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Gravity waves in the equatorial thermosphere and their relation to lower atmospheric variability

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Figure

Fig. 1.(a) Frequency-height distribution of the cospectral density of u′w′ near the equator (0.4◦N) for zonal wave number 20 (s = 20, the zonalwavelength λx ≈ 2000 km) averaged over the period from 1 June to 14 June
Fig. 2. Height distributions of the vertical wavelength of dominant gravitywaves with s = 20, 40, 60 and 80
Fig. 4.(a) Longitudinal distribution of vertical flux of energy for theshort-period gravity waves (1–4 h) averaged over 14 days at a height of300 km (1–14 June); units are × 10−5 kg m−1 s−1
Fig. 5.(a) Longitudinal distribution of the total (kinetic pus potential)energy associated with the short-period gravity waves near the equator(10◦N–10◦S) at a height of 300 km averaged over the period from 21March to 31 March; units are ×10−8 kg m2 s−2
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