Numerical simulations of thermospheric dynamics: divergence as a proxy for vertical winds

A local scale, time dependent three-dimensional model of the neutral thermosphere was used to test the applicability of two previously published empirical relations between thermospheric vertical wind and velocity divergence, i.e., those due to Burnside et al. (1981) and Brekke (1997). The model...

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Main Authors: S. L. Cooper, M. Conde, P. Dyson
Format: Article
Language:English
Published: Copernicus Publications 2009-06-01
Series:Annales Geophysicae
Online Access:https://www.ann-geophys.net/27/2491/2009/angeo-27-2491-2009.pdf
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spelling doaj-d9d5122fb7cf4bc78ca3bad6d44a2b7e2020-11-24T23:18:48ZengCopernicus PublicationsAnnales Geophysicae0992-76891432-05762009-06-01272491250210.5194/angeo-27-2491-2009Numerical simulations of thermospheric dynamics: divergence as a proxy for vertical windsS. L. Cooper0M. Conde1P. Dyson2Department of Physics, La Trobe University, Melbourne, Victoria, AustraliaDepartment of Physics, University of Alaska, Fairbanks, AK, USADepartment of Physics, La Trobe University, Melbourne, Victoria, AustraliaA local scale, time dependent three-dimensional model of the neutral thermosphere was used to test the applicability of two previously published empirical relations between thermospheric vertical wind and velocity divergence, i.e., those due to Burnside et al. (1981) and Brekke (1997). The model self-consistently solves for vertical winds driven by heat and momentum deposited into the neutral atmosphere by high latitude ion convection. The Brekke condition accurately mimicked the overall "shape" of the three-dimensional model vertical wind field although, as written, it consistently overestimated the vertical wind magnitude by a factor of approximately 5/3, for the heating scenarios that we considered. This same general behavior was observed regardless of whether the forcing was static or rapidly changing with time. We discuss the likely reason for the Brekke condition overestimating the magnitude of our vertical winds, and suggest an alternative condition that should better describe vertical winds that are driven by local heating. The applicability of the Burnside condition was, by contrast, quite variable. During static heating, both the magnitude and the sign of the model vertical winds were predicted reliably at heights above those of maximum energy and momentum deposition per unit mass. However, below the thermal forcing, the Burnside condition predicted vertical winds of the wrong sign. It also introduced significant artefacts into the predicted vertical wind field when the forcing changed suddenly with time. If these results are of general applicability (which seems likely, given the way these relations are derived) then the Burnside condition could usually be used safely at altitudes above <I>h<sub>m</sub></I>F<sub>2</sub>. But it should be avoided below this height at all times, and even at high altitudes during periods of dynamic forcing. While the Brekke condition (or our modified version of it) could likely be used in all circumstances, there are few experimental scenarios for which this would be useful. This is because evaluation of the Brekke condition would not usually be possible unless the vertical wind was already known in advance.https://www.ann-geophys.net/27/2491/2009/angeo-27-2491-2009.pdf
collection DOAJ
language English
format Article
sources DOAJ
author S. L. Cooper
M. Conde
P. Dyson
spellingShingle S. L. Cooper
M. Conde
P. Dyson
Numerical simulations of thermospheric dynamics: divergence as a proxy for vertical winds
Annales Geophysicae
author_facet S. L. Cooper
M. Conde
P. Dyson
author_sort S. L. Cooper
title Numerical simulations of thermospheric dynamics: divergence as a proxy for vertical winds
title_short Numerical simulations of thermospheric dynamics: divergence as a proxy for vertical winds
title_full Numerical simulations of thermospheric dynamics: divergence as a proxy for vertical winds
title_fullStr Numerical simulations of thermospheric dynamics: divergence as a proxy for vertical winds
title_full_unstemmed Numerical simulations of thermospheric dynamics: divergence as a proxy for vertical winds
title_sort numerical simulations of thermospheric dynamics: divergence as a proxy for vertical winds
publisher Copernicus Publications
series Annales Geophysicae
issn 0992-7689
1432-0576
publishDate 2009-06-01
description A local scale, time dependent three-dimensional model of the neutral thermosphere was used to test the applicability of two previously published empirical relations between thermospheric vertical wind and velocity divergence, i.e., those due to Burnside et al. (1981) and Brekke (1997). The model self-consistently solves for vertical winds driven by heat and momentum deposited into the neutral atmosphere by high latitude ion convection. The Brekke condition accurately mimicked the overall "shape" of the three-dimensional model vertical wind field although, as written, it consistently overestimated the vertical wind magnitude by a factor of approximately 5/3, for the heating scenarios that we considered. This same general behavior was observed regardless of whether the forcing was static or rapidly changing with time. We discuss the likely reason for the Brekke condition overestimating the magnitude of our vertical winds, and suggest an alternative condition that should better describe vertical winds that are driven by local heating. The applicability of the Burnside condition was, by contrast, quite variable. During static heating, both the magnitude and the sign of the model vertical winds were predicted reliably at heights above those of maximum energy and momentum deposition per unit mass. However, below the thermal forcing, the Burnside condition predicted vertical winds of the wrong sign. It also introduced significant artefacts into the predicted vertical wind field when the forcing changed suddenly with time. If these results are of general applicability (which seems likely, given the way these relations are derived) then the Burnside condition could usually be used safely at altitudes above <I>h<sub>m</sub></I>F<sub>2</sub>. But it should be avoided below this height at all times, and even at high altitudes during periods of dynamic forcing. While the Brekke condition (or our modified version of it) could likely be used in all circumstances, there are few experimental scenarios for which this would be useful. This is because evaluation of the Brekke condition would not usually be possible unless the vertical wind was already known in advance.
url https://www.ann-geophys.net/27/2491/2009/angeo-27-2491-2009.pdf
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