Abstract
The present study consists of two parts. Here in Part 1, a model
set
of conservation
laws exactly preserving the MHD hyperbolic singularities is investigated
to develop
the general theory of the nonlinear evolution of MHD shock waves. Great
emphasis
is placed on shock admissibility conditions. By developing the viscosity
admissibility condition, it is shown that the intermediate shocks are
necessary to ensure
that the planar Riemann problem is well-posed. In contrast, it turns out
that the
evolutionary condition is inappropriate for determining physically relevant
MHD
shocks. In the general non-planar case, by studying canonical cases, we
show that
the solution of the Riemann problem is not necessarily unique –
in particular, that
it depends not only on reference states but also on the associated internal
structure. Finally, the stability of intermediate shocks is discussed,
and a theory of their
nonlinear evolution is proposed. In Part 2, the theory of nonlinear waves
developed
for the model is applied to the MHD problem. It is shown that the topology
of the
MHD Hugoniot and wave curves is identical to that of the model problem.
Publisher
Cambridge University Press (CUP)
Cited by
31 articles.
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