Please use this identifier to cite or link to this item: http://nopr.niscpr.res.in/handle/123456789/38081
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dc.contributor.authorMahajan, K. K.-
dc.contributor.authorKumari, Sudesh-
dc.date.accessioned2016-12-02T06:58:09Z-
dc.date.available2016-12-02T06:58:09Z-
dc.date.issued1972-09-
dc.identifier.issn0975-105X (Online); 0367-8393 (Print)-
dc.identifier.urihttp://nopr.niscair.res.in/handle/123456789/38081-
dc.description211-213en_US
dc.description.abstractExperimentally observed electron concentration, electron temperature and ion temperature profiles for ionospheric conditions, corresponding to low and middle latitudes, are used to calculate the electron cooling rates arising from the two major cooling mechanisms in the F2-region, namely the electron.ion collisions and the electron impact-induced transitions among the fine structure levels of atomic oxygen. When electron concentration is low, the cooling due, to fine structure excitation of atomic oxygen dominates and conversely, when electron concentration is high the cooling due to oxygen ions dominates. For midlatitudes the electron concentration rarely exceeds 5 x 105/cm3 and so, for these latitudes, the dominant cooling mechanism is the fine structure excitation of atomic oxygen. For low latitudes, the electron concentration is generally more than 6 x 105/cm3 and thus, the electron-ion collisions become the dominant cooling mechanism.en_US
dc.language.isoen_USen_US
dc.publisherNISCAIR-CSIR, Indiaen_US
dc.rights CC Attribution-Noncommercial-No Derivative Works 2.5 Indiaen_US
dc.sourceIJRSP Vol.01(3) [September 1972]en_US
dc.titleElectron Cooling in the, F2-Region at Low & Middle Latitudesen_US
dc.typeArticleen_US
Appears in Collections:IJRSP Vol.01(3) [September 1972]

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