Geomagnetic influences on thermospheric winds observed in the auroral zone
dc.contributor.author | Wallis, Donald Douglas James Herbert | |
dc.contributor.author | Romick, Gerald J. | |
dc.date.accessioned | 2024-11-22T19:14:33Z | |
dc.date.available | 2024-11-22T19:14:33Z | |
dc.date.issued | 1974-05 | |
dc.identifier.uri | http://hdl.handle.net/11122/15636 | |
dc.description | UAG R-227; Scientific Report. This title also submitted as a dissertation to the faculty of the University of Alaska in partial fulfillment of the requirements for the degree of Doctor of Philosophy, May, 1974. | en_US |
dc.description.abstract | A large body of observations of the wind field in the high-latitude thermosphere (140 to 350 km) is examined to characterize the winds and to determine their probably source. Theories and existing models of these winds are first reviewed. The morphologies of auroral particle precipitation, electric fields, and current systems are discussed to elucidate the effects of these factors upon the wind field. Existing models suggest that the effects of auroral electric fields and heating can be separated in a geomagnetic coordinate frame. It is shown, in this study, that the mean temporal dependence of the (geomagnetic) meridional component is similar to that predicted by tidal models except the magnitudes of the observed winds are smaller than predicted (observed peak speeds – 150 m sec⁻¹). Deviations (up to 200 m sec⁻¹) of the observed meridional winds from this mean behavior are probably caused by heating of the thermosphere by Joule dissipation in the auroral electrojets. Zonal winds are shown to be principally driven by collisions of the neutrals with ions drifting under the action of the auroral zone electric field. Zonal speeds from 200 to 400 m sec⁻¹ are typical. The observed zonal winds are correlated with the direction of the auroral electric fields as inferred from magnetometer records. The response time of the observed winds to changes in direction of the electric field (northward to southward) is found to be ≈ 1¹/₂ hours. Tidal winds are of secondary importance for the zonal component (peak speeds ≈ 150 m sec⁻¹). Electric fields and Joule dissipation in the high-latitude thermosphere are concluded to be responsible for the principal observed characteristics of auroral-zone thermospheric winds. | en_US |
dc.description.sponsorship | Funding of this research was provided by the State of Alaska, and National Science Foundation, Division of Env grants: GA-31876 and GA-32119. Some of the barium release data used in this study was acquired under Air Force Contract F 30602-C-0063 and Defense Atomic Support Agency Contract DASA 01-69-C-0047. | en_US |
dc.description.tableofcontents | Abstract – Acknowledgements – Table of contents – List of illustrations – List of tables – Ch.1. Neutral wind in the thermosphere – 1.1. Introduction – 1.2. High-latitude thermospheric winds – 1.3. Format of this study – 1.4. Conventions used in this study – Ch.2. Review of the equations of motion and the factors which govern the wind field in the thermosphere – 2.1. The equation of motion for the neutral thermosphere – The inertial term – The Coriolis term – The pressure-gradient term – The viscous-drag term – The ion-drag term – Other equations of importance for thermospheric winds – 2.2. Comparison of the magnitude of the terms in the equation of motion – 2.3. Response of the thermosphere to a heat source – 2.4. Response of the neutral thermosphere to crossed electric and magnetic fields – 2.5. Morphology and effects of auroral particle precipitation – 2.6. Morphology of auroral electric fields – 2.7. Morphology of high-latitude currents – Ch.3. Models of thermospheric winds – 3.1. Tidal wind models – Challinor’s model – Kohl’s model – Vest’s model – 3.2. Comparison of tidal wind models with observations – Winds deduced from the Sq magnetic variation – Low- and middle-latitude winds deduced from trail releases – 3.3. Models of the high-latitude wind field perturbation due to ion-drag – Fedder and Banks’ model of ion-drag winds – Heaps’ model of ion-drag winds – 3.4. Models of thermospheric winds generated by auroral heating – Vest’s model of meridional winds – Heaps’ model of meridional wind perturbations – 3.5. Summary of thermospheric wind models – Ch.4. Observations of the meridional wind component - 4.1. Methods and errors of observation – 4.2. Mean temporal behavior of meridional winds – 4.3. Correlation of meridional winds with various indices – 4.4. Deviations of the meridional winds from their mean behavior – 4.5. The sources of meridional winds – Ch.5. Observations of the zonal wind component – 5.1. Methods and errors of observation – 5.2. Observations of zonal thermospheric winds from barium releases – 5.3. Observations of zonal winds by 6300Å interferometry – 5.4. Trail release wind observations at Fort Churchill, Canada – Ch.6. Conclusions – Appendix A. List of symbols – Appendix B. Approximate locations of stations mentioned in this study – Appendix C. Interferometer wind measurements – Appendix D. Release techniques – Appendix E. Triangulation errors – References. | en_US |
dc.language.iso | en_US | en_US |
dc.subject | Winds aloft | en_US |
dc.subject | Thermosphere | en_US |
dc.subject | Geomagnetism | en_US |
dc.subject | Auroras | en_US |
dc.title | Geomagnetic influences on thermospheric winds observed in the auroral zone | en_US |
dc.type | Report | en_US |
refterms.dateFOA | 2024-11-22T19:14:35Z |
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