scholarly journals Solar chromosphere heating and generation of plasma outflows by impulsively generated two-fluid Alfvén waves

Author(s):  
M. Pelekhata ◽  
K. Murawski ◽  
S. Poedts
2014 ◽  
Vol 573 ◽  
pp. A79 ◽  
Author(s):  
R. Soler ◽  
J. L. Ballester ◽  
T. V. Zaqarashvili

1996 ◽  
Vol 3 (8) ◽  
pp. 2879-2884 ◽  
Author(s):  
De‐Jin Wu ◽  
Guang‐Li Huang ◽  
De‐Yu Wang ◽  
Carl‐Gunne Fälthammar

2020 ◽  
Vol 639 ◽  
pp. A45
Author(s):  
B. Kuźma ◽  
D. Wójcik ◽  
K. Murawski ◽  
D. Yuan ◽  
S. Poedts

Context. We present new insight into the long-standing problem of plasma heating in the lower solar atmosphere in terms of collisional dissipation caused by two-fluid Alfvén waves. Aims. Using numerical simulations, we study Alfvén wave propagation and dissipation in a magnetic flux tube and their heating effect. Methods. We set up 2.5-dimensional numerical simulations with a semi-empirical model of a stratified solar atmosphere and a force-free magnetic field mimicking a magnetic flux tube. We consider a partially ionized plasma consisting of ion + electron and neutral fluids, which are coupled by ion-neutral collisions. Results. We find that Alfvén waves, which are directly generated by a monochromatic driver at the bottom of the photosphere, experience strong damping. Low-amplitude waves do not thermalize sufficient wave energy to heat the solar atmospheric plasma. However, Alfvén waves with amplitudes greater than 0.1 km s−1 drive through ponderomotive force magneto-acoustic waves in higher atmospheric layers. These waves are damped by ion-neutral collisions, and the thermal energy released in this process leads to heating of the upper photosphere and the chromosphere. Conclusions. We infer that, as a result of ion-neutral collisions, the energy carried initially by Alfvén waves is thermalized in the upper photosphere and the chromosphere, and the corresponding heating rate is large enough to compensate radiative and thermal-conduction energy losses therein.


1986 ◽  
Vol 91 (A3) ◽  
pp. 2950 ◽  
Author(s):  
Ruth Esser ◽  
Egil Leer ◽  
Shadia R. Habbal ◽  
George L. Withbroe

1994 ◽  
Vol 423 ◽  
pp. 500 ◽  
Author(s):  
Ornulf Sandbaek ◽  
Egil Leer

1997 ◽  
Vol 58 (3) ◽  
pp. 433-440 ◽  
Author(s):  
GUANG-LI HUANG ◽  
REN-YING WANG

On the basis of a two-fluid, cold-plasma, linear stability calculation with linear friction between electrons and ions, the growth rate of Alfvén waves is derived from the dispersion relation for a uniformly magnetized plasma, in which the plasma resistivity and a uniform electric current carried by an electron beam are both considered. The growth rate is directly proportional to the plasma resistivity, the electric current density and the value of the parameter ωxpe/Ωe (where ωxpe and Ωe are the electron plasma and cyclotron frequency respectively). Moreover, the growth of Alfvén waves is mainly excited in a direction nearly parallel to the ambient magnetic field. The critical value of the velocity of the electron fluid is just equal to the Alfvén velocity. The results of this paper are compared with those for the linear tearing mode.


2005 ◽  
Vol 442 (3) ◽  
pp. 1091-1098 ◽  
Author(s):  
J. E. Leake ◽  
T. D. Arber ◽  
M. L. Khodachenko

2013 ◽  
Vol 767 (2) ◽  
pp. 171 ◽  
Author(s):  
R. Soler ◽  
M. Carbonell ◽  
J. L. Ballester ◽  
J. Terradas

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