmid, P. Ricchiazzi
2008-05-06

SCID:  54.1/yf7x4nu5
Understanding sources of uncertainty in aerosol direct radiative forcing (DRF), the difference in a given radiative flux component with and without aerosol, is essential to quantifying changes in Earth's radiation budget. We examine the uncertainty in DRF owing to measurement uncertainty in the quantities on which it depends: aerosol optical depth, single scattering albedo, asymmetry parameter, solar geometry, and surface albedo. Direct radiative forcing at the top of the atmosphere and at the surface is calculated at three locations representing distinct aerosol types and radiative environments. Sensitivities, the changes in DRF in response to unit changes in individual aerosol or surface properties, are also calculated for these conditions. The uncertainty in DRF associated with a given property is computed as the product of the sensitivity and typical measurement uncertainty in the respective property. Sensitivity and uncertainty values permit estimation of total uncertainty in calculated DRF and identification of properties that most limit accuracy in estimating forcing. Absolute total uncertainties in modeled local diurnally averaged forcing range from 0.2 to 3.1 W m −2 for the ranges of properties examined here. Relative total uncertainties range from ∼20 to 80% with larger values at higher latitudes, where fluxes are low. The largest contributor to total uncertainty in DRF is single scattering albedo; however, decreasing measurement uncertainties for any property would increase accuracy in DRF. Comparison of two radiative transfer models suggests the contribution of modeling error is small compared to the total uncertainty although comparable to uncertainty arising from some individual properties.
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2008-05-06
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Hong Guan
J. A. Ogren
Ernie R. Lewis
Allison McComiskey
Stephen E. Schwartz
B. Schmid
P. Ricchiazzi
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