“…The most important heating and cooling processes in the upper atmosphere of Earth are summarized as follows (e.g., Izakov 1971;Blum et al, 1972;Dickinson, 1972Dickinson, , 1984Dickinson et al, 1974;Chandra and Sinha, 1974;Gridchin et al, 1975;Gordiets et al, 1978Gordiets et al, , 1982Kulikov, 1981, 1985;Dickinson et al, 1987;Crowley, 1991;Bauer and Lammer, 2004): heating due to N 2 , O 2 , and O photoionization by solar (or stellar) XUV ( Յ102.7 nm), heating due to O 2 and O 3 photodissociation by solar ultraviolet radiation, chemical heating in exothermic reactions with O and O 3 , neutral gas heat conduction, IR cooling in the vibrational-rotational bands of CO 2 , NO, O 3 , OH, NO ϩ , 14 N 15 N, CO, O 2 , etc., and heating and cooling due to contraction and expansion of the thermosphere (to model the thermosphere diurnal variations), as well as turbulent energy dissipation and heat conduction. Gordiets et al (1982) applied a numerical model to calculate the thermal budget of the Earth's upper atmosphere in the altitude range of 90-500 km by including the main energy sources and sinks, such as IR radiative cooling in the vibrational-rotational bands of NO, CO 2 , OH, and O 3 , as well as heating and cooling arising from dissipation of turbulent energy and eddy heat transport.…”