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Ramanathan, V.1
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0040723262
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The radiation scheme used combines the delta-Eddington method with an exponential-sum fitting technique to handle multiple-scattering and molecular absorption (12). The parameterization has been developed and calibrated with high spectral resolution line-by-line adding-doubling solutions of Ramaswamy and Freidenreich [J. Geophys. Res. 103, 23255 (1998)]. [See also S. M. Freidenreich and V. Ramaswamy, Ninth Conference on Atmospheric Radiation, Long Beach, CA, American Meteorological Society, February 1997, pp. 129-130; S. M. Freidenreich and V. Ramaswamy, in preparation.]
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Long Beach, CA, American Meteorological Society, February
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The radiation scheme used combines the delta-Eddington method with an exponential-sum fitting technique to handle multiple-scattering and molecular absorption (12). The parameterization has been developed and calibrated with high spectral resolution line-by-line adding-doubling solutions of Ramaswamy and Freidenreich [J. Geophys. Res. 103, 23255 (1998)]. [See also S. M. Freidenreich and V. Ramaswamy, Ninth Conference on Atmospheric Radiation, Long Beach, CA, American Meteorological Society, February 1997, pp. 129-130; S. M. Freidenreich and V. Ramaswamy, in preparation.]
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Freidenreich, S.M.1
Ramaswamy, V.2
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19
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84920312695
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in preparation
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The radiation scheme used combines the delta-Eddington method with an exponential-sum fitting technique to handle multiple-scattering and molecular absorption (12). The parameterization has been developed and calibrated with high spectral resolution line-by-line adding-doubling solutions of Ramaswamy and Freidenreich [J. Geophys. Res. 103, 23255 (1998)]. [See also S. M. Freidenreich and V. Ramaswamy, Ninth Conference on Atmospheric Radiation, Long Beach, CA, American Meteorological Society, February 1997, pp. 129-130; S. M. Freidenreich and V. Ramaswamy, in preparation.]
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Freidenreich, S.M.1
Ramaswamy, V.2
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21
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84920312693
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note
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The methodology of using the Geophysical Fluid Dynamics Laboratory (GFDL) Climate GCM for the particular set of experiments is similar to (72). The aerosol radiative effects do not feedback onto the GCM's dynamics. A single year is sufficient to accurately describe the annual clear-sky irradiances from the GCM because the sensitivity of the TOA irradiance to changes in meteorology (mainly water vapor concentrations) is small, and the prescribed ocean surface reflectance in the GCM does not have any interannual variation.
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24
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0001093785
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3) to the local surface wind speed (m/s).
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Tellus
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Lovett, R.F.1
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32
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84920312691
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note
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2/g and an asymmetry factor of 0.78 at 0.55 μm for the present calculations. Note that the value of the specific extinction is substantially greater than the one obtained by considering supermicrometer particles only (18).
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33
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84920312690
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note
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2 or less (11). Bias estimates for zonal and global means are likely to be even smaller than for the regional means.
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34
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0039537772
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S. Cusack, A. Slingo, J. M. Edwards, M. Wild, Q. J. R. Meterol. Soc. 124, 2181 (1998); J. T. Kiehl, J. J. Hack, J. W. Hurrell, J. Climatol. 11, 1151 (1998).
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Q. J. R. Meterol. Soc.
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S. Cusack, A. Slingo, J. M. Edwards, M. Wild, Q. J. R. Meterol. Soc. 124, 2181 (1998); J. T. Kiehl, J. J. Hack, J. W. Hurrell, J. Climatol. 11, 1151 (1998).
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Kiehl, J.T.1
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Hurrell, J.W.3
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84920312689
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note
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As an indication of the sensitivity to uncertainties in water vapor, additional calculations for July 1988, with European Center for Medium Range Weather Forecasts (ECMWF) assimilated analyses of water vapor in place of the GCM water vapor fields, revealed differences of less than 20% from the biases shown in Fig. 1A.
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84920312688
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note
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Offline calculations performed with daily-mean rather than monthly-mean wind speeds yielded sea-salt concentrations that differ by ∼ 15% on average. This difference is much smaller than the uncertainty in the mass-loading versus wind speed relation (19).
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39
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0032485371
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2 to sulfate. The connection between sea-salt and sulfur cycles is also discussed by H. Sievering et al. [ibid. 360, 571 (1992)] and N. A. Clegg and R. Toumi [J. Geophys. Res. 103, 31095 (1998)]. Thus, for particles in the radiatively important size regime, the radiative contributions of sea-salt and sulfur may be linked. P. Quinn et al. [ibid., p. 16547] point out that sea-salt controls the aerosol optical properties in the southern ocean in both the sub-and supermicrometer modes.
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Nature
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Murphy, D.M.1
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0027063609
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2 to sulfate. The connection between sea-salt and sulfur cycles is also discussed by H. Sievering et al. [ibid. 360, 571 (1992)] and N. A. Clegg and R. Toumi [J. Geophys. Res. 103, 31095 (1998)]. Thus, for particles in the radiatively important size regime, the radiative contributions of sea-salt and sulfur may be linked. P. Quinn et al. [ibid., p. 16547] point out that sea-salt controls the aerosol optical properties in the southern ocean in both the sub-and supermicrometer modes.
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(1992)
Nature
, vol.360
, pp. 571
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Sievering, H.1
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41
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0032553916
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2 to sulfate. The connection between sea-salt and sulfur cycles is also discussed by H. Sievering et al. [ibid. 360, 571 (1992)] and N. A. Clegg and R. Toumi [J. Geophys. Res. 103, 31095 (1998)]. Thus, for particles in the radiatively important size regime, the radiative contributions of sea-salt and sulfur may be linked. P. Quinn et al. [ibid., p. 16547] point out that sea-salt controls the aerosol optical properties in the southern ocean in both the sub-and supermicrometer modes.
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J. Geophys. Res.
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Clegg, N.A.1
Toumi, R.2
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42
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0032485371
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2 to sulfate. The connection between sea-salt and sulfur cycles is also discussed by H. Sievering et al. [ibid. 360, 571 (1992)] and N. A. Clegg and R. Toumi [J. Geophys. Res. 103, 31095 (1998)]. Thus, for particles in the radiatively important size regime, the radiative contributions of sea-salt and sulfur may be linked. P. Quinn et al. [ibid., p. 16547] point out that sea-salt controls the aerosol optical properties in the southern ocean in both the sub-and supermicrometer modes.
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J. Geophys. Res.
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Quinn, P.1
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44
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84920317607
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The radiative effects of wind speed upon the sea-surface reflectance can be accounted for by including both a parameterization for the Fresnel effect [J. E. Hansen et al., Mon. Weather Rev. 4, 609 (1983)] and the effects of whitecaps [
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45
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0000427210
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E. C. Monahan, J. Phys. Oceanogr. 1, 139 (1971)]. Calculations performed with the assumption that the whitecaps are diffuse reflectors with an albedo of 0.6 suggest that the global surface reflectance is likely to decrease rather than increase as a function of wind speed; this cannot, therefore, explain the bias between model and observed reflected irradiances at the TOA seen in Fig. 1A.
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J. Phys. Oceanogr.
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Monahan, E.C.1
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84920312686
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note
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We thank P. Kasibhatla and J. Langner for providing the sulfate climatologies, W. Cooke for providing the black carbon climatologies, I. Tegen for providing the dust climatologies, the NASA/Langley Distributed Active Archive Center (DAAC) for providing the ERBE data, the NASA/Jet Propulsion Laboratory DAAC for providing the SSMI data, and A. Broccoli, D. Schwarzkopf, R. Stouffer, and two anonymous reviewers for their comments and suggestions.
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