Global three-dimensional modeling of the water vapor concentration of the mesosphere-mesopause region and implications with respect to the noctilucent cloud region
U. Korner et Gr. Sonnemann, Global three-dimensional modeling of the water vapor concentration of the mesosphere-mesopause region and implications with respect to the noctilucent cloud region, J GEO RES-A, 106(D9), 2001, pp. 9639-9651
A global three-dimensional model of the dynamics (0-150 km) and chemistry (
30-150 km) of the middle atmosphere has been developed and applied to the p
roblem of the water vapor distribution of the mesosphere-mesopause region.
The mesopause region is one of the most intricate domains of the atmosphere
and requires an extraordinarily careful modeling. In order to interpret th
e specific feature of the water vapor distribution, particular attention wa
s paid to the problem of the effective characteristic chemical time and the
comparison of this time with the characteristic transport time. The result
s confirm measurements which show highest concentrations during the summer
months and lowest concentrations in the winter in the middle and high latit
udes of the mesosphere because of the seasonal variation of the vertical wi
nd system and change in the altitudes of levels of constant pressure as a r
esult of a mean cooling or warming below the respective heights. The equato
r region is marked by a semiannual variation with maxima around the equinox
es. By way of contrast, the Halogen Occultation Experiment (HALOE) measurem
ents show maxima around solstices, however, with some exceptions for which
a maximum also occurs during the equinox. This points to a dynamically sens
itive equatorial region. At high latitudes the extremely low temperatures w
ithin the mesopause region in summer and the relatively high water vapor co
ncentrations cause a supersaturation of water vapor which is the condition
for the formation of noctilucent clouds (NLCs). The calculated seasonal and
latitudinal border of the domain of supersaturation corresponds quite well
with the mean areas of the occurrence of NLCs, however, it is impossible t
o model specific events on the basis of such a coarse model as the occurren
ce of NLCs at middle latitudes. There is no direct hemispheric transport fr
om the summer to the winter hemisphere within the mesosphere-lower thermosp
here, but the meridional transport occurs in a more complicated manner.