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Although the ozone concentration peaks in the stratosphere, the radiance contribution from the troposphere is not negligible due to the increased temperature near the earth's surface. Tropospheric radiance can be minimized by choosing a spectral region whose weighting function peaks at a maximum altitude (van Delst, 1996).
The atmospheric window baseline radiance, , must
be
separated from the measured radiance,
, in the
spectral region of interest to yield the contribution due to ozone,
,
Microwindow radiance, centered at 1080 cm, is
converted to a
brightness temperature, which represents the baseline window value.
is then calculated from the derived brightness
temperature at the ozone wavenumber; which is chosen in the 9.6
m wings, 1063 cm
, to represent upper
atmospheric emission.
Given at each time
interval in the data set
and a clear sky reference value,
, one can use
Beer's Law (neglecting cloud reflectance of surface emission) to
determine the cloud optical depth,
,
The error associated with this approach is obvious when the reference radiance is specified in layers,
such that
where and
represent ozone radiance above and below the cloud, respectively, and the
spectral dependence is implied. A further assumption requires that the
ozone emitted radiance within the cloud and atmospheric transmissivity
below the cloud are negligible.
Substitution of Equation 18 into Equation 19
produces
Therefore, knowledge of the ozone radiance below the cloud is necessary to
properly determine the optical depth using this technique. This
results in an underestimated optical depth measurement. Application of
FASCOD3P data below the cloud base is utilized to determine
. Unfortunately, a local ozone profile is not available
and a mid-latitude standard model is assumed. Nonetheless, this
provides a first order correction to the measured cloud radiance.