In this section, the impact of aerosol vertical thickness is assessed.
This is done by simply scaling the standard profile of Figure 5.1 by factors
of 0.6, 0.8, 1.2 and 1.4 for a maximum variation of
in
number density and aerosol optical depth.
Results are presented in Figure 5.4 at 750 nm.
Decreasing the aerosol acted to decrease the radiance and increase
polarization. This is simply the result of fewer scatterers and
hence less scattering into the line of sight by the depolarizing aerosols.
Below
there was little effect due to
the large contribution of surface reflected radiation. Comparing
radiance curves representing scaling factors of 0.6 and 0.8,
there is
approximately a 20% difference for uplooking angles. This
difference drops to 6% at
and is nearly zero below
.
Also, the larger the scaling factor, the smaller the
difference between neighbouring curves; differences of about
half those quoted above were found between factors of
1.2 and 1.4.
Between neighbouring curves polarization was observed to change
by roughly 0.02 between scaling factors of 0.6 and 0.8 and less than
0.01 between scaling factors of 1.2 and 1.4. The decreasing
impact with increasing aerosol amount is a saturation-type effect
as the slant optical depths get increasing larger as does the fraction
of Mie scattering.
A similar analysis was carried out previously in which a sharply
peaked aerosol profile was used (McLinden et al., 1998).
Results similar to those above were found.