Hw. Barker et Ba. Wielicki, PARAMETERIZING GRID-AVERAGED LONGWAVE FLUXES FOR INHOMOGENEOUS MARINEBOUNDARY-LAYER CLOUDS, Journal of the atmospheric sciences, 54(24), 1997, pp. 2785-2798
This paper examines the relative impacts on grid-averaged longwave flu
x transmittance (emittance) for marine boundary layer (MEL) cloud fiel
ds arising from horizontal variability of optical depth tau and cloud
sides. First, using fields of Landsat-inferred tau and a Monte Carlo p
hoton transport algorithm, it is demonstrated that mean all-sky transm
ittances for 3D variable MBL clouds can be computed accurately by the
conventional method of linearly weighting clear and cloudy transmittan
ces by their respective sky fractions. Then, the approximations of dec
oupling cloud and radiative properties and assuming independent column
s are shown to be adequate for computation of mean flux transmittance.
Since real clouds have nonzero geometric thicknesses, cloud fractions
(A) over cap(c) presented to isotropic beams usually exceed the more
familiar vertically projected cloud fractions A(c). It is shown, howev
er, that when A(c) less than or similar to 0.9, biases for all-sky tra
nsmittance stemming from use of A(c) as opposed to (A) over cap(c) are
roughly 2-5 times smaller than, and opposite in sign to, biases due t
o neglect of horizontal variability of tau. By neglecting variable tau
, all-sky transmittances are underestimated often by more than 0.1 for
A(c) near 0.75 and this translates into relative errors that can exce
ed 40% (corresponding errors for all-sky emittance are about 20% for m
ost values of A(c)). Thus, priority should be given to development of
general circulation model (GCM) parameterizations that account for the
effects of horizontal variations in unresolved tau, effects of cloud
sides are of secondary importance. On this note, an efficient stochast
ic model for computing grid-averaged cloudy-sky flux transmittances is
furnished that assumes that distributions of tau, for regions compara
ble in size to GCM grid cells, can be described adequately by gamma di
stribution functions. While the plane-parallel, homogeneous model unde
restimates cloud transmittance by about an order of magnitude when 3D
variable cloud transmittances are less than or similar to 0.2 and by s
imilar to 20% to 100% otherwise, the stochastic model reduces these bi
ases often by more than 80%.