The roles of vertical advection and eddy diffusion in the equatorial mesospheric semi-annual oscillation (MSAO)

Observations of the mesospheric semi-annual oscillation (MSAO) in the equatorial region have been reported dating back several decades. Seasonal variations in both species densities and airglow emissions are well documented. The extensive observations available offer an excellent case study for comp...

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Main Authors: R. L. Gattinger, E. Kyrölä, C. D. Boone, W. F. J. Evans, K. A. Walker, I. C. McDade, P. F. Bernath, E. J. Llewellyn
Format: Article
Language:English
Published: Copernicus Publications 2013-08-01
Series:Atmospheric Chemistry and Physics
Online Access:http://www.atmos-chem-phys.net/13/7813/2013/acp-13-7813-2013.pdf
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spelling doaj-838866fce3914699900fbbaad4385cac2020-11-24T23:12:51ZengCopernicus PublicationsAtmospheric Chemistry and Physics1680-73161680-73242013-08-0113157813782410.5194/acp-13-7813-2013The roles of vertical advection and eddy diffusion in the equatorial mesospheric semi-annual oscillation (MSAO)R. L. GattingerE. KyröläC. D. BooneW. F. J. EvansK. A. WalkerI. C. McDadeP. F. BernathE. J. LlewellynObservations of the mesospheric semi-annual oscillation (MSAO) in the equatorial region have been reported dating back several decades. Seasonal variations in both species densities and airglow emissions are well documented. The extensive observations available offer an excellent case study for comparison with model simulations. A broad range of MSAO measurements is summarised with emphasis on the 80–100 km region. The objective here is not to address directly the complicated driving forces of the MSAO, but rather to employ a combination of observations and model simulations to estimate the limits of some of the underlying dynamical processes. Photochemical model simulations are included for near-equinox and near-solstice conditions, the two times with notable differences in the observed MSAO parameters. Diurnal tides are incorporated in the model to facilitate comparisons of observations made at different local times. The roles of water vapour as the "driver" species and ozone as the "response" species are examined to test for consistency between the model results and observations. The simulations suggest the interactions between vertical eddy diffusion and background vertical advection play a significant role in the MSAO phenomenon. Further, the simulations imply there are rigid limits on vertical advection rates and eddy diffusion rates. For August at the Equator, 90 km altitude, the derived eddy diffusion rate is approximately 1 × 10<sup>6</sup> cm<sup>2</sup> s<sup>−1</sup> and the vertical advection is upwards at 0.8 cm s<sup>−1</sup>. For April the corresponding values are 4 × 10<sup>5</sup> cm<sup>2</sup> s<sup>−1</sup> and 0.1 cm s<sup>−1</sup>. These results from the current 1-D model simulations will need to be verified by a full 3-D simulation. Exactly how vertical advection and eddy diffusion are related to gravity wave momentum as discussed by Dunkerton (1982) three decades ago remains to be addressed.http://www.atmos-chem-phys.net/13/7813/2013/acp-13-7813-2013.pdf
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language English
format Article
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author R. L. Gattinger
E. Kyrölä
C. D. Boone
W. F. J. Evans
K. A. Walker
I. C. McDade
P. F. Bernath
E. J. Llewellyn
spellingShingle R. L. Gattinger
E. Kyrölä
C. D. Boone
W. F. J. Evans
K. A. Walker
I. C. McDade
P. F. Bernath
E. J. Llewellyn
The roles of vertical advection and eddy diffusion in the equatorial mesospheric semi-annual oscillation (MSAO)
Atmospheric Chemistry and Physics
author_facet R. L. Gattinger
E. Kyrölä
C. D. Boone
W. F. J. Evans
K. A. Walker
I. C. McDade
P. F. Bernath
E. J. Llewellyn
author_sort R. L. Gattinger
title The roles of vertical advection and eddy diffusion in the equatorial mesospheric semi-annual oscillation (MSAO)
title_short The roles of vertical advection and eddy diffusion in the equatorial mesospheric semi-annual oscillation (MSAO)
title_full The roles of vertical advection and eddy diffusion in the equatorial mesospheric semi-annual oscillation (MSAO)
title_fullStr The roles of vertical advection and eddy diffusion in the equatorial mesospheric semi-annual oscillation (MSAO)
title_full_unstemmed The roles of vertical advection and eddy diffusion in the equatorial mesospheric semi-annual oscillation (MSAO)
title_sort roles of vertical advection and eddy diffusion in the equatorial mesospheric semi-annual oscillation (msao)
publisher Copernicus Publications
series Atmospheric Chemistry and Physics
issn 1680-7316
1680-7324
publishDate 2013-08-01
description Observations of the mesospheric semi-annual oscillation (MSAO) in the equatorial region have been reported dating back several decades. Seasonal variations in both species densities and airglow emissions are well documented. The extensive observations available offer an excellent case study for comparison with model simulations. A broad range of MSAO measurements is summarised with emphasis on the 80–100 km region. The objective here is not to address directly the complicated driving forces of the MSAO, but rather to employ a combination of observations and model simulations to estimate the limits of some of the underlying dynamical processes. Photochemical model simulations are included for near-equinox and near-solstice conditions, the two times with notable differences in the observed MSAO parameters. Diurnal tides are incorporated in the model to facilitate comparisons of observations made at different local times. The roles of water vapour as the "driver" species and ozone as the "response" species are examined to test for consistency between the model results and observations. The simulations suggest the interactions between vertical eddy diffusion and background vertical advection play a significant role in the MSAO phenomenon. Further, the simulations imply there are rigid limits on vertical advection rates and eddy diffusion rates. For August at the Equator, 90 km altitude, the derived eddy diffusion rate is approximately 1 × 10<sup>6</sup> cm<sup>2</sup> s<sup>−1</sup> and the vertical advection is upwards at 0.8 cm s<sup>−1</sup>. For April the corresponding values are 4 × 10<sup>5</sup> cm<sup>2</sup> s<sup>−1</sup> and 0.1 cm s<sup>−1</sup>. These results from the current 1-D model simulations will need to be verified by a full 3-D simulation. Exactly how vertical advection and eddy diffusion are related to gravity wave momentum as discussed by Dunkerton (1982) three decades ago remains to be addressed.
url http://www.atmos-chem-phys.net/13/7813/2013/acp-13-7813-2013.pdf
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