...
首页> 外文期刊>Atmospheric chemistry and physics >Response of OH airglow emissions to mesospheric gravity waves and comparisons with full-wave model simulation at a low-latitude Indian station
【24h】

Response of OH airglow emissions to mesospheric gravity waves and comparisons with full-wave model simulation at a low-latitude Indian station

机译:低纬度印度台站OH辉光排放对中层重力波的响应以及与全波模型模拟的比较

获取原文

摘要

Quasi-monochromatic gravity-wave-induced oscillations, monitored using the mesospheric OH airglow emission over Kolhapur (16.8°?N, 74.2°?E), India, during January to April?2010 and January to December?2011, have been characterized using the Krassovsky method. The nocturnal variability reveals prominent wave signatures with periods ranging from 5.2 to 10.8?h as the dominant nocturnal wave with embedded short-period waves having wave periods of 1.5–4.4?h. The results show that the magnitude of the Krassovsky parameter, viz. |iη/i|, ranged from 2.1 to 10.2?h for principal or long nocturnal waves (5.2–10.8?h observed periods), and from 1.5 to 5.4?h for the short waves (1.5–4.4?h observed periods) during the years of 2010 and 2011, respectively. The phase (i.e., Φ) values of the Krassovsky parameters exhibited larger variability and varied from ?8.1 to ?167°. The deduced mean vertical wavelengths are found to be approximately ?60.2?±?20 and ?42.8?±?35?km for long- and short-period waves for the year 2010. Similarly, for 2011 the mean vertical wavelengths are found to be approximately ?77.6?±?30 and ?59.2?±?30?km for long and short wave periods, respectively, indicating that the observations over Kolhapur were dominated by upward-propagating waves. We use a full-wave model to simulate the response of OH emission to the wave motion and compare the results with observed values.
机译:利用2010年1月至4月和2011年1月至2011年12月在印度Kolhapur(16.8°N,74.2°E)的中层OH气辉发射监测的准单色重力波诱发的振荡已得到表征。 Krassovsky方法。夜间变化显示出显着的波特征,其周期为5.2至10.8?h,是占主导地位的夜间波,其中嵌入的短周期波的波周期为1.5-4.4?h。结果表明,Krassovsky参数的大小即vi。 | η |,对于主要或长夜行波(观测周期为5.2-10.8?h),范围从2.1到10.2?h;对于短波(1.5-4.4?h),范围从1.5至5.4?h。 h观测期)分别在2010年和2011年。 Krassovsky参数的相位(即Φ)值表现出较大的可变性,并且在θ8.1至167°之间变化。对于2010年的长短波,推论出的平均垂直波长大约是60.2±20,而垂直线大约是42.8±35 km。类似地,在2011年,平均垂直波长被发现是长波和短波周期分别约为77.6±30°和59.2±30km,这表明在Kolhapur上的观测以向上传播的波为主。我们使用全波模型来模拟OH排放对波动的响应,并将结果与​​观测值进行比较。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号