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

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dc.contributor.author Ghodpage, R.N.
dc.contributor.author Hickey, Michael P.
dc.contributor.author Taori, Alok K.
dc.contributor.author Siingh, Devendraa
dc.contributor.author Patil, P.T.
dc.date.accessioned 2017-10-26T11:47:50Z
dc.date.accessioned 2021-02-12T09:45:18Z
dc.date.available 2017-10-26T11:47:50Z
dc.date.available 2021-02-12T09:45:18Z
dc.date.issued 2016
dc.identifier.citation Atmospheric Chemistry and Physics, 16, 5611–5621, doi: 10.5194/acp-16-5611-2016 en_US
dc.identifier.uri http://localhost:8080/xmlui/handle/123456789/1000
dc.description.abstract 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. |η|, 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., 8) 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 longand 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. In the present report, we discuss the observed wave characteristics and cause of the noted diferences. en_US
dc.language.iso en en_US
dc.subject OH Airglow en_US
dc.subject Krassovsky method en_US
dc.subject Multispectral photometer en_US
dc.title Response of OH airglow emissions to mesospheric gravity waves and comparisons with full-wave model simulation at a low-latitude Indian station en_US
dc.type Article en_US
dc.identifier.accession 091542


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