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作 者:LIU Xiao XU JiYao MA RuiPing
机构地区:[1]State Key Laboratory of Space Weather,Center for Space Science and Applied research,Chinese Academy of Sciences,Beijing 100080,China [2]Graduate University of Chinese Academy of Sciences,Beijing 100049,China
出 处:《Science China Earth Sciences》2007年第8期1273-1279,共7页中国科学(地球科学英文版)
基 金:the National Natural Science Foundation of China (Grant Nos. 40621003, 40225011 and 40674088);the National Major Basic Research Project (Grant No. 2006CB806306);in part by the Foundation of the Key Laboratory of Geospace Environment & Geodesy of Ministry of Education, China
摘 要:In this study, we present the nonlinear interactions between gravity waves (GWs) and tides by using the 2D numerical model for the nonlinear propagation of GWs in the compressible atmosphere. During the propagation in the tidal background, GWs become instable in three regions, that is z = 75―85 km, z = 90―110 km and z = 115―130 km. The vertical wavelength firstly varies gradually from the initial 12 km to 27 km. Then the newly generated longer waves are gradually compressed. The longer and shorter waves occur in the regions where GWs propagate in the reverse and the same direction of the hori-zontal mean wind respectively. In addition, GWs can propagate above the main breaking region (90—110 km). During GWs propagation, not only the mean wind is accelerated, but also the amplitude of tide is amplified. Especially, after GWs become instable, this amplified effect to the tidal amplitude is much obvious.In this study, we present the nonlinear interactions between gravity waves (GWs) and tides by using the 2D numerical model for the nonlinear propagation of GWs in the compressible atmosphere. During the propagation in the tidal background, GWs become instable in three regions, that is z = 75–85 km, z =90–110 km and z = 115–130 km. The vertical wavelength firstly varies gradually from the initial 12 km to 27 km. Then the newly generated longer waves are gradually compressed. The longer and shorter waves occur in the regions where GWs propagate in the reverse and the same direction of the horizontal mean wind respectively. In addition, GWs can propagate above the main breaking region (90–110 km). During GWs propagation, not only the mean wind is accelerated, but also the amplitude of tide is amplified. Especially, after GWs become instable, this amplified effect to the tidal amplitude is much obvious.
关 键 词:GRAVITY WAVES TIDES mean WIND nonlinear INTERACTIONS GRAVITY WAVES PARAMETERIZATION
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