Comparison of modeled and observed effects of radiation belt electron precipitation on mesospheric hydroxyl and ozone

Observations have shown that mesospheric hydroxyl (OH) is affected by energetic electron precipitation (EEP) at magnetic latitudes connected to the outer radiation belt. It is not clear, however, if the current satellite‐based electron flux observations can be used to accurately describe EEP in atmo...

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Veröffentlicht in:Journal of geophysical research. Atmospheres 2013-10, Vol.118 (19), p.11,419-11,428
Hauptverfasser: Verronen, Pekka T., Andersson, Monika E., Rodger, Craig J., Clilverd, Mark A., Wang, Shuhui, Turunen, Esa
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container_end_page 11,428
container_issue 19
container_start_page 11,419
container_title Journal of geophysical research. Atmospheres
container_volume 118
creator Verronen, Pekka T.
Andersson, Monika E.
Rodger, Craig J.
Clilverd, Mark A.
Wang, Shuhui
Turunen, Esa
description Observations have shown that mesospheric hydroxyl (OH) is affected by energetic electron precipitation (EEP) at magnetic latitudes connected to the outer radiation belt. It is not clear, however, if the current satellite‐based electron flux observations can be used to accurately describe EEP in atmospheric models. We use the Sodankylä Ion and Neutral Chemistry (SIC) model to reproduce the changes in OH and ozone observed by the Microwave Limb Sounder (MLS/Aura) during four strong EEP events. The daily mean electron energy‐flux spectrum, needed for ionization rate calculations, is determined by combining the Medium Energy Proton and Electron Detector fluxes and spectral form from the instrument for the detection of particles high‐energy electron detector on board the DEMETER satellite. We show that in general SIC is able to reproduce the observed day‐to‐day variability of OH and ozone. In the lower mesosphere, the model tends to underestimate the OH concentration, possibly because of uncertainties in the electron spectra for energies >300 keV. The model predicts OH increases at 60–80 km, reaching several hundred percent at 70–80 km during peak EEP forcing. Increases in OH are followed by ozone depletion, up to several tens of percent. The magnitude of modeled changes is similar to those observed by MLS and comparable to effects of individual solar proton events. Our results suggest that the combined satellite observations of electrons can be used to model the EEP effects above 70 km during geomagnetic storms, without a need for significant adjustments. However, for EEP energies >300 keV impacting altitudes 300 keV
doi_str_mv 10.1002/jgrd.50845
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It is not clear, however, if the current satellite‐based electron flux observations can be used to accurately describe EEP in atmospheric models. We use the Sodankylä Ion and Neutral Chemistry (SIC) model to reproduce the changes in OH and ozone observed by the Microwave Limb Sounder (MLS/Aura) during four strong EEP events. The daily mean electron energy‐flux spectrum, needed for ionization rate calculations, is determined by combining the Medium Energy Proton and Electron Detector fluxes and spectral form from the instrument for the detection of particles high‐energy electron detector on board the DEMETER satellite. We show that in general SIC is able to reproduce the observed day‐to‐day variability of OH and ozone. In the lower mesosphere, the model tends to underestimate the OH concentration, possibly because of uncertainties in the electron spectra for energies &gt;300 keV. The model predicts OH increases at 60–80 km, reaching several hundred percent at 70–80 km during peak EEP forcing. Increases in OH are followed by ozone depletion, up to several tens of percent. The magnitude of modeled changes is similar to those observed by MLS and comparable to effects of individual solar proton events. Our results suggest that the combined satellite observations of electrons can be used to model the EEP effects above 70 km during geomagnetic storms, without a need for significant adjustments. However, for EEP energies &gt;300 keV impacting altitudes &lt;70 km, correction factors may be required. 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In the lower mesosphere, the model tends to underestimate the OH concentration, possibly because of uncertainties in the electron spectra for energies &gt;300 keV. The model predicts OH increases at 60–80 km, reaching several hundred percent at 70–80 km during peak EEP forcing. Increases in OH are followed by ozone depletion, up to several tens of percent. The magnitude of modeled changes is similar to those observed by MLS and comparable to effects of individual solar proton events. Our results suggest that the combined satellite observations of electrons can be used to model the EEP effects above 70 km during geomagnetic storms, without a need for significant adjustments. However, for EEP energies &gt;300 keV impacting altitudes &lt;70 km, correction factors may be required. 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It is not clear, however, if the current satellite‐based electron flux observations can be used to accurately describe EEP in atmospheric models. We use the Sodankylä Ion and Neutral Chemistry (SIC) model to reproduce the changes in OH and ozone observed by the Microwave Limb Sounder (MLS/Aura) during four strong EEP events. The daily mean electron energy‐flux spectrum, needed for ionization rate calculations, is determined by combining the Medium Energy Proton and Electron Detector fluxes and spectral form from the instrument for the detection of particles high‐energy electron detector on board the DEMETER satellite. We show that in general SIC is able to reproduce the observed day‐to‐day variability of OH and ozone. In the lower mesosphere, the model tends to underestimate the OH concentration, possibly because of uncertainties in the electron spectra for energies &gt;300 keV. The model predicts OH increases at 60–80 km, reaching several hundred percent at 70–80 km during peak EEP forcing. Increases in OH are followed by ozone depletion, up to several tens of percent. The magnitude of modeled changes is similar to those observed by MLS and comparable to effects of individual solar proton events. Our results suggest that the combined satellite observations of electrons can be used to model the EEP effects above 70 km during geomagnetic storms, without a need for significant adjustments. However, for EEP energies &gt;300 keV impacting altitudes &lt;70 km, correction factors may be required. Key Points Electron precipitation effect can be comparable to that of solar proton events Model results generally agree with satellite observations above 70 km Correction of electron flux observations might be needed at energies &gt; 300 keV</abstract><cop>Hoboken, NJ</cop><pub>Blackwell Publishing Ltd</pub><doi>10.1002/jgrd.50845</doi><tpages>10</tpages><oa>free_for_read</oa></addata></record>
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source Wiley Online Library Journals Frontfile Complete; Wiley Online Library Free Content; Alma/SFX Local Collection
subjects Absorption and scattering of radiation
Atmospheric chemistry
Boards
Earth, ocean, space
Electron density
Electron precipitation
Electrons
Exact sciences and technology
External geophysics
Fluctuations
Geophysics
hydroxyl
Ionization
Mathematical models
mesosphere
Meteorology
Ozone
Ozone depletion
Physics of the high neutral atmosphere
Satellite observation
Solar protons
Spectra
title Comparison of modeled and observed effects of radiation belt electron precipitation on mesospheric hydroxyl and ozone
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