A Model for Bright Extreme‐Ultraviolet Knots in Solar Flare Loops

2004 ◽  
Vol 614 (2) ◽  
pp. 1022-1027 ◽  
Author(s):  
S. Patsourakos ◽  
S. K. Antiochos ◽  
J. A. Klimchuk
2019 ◽  
Vol 877 (1) ◽  
pp. L11 ◽  
Author(s):  
Wenzhi Ruan ◽  
Chun Xia ◽  
Rony Keppens

2012 ◽  
Vol 748 (1) ◽  
pp. L14 ◽  
Author(s):  
Ryan O. Milligan ◽  
Phillip C. Chamberlin ◽  
Hugh S. Hudson ◽  
Thomas N. Woods ◽  
Mihalis Mathioudakis ◽  
...  

1973 ◽  
Vol 180 ◽  
pp. 285 ◽  
Author(s):  
Robert D. Cowan ◽  
Kenneth G. Widing

1999 ◽  
Vol 527 (2) ◽  
pp. 945-957 ◽  
Author(s):  
Vahe Petrosian ◽  
Timothy Q. Donaghy

2019 ◽  
Vol 9 ◽  
pp. A43 ◽  
Author(s):  
Edward M. B. Thiemann ◽  
Francis G. Eparvier ◽  
Don Woodraska ◽  
Phillip C. Chamberlin ◽  
Janet Machol ◽  
...  

The Geostationary Operational Environmental Satellite R (GOES-R) series of four satellites are the next generation NOAA GOES satellites. Once on orbit and commissioned, they are renamed GOES 16–19, making critical terrestrial and space weather measurements through 2035. GOES 16 and 17 are currently on orbit, having been launched in 2016 and 2018, respectively. The GOES-R satellites include the Extreme Ultraviolet (EUV) and X-ray Irradiance Sensors (EXIS) instrument suite, which measures calibrated solar irradiance in eight lines or bands between 25 nm and 285 nm with the Extreme Ultraviolet Sensors (EUVS) instrument. EXIS also includes the X-Ray Sensor (XRS) instrument, which measures solar soft X-ray irradiance at the legacy GOES bands. The EUVS Measurements are used as inputs to the EUVS Model, a solar spectral irradiance model for space weather operations that predicts irradiance in twenty-two 5 nm wide intervals from 5 nm to 115 nm, and one 10 nm wide interval from 117 to 127 nm at 30 s cadence. Once fully operational, NOAA will distribute the EUVS Model irradiance with 1 min latency as a primary space weather data product, ushering in a new era of rapid dissemination and measurement continuity of EUV irradiance spectra. This paper describes the EUVS Model algorithms, data sources, calibration methods and associated uncertainties. Typical model (relative) uncertainties are less than ~5% for variability at time-scales longer than 6 h, and are ~25% for solar flare induced variability. The absolute uncertainties, originating from the instruments used to calibrate the EUVS Model, are ~10%. Examples of model results are presented at both sub-daily and multi-year timescales to demonstrate the model’s capabilities and limitations. Example solar flare irradiances are also modeled.


2017 ◽  
Vol 604 ◽  
pp. A76 ◽  
Author(s):  
Sophie Masson ◽  
Étienne Pariat ◽  
Gherardo Valori ◽  
Na Deng ◽  
Chang Liu ◽  
...  

Context. The dynamics of ultraviolet (UV) emissions during solar flares provides constraints on the physical mechanisms involved in the trigger and the evolution of flares. In particular it provides some information on the location of the reconnection sites and the associated magnetic fluxes. In this respect, confined flares are far less understood than eruptive flares generating coronal mass ejections. Aims. We present a detailed study of a confined circular flare dynamics associated with three UV late phases in order to understand more precisely which topological elements are present and how they constrain the dynamics of the flare. Methods. We perform a non-linear force-free field extrapolation of the confined flare observed with the Helioseismic and Magnetic Imager (HMI) and Atmospheric Imaging Assembly (AIA) instruments on board Solar Dynamics Observatory (SDO). From the 3D magnetic field we compute the squashing factor and we analyse its distribution. Conjointly, we analyse the AIA extreme ultraviolet (EUV) light curves and images in order to identify the post-flare loops, and their temporal and thermal evolution. By combining the two analyses we are able to propose a detailed scenario that explains the dynamics of the flare. Results. Our topological analysis shows that in addition to a null-point topology with the fan separatrix, the spine lines and its surrounding quasi-separatix layer (QSL) halo (typical for a circular flare), a flux rope and its hyperbolic flux tube (HFT) are enclosed below the null. By comparing the magnetic field topology and the EUV post-flare loops we obtain an almost perfect match between the footpoints of the separatrices and the EUV 1600 Å ribbons and between the HFT field line footpoints and bright spots observed inside the circular ribbons. We show, for the first time in a confined flare, that magnetic reconnection occurred initially at the HFT below the flux rope. Reconnection at the null point between the flux rope and the overlying field is only initiated in a second phase. In addition, we showed that the EUV late phase observed after the main flare episode is caused by the cooling loops of different length which have all reconnected at the null point during the impulsive phase. Conclusions. Our analysis shows in one example that flux ropes are present in null-point topology not only for eruptive and jet events, but also for confined flares. This allows us to conjecture on the analogies between conditions that govern the generation of jets, confined flares or eruptive flares.


2004 ◽  
Vol 601 (1) ◽  
pp. 565-569 ◽  
Author(s):  
F. P. Keenan ◽  
A. C. Katsiyannis ◽  
K. G. Widing

Solar Physics ◽  
2010 ◽  
Vol 263 (1-2) ◽  
pp. 163-174 ◽  
Author(s):  
I. V. Zimovets ◽  
A. B. Struminsky

Sign in / Sign up

Export Citation Format

Share Document