Tracing magnetic helicity from the solar corona to the interplanetary space

2005 ◽  
Vol 67 (17-18) ◽  
pp. 1734-1743 ◽  
Author(s):  
M.L. Luoni ◽  
C.H. Mandrini ◽  
Sergio Dasso ◽  
L. van Driel-Gesztelyi ◽  
P. Démoulin
2018 ◽  
Vol 613 ◽  
pp. A27 ◽  
Author(s):  
Shangbin Yang ◽  
Jörg Büchner ◽  
Jan Skála ◽  
Hongqi Zhang

Context. For a better understanding of the dynamics of the solar corona, it is important to analyse the evolution of the helicity of the magnetic field. Since the helicity cannot be directly determined by observations, we have recently proposed a method to calculate the relative magnetic helicity in a finite volume for a given magnetic field, which however required the flux to be balanced separately on all the sides of the considered volume. Aims. We developed a scheme to obtain the vector potential in a volume without the above restriction at the boundary. We studied the dissipation and escape of relative magnetic helicity from an active region. Methods. In order to allow finite magnetic fluxes through the boundaries, a Coulomb gauge was constructed that allows for global magnetic flux balance. The property of sinusoidal function was used to obtain the vector potentials at the 12 edges of the considered rectangular volume extending above an active region. We tested and verified our method in a theoretical fore-free magnetic field model. Results. We applied the new method to the former calculation data and found a difference of less than 1.2%. We also applied our method to the magnetic field above active region NOAA 11429 obtained by a new photospheric-data-driven magnetohydrodynamics (MHD) model code GOEMHD3. We analysed the magnetic helicity evolution in the solar corona using our new method. We find that the normalized magnetic helicity (H∕Φ2) is equal to −0.038 when fast magnetic reconnection is triggered. This value is comparable to the previous value (−0.029) in the MHD simulations when magnetic reconnection happened and the observed normalized magnetic helicity (−0.036) from the eruption of newly emerging active regions. We find that only 8% of the accumulated magnetic helicity is dissipated after it is injected through the bottom boundary. This is in accordance with the Woltjer conjecture. Only 2% of the magnetic helicity injected from the bottom boundary escapes through the corona. This is consistent with the observation of magnetic clouds, which could take magnetic helicity into the interplanetary space. In the case considered here, several halo coronal mass ejections (CMEs) and two X-class solar flares originate from this active region.


2000 ◽  
Vol 179 ◽  
pp. 177-183
Author(s):  
D. M. Rust

AbstractSolar filaments are discussed in terms of two contrasting paradigms. The standard paradigm is that filaments are formed by condensation of coronal plasma into magnetic fields that are twisted or dimpled as a consequence of motions of the fields’ sources in the photosphere. According to a new paradigm, filaments form in rising, twisted flux ropes and are a necessary intermediate stage in the transfer to interplanetary space of dynamo-generated magnetic flux. It is argued that the accumulation of magnetic helicity in filaments and their coronal surroundings leads to filament eruptions and coronal mass ejections. These ejections relieve the Sun of the flux generated by the dynamo and make way for the flux of the next cycle.


1959 ◽  
Vol 9 ◽  
pp. 3-7
Author(s):  
F. G. Smith

Radio astronomy has been expanding into outer space so fast in recent years that it is pleasant to find our own solar system at last receiving the attention it deserves. In this session we are concerned with everything within the system except the sun and our own planet. I start with a question, to which I shall return later: Where does the sun end? In another session you will hear of the experiments on the far-out parts of the solar corona; here we are concerned with interplanetary space as well as with the planets themselves, and what lies within this region may or may not be considered part of the solar corona.


2009 ◽  
Vol 706 (1) ◽  
pp. 238-243 ◽  
Author(s):  
D. Telloni ◽  
R. Bruno ◽  
V. Carbone ◽  
E. Antonucci ◽  
R. D'Amicis

2018 ◽  
Vol 856 (1) ◽  
pp. 86 ◽  
Author(s):  
Sudheer K. Mishra ◽  
Talwinder Singh ◽  
P. Kayshap ◽  
A. K. Srivastava

2003 ◽  
Vol 32 (10) ◽  
pp. 1917-1922 ◽  
Author(s):  
K. Kusano ◽  
T. Maeshiro ◽  
T. Yokoyama ◽  
T. Sakurai

2000 ◽  
Vol 25 (9) ◽  
pp. 1973-1978 ◽  
Author(s):  
I.V. Chashei ◽  
A.I. Efimov ◽  
L.N. Samoznaev ◽  
M.K. Bird ◽  
M. Pätzold

2009 ◽  
Vol 5 (S264) ◽  
pp. 181-190
Author(s):  
Hongqi Zhang

AbstractThe helicity is an important quantity to present the basic topological configuration of magnetic field transferred form the solar subatmosphere into the interplanetary space. In this paper, we present the observational solar magnetic field and the relationship with the magnetic helicity.


1980 ◽  
Vol 91 ◽  
pp. 541-545
Author(s):  
H. Porsche ◽  
H. Volland ◽  
K. Bird ◽  
P. Edenhofer

The mission of HELIOS had been started in order to investigate in situ the innermost regions of the interplanetary space. The two spacecraft achieved a perihelion of about 0.3 AU solar distance. Fig. 1 is a sketch of the two orbits. The orbital periods are 190 resp. 186 d.


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