Jm. Prusa et al., PROPAGATION AND BREAKING AT HIGH-ALTITUDES OF GRAVITY-WAVES EXCITED BY TROPOSPHERIC FORCING, Journal of the atmospheric sciences, 53(15), 1996, pp. 2186-2216
An anelastic approximation is used with a time-variable coordinate tra
nsformation to formulate a two-dimensional numerical model that descri
bes the evolution of gravity waves. The model is solved using a semi-L
agrangian method with monotone (nonoscillatory) interpolation of all a
dvected fields. The time-variable transformation is used to generate d
isturbances at the lower boundary that approximate the effect of a tra
veling line of thunderstorms (a squall line) or of flow over a broad t
opographic obstacle. The vertical propagation and breaking of the grav
ity wave field (under conditions typical of summer solstice) is illust
rated for each of these cases. It is shown that the wave field at high
altitudes is dominated by a single horizontal wavelength, which is no
t always related simply to the horizontal dimension of the source. The
morphology of wave breaking depends on the horizontal wavelength; for
sufficiently short waves, breaking involves roughly one half of the w
avelength. In common with other studies, it is found that the breaking
waves undergo ''self-acceleration,'' such that the zonal-mean intrins
ic frequency remains approximately constant in spite of large changes
in the background wind. It is also shown that many of the features obt
ained in the calculations can be understood in terms of linear wave th
eory. In particular, linear theory provides insights into the waveleng
th of the waves that break at high altitudes, the onset and evolution
of breaking, the horizontal extent of the breaking region and its posi
tion relative to the forcing, and the minimum and maximum altitudes wh
ere breaking occurs. Wave breaking ceases at the altitude where the ba
ckground dissipation rate (which in our model is a proxy for molecular
diffusion) becomes greater than the rate of dissipation due to wave b
reaking. This altitude, in effect, the model turbopause, is shown to d
epend on a relatively small number of parameters that characterize the
waves and the background state.