BROAD-BAND SOLAR FLUXES AND HEATING RATES FOR ATMOSPHERES WITH 3D BROKEN CLOUDS

Citation
Hw. Barker et al., BROAD-BAND SOLAR FLUXES AND HEATING RATES FOR ATMOSPHERES WITH 3D BROKEN CLOUDS, Quarterly Journal of the Royal Meteorological Society, 124(548), 1998, pp. 1245-1271
Citations number
52
Categorie Soggetti
Metereology & Atmospheric Sciences
ISSN journal
00359009
Volume
124
Issue
548
Year of publication
1998
Part
B
Pages
1245 - 1271
Database
ISI
SICI code
0035-9009(1998)124:548<1245:BSFAHR>2.0.ZU;2-X
Abstract
A 3D Monte Carlo photon transport algorithm is presented that computes broadband solar fluxes and heating rates. It treats attenuation by cl oud droplets and gases separately and can produce 3D distributions of constituent absorptances. Underlying surfaces are accounted for and di urnal-mean calculations can be achieved in the same time as typical si ngle-zenith-angle experiments. Domain-averaged fluxes and heating rate profiles are presented for two very different 3D cloud fields: (i) sc attered, shallow cumuli inferred from Landsat imagery; and (ii) toweri ng clouds simulated by a cloud-resolving model. Plane-parallel, homoge neous (PPH), independent column approximation (ICA), and clear-sky ver sions of the 3D fields were generated and used as well. For both cloud fields, total atmospheric absorptance depends very weakly on cloud ge ometry. Cloud geometry does, however, invoke major differences in surf ace absorptance and, hence, reflectance to space. At high sun, albedos for 3D clouds are less than corresponding PPH values, but are in almo st perfect agreement with ICA estimates. This indicates that simple ho rizontal variability of cloud optical depth outweighs the impact of cl oud sides. At very low sun 3D fields reflect most because of intercept ion of radiation by cloud sides, while PPH and ICA albedos come into b etter agreement. For the towering cloud field, radiative fluxes are de termined largely by clouds below 6 km, despite some clouds reaching 12 km. Heating rate profiles are also affected by cloud geometry. For mo st sun angles, PPH clouds exhibit anomalously large heating near cloud tops and anomalously small heating beneath clouds. On the other hand, profiles for 3D and ICA fields are very similar and depend much less on altitude; partly because of side illumination but also because the dense cores of inhomogeneous clouds are often radiatively-shielded (un like their PPH counterparts). Finally, regular arrays of idealized clo ud forms are used to demonstrate the potential ambiguity of using clou d radiative forcing ratios, R, as proxy measures for the impact of clo uds on atmospheric absorptance. In essence, R depends not only on how clouds influence atmospheric al,sorption, but also on how they partiti on radiation between albedo and transmittance.