Lunar and luni-solar variations of the geomagnetic field in the Indian region

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dc.contributor.author Rao, D.R.K.
dc.date.accessioned 2015-05-19T11:05:01Z
dc.date.accessioned 2021-02-12T09:21:05Z
dc.date.available 2015-05-19T11:05:01Z
dc.date.available 2021-02-12T09:21:05Z
dc.date.issued 1972
dc.identifier.citation Pure and Applied Geophysics, v.95/1, p.131-140, 1972, doi: 10.1007/BF00878861 en_US
dc.identifier.uri http://localhost:8080/xmlui/handle/123456789/109
dc.description.abstract Lunar and luni-solar geomagnetic components have been computed upto four harmonics for low latitude station Alibag, outside equatorial electrojet belt, and the equatorial electrojet stations Annamalainagar, Kodaikanal and Trivandrum in the south Indian region. The computations are confined to data of very high solar activity period 1958–61. Amplitudes of lunar semidiurnal component (L 2), in the horizontal intensity (H), undergo an equatorial enhancement. Phase difference of 2 hrs is noticed inL 2 (H) between nonelectrojet and electrojet stations. In the vertical intensity (Z), L 2 is maximum ine andj-seasons at Trivandrum, close to the magnetic equator. Ind-season, however, maximumL 2 (Z) occurs at Annamalainagar (dip 5°.4N). The phase difference between the electrojet and nonelectrojet stations observed inL 2 (H) is not noticed inL 2 (Z). The differential vertical upward drift motion of charged particles may explain the observed phase difference inL 2 (H). Seasonal variations in amplitudes and times of maxima are noticed at all the stations inL 2 (H) andL 2 (Z). Similar variation is also noticed at Alibag inL 2 of declination (D). en_US
dc.language.iso en en_US
dc.subject Geomagnetic field en_US
dc.subject Equatorial electrojet en_US
dc.subject Geomagnetic components en_US
dc.subject Luni-solar geomagnetic en_US
dc.subject Lunar geomagnetic en_US
dc.title Lunar and luni-solar variations of the geomagnetic field in the Indian region en_US
dc.type Article en_US
dc.identifier.accession 090602


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