首页> 外文期刊>Journal of Geophysical Research, D. Atmospheres: JGR >Signature of a Quasi 30‐Day Oscillation at Midlatitude Based on Wind Observations From MST Radar and Meteor Radar
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Signature of a Quasi 30‐Day Oscillation at Midlatitude Based on Wind Observations From MST Radar and Meteor Radar

机译:基于MST雷达和流星雷达的风观察,在中间际时签署了二际振荡

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Lots of works make contributions to revealing propagation features and excitation mechanisms of intraseasonal oscillations (ISOs) in the tropics; however, there are few reports on ISOs at higher latitudes. By using measurements of mesosphere‐stratosphere‐troposphere radar at Xianghe (39.8°N, 116.5°E) and meteor radar at Beijing (40.3°N, 116.2°E) and reanalysis data for 105 days from 16 November 2013 to 28 February 2014, we study an ISO with about 30‐day period at midlatitude and high latitude. Radar observations indicate that in the troposphere, the oscillation attains an amplitude peak in zonal wind at about 9 km and propagates downward below 9 km. At about 9–16 km, the oscillation gradually decays with height and then strengthens again as it propagates upward in the stratosphere. In the mesosphere, the oscillation obviously appears at 78–86 km with a maximum amplitude at 80 km. Reanalysis data show that in the troposphere, the oscillation propagates southward. At about 100 (~16 km)‐ to 10 (~32 km)‐hPa levels, the oscillation is gradually reflected back to propagate northward, and then propagates poleward at higher altitude. Refractive index can explain its complex propagation characteristics very well. Consistence and coherence of its phase progression indicate that in the lower atmosphere, the oscillation comes from the polar region. Hence, ISOs can not only originate from but also propagate in the atmosphere at mid and high latitudes.
机译:许多作品为在热带地区揭示了渗透震荡(ISOS)的传播特征和激励机制;但是,在较高纬度地区仍有很少的报告。通过在北京(40.3°N,116.2°E)和2013年11月16日至2014年2月28日,北京(40.3°N,116.5°E)和雷达的Mesrophy-Stratys-Tropers雷达(40.3°N,116.2°E)和再分析数据,从2013年11月16日开始测量我们研究了大约30天的中度和高纬度的ISO。雷达观测表明,在对流层中,振荡在撒蒙风中的幅度峰值达到约9km,向下传播9公里。在大约9-16公里处,振荡逐渐衰减高度,然后在平流层向上传播时再次加强。在介质圈,振荡显然出现在78-86公里处,最大振幅在80公里处。重新分析数据显示,在对流层中,振荡向南传播。在约100(〜16公里) - 至10(〜32km)-HPA水平时,振荡逐渐反射回向北传播,然后在较高海拔地区传播极端。折射率可以很好地解释其复杂的传播特性。其相进展的一致性和相干性表明,在较低的大气中,振荡来自极地区域。因此,ISOS不仅可以源自中期和高纬度的大气中的繁殖。

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