Mt. Kiendl et al., MHD ANALYSIS OF PETSCHEK-TYPE RECONNECTION IN NONUNIFORM FIELD AND FLOW GEOMETRIES, Space science reviews, 79(3-4), 1997, pp. 709-755
Analytical studies of reconnection have, for the most part, been confi
ned to steady and uniform current sheet geometries. In contrast to the
se implifications, natural phenomena associated with the presence of c
urrent sheets indicate highly non-uniform structure and time-varying b
ehaviour. Examples include the violent outbursts of energy on the Sun
known as solar flares, and magnetospheric phenomena such as flux trans
fer events, plasmoids, and amoral activity. Unlike the theoretical mod
els, reconnection therefore occurs in a highly dynamic and structured
plasma environment. In this article we review the mathematical tools a
nd techniques which are available to formulate models capable of descr
ibing the effects of reconnection in such situations. We confine atten
tion to variants of the reconnection model first discussed by Petschek
in the 1960s, in view of its successful application in predicting and
interpreting phenomena in the terrestrial magnetosphere. The analysis
of Petschek-type reconnection is based on the equations of ideal magn
etohydrodynamics (MHD), which describe the large-scale behaviour of th
e magnetic field and plasma flow outside the diffusion region, which w
e determine as a localised part of the current sheet in which reconnec
tion is initiated. The approach we adopt here is to transform the MHD
equations into a Lagrangian or so-called 'frozen-in' coordinate system
. In this coordinate system, the equation of motion transforms into a
set of coupled nonlinear equations, in which the presence of inhomogen
eous magnetic fields and/or plasma flows gives rise to a term similar
to that which appears in the study of the ordinary string equation in
a non-homogeneous medium. As demonstrated here, this approach not only
clarifies and highlights the effects of such non-uniformities, it als
o simplifies the solution of the original set of MHD equations. In par
ticular, this is true for those types of problem in which the total pr
essure can be considered as a known quantity from the outset. To illus
trate the method we solve several 2D problems involving magnetic field
and flow non-uniformities: reconnection in a stagnation-point how geo
metry with antiparallel magnetic fields; reconnection in a Y-type magn
etic field geometry with and without velocity shear across the current
sheet; and reconnection in a force-free magnetic field geometry with
field lines of the form xy = const. These case examples, chosen for th
eir tractability, each incorporate some aspects of the field and flow
geomtries encountered in solar-terrestrial applications, and they prov
ide a starting point for further analytical as well as numerical studi
es of reconnection.