D. Kondrashov et al., Three-dimensional magnetohydrodynamic simulations of the interaction of magnetic flux tubes, ASTROPHYS J, 519(2), 1999, pp. 884-898
We use a three-dimensional Cartesian resistive MHD code to investigate thre
e-dimensional aspects of the interaction of magnetic flux tubes as observed
in the solar atmosphere and studied in laboratory experiments. We present
here the first results from modeling the reconnection of two Gold-Hoyle mag
netic flux tubes that follow the system. evolution to a final steady state.
The energy evolution and reconnection rate for flux tubes with both parall
el and antiparallel axial fields and with equal and nonequal strengths are
studied. For the first time, we calculate a gauge-invariant relative magnet
ic helicity of the system and compare its evolution for all the above cases
. We observed that the rate at which helicity is dissipated may vary signif
icantly for different cases, and it may be comparable with the energy dissi
pation rate. The footpoints of the interacting flux tubes were held fixed o
r allowed to move to simulate different conditions in the solar photosphere
. The cases with fixed footpoints had lower magnetic energy release and rea
ched a steady state faster than cases with moving footpoints. For all compu
ted cases the magnetic energy was released mostly through work done on the
plasma by the electromagnetic forces rather than through resistive dissipat
ion. The reconnection rate of the poloidal magnetic held is faster for the
case with antiparallel flux tubes than for the case with parallel flux tube
s, consistent with laboratory experiments. We find that during reconnection
supersonic (but sub-Alfvenic) flows develop, and it may take a considerabl
y longer time for the system to reach a steady state than for magnetic Bur
to reconnect. It is necessary to retain the pressure gradient in the moment
um equation; the plasma pressure may be significant for the final equilibri
um steady state even with low-beta initial conditions, and the work done on
the plasma by compression is important in energy exchange.