Abstract

Abstract. The companion paper by Zou et al. shows that the annual and semiannual variations in the peak F2-layer electron density (NmF2) at midlatitudes can be reproduced by a coupled thermosphere-ionosphere computational model (CTIP), without recourse to external influences such as the solar wind, or waves and tides originating in the lower atmosphere. The present work discusses the physics in greater detail. It shows that noon NmF2 is closely related to the ambient atomic/molecular concentration ratio, and suggests that the variations of NmF2 with geographic and magnetic longitude are largely due to the geometry of the auroral ovals. It also concludes that electric fields play no important part in the dynamics of the midlatitude thermosphere. Our modelling leads to the following picture of the global three-dimensional thermospheric circulation which, as envisaged by Duncan, is the key to explaining the F2-layer variations. At solstice, the almost continuous solar input at high summer latitudes drives a prevailing summer-to-winter wind, with upwelling at low latitudes and throughout most of the summer hemisphere, and a zone of downwelling in the winter hemisphere, just equatorward of the auroral oval. These motions affect thermospheric composition more than do the alternating day/night (up-and-down) motions at equinox. As a result, the thermosphere as a whole is more molecular at solstice than at equinox. Taken in conjunction with the well-known relation of F2-layer electron density to the atomic/molecular ratio in the neutral air, this explains the F2-layer semiannual effect in NmF2 that prevails at low and middle latitudes. At higher midlatitudes, the seasonal behaviour depends on the geographic latitude of the winter downwelling zone, though the effect of the composition changes is modified by the large solar zenith angle at midwinter. The zenith angle effect is especially important in longitudes far from the magnetic poles. Here, the downwelling occurs at high geographic latitudes, where the zenith angle effect becomes overwhelming and causes a midwinter depression of electron density, despite the enhanced atomic/molecular ratio. This leads to a semiannual variation of NmF2. A different situation exists in winter at longitudes near the magnetic poles, where the downwelling occurs at relatively low geographic latitudes so that solar radiation is strong enough to produce large values of NmF2. This circulation-driven mechanism provides a reasonably complete explanation of the observed pattern of F2 layer annual and semiannual quiet-day variations. Key words: Atmospheric composition and structure (thermosphere-composition and chemistry) - Ionosphere (mid-latitude ionosphere; modelling and forecasting)

Highlights

  • The preceding work by Zou et al (2000), here called Paper I, gives details of the use of the coupled thermosphere±ionosphere±plasmasphere model CTIP (Fuller-Rowell et al, 1996; Millward et al, 1996b) to investigate the global morphology of the quiet F2-layer at midlatitudes

  • As in Paper I, we refer tonear-pole'' andfar-from-pole'' longitude sectors (``pole'' here meaning magnetic pole), and denote zones of latitude as follows: Equatorial: the zone within about 20° of the magnetic equator, in which F2-layer behaviour is strongly inuenced by the low-latitude system of electric ®elds; Midlatitudes: zones between magnetic equatorial zone and auroral ovals, divided at roughly 45° magnetic latitude intolower'' andhigher'' midlatitudes; Auroral ovals: belts 10°±15° wide, the low latitude boundary being at about 75° magnetic latitude at noon, and 66° magnetic latitude at midnight; Polar caps: regions poleward of the auroral ovals

  • We examine in more detail how the composition varies with latitude throughout the year, as a step towards developing an overall description of the quietday thermospheric circulation

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Summary

The Modelling

The preceding work by Zou et al (2000), here called Paper I, gives details of the use of the coupled thermosphere±ionosphere±plasmasphere model CTIP (Fuller-Rowell et al, 1996; Millward et al, 1996b) to investigate the global morphology of the quiet F2-layer at midlatitudes. Most runs include middle/low-latitude electric ®elds as given by the model of Richmond et al (1980), H. Rishbeth et al.: Annual and semiannual variations in the ionospheric F2-layer though some omit these electric ®elds.

Theory
Complications
An overall description of the thermospheric circulation
Zonal averages of the composition P-parameter
The meridional circulation at solstice
The circulation at equinox
The time constant s
Time scale of seasonal changes
Semiannual variations of the neutral thermosphere?
Electron density and neutral composition
Six possible explanations of annual and semiannual variations of NmF2
Findings
The annual variation
Conclusion
Full Text
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