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Magnetic Dissipation in the Photosphere and Heating of the Corona. Valentyna Abramenko Big Bear Solar Observatory and Alexei Pevtsov National Solar Observatory. Soft X-ray luminosity of the corona. Objects: Active regions near the center of the solar disk.
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Magnetic Dissipation in the Photosphere and Heating of the Corona Valentyna Abramenko Big Bear Solar Observatory and Alexei Pevtsov National Solar Observatory
Objects: Active regions near the center of the solar disk Objects: Active regions near the center of the solar disk ? CORONA PHOTOSPHERE Data: Yohkoh/SXT Data: Al 0.1 μm channel AlMgMn-sandwich channel Data: SOHO/MDI high resolution magnetograms • Analyzed Quantities: • Averaged (over an area) flux • in each channel • Temperature • Emission Measure • Analyzed Quantitiy: • Averaged (over an area) magnetic • energy dissipation rate
Structure of Magnetic Energy Dissipation Magnetic energy dissipation, ε/η Line-of-sight Magnetic Field, Bz
Flux density (Al.1) Flux density (AlMgMn) Magnetic dissipation versus averaged flux in Al.1 and AlMgMn channels
Magnetic dissipation versus temperature and emission measure
η = (150 ÷ 300) km2/s If we accept the effective thickness of the photosphere h = 500 km, the energy flux F=∫ εَ dh for different ARs varies in the range of F = (1 ÷ 14)×106 erg cm-2 s-1 Energy Flux Estimation Abramenko, Pevtsov, Romano,2006, ApJL 646
Bz Bz Vh Poynting Flux vs X-ray Flux:area-averaged values Follow-up study: Tan, Jing, Abramenko, Pevtsov, Song, Park, Haimin Wang, 2007 ApJ, accepted Poynting Flux ~ Bh Bz Vh
Poynting Flux vs X-ray Flux:area-integrated values Follow-up study: Tan, Jing, Abramenko, Pevtsov, Song, Park, Haimin Wang, 2007 ApJ, accepted
Conclusions • Energy input due to the random motions strongly correlates with brightness, temperature and emission measure of the corona. • Energy flux is (1 ÷ 14)×106 erg cm-2 s-1, which is quite sufficient to heat the corona above ARs. • Magnetic diffusivity in ARs is (150 ÷ 300) km2/s, which is twice lower than in QS areas.
Index of the magnetic power spectrum versus averaged flux in Al.1 and AlMgMn channels