Exact Solutions for Spine Reconnective Magnetic Annihilation

Physics – Fluid Dynamics

Scientific paper

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Scientific paper

Solutions for spine reconnective annihilation are presented which satisfy exactly the three-dimensional equations of steady-state resistive incompressible magnetohydrodynamics (MHD). The magnetic flux function (A) and stream function have the form $A = A_{0}(R) sin phi + A_{1}(R)z, qquad Psi = Psi _{0}(R) sin phi + Psi _{1}(R)z,$ in terms of cylindrical polar coordinates (R,,z). First of all, two non-linear fourth-order equations for A1 and are solved by the method of matched asymptotic expansions when the magnetic Reynolds number is much larger than unity. The solution, for which a composite asymptotic expansion is given in closed form, possesses a weak boundary layer near the spine (R = 0). These solutions are used to solve the remaining two equations for A0 and . Physically, the magnetic field is advected across the fan separatrix surface and diffuses across the spine curve. Different members of a family of solutions are determined by values of a free parameter and the components (BRe, Bze) and (vRe, vze) of the magnetic field and plasma velocity at a fixed external point (R,,z) = (1,/2,0), say.

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