Magnetic reconnection, or the ability of the magnetic field lines that are
frozen in plasma to change their topology, is a fundamental problem of
magnetohydrodynamics (MHD). We briefly examine the problem starting with the
well-known Sweet-Parker scheme, discuss effects of tearing modes, anomalous
resistivity and the concept of hyperresistivity. We show that the field
stochasticity by itself provides a way to enable fast reconnection even if, at
the scale of individual turbulent wiggles, the reconnection happens at the slow
Sweet-Parker rate. We show that fast reconnection allows efficient mixing of
magnetic field in the direction perpendicular to the local direction of
magnetic field. While the idea of stochastic reconnection still requires
numerical confirmation, our numerical simulations testify that mixing motions
perpendicular to the local magnetic field are up to high degree hydrodynamical.
This suggests that the turbulent heat transport should be similar to that in
non-magnetized turbulent fluid, namely, should have a diffusion coefficient
\sim LV_L, where V_L is the amplitude of the turbulent velocity and L is the
scale of the turbulent motions. We present numerical simulations which support
this conclusion. The application of this idea to thermal conductivity in
clusters of galaxies shows that this mechanism may dominate the diffusion of
heat and may be efficient enough to prevent cooling flow formation.Comment: 12 pages, 2 figures, invited talk at JENAM2002 - The Unsolved
Universe:Challenges for the Future (v2: minor changes