We present simulations of the non-linear evolution of the m = 1 kink m
ode in line-tied coronal loops. We focus on the structure of the curre
nt concentrations which develop as a consequence of the instability in
two different types of magnetic field configuration, one containing a
net axial current and the other with a vanishing total axial current.
Tn the first case, current sheets develop one third of the way from f
ootpoint to loop apex (where the non-linear kink mode folds on itself)
within the body of the current channel, while in the second case the
current sheet develops at the loop apex at the interface between the c
urrent containing channel and the outer axial potential field. In both
cases line-tying, while playing a stabilizing role in the linear theo
ry, acts as a destabilizing agent for the non-linear resistive evoluti
on. The unwrapping of magnetic field lines in the vanishing axial curr
ent model appears to be consistent with the geometry of compact recurr
ent loop flares.