In the meantime, there are some informative videos available on the Web that display the characteristics of these very stable layers. Simon Christen's time-lapse movies of the evolution of capping inversions are beautiful, and very informative:
Christen's time-lapse movie The Unseen Sea
There is a nice display of crepuscular rays between 0:15 and 0:20 in this video. From 1:06 to 1:17, the clouds in the capping inversion partly evaporate as the inversion passes over a depression in the landscape a little to the right of center — and then re-condense as the air climbs back out of this hole, nearly in the middle of the images.
(Also, notice the progressive flattening of the Moon by differential refraction from 2:30 to 2:43 as it approaches the horizon.)
Similar effects of evaporation of the capping cloud as the air flows downhill are shown in the next video, especially from 1:20 to 1:26 :
Christen's time-lapse movie Adrift
Another set of time-lapse movies of extremely stable layers, seen at close range, is available at submeso.org. These, too, are extremely informative. They show the “sheet and layer” structure that is now known to be ubiquitous in the atmosphere.
The temperature gradient is steepest near the ground, because the presence of a solid surface inhibits convection. This makes inferior mirages visible over smooth surfaces. Even when the sky is overcast, enough sunlight reaches the ground to produce a shallow convective layer. Weak inferior mirages have been detected even when rain was falling.
The convection is strongest in the middle of the day, when the sun is highest in the sky, sending about a kilowatt per square meter to the surface at temperate latitudes. By the end of the afternoon, the thickness of the convectively heated region is usually a few hundred meters.
Heat is also radiated to the cold space beyond the atmosphere. This radiation is mostly at middle infrared wavelengths, between the strong carbon dioxide bands near 15 microns wavelength and the 6-micron band of water vapor. Most of the radiated heat is from the ground, because the overlying air is generally cooler than the ground. Convection ceases, and the surface (and the adjacent air) begins to cool.
Copyright © 2014, 2025 Andrew T. Young
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