Ionopspheric propagation of magnetohydrodynamic disturbances from the equatorial electrojet

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dc.contributor.author Fedorov, E.
dc.contributor.author Pilipenko, V.
dc.contributor.author Surkov, V.
dc.contributor.author Rao, D.R.K.
dc.contributor.author Yamuto, K.
dc.date.accessioned 2015-05-14T10:02:11Z
dc.date.accessioned 2021-02-12T09:22:32Z
dc.date.available 2015-05-14T10:02:11Z
dc.date.available 2021-02-12T09:22:32Z
dc.date.issued 1999
dc.identifier.citation JGR, v.104/A3, p.4329-4336, 1999. en_US
dc.identifier.uri http://localhost:8080/xmlui/handle/123456789/73
dc.description.abstract The propagation features of magnetohydrodynamic (MHD) disturbances along the ionosphere are considered from a theoretical point of view. Special attention is paid to the possibility of ionospheric propagation of disturbances produced by variations in the equatorial electrojet. The possible MHD modes within the E layer include oscillations that have damping scales of about effective ionospheric skin depth or less. The existence of a large-scale compressional surface mode at small inclinations of the geomagnetic field along the E layer is shown. The propagation of this mode, called the gyrotropic surface mode, takes place in a diffusive-like way along the E layer. Its damping scale is much greater than the ionospheric skin depth, and it may reach several hundred to thousand kilometers. The apparent propagation velocity of the gyrotropic mode at the near-equatorial latitudes is determined by height-integrated Cowling conductivity; its value is estimated to be about 20 – 100 km/s for the Pc3–4 frequency range. We suggest that the equatorial electrojet may contribute to the ULF geomagnetic variations observed at near-equatorial stations. en_US
dc.language.iso en en_US
dc.subject Magnetohydrodynamic en_US
dc.subject Equatorial electrojet en_US
dc.subject Ionospspheric en_US
dc.title Ionopspheric propagation of magnetohydrodynamic disturbances from the equatorial electrojet en_US
dc.type Article en_US
dc.identifier.accession 090562


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