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vhf-radar observations of temperature sheets in the stratospheric ...

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measurements, is shown <strong>in</strong> figure 1(c). From this figure high aspect sensitivity can be noticedaround <strong>the</strong> <strong>temperature</strong> <strong>sheets</strong>, which <strong>in</strong> turn confirms <strong>the</strong> layered structure <strong>of</strong> <strong>the</strong>backscatters.In order to know <strong>the</strong> vertical wave length <strong>of</strong> <strong>temperature</strong> and SNR perturbations,wave analysis have been carried out and is shown <strong>in</strong> figure 2. As <strong>the</strong>re was no cont<strong>in</strong>uous<strong>radar</strong> <strong>observations</strong>, <strong>the</strong> wave anlysis is done <strong>in</strong> height doma<strong>in</strong> only to f<strong>in</strong>d out <strong>the</strong> verticalwavelenth <strong>of</strong> <strong>the</strong> observed perturbations. Both SNR and <strong>temperature</strong> show a peak <strong>in</strong>amplitude at <strong>the</strong> vertical wavelength <strong>of</strong> 1.6 km. This suggests that <strong>the</strong> modulation <strong>of</strong><strong>temperature</strong> is due to <strong>the</strong> propagation <strong>of</strong> atmospheric waves, which <strong>in</strong> turn reflects <strong>in</strong> <strong>the</strong>SNR <strong>observations</strong>. As mentioned earlier,due to <strong>the</strong> lack <strong>of</strong> cont<strong>in</strong>uous <strong>observations</strong> (both<strong>temperature</strong> and <strong>radar</strong> <strong>in</strong>tensity), wave periodicities are not estimated.Realiz<strong>in</strong>g <strong>the</strong> importance <strong>of</strong> <strong>the</strong>se studies a comprehensive campaign is carried out t<strong>of</strong>ur<strong>the</strong>r understand <strong>the</strong> existence <strong>of</strong> <strong>temperature</strong> <strong>sheets</strong>. Dur<strong>in</strong>g this campaign, we found asimilar k<strong>in</strong>d <strong>of</strong> structure as discussed above on September 25, 2002. On this day, cont<strong>in</strong>uous<strong>radar</strong> <strong>observations</strong> were taken for a period <strong>of</strong> 12 hours with time and height resolutions <strong>of</strong>7m<strong>in</strong> and 150 m respectively. The <strong>radar</strong> <strong>observations</strong> are also supported by <strong>the</strong> simultaneousGPS measurements at <strong>the</strong> <strong>radar</strong> site. Figure 3(a) shows <strong>the</strong> height pr<strong>of</strong>ile <strong>of</strong> <strong>temperature</strong>,which is reveal<strong>in</strong>g <strong>the</strong> prom<strong>in</strong>ent <strong>temperature</strong> structures <strong>in</strong> <strong>the</strong> lower stratosphere.September 4, 2000SNR (dB)(a) (b) (c)Figure 1. (a) Height pr<strong>of</strong>ile <strong>of</strong> <strong>temperature</strong> derived from GPS-Sonde measurements, (b)Height-Time-SNR section obta<strong>in</strong>ed from Gadanki VHF <strong>radar</strong> and (c) height pr<strong>of</strong>ile <strong>of</strong> SNRdifference between vertical and <strong>of</strong>f-vertical (10°) beam directions on September 4, 2000.September 4, 2000Figure 2. Vertical wave number spectra <strong>of</strong> <strong>temperature</strong> and SNR obta<strong>in</strong>ed on September 42000 (arrow <strong>in</strong>dicates <strong>the</strong> dom<strong>in</strong>ant wave number)

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