dc.contributor.author |
Gokhale, M. H |
|
dc.date.accessioned |
2010-02-24T11:04:04Z |
|
dc.date.available |
2010-02-24T11:04:04Z |
|
dc.date.issued |
1979-11 |
|
dc.identifier.citation |
Kodaikanal Observatory Bulletins Series A, Vol. 2, No. 3, pp 222–223 |
en |
dc.identifier.issn |
0374-3632 |
|
dc.identifier.uri |
http://hdl.handle.net/2248/5031 |
|
dc.description.abstract |
The two component nature of the solar activity cycle as resulting from the shock-transition model of the solar magnetic cycle, provides for a correlation between a measure of coronal hole formations during the ending years of one solar cycle and the maximum annual sunspot number R/submax of the next cycle. This might account for the observed correlation between the geomagnetic activity during the last few years of one cycle and the R/submax of the next cycle. |
en |
dc.language.iso |
en |
en |
dc.publisher |
Indian Institute of Astrophysics |
en |
dc.rights |
© Indian Institute of Astrophysics |
en |
dc.subject |
Solar Cycle |
en |
dc.subject |
Solar Magnetic Fields |
en |
dc.subject |
Geomagnetic Activity |
en |
dc.subject |
Solar Cycle Theory |
en |
dc.title |
Why is geomagnetic activity during the ending years of a solar cycle well correlated to the maximum of the next cycle? |
en |
dc.type |
Article |
en |