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New Insights into Aerosol Asymmetry Parameter

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Single-scattering albedo (SSA) and backscatter fraction (BFR) co-vary, so that ... The box-whisker plot represents the frequency distribution of asymmetry ... – PowerPoint PPT presentation

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Title: New Insights into Aerosol Asymmetry Parameter


1
New Insights into Aerosol Asymmetry Parameter
  • John Ogren, Betsy Andrews, Anne Jefferson,
    Allison McComiskey, Pat SheridanNOAA/ESRL,
    Boulder, CO

http//www.cmdl.noaa.gov/aero/
2
Absorption and Angular Scattering Are Both
Important to Variability of RFE
Single-scattering albedo (SSA) and backscatter
fraction (BFR) co-vary, so that total variability
is less than what would be expected from
individual variabilities.
SGP daily averages, 1996-2005
3
The Asymmetry Parameter g
  • Defined as the cosine weighted integral of the
    phase function, alternatively, the average cosine
    of the scattering angle
  • Phase function P(T) is the probability of
    radiation being scattered in a given direction
  • Values can range from -1 (180-degree backwards
    scattering) to 1 (0-degree forward scattering),
    with a value of 0.7 commonly used in radiative
    transfer models.
  • Single value that describes the angular
    scattering properties of aerosols,
    computationally efficient for radiative transfer
    modeling
  • Controlled by particle size, shape, and
    refractive index
  • No method exists for direct measurement
  • Polar nephelometers, which measure P(T), lack
    sensitivity
  • Indirect methods are used to derive g

4
Schemes for Deriving
Aerosol size distribution Chemistry (Refractive
Index)
  • Limitations/Assumptions
  • Spherical particles

Mie theory
Inversion (e.g, King et al ., 1978)
Asymmetry Parameter
Spectral Aerosol Optical Depth Chemistry
(Refractive Index)
Inversion (e.g, Fiebig and Ogren, 2006)
Wiscombe and Grams, (1976) relationship
Spectral light scattering (total, back) Light
absorption Size cut information
Back-scattering fraction
5
Comparison of Schemes
  • Results from ARM 2003 Aerosol IOP
  • A 10 change in g leads to a 19 percent change
    in TOA forcing
  • Source Andrews et al., JGR, 2006.

6
Estimation from Backscatter Fraction
Assumption of Henyey-Greenstein phase function
gives a reasonable first estimate of g, but with
systematic differences compared to Fiebig
retrieval
7
Climatology at ARM Sites
asymmetry parameter
Daily averages for 2001-2004 at 450, 550, and 700
nm wavelengthSource Fiebig and Ogren, J.
Geophys. Res., 2006, submitted.
8
Climatology of g for Marine Aerosols
  • RH CMDL Data lt40 AERONET Data at ambient RH
  • Asymmetry parameter from literature and CMDL
    estimated from empirical relationship to bfr
  • ?532-550 nm from literature ?550 nm for CMDL
    Data ?550 nm for AERONET Data

9
RH-dependence at SGP
10
Vertical Profiles over SGP
Values from five years of flights with IAP
airplane, for Dp lt 1 ?m.
11
Effect of Cloud Scavenging
Cloud scavenging preferentially removes larger
particles, leaving behind particles with
systematically lower values of g in interstitial
air
12
Sensitivity of Forcing to Asymmetry Parameter
Deficit of diurnally-averaged downwelling solar
irradiance relative to value for g0.7 at SGP.
Dashed curves indicate values calculated using
observed wavelength dependence of asymmetry
parameter. The box-whisker plot represents the
frequency distribution of asymmetry parameter
(550 nm) at SGP from in-situ measurements.
13
Summary and Conclusions
  • There is no method for direct measurement of
    asymmetry parameter
  • There are several approaches to deriving
    asymmetry parameter from measurements of aerosols
    and radiation
  • Different measurement approaches yield systematic
    differences in values and climatologies
  • There is a large range in asymmetry parameter
  • Natural atmospheric variability (size
    distribution)
  • Measurement error
  • Aerosol radiative forcing is sensitive to the
    variability of g
  • Process-level research is needed to reconcile the
    differences among the various approaches for
    determining asymmetry parameter
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