{ "id": "1704.01993", "version": "v1", "published": "2017-04-06T19:24:37.000Z", "updated": "2017-04-06T19:24:37.000Z", "title": "Global Energetics of Solar Flares: VI. Refined Energetics of Coronal Mass Ejections", "authors": [ "Markus J. Aschwanden" ], "comment": "31 pages, 10 Figures", "categories": [ "astro-ph.SR" ], "abstract": "In this study we refine a CME model presented in an earlier study on the global energetics of solar flares and associated CMEs, and apply it to all (860) GOES M- and X-class flare events observed during the first 7 years (2010-2016) of the Solar Dynamics Observatory (SDO) mission, which doubles the statistics of the earlier study. The model refinements include: (1) the CME geometry in terms of a 3D sphere undergoing self-similar adiabatic expansion; (2) the inclusion of solar gravitational deceleration during the acceleration and propagation of the CME, which discriminates eruptive and confined CMEs; (4) a self-consistent relationship between the CME center-of-mass motion detected during EUV dimming and the leading-edge motion observed in white-light coronagraphs; (5) the equi-partition of the CME kinetic and thermal energy; and (6) the Rosner-Tucker-Vaiana (RTV) scaling law. The refined CME model is entirely based on EUV dimming observations (using AIA/SDO data) and complements the traditional white-light scattering model (using LASCO/SOHO data), and both models are independently capable to determine fundamental CME parameters such as the CME mass, speed, and energy. Comparing the two methods we find that: (1) LASCO is less sensitive than AIA in detecting CMEs (in 24$\\%$ of the cases); (2) CME masses below $m_{cme} \\sim 10^{14}$ g are under-estimated by LASCO; (3) AIA and LASCO masses, speeds, and energy agree closely in the statistical mean after elimination of outliers; (4) the CMEs parameters of the speed $v$, emission measure-weighted flare peak temperature $T_e$, and length scale $L$ are consistent with the following scaling laws (derived from first principles): $v \\propto T_e^{1/2}$, $v \\propto (m_{cme})^{1/4}$, and $m_{cme} \\propto L^2$.", "revisions": [ { "version": "v1", "updated": "2017-04-06T19:24:37.000Z" } ], "analyses": { "keywords": [ "coronal mass ejections", "global energetics", "solar flares", "sphere undergoing self-similar adiabatic", "refined energetics" ], "note": { "typesetting": "TeX", "pages": 31, "language": "en", "license": "arXiv", "status": "editable" } } }