Abstract

Abstract. HRDI (High Resolution Doppler Interferometer-UARS) winds data have been analyzed in 4°-latitude by 10°-longitude cells at 96km to obtain the global distribution of the solar-tidal amplitudes and phases. The solstices June–July (1993), December–January (1993–1994), and one equinox (September–October, 1994) are analyzed. In an earlier paper (Manson et al., 2002b) the emphasis was solely upon the longitudinal and latitudinal variations of the amplitudes and phases of the semidiurnal (12h) and diurnal (24h) tides. The longitudinal structures were shown to be quite distinctive, and in the case of the EW component of the diurnal tide there were typically four maxima/perturbations of amplitudes or phases around a latitude circle. In this case they tended to be associated with the locations of the major oceans. Here, a spatial complex spectral analysis has been applied to the data set, to obtain the zonal wave numbers for the tides as functions of latitude. For the diurnal tide the dominant s=1 migrating component and nonmigrating tides with wave numbers s=–3, –2, 0, 2 are identified; and for the semidiurnal tide, as well as the dominant s=2 migrating component, the spectra indicate the presence of nonmigrating tides with wave numbers s=–2, 0, 4. These wave numbers are also simply related to the global longitudinal structures in the tidal amplitudes and phases. Comparisons are made with the Global Scale Wave Model (GSWM-02), which now incorporates migrating and nonmigrating tides associated with tropospheric latent heat processes, and offers monthly outputs. For the diurnal tide the dominant nonmigrating tidal spectral feature (94km) is for wave number s=–3; it is relatively stronger than in the HRDI winds, and produces quite consistent structures in the global tidal fields with four longitudinal maxima. Overall, the modelled 24-h tidal amplitudes are larger than observed during the equinox beyond 40° latitude. For the semidiurnal tide, nonmigrating tides are frequently indicated in the spectra with wave numbers s=–2, 0, 6; and there are complementary longitudinal structures in the global tidal fields with two and four maxima evident. Modelled 12-h tidal amplitudes are much smaller than observed during non-winter months beyond 30°. There is a detailed discussion of the spectral features, their seasonal variations, and the similarities with the HRDI tidal data. This discussion is in the context of the inherent limitations of the model.Key words. Meteorology and atmospheric dynamics (middle atmosphere dynamics; thermospheric dynamics; waves and tides)

Highlights

  • The observations of the global tides of the middle atmosphere, or “mesosphere lower thermosphere” (MLT), at heights from 60–100 km, have been dominated by sampling from radar systems: Medium Frequency (MF) and “meteor wind” radars

  • 3.1 HRDI global tides at 96 km Following Paper 1, where the global tidal structures were provided for the solstices of December–January (1993– 1994), June–July (1993), and September–October (1994), the complex spatial frequencies appropriate to the global tides are provided and discussed

  • Overall there is good agreement between our analysis and that of Forbes et al (2003), even though the data sets and analysis differ somewhat; we have shown the relative strengths of the migrating and nonmigrating tides and the resulting standing wave patterns in the global tidal structures

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Summary

Introduction

The observations of the global tides of the middle atmosphere, or “mesosphere lower thermosphere” (MLT), at heights from 60–100 km, have been dominated by sampling from radar systems: Medium Frequency (MF) and “meteor wind” radars. Nonlinear interactions between the stationary planetary wave (wave number 1) and migrating tides leads to s=0, 2 for the diurnal tide (modelling exercise; Hagan and Roble, 2001), and to s=1, 3 for the semidiurnal tide (UARS winds; Angelats i Coll and Forbes, 2002) The existence of such tides (or components), and the related global longitudinal structures in amplitude and phase within the MLT, depend upon a myriad of factors, which reflect upon the importance of studying tidal activity within the lower and middle atmospheres. Some comparisons between middle atmosphere climatologies from the GSWM-02 and radar data are shown for completeness in each section

Data analysis
Diurnal Tides
GSWM-02 global tides at 94 km
Semi-diurnal tides
Summary and conclusions
Full Text
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