Abstract

Abstract. A new, empirical model for NO densities is developed, to include physically reasonable variations with local time, season, latitude and solar cycle. Model calculations making full allowance for secondary production, and ionising radiations at wavelengths down to 25 Å, then give values for the peak density NmE that are only 6% below the empirical IRI values for summer conditions at solar minimum. At solar maximum the difference increases to 16%. Solar-cycle changes in the EUVAC radiation model seem insufficient to explain the observed changes in NmE, with any reasonable modifications to current atmospheric constants. Hinteregger radiations give the correct change, with results that are just 2% below the IRI values throughout the solar cycle, but give too little ionisation in the E-F valley region. To match the observed solar increase in NmE, the high-flux reference spectrum in the EUVAC model needs an overall increase of about 20% (or 33% if the change is confined to the less well defined radiations at λ < 150 Å). Observed values of NmE show a seasonal anomaly, at mid-latitudes, with densities about 10% higher in winter than in summer (for a constant solar zenith angle). Composition changes in the MSIS86 atmospheric model produce a summer-to-winter change in NmE of about –2% in the northern hemisphere, and +3% in the southern hemisphere. Seasonal changes in NO produce an additional increase of about 5% in winter, near solar minimum, to give an overall seasonal anomaly of 8% in the southern hemisphere. Near solar maximum, reported NO densities suggest a much smaller seasonal change that is insufficient to produce any winter increase in NmE. Other mechanisms, such as the effects of winds or electric fields, seem inadequate to explain the observed change in NmE. It therefore seems possible that current satellite data may underestimate the mean seasonal variation in NO near solar maximum. A not unreasonable change in the data, to give the same 2:1 variation as at solar minimum, can produce a seasonal anomaly in NmE that accounts for 35–70% of the observed effect at all times.

Highlights

  • In recent years it has become possible to model, with reasonable accuracy, most of the processes involved in the formation of the ionosphere

  • In both the EUVAC and Hinteregger radiation models, the the EUV fluxes are average value noovef rthaendainiltyerFval oifn8d1exdaanyds centred on the current date

  • An increase of 20% in the solar maximum reference spectrum used in the EUVAC shown by the broken model line in

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Summary

Introduction

In recent years it has become possible to model, with reasonable accuracy, most of the processes involved in the formation of the ionosphere. Ionosphere model IRI-90 (Bilitza, 1990) This model uses analytic expressions that have been fitted to a large amount of monthly median data, to best reproduce mean observed values of ion density at different heights. It gives results obtained by values Kouris aonf dNMKEugcgolertroensp(o1n97d3inag, bt)ofrothme an extended study of monthly median values of foE, for each hour between 0900 and 1500, from 45 sites spaced around the globe, and covering a full 11-year solar cycle

The modelling program
The production and loss of NO
A high-latitude model
Diurnal variations
Changes with height
Ion composition
Electron density
Changes with solar flux
Seasonal changes
Conclusions
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