1960
DOI: 10.1016/0021-9169(60)90081-7
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The equatorial F-region of the ionosphere

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Cited by 170 publications
(91 citation statements)
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“…Each of these effects has different weight depending on the geomagnetic/geographic location, solar and geomagnetic activity, season and local time. While production is mainly controlled by solar EUV radiation, transport at the low latitude region is dominated by the equatorial fountain effect (Appleton 1946;Martyn 1955;Duncan 1959;Ross 1966;Das Gupta & Basu 1973;Richmond et al 1976;Balan et al 1993;Doherty et al 2000). The electron production by photo-ionization of neutral atoms and molecules is proportional to the intensity of solar radiation, governed by the Beer Lambert law.…”
Section: Model Developmentmentioning
confidence: 99%
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“…Each of these effects has different weight depending on the geomagnetic/geographic location, solar and geomagnetic activity, season and local time. While production is mainly controlled by solar EUV radiation, transport at the low latitude region is dominated by the equatorial fountain effect (Appleton 1946;Martyn 1955;Duncan 1959;Ross 1966;Das Gupta & Basu 1973;Richmond et al 1976;Balan et al 1993;Doherty et al 2000). The electron production by photo-ionization of neutral atoms and molecules is proportional to the intensity of solar radiation, governed by the Beer Lambert law.…”
Section: Model Developmentmentioning
confidence: 99%
“…It may be mentioned that TEC is a height-integrated parameter and is weighted mostly by the electrons in the F-regions, with 2/3rd of the contribution coming from regions above the altitude of the F-region peak. The vertical E · B drift of plasma driven by the orthogonal configuration of the geomagnetic field (B) and zonal electric field (E) over the magnetic equator, and subsequent diffusion along the geomagnetic field lines due to gravitational and pressure gradient forces lead to the development of the EIA (Martyn 1955;Duncan 1959). The EIA is a double humped structure in the latitudinal distribution of the ionization at low magnetic latitudes.…”
Section: Model Developmentmentioning
confidence: 99%
“…Since the geomagnetic ®eld lines passing through the F-layer crests (at about 15°±20°magnetic latitude) cross the equator at about 800±1000 km height, where the production rate q is small, some other source of plasma seems necessary. Martyn (1947) and Duncan (1960) envisaged that the plasma comes from lower levels in the F2-layer; it is lifted to great heights by the eastward electric ®elds that exist in low latitudes by day, and then diuses downward along ®eld lines, as Mitra (1946) suggested. As Kendall and Pickering (1967) say,``The electron-ion pairs may be thought of as sliding down the magnetic ®eld lines with a diusive motion, while at the same time the whole ®eld line drifts at right angles to itself.''…”
Section: The Equatorial Fountainmentioning
confidence: 99%
“…This is popularly known as the "Fountain Effect." The various aspects of equatorial anomaly have been studied quite extensively both experimentally and theoretically (RASTOGI, 1959(RASTOGI, , 1966RASTOGI and RAJARAM, 1971;DUNCAN, 1960;LYON, 1963;MOFFETT and HANSON, 1965;BRAMLEY and PEART, 1965;HANSON and MOFFETT, 1966;ANDERSON, 1971;RAJARAM and RASTOGI, 1974; Rotation measurements, which give ionospheric Total Electron Content (TEC), are being widely used for ionospheric studies. Latitudinal variation of TEC has been studied by various workers (BASU and DAS GUPTA, 1968;TITHERIDGE and SMITH, 1969;MENDONCA et al, 1969;GOLTON and WALKER, 1971;RASTOGI et al, 1973RASTOGI et al, , 1975IYER et al, 1976).…”
mentioning
confidence: 99%