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scostep 2010 (stp12) - Leibniz-Institut für Atmosphärenphysik an der ...

scostep 2010 (stp12) - Leibniz-Institut für Atmosphärenphysik an der ...

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STP12 Abstracts<br />

Berlin, 12 - 16 July <strong>2010</strong><br />

SCOSTEP Symposium <strong>2010</strong><br />

A 3D magneto-hydrodynamic model of solar prominences<br />

Aiouaz Tayeb, Toeroek Tibor<br />

We aim to model a solar prominence embedded in the upper solar atmosphere taking in<br />

account a fully 3D magnetic field, realistic thermodynamics, <strong>an</strong>d energy sources, using a 3D<br />

MHD simulation. As initial condition for the magnetic field we use the <strong>an</strong>alytical model of a<br />

bipolar active region by Titov & Demoulin (1999). This approximate force-free equilibrium<br />

consist of <strong>an</strong> arched <strong>an</strong>d twisted magnetic flux tube embedded into <strong>an</strong> ambient potential field.<br />

This magnetic configuration contains "dips", i.e., locations where the field lines are concave<br />

upward (U-shaped) <strong>an</strong>d c<strong>an</strong> carry dense plasma against gravity. The thermodynamic model<br />

contains as initial condition a hydrostatic, pressure-bal<strong>an</strong>ced atmosphere that sp<strong>an</strong>s from the<br />

high chromosphere through the tr<strong>an</strong>sition region to the solar corona. The energy equation<br />

includes radiative losses (Rosner, 1978), thermal conduction along the magnetic field<br />

(Spitzer, 1962), electric current dissipation, <strong>an</strong>d <strong>an</strong> ad-hoc heating function for the corona<br />

(Serio et al, 1981).<br />

Due to the spurious forces present in the magnetic field <strong>an</strong>d the response of the atmosphere,<br />

the system develops a complex dynamic behavior from the very beginning of the simulation.<br />

The source terms of the energy equation seek to bal<strong>an</strong>ce each other given the constraints<br />

imposed by the magnetic field. This evolution results in evaporation of chromospheric<br />

plasma that is expected to trigger a thermal instability <strong>an</strong>d plasma condensation in the<br />

ongoing simulation, i.e., the formation of prominence material.

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