A Topological Problem in
Magnetohydrodynamics
(Abstract)
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In magnetohydrodynamics, a magnetic field B evolves in time with no change in the topology T(B) of its lines of force defined by In this physical sense, a field in static equilibrium governed by
the force-free equations: is subject to a prescribed T (B)
the field happens to possess from its evolutionary past. I will describe the challenge of expressing
T (B) as integral equations, the mixed
(hyperbolic & elliptic) nature of the force-free pdes, and, the general
need for this nonlinear, nonlocal problem to admit weak solutions in which B is tangentially discontinuous at
suitably placed surfaces. It is
instructive to contrast this kind of weak solutions with those containing
shocks associated with intersecting characteristics in compressive
hydrodynamics as a purely hyperbolic pde system. The construction of such equilibrium
states by numerical simulation, via 3D time-dependent topology-preserving
relaxation, will be briefly discussed, pointing out an interesting break
through. The formation of magnetic
discontinuities as proposed by E. N. Parker is a promising explanation of the
million-degree temperature of the outer atmosphere of the Sun. (Dr. Boon Chye Low
is an accomplished mathematical physicist.
He is currently the section head for solar atmosphere and heliosphere,
High Altitude Observatory, at |