Magnetic Field-Chromospheric Plasma Interaction and the Problem of the Braking Force in Surge Dynamics

1990 ◽  
pp. 435-437
Author(s):  
V. Dermendjiev
1990 ◽  
Vol 142 ◽  
pp. 435-437
Author(s):  
V. Dermendjiev

An important stage in the evolution of solar flares is the generation of a number of dynamic phenomena, greatly varying in size and velocity, but actually representing plasma ejections. They are responsible for the transport of mass and energy and are usually considered to be result of the development of local magnetic features accompanied by a magnetic energy increase in the solar atmosphere. One of these phenomena is the surge prominence. In this contribution, we propose a possible explanation for the nature of the braking force acting in the decelerated ascending phase of surge dynamics. The possibility of structuralization of the chromospheric plasma during surge formation and the plasma action on the external, colimating magnetic field is taken into account.


2017 ◽  
Vol 24 (6) ◽  
pp. 062312 ◽  
Author(s):  
Prem Pyari Tiwary ◽  
Swati Sharma ◽  
Ram Kishor Singh ◽  
Anju Kumari ◽  
V. R. Satsangi ◽  
...  

1968 ◽  
Vol 28 (5) ◽  
pp. 331-332
Author(s):  
J. Jančařik ◽  
V. Piffl ◽  
M. Seidl

2009 ◽  
Vol 27 (9) ◽  
pp. 3349-3365 ◽  
Author(s):  
S. Simon

Abstract. The plasma environment of Saturn's largest satellite Titan is known to be highly variable. Since Titan's orbit is located within the outer magnetosphere of Saturn, the moon can leave the region dominated by the magnetic field of its parent body in times of high solar wind dynamic pressure and interact with the thermalized magnetosheath plasma or even with the unshocked solar wind. By applying a three-dimensional hybrid simulation code (kinetic description of ions, fluid electrons), we study in real-time the transition that Titan's plasma environment undergoes when the moon leaves Saturn's magnetosphere and enters the supermagnetosonic solar wind. In the simulation, the transition between both plasma regimes is mimicked by a reversal of the magnetic field direction as well as a change in the composition and temperature of the impinging plasma flow. When the satellite enters the solar wind, the magnetic draping pattern in its vicinity is reconfigured due to reconnection, with the characteristic time scale of this process being determined by the convection of the field lines in the undisturbed plasma flow at the flanks of the interaction region. The build-up of a bow shock ahead of Titan takes place on a typical time scale of a few minutes as well. We also analyze the erosion of the newly formed shock front upstream of Titan that commences when the moon re-enters the submagnetosonic plasma regime of Saturn's magnetosphere. Although the model presented here is far from governing the full complexity of Titan's plasma interaction during a solar wind excursion, the simulation provides important insights into general plasma-physical processes associated with such a disruptive change of the upstream flow conditions.


2013 ◽  
Vol 25 (7) ◽  
pp. 1709-1714
Author(s):  
阿不都热苏力 Abudurexiti A ◽  
帕孜来提 Pazilaiti A ◽  
帕力哈提 Mijit F

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