Disruption of sheet-like structures in Alfvénic turbulence by magnetic reconnection

We propose a mechanism whereby the intense, sheet-like structures naturally formed by dynamically aligning Alfv´enic turbulence are destroyed by magnetic reconnection at a scale ˆλ D, larger than the dissipation scale predicted by models of intermittent, dynamically aligning turbulence. The reconnection process proceeds in several stages: first, a linear tearing mode with N magnetic islands grows and saturates, and then the X-points between these islands collapse into secondary current sheets, which then reconnect until the original structure is destroyed. This effectively imposes an upper limit on the anisotropy of the structures within the perpendicular plane, which means that at scale ˆλD the turbulent dynamics change: at scales larger than ˆλD, the turbulence exhibits scale-dependent dynamic alignment and a spectral indexapproximately equal to −3/2, while at scales smaller than ˆλD, the turbulent structures undergo a succession of disruptions due to reconnection, limiting dynamic alignment, steepening the effective spectral index and changing the final dissipation scale. The scaling of ˆλD with the Lundquist (magnetic Reynolds) number SL⊥ depends on the order of the statistics being considered, and on the specific model of intermittency; the transition between the two regimes in the energy spectrum is predicted at approximately ˆλD ∼ SL⊥^−0.6 . The spectral index below ˆλD is bounded between −5/3 and −2.3. The final dissipation scale is at ˆλη,∞ ∼ SL⊥^−3/4, the same as the Kolmogorov scale arising in theories of turbulence that do not involve scale-dependent dynamic alignment.

[1]  S. Boldyrev,et al.  Role of Magnetic Reconnection in Magnetohydrodynamic Turbulence. , 2016, Physical review letters.

[2]  G. Kowal,et al.  Statistics of Reconnection-driven Turbulence , 2016, 1611.03914.

[3]  C. H. Chen,et al.  Recent progress in astrophysical plasma turbulence from solar wind observations , 2016, Journal of Plasma Physics.

[4]  M. Velli,et al.  ‘Ideally’ unstable current sheets and the triggering of fast magnetic reconnection , 2016, Journal of Plasma Physics.

[5]  P. M. Morse,et al.  Electromagnetic Phenomena in Cosmical Physics , 2016 .

[6]  A. Schekochihin,et al.  A statistical model of three-dimensional anisotropy and intermittency in strong Alfvénic turbulence , 2016, 1606.00466.

[7]  S. Boldyrev,et al.  Scalings of intermittent structures in magnetohydrodynamic turbulence , 2016, 1602.05289.

[8]  Ashis Bhattacharjee,et al.  TURBULENT MAGNETOHYDRODYNAMIC RECONNECTION MEDIATED BY THE PLASMOID INSTABILITY , 2015, 1512.01520.

[9]  T. Horbury,et al.  Measures of three-dimensional anisotropy and intermittency in strong Alfvénic turbulence , 2015, 1512.01461.

[10]  R. Grappin,et al.  IMPRINTS OF EXPANSION ON THE LOCAL ANISOTROPY OF SOLAR WIND TURBULENCE , 2015, 1506.03450.

[11]  N. Loureiro,et al.  Magnetic Reconnection Onset via Disruption of a Forming Current Sheet by the Tearing Instability. , 2014, Physical review letters.

[12]  S. Boldyrev,et al.  SCALING PROPERTIES OF SMALL-SCALE FLUCTUATIONS IN MAGNETOHYDRODYNAMIC TURBULENCE , 2014, 1409.2728.

[13]  A. Beresnyak ON THE PARALLEL SPECTRUM IN MAGNETOHYDRODYNAMIC TURBULENCE , 2014, 1407.2613.

[14]  A. Schekochihin,et al.  Refined critical balance in strong Alfvénic turbulence , 2014, 1406.5658.

[15]  A. Schekochihin,et al.  INTERMITTENCY AND ALIGNMENT IN STRONG RMHD TURBULENCE , 2014, 1403.6354.

[16]  Andrey Beresnyak,et al.  SPECTRA OF STRONG MAGNETOHYDRODYNAMIC TURBULENCE FROM HIGH-RESOLUTION SIMULATIONS , 2014, 1410.0957.

[17]  S. Boldyrev,et al.  STATISTICAL ANALYSIS OF CURRENT SHEETS IN THREE-DIMENSIONAL MAGNETOHYDRODYNAMIC TURBULENCE , 2013, 1302.1460.

[18]  A. Beresnyak THREE-DIMENSIONAL SPONTANEOUS MAGNETIC RECONNECTION , 2013, 1301.7424.

[19]  A. Beresnyak Basic properties of magnetohydrodynamic turbulence in the inertial range , 2011, 1111.5329.

[20]  T. Horbury,et al.  THREE-DIMENSIONAL STRUCTURE OF SOLAR WIND TURBULENCE , 2011, 1109.2558.

[21]  R. Samtaney,et al.  Magnetic reconnection and stochastic plasmoid chains in high-Lundquist-number plasmas , 2011, 1108.4040.

[22]  T. Horbury,et al.  Anisotropy of Alfvénic turbulence in the solar wind and numerical simulations , 2010, 1009.0662.

[23]  A. Schekochihin,et al.  Fast magnetic reconnection in the plasmoid-dominated regime. , 2010, Physical review letters.

[24]  T. Horbury,et al.  Power and spectral index anisotropy of the entire inertial range of turbulence in the fast solar wind , 2010, 1002.2096.

[25]  A. Bhattacharjee,et al.  Fast Reconnection in High-Lundquist-Number Plasmas Due to Secondary Tearing Instabilities , 2009 .

[26]  Yi-Min Huang,et al.  Fast reconnection in high-Lundquist-number plasmas due to the plasmoid Instability , 2009, 0906.5599.

[27]  A. Schekochihin,et al.  Turbulent Magnetic Reconnection in Two Dimensions , 2009, 0904.0823.

[28]  R. Samtaney,et al.  Formation of plasmoid chains in magnetic reconnection. , 2009, Physical review letters.

[29]  J. Podesta DEPENDENCE OF SOLAR-WIND POWER SPECTRA ON THE DIRECTION OF THE LOCAL MEAN MAGNETIC FIELD , 2009, 0901.4940.

[30]  Sean Oughton,et al.  Anisotropic scaling of magnetohydrodynamic turbulence. , 2008, Physical review letters.

[31]  W. Dorland,et al.  ASTROPHYSICAL GYROKINETICS: KINETIC AND FLUID TURBULENT CASCADES IN MAGNETIZED WEAKLY COLLISIONAL PLASMAS , 2007, 0704.0044.

[32]  A. Schekochihin,et al.  Instability of current sheets and formation of plasmoid chains , 2007, astro-ph/0703631.

[33]  S. Boldyrev,et al.  Dynamic alignment in driven magnetohydrodynamic turbulence. , 2006, Physical review letters.

[34]  A. Lazarian,et al.  Polarization Intermittency and Its Influence on MHD Turbulence , 2005, astro-ph/0512315.

[35]  W. Dorland,et al.  X-point collapse and saturation in the nonlinear tearing mode reconnection. , 2005, Physical review letters.

[36]  S. Boldyrev On the Spectrum of Magnetohydrodynamic Turbulence , 2005, Physical review letters.

[37]  P. Dmitruk,et al.  Reduced magnetohydrodynamics and parallel spectral transfer , 2004 .

[38]  P. Goldreich,et al.  Magnetohydrodynamic Turbulence Revisited , 1997 .

[39]  P. Goldreich,et al.  MHD Turbulence Revisited , 1996, astro-ph/9612243.

[40]  She,et al.  Quantized energy cascade and log-Poisson statistics in fully developed turbulence. , 1995, Physical review letters.

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

[42]  P. Morrison,et al.  The effect of viscosity on the resistive tearing mode with the presence of shear flow , 1990 .

[43]  P. Morrison,et al.  Resistive tearing instability with equilibrium shear flow , 1990 .

[44]  John V. Shebalin,et al.  Anisotropy in MHD turbulence due to a mean magnetic field , 1983, Journal of Plasma Physics.

[45]  Paul H. Rutherford,et al.  Nonlinear growth of the tearing mode , 1973 .

[46]  Harold P. Furth,et al.  Finite‐Resistivity Instabilities of a Sheet Pinch , 1963 .

[47]  Eugene N. Parker,et al.  Sweet's mechanism for merging magnetic fields in conducting fluids , 1957 .

[48]  Walter M. Elsasser,et al.  The Hydromagnetic Equations , 1950 .

[49]  H. R. Strauss,et al.  Nonlinear, three‐dimensional magnetohydrodynamics of noncircular tokamaks , 1976 .

[50]  E. G. Harris On a plasma sheath separating regions of oppositely directed magnetic field , 1962 .

[51]  S. Chandrasekhar Hydrodynamic and Hydromagnetic Stability , 1961 .