THE SPATIAL AND TEMPORAL DEPENDENCE OF CORONAL HEATING BY ALFVÉN WAVE TURBULENCE

The solar atmosphere may be heated by Alfven waves that propagate up from the convection zone and dissipate their energy in the chromosphere and corona. To further test this theory, we consider wave heating in an active region observed on 2012 March 7. A potential field model of the region is constructed, and 22 field lines representing observed coronal loops are traced through the model. Using a three-dimensional (3D) reduced magnetohydrodynamics code, we simulate the dynamics of Alfven waves in and near the observed loops. The results for different loops are combined into a single formula describing the average heating rate Q as a function of position within the observed active region. We suggest this expression may be approximately valid also for other active regions, and therefore may be used to construct 3D, time-dependent models of the coronal plasma. Such models are needed to understand the role of thermal non-equilibrium in the structuring and dynamics of the Sun's corona.

[1]  S. Cranmer,et al.  Self-consistent Coronal Heating and Solar Wind Acceleration from Anisotropic Magnetohydrodynamic Turbulence , 2007, astro-ph/0703333.

[2]  L. Burlaga Lognormal and multifractal distributions of the heliospheric magnetic field , 2001 .

[3]  L. R. V. D. Voort,et al.  Dynamics of the solar magnetic bright points derived from their horizontal motions , 2012, 1204.4362.

[4]  J. V. Hollweg Transition region, corona, and solar wind in coronal holes , 1986 .

[5]  Fabio Reale,et al.  Emission Measure Distribution in Loops Impulsively Heated at the Footpoints , 2004, astro-ph/0412482.

[6]  L. Golub,et al.  OBSERVATIONS AND MAGNETIC FIELD MODELING OF THE FLARE/CORONAL MASS EJECTION EVENT ON 2010 APRIL 8 , 2011 .

[7]  P. Démoulin,et al.  Magnetic Field and Plasma Scaling Laws: Their Implications for Coronal Heating Models , 2000 .

[8]  B. Pontieu,et al.  Alfvénic waves with sufficient energy to power the quiet solar corona and fast solar wind , 2011, Nature.

[9]  J. Linker,et al.  The Formation of Coronal Loops by Thermal Instability in Three Dimensions , 2008 .

[10]  R. Rosner,et al.  Dynamics of the quiescent solar corona , 1978 .

[11]  S. Tsuneta,et al.  PROPERTIES OF MAGNETOHYDRODYNAMIC WAVES IN THE SOLAR PHOTOSPHERE OBTAINED WITH HINODE , 2009, 0907.3025.

[12]  Turbulent Coronal Heating and the Distribution of Nanoflares , 1997, astro-ph/9705050.

[13]  K. Shibata,et al.  NONLINEAR PROPAGATION OF ALFVÉN WAVES DRIVEN BY OBSERVED PHOTOSPHERIC MOTIONS: APPLICATION TO THE CORONAL HEATING AND SPICULE FORMATION , 2010, 1001.4307.

[14]  J. Higdon Density fluctuations in the interstellar medium: evidence for anisotropic magnetogasdynamic turbulen , 1984 .

[15]  S. Antiochos,et al.  CAN THERMAL NONEQUILIBRIUM EXPLAIN CORONAL LOOPS? , 2009, 0912.0953.

[16]  S. Cranmer,et al.  HEATING OF THE SOLAR CHROMOSPHERE AND CORONA BY ALFVÉN WAVE TURBULENCE , 2011, 1105.0402.

[17]  P. Démoulin,et al.  The Long-Term Evolution of AR 7978: Testing Coronal Heating Models , 2003 .

[18]  S. Sridhar,et al.  Toward a theory of interstellar turbulence. 2. Strong Alfvenic turbulence , 1994 .

[19]  K. Shibata,et al.  THE ROLE OF TORSIONAL ALFVÉN WAVES IN CORONAL HEATING , 2009, 0910.0962.

[20]  USA,et al.  High-Resolution Observations and Modeling of Dynamic Fibrils , 2007, astro-ph/0701786.

[21]  W. Matthaeus,et al.  Linear transport of solar wind fluctuations , 1995 .

[22]  A. Lazarian,et al.  Simulations of Magnetohydrodynamic Turbulence in a Strongly Magnetized Medium , 2001, astro-ph/0105235.

[23]  A. A. van Ballegooijen,et al.  MODEL FOR ALFVÉN WAVE TURBULENCE IN SOLAR CORONAL LOOPS: HEATING RATE PROFILES AND TEMPERATURE FLUCTUATIONS , 2012 .

[24]  S. Sridhar,et al.  Magnetohydrodynamic Turbulence Revisited , 1997 .

[25]  Ashis Bhattacharjee,et al.  Random Scattering and Anisotropic Turbulence of Shear-Alfvén Wave Packets in the Interstellar Medium and the Solar Wind , 2000 .

[26]  L. Milano,et al.  A Reduced Magnetohydrodynamic Model of Coronal Heating in Open Magnetic Regions Driven by Reflected Low-Frequency Alfvén Waves , 2001 .

[27]  K. Shibata,et al.  Alfvén Wave Model of Spicules and Coronal Heating , 1999 .

[28]  M. Aschwanden,et al.  The Coronal Heating Mechanism as Identified by Full-Sun Visualizations , 2004 .

[29]  R. Ulrich Observations of Magnetohydrodynamic Oscillations in the Solar Atmosphere with Properties of Alfvén Waves , 1996 .

[30]  S. Antiochos,et al.  The Origin of High-Speed Motions and Threads in Prominences , 2006 .

[31]  P. Dmitruk,et al.  Statistical association of discontinuities and reconnection in magnetohydrodynamic turbulence , 2011 .

[32]  H. Ji,et al.  OBSERVATIONS AND NONLINEAR FORCE-FREE FIELD MODELING OF ACTIVE REGION 10953 , 2009 .

[33]  B. Pontieu,et al.  Chromospheric Alfvénic Waves Strong Enough to Power the Solar Wind , 2007, Science.

[34]  D. Müller,et al.  Dynamics of solar coronal loops I. Condensation in cool loops and its effect on transition region lines , 2003 .

[35]  S. Cranmer AN EFFICIENT APPROXIMATION OF THE CORONAL HEATING RATE FOR USE IN GLOBAL SUN–HELIOSPHERE SIMULATIONS , 2009, 0912.5333.

[36]  S. Antiochos,et al.  A model for the formation of solar prominences , 1991 .

[37]  A nanoflare model of quiet Sun EUV emission , 2006, astro-ph/0612585.

[38]  Caltech,et al.  Nonlinear Dynamics of the Parker Scenario for Coronal Heating , 2007, 0709.3687.

[39]  S. Tomczyk,et al.  TIME–DISTANCE SEISMOLOGY OF THE SOLAR CORONA WITH CoMP , 2009, 0903.2002.

[40]  T. Yokoyama,et al.  The Nonlinear Alfvén Wave Model for Solar Coronal Heating and Nanoflares , 2004 .

[41]  Harry P. Warren,et al.  Hydrodynamic Modeling of Active Region Loops , 2002 .

[42]  F. Malara,et al.  Modeling a Coronal Loop Heated by Magnetohydrodynamic Turbulence Nanoflares , 2005, astro-ph/0506694.

[43]  George L. Withbroe,et al.  Mass and Energy Flow in the Solar Chromosphere and Corona , 1977 .

[44]  M. Kundu,et al.  Microflares and the Statistics of X-ray Flares , 2011, 1108.6203.