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Black Carbon in Snow: Treatment and Results Mark Flanner 1 Charlie Zender 2 Jim Randerson 2 Phil Rasch 1 1 NCAR 2 University of California at Irvine.

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Presentation on theme: "Black Carbon in Snow: Treatment and Results Mark Flanner 1 Charlie Zender 2 Jim Randerson 2 Phil Rasch 1 1 NCAR 2 University of California at Irvine."— Presentation transcript:

1 Black Carbon in Snow: Treatment and Results Mark Flanner 1 Charlie Zender 2 Jim Randerson 2 Phil Rasch 1 1 NCAR 2 University of California at Irvine

2 2 Motivation Hansen and Nazarenko (2004) Soot climate forcing via snow and ice albedo, PNAS.

3 3 The SNICAR Model Replaces existing snow albedo and heating representation in CLM Applies a two-stream, multi-layer radiative transfer model (Toon et al., 1989) to predict fluxes with any air/ice/aerosol mixtures.  Mie scattering solutions predicted offline for ice and aerosols  Assumes internally and externally-mixed BC Uses 5 spectral bands and vertical layers that match CLM thermal snow layers BC (2 species) deposits from atmosphere (prognostic aerosol model), influences radiation, and flushes through snow column with meltwater Prognoses effective grain size with a microphysical model, parameterized for GCM

4 4 The importance of snow aging Snow exhibits large variability in grain size  (30 < r e < 2000 μm) Snow effective grain size determines:  Pure-snow reflectance  Depth-profile of solar absorption  Magnitude of perturbation by impurities Albedo perturbation caused by a given mass of BC varies more than three-fold for a reasonable range of effective grain size. Microphysical model predicts snow specific surface area (effective radius) from diffusive vapor flux amongst grains, depending on: snow T, dT/dz, density, and initial size distribution (Flanner and Zender, 2006, JGR).

5 5 Aerosol induced snow heating: multiple positive feedbacks Snow/Ice Cover Albedo R_net (-) (+) (-) + Snow Grain Size (-) (+) +G Soot (-) (+) + (+) ? Concentration of hydrophobic and large impurities at the surface during melting? (+)

6 6 Measured and modeled BC in snow Flanner et al. (2007) Present day climate forcing and response from black carbon in snow, J. Geophys. Res.

7 7 Radiative forcing pattern of BC in snow Forcing operates mostly in local springtime, when and where there is large snow cover exposed to intense insolation, coincidentally with peak snowmelt. Hence, it is a strong trigger of snow-albedo feedback, which is maximal in spring (Hall and Qu, 2006). Forcing is dominated by FF+BF sources, but strong biomass burning events can have significant impact on Arctic

8 8 Global mean forcing and temperature response ExperimentForcing (W m -2 )∆TsEfficacy 1998:+0.054 (0.007-0.13)+0.154.5 2001:+0.049 (0.007-0.12)+0.103.3 FF+BF only:+0.043 10x 1998:+0.28+0.443.1 Hansen, et al. (2005) The efficacy of climate forcings, J. Geophys. Res.

9 9 Climate response Earlier snowmelt Reduced surface albedo Surface air warming

10 10 Driver of springtime snow cover change Case PI1: Full pre-industrial equilibrium conditions Case PI2: PI1 with 380 ppm CO 2 Case PI3: PI1 with present-day FF+BF BC+OC active in the atmosphere Case PI4: PI1 with present-day FF+BF BC active in snow Case PI5: PI1 with present-day FF+BF BC+OC active in atmosphere and snow Case PI6: PI5 with 380 ppm CO 2

11 11 Conclusions Snow microphysical model (SSA evolution) could be useful for other CHEM studies  e.g., “bromine explosion” Springtime snowpack is highly sensitive to reflectance changes Snow-albedo and microphysical feedbacks amplify initial (small) radiative forcing from BC, producing greater “efficacy” than any other forcing agent Future: Examine radiative effects of dust (Zender), OC (new, absorptive optical properties), algae (?)


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