Tidal associated temperature disturbances observed at the middle atmosphere (30–65 km) by a Rayleigh lidar at 23°S

A lidar has been operated in São José dos Campos, Brazil (23.2°S, 45.8°W) since 1972, mainly dedicated to the study of mesospheric sodium at the 589 nm resonant line. The molecular Rayleigh scattering can also be used provided we limit the height to ∼75 km where the sodium scattering begins. Nevertheless, the weak signal obtained only permits the determination of density and temperature profiles by accumulating a large number of shots giving only nocturnal average profiles. Temporal variations in density and temperature on the scale of hours can however, be obtained by performing a superposed epoch analysis for a given time interval and covering a period of several days. In this way we obtained hourly mean profiles grouped by months, seasons and overall, with data acquired from 1993 to 2004. The difference between the hourly temperatures and the nocturnal means shows for some months, with enough data coverage, downward propagating structures that apparently have tidal origin. The seasonal averages show a recurrent feature with high temperatures before and low temperatures after midnight above 50 km. Some similarity is found with the GSWM model, but the observed temperature amplitudes are twice of that for the model.     

Sporadic sodium layers and the average vertical distribution of atmospheric sodium: Comparison of different Nas layer strengths

In an earlier study of sporadic sodium layers (Na_s) [Simonich, D.M., Clemesha B.R., Batista, P.P. Sporadic layers and the vertical distribution of atmospheric sodium. Adv. Space Res. 35, 1976–1980, 2005], observed by lidar at São José do Campos (23°S, 46°W) we found that, although individual profiles give the impression that Na_s layers involve sodium additional to the normal background layer, there is very little difference between the long-term averages of profiles with and without the presence of Na_s. This led us to conclude that Na_s layers result from the redistribution of an omnipresent source, rather than an additional source mechanism. We have now extended this study to investigate whether or not the relative magnitude of Na_s layers influences this conclusion. To this end we manually characterized all the profiles obtained in the time interval from 1900 to 2200 LT for the years 1993–2004. This involved registering the upper and lower limits to each Na_s layer observed, the height of the peak and the sodium concentration at each of these three points. We then computed average profiles for Na_s layers of differing strengths, with strength defined as the concentration at the peak divided by the mean of the concentrations at the upper and lower boundaries. For strengths up to 4 the results confirmed our earlier conclusion but for Na_s layer strengths greater than 4 we found a significant difference between the average profiles with and without Na_s. For the strong Na_s layers both the average abundance and the average peak sodium concentration were about 10% greater than for layers without Na_s. This leads to the possibility that a different mechanism might be responsible for very stronger sporadic layers although we do not think this very likely.