SA001-0013
Sixteen years (2002-2018) of SABER measurements and the MSIS model were used to study the average SAO (semi-annual oscillation) and AO (annual oscillation) variations of kzz (eddy diffusion coefficient) in the mesosphere (80-96 km).
Sixteen years (2002-2018) of SABER measurements and the MSIS model were used to study the average SAO (semi-annual oscillation) and AO (annual oscillation) variations of kzz (eddy diffusion coefficient) in the mesosphere (80-96 km).
Monday, 7 December 2020
Poster
Abstract:
The climatology of atomic oxygen in the MLT (mesosphere and lower thermosphere) is balanced by O production via photodissociation of O2 in the lower thermosphere and recombination in the upper mesosphere. This work serves to establish a climatology of eddy diffusion and eddy diffusive velocity, including its intra-annual variations in the MLT based on the climatology of the region as a function of latitude and altitude. Atomic oxygen kzz velocity profiles and fluxes (80-96 km) are balanced by the continuity of chemical loss, a method originally developed in the 1960’s, was refined in 2019, in order to determine global mean kzz profiles. In the current study, the intra-annual cycle was divided into twenty six (two-week periods) for each of three zones, the northern hemisphere (NH, 15 to 55o), southern hemisphere (SH, -15 to -55o), and the equatorial region (EQ, 15 to -15o). Sixteen years of TIMED SABER O density measurements (2002-2018) and the most recent MSIS model N2, O2, H, and temperature profiles were used to calculate the chemical loss rates and determine the eddy diffusive velocities and fluxes of atomic oxygen. Our primary findings include a dominant SAO (semiannual oscillation) at all altitudes between 80-96 km at the equator, and a dominant AO (annual oscillation) below 87 km in the NH and SH, with a factor of 3-4 kzz increase from winter to summer at 83 km. Although kzz variability in the NH and SH is minimal at 96 km, an important height for thermospheric and ionospheric global circulation models, the O density increases by a factor of 1.5 between winter and summer.