Lebsock M. D., T. S. L'Ecuyer and R. Pincus (November 2017): An Observational View of Relationships Between Moisture Aggregation, Cloud, and
Radiative Heating Profiles.
The temperature drops with height due to convective adjustment (standard atmosphere vertical temperature profile with decreasing temperature with height) and
the radiative heating profile (Fleagle and Businger 1980; Houghton 1991; Peixoto and Oort 1992; Hartmann 1994), and equals the emission temperature of 254 K at around 6.5 km above the ground (Fig.
Not exact matches
The differential
heating imposed on the troposphere + surface layer is sufficient that LW emissions from within the layer are not able to establish pure
radiative equilibrium without having the temperature
profile become unstable to convection.
There are multiple non-
radiative energy fluxes at the surface (latent and sensible
heat fluxes predominantly) which obviously affect the atmospheric temperature
profiles, but when it comes to outer paces, that flux is purely
radiative.
In the tugging on the temperature
profile (by net radiant
heating / cooling resulting from
radiative disequilibrium at single wavelengths) by the absorption (and emission) by different bands, the larger - scale aspects of the temperature
profile will tend to be shaped more by the bands with moderate amounts of absorption, while finer - scale variations will be more influenced by bands with larger optical thicknesses per unit distance (where there can be significant emission and absorption by a thinner layer).
Re my 441 — competing bands — To clarify, the absorption of each band adds to a warming effect of the surface + troposphere; given those temperatures, there are different equilibrium
profiles of the stratosphere (and different
radiative heating and cooling rates in the troposphere, etc.) for different amounts of absorption at different wavelengths; the bands with absorption «pull» on the temperature
profile toward their equilibria; disequilibrium at individual bands is balanced over the whole spectrum (with zero net LW cooling, or net LW cooling that balances convective and solar
heating).
In brief, the temperature
profile of the atmosphere is set by convection & latent -
heat considerations (= > adiabatic lapse rate); based upon that temperature
profile, the
radiative transfer processes give rise to the
radiative forcing which is the GHE.
As described, the whole temperature
profile gives rise to the
radiative transport, which gives rise to the
heating at ground level, which gradually raises the whole temperature
profile (via convection) until
radiative balance is achieved.
Turner D. D., M. D. Shupe and A. B. Zwink (April 2018): Characteristic Atmospheric
Radiative Heating Rate
Profiles in Arctic Clouds as Observed at Barrow, Alaska.