Migrating tides, Migrating tide in CRISTA-1 data,
Nonmigrating tides,
References
Migrating solar
tides persist throughout
the middle atmosphere and become one of the
most striking features in the upper mesosphere
and lower thermosphere (MLT). They are global-scale
waves with periods that are subharmonics
of a solar day and propagate westward with
the apparent motion of the sun. Some basic
features of the diurnal and semidiurnal tidal
components can be described by classical
tidal theory [e.g. Chapman and Lindzen,
1970] but for a more quantitative understanding
a realistic background atmosphere as well
as an appropriate parameterization of tidal
forcing and dissipation have to be taken
into account.
The amount of data available for tidal analysis
on a global scale has significantly increased
in the past few years. This motivated the
development of numerical models which include
realistic background wind and temperature
fields in combination with improved tidal
forcing and dissipation. In particular, ground-based
wind and temperature measurements have been
used to develop tidal climatologies and to
establish the spatial and temporal characteristics
of the tides [e.g. Chang and Avery,
1997; Fritts and Isler, 1994; Gille et al., 1991; Manson et al., 1989; Vincent et al., 1989].
The first global measurement of atmospheric
tides was obtained by using temperature data
from the Limb Infrared Monitor of the Stratosphere
instrument (LIMS) on the Nimbus 7 satellite.
Hitchman and Leovy [1985] showed
that basic tidal signatures
deduced from the day/night temperature differences
are consistent with model predictions [Forbes,
1982] of the first symmetric propagating
mode of the diurnal tide. Wind observations
from the High Resolution Doppler Imager (HRDI)
[Hays et al., 1993] and the Wind Imaging
Interferometer
(WINDII) [Shepherd et al., 1993] on
the Upper Atmosphere Research
Satellite (UARS) were used to study the seasonal
dependence of the diurnal and semidiurnal
tide [Burrage et al., 1995a, b; McLandress et al., 1996] and the
interannual variability [Burrage et al.,
1995a]. Temperature measurements from the
Improved Stratospheric and Mesospheric Sounder
(ISAMS) on UARS confirmed the LIMS results
[Dudhia et al., 1993]. In contrast, Wu et al. [1998] reported on trapped modes in
the
equatorial diurnal tide evident in temperature
data from the Microwave Limb Sounder (MLS,
[Barath et al., 1993]) on UARS. The
UARS data have been
primarily used to improve the tidal forcing
and dissipation, and the background temperature
and wind fields used in earlier modeling
work [e.g. Forbes, 1984; Vial, 1989]. Khattatov
et al. [1997] derived tidal dissipation from HRDI
measurements using a linear model. Geller et
al. [1997] showed that dissipation in the MLT
region is a major controlling factor in the
annual variation of the diurnal tide. They
replaced the tidal dissipation in the global-scale
wave model (GSWM-95, [Hagan et al.,
1995]) with the Khattatov values and achieved
better agreement between the resultant calculation
and the HRDI measurements. Yudin et al.
[1998] used the tuned mechanistic tidal
model (TMTM) to evaluate tidal dissipation
and background zonal winds from UARS wind
data and demonstrated the consistency of
the tides observed in HRDI/WINDII temperature,
airglow, and wind data. Ward [1999b]
demonstrated that vertical advection
associated with the migrating diurnal tide
is the prime process causing local time variations
in the airglow observations performed by
WINDII and HRDI.
An alternate approach to determine self-consistent
amplitudes and phases of the diurnal tide
uses a tuned version of the recently revised
global-scale wave model (GSWM-98, [Hagan et al.,
1999a]) which includes tidal heating and
dissipation schemes for November conditions.
The model background atmosphere is updated
using measurements of temperature, pressure,
mass density, ozone, and geostrophic wind
from the CRISTA experiment [Offermann et al.,
1999] that was part of the US Space Shuttle
mission STS-66. The high spatial resolution
and the large vertical coverage of the CRISTA
data provide a special opportunity to examine
tidal signatures throughout the middle atmosphere.
Although the local solar time coverage during
the 7 days of measurements (Nov. 5-11, 1994)
is too short for spectral analysis, tidal
signatures can be estimated on a daily base
by calculating the temperature differences
between the zonal mean data from the ascending
and descending portions of the orbits from
20 - 90 km altitude and from 52°S - 62°N.
The ascending/descending temperature differences
show a striking pattern of alternating positive
and negative differences persisting throughout
the mission. Ward et al. [1999a]
showed that this feature is tidal
in nature and consistent with the first symmetric
propagating mode of the diurnal tide. These
authors compared the CRISTA data to the GSWM-95
predictions for equinox conditions and found
good qualitative agreement but also quantitative
differences in the equatorial amplitude and
phase distributions. By comparing CRISTA
measurements and GSWM-95 predictions in terms
of equivalent vertical displacement, they
attribute the deviations to the climatological
temperature and wind fields assumed in the
GSWM-95 calculations. The following results
quantify this sensitivity of model/observation
intercomparisons to realistic atmospheric
background conditions. The examination of
any remaining differences may provide further
insight into tidal dissipation and/or coupling
with other waves. The complete paper by Oberheide
et al. [2000] can be found here.
| The migrating diurnal tide at 7.5oN
as measured by the CRISTA-1 instrument during 9 November 1994. The animation
(1.2 MB) shows the temperature perturbation as function of local time
and was computed by using the measured tidal amplitude and phase.
Please note that the downward phase progression corresponds to upward
energy propagation. The dashed lines indicate exponential amplitude
growth. Wave breaking/dissipation ocurrs above the mesopause. |
|
|
GSWM ascending/descending orbit portion temperature differences for the diurnal tide, calculated for the LST's of CRISTA-1 measurements taken on November 9, 1994. The contour interval is 2 K. All model runs show a pattern of alternating positive (solid lines) and negative (dashed lines) values characteristic of the first symmetric propagating mode of the diurnal tide. (upper left) GSWM-98 for equinox (October) conditions. (upper right) GSWM-98 with climatological values for November. (lower left) Same as upper right but with CRISTA geostrophic zonal wind. (lower right) Same as lower left but with CRISTA geostrophic wind and temperature. Click on image for larger figure. |
|
|
(upper left) CRISTA-1 ascending/descending orbit portion difference for November 9, 1994. (upper right) GSWM-98 diurnal prediction updated with zonal wind, temperature, pressure, density and ozone concentration from the CRISTA measurements. (lower left) Same as upper right but for the semi-diurnal component. (lower right) Diurnal and semi-diurnal component. This panel suggests that GSWM predicts the semi-diurnal component less well than the diurnal mode. Click on image for larger figure. |
|
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(left) Phases of the diurnal tide for the 0°-10°N latitudinal band. (right) Amplitudes of the diurnal tide for 0°-10°N latitudinal band. Symbols mark CRISTA results; dotted lines indicate GSWM prediction for equinox (October) conditions. GSWM with climatological November values (base case) is indicated by dashed lines, and solid lines show the model predictions for the updated background atmosphere (final case). Dashed-dotted lines indicate the model results with CRISTA geostrophic zonal wind, and dashed-dotted-dotted-dotted lines are the model results with CRISTA wind and temperature. The background atmosphere update, particularly the wind update, significantly increases the phase predictions. The observed amplitudes decrease above 75 km. This is not observed in the model. Click on image for larger figure. |
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