2008
DOI: 10.5194/angeo-26-3765-2008
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Studies of vertical fluxes of horizontal momentum in the lower atmosphere using the MU-radar

Abstract: Abstract.We study the momentum flux of the atmospheric motions in the height ranges between 6 and 22 km observed using the MU radar at Shigaraki in Japan during a 3 day period in January 1988. The data were divided by double Fourier transformation into data set of waves with downward-phase-velocity and data set of waves with upward-phase-velocity for independent momentum flux calculation. The result showed that both the 72 h averaged upward flux and downward flux of zonal momentum were negative at nearly each … Show more

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Cited by 4 publications
(18 citation statements)
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“…When the background wind is not negligible, such as the case of the winter data in this study, the azimuth angle of the horizontal wave vector 3748 F. S. Kuo et al: Statistical characteristics of AGW wave packet propagation no longer equals to the azimuth angle of the horizontal group velocity (see Appendix B), we must take horizontal group velocity into consideration. Phase-and-group-velocity-tracing technique had been proved to be efficient to estimate the vertical group-andphase-velocities (v gz and v pz ) as well as the period τ of a wave packet (Kuo et al, 2003(Kuo et al, , 2007(Kuo et al, , 2008. In this study, we further proposed a process to calculate the horizontal group velocity v gh from the dispersion equations using the measured values of v gz , v pz , and τ .…”
Section: Summaries and Discussionmentioning
confidence: 99%
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“…When the background wind is not negligible, such as the case of the winter data in this study, the azimuth angle of the horizontal wave vector 3748 F. S. Kuo et al: Statistical characteristics of AGW wave packet propagation no longer equals to the azimuth angle of the horizontal group velocity (see Appendix B), we must take horizontal group velocity into consideration. Phase-and-group-velocity-tracing technique had been proved to be efficient to estimate the vertical group-andphase-velocities (v gz and v pz ) as well as the period τ of a wave packet (Kuo et al, 2003(Kuo et al, , 2007(Kuo et al, , 2008. In this study, we further proposed a process to calculate the horizontal group velocity v gh from the dispersion equations using the measured values of v gz , v pz , and τ .…”
Section: Summaries and Discussionmentioning
confidence: 99%
“…So from Table 1, we can readily identify T3c for example, to represent the time range of 4∼24 h and Z4 to represent the height range of 5.9∼17.7 km. Different windows in Table 1 have different upper frequency and wave number boundaries, but may have the same lower frequency and wave number boundaries, because only the high frequency end (high wave number end) dictates the characteristic wave period (wavelength) of the wave packets as we had frequently explained in our previous papers (Kuo et al, 2003(Kuo et al, , 2008Kuo and Röttger, 2005). The number of gravity wave packets (in bold) along with the original number of wave packets being measured (the number under the slash) in different window were listed in Table 2 (for winter data set) and Table 3 (for summer data set), where the content in the 5th column of the 4th row represents the content of window T3cZ5, and the 2nd column of the 3rd row represents the content of window T2Z4, and so on.…”
Section: Propagation Parameters Of Wave Packets Calculated By Dispersmentioning
confidence: 99%
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