Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/3546
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dc.contributor.authorRaja, K. Sasikumaren_US
dc.contributor.authorSUBRAMANIAN, PRASADen_US
dc.contributor.authorRamesh, R.en_US
dc.contributor.authorVourlidas, Angelosen_US
dc.contributor.authorINGALE, MADHUSUDANen_US
dc.date.accessioned2019-07-01T05:55:59Z
dc.date.available2019-07-01T05:55:59Z
dc.date.issued2017-11en_US
dc.identifier.citationAstrophysical Journal, 850(2), 129.en_US
dc.identifier.issn0004-637Xen_US
dc.identifier.issn1538-4357en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/3546-
dc.identifier.urihttps://doi.org/10.3847/1538-4357/aa94cden_US
dc.description.abstractWe obtain scatter-broadened images of the Crab Nebula at 80 MHz as it transits through the inner solar wind in 2017 and 2016 June. These images are anisotropic, with the major axis oriented perpendicular to the radially outward coronal magnetic field. Using these data, we deduce that the density modulation index ($\delta {N}_{e}/{N}_{e}$) caused by turbulent density fluctuations in the solar wind ranges from $1.9\times {10}^{-3}$ to $7.7\times {10}^{-3}$ between 9 and 20 R ⊙. We also find that the heating rate of solar wind protons at these distances ranges from $2.2\times {10}^{-13}$ to $1.0\times {10}^{-11}\,\mathrm{erg}\,{\mathrm{cm}}^{-3}\,{{\rm{s}}}^{-1}$. On two occasions, the line of sight intercepted a coronal streamer. We find that the presence of the streamer approximately doubles the thickness of the scattering screen.en_US
dc.language.isoenen_US
dc.publisherIOP Publishingen_US
dc.subjectTurbulent Densityen_US
dc.subjectFluctuationsen_US
dc.subjectProton Heating Rateen_US
dc.subjectSolar Winden_US
dc.subject2017en_US
dc.titleTurbulent Density Fluctuations and Proton Heating Rate in the Solar Wind from 9–20 R ⊙en_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitleAstrophysical Journalen_US
dc.publication.originofpublisherForeignen_US
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