We construct numerical examples of a 'modon' (counter-rotating vortice
s) in an Euler flow by exploiting the analogy between steady Euler how
s and magnetostatic equilibria in a perfectly conducting fluid. A nume
rical modon solution can be found by determining its corresponding mag
netostatic equilibrium, which we refer to as a 'magnetic modon'. Such
an equilibrium is obtained numerically by a relaxation procedure that
conserves the topology of the relaxing field. Our numerical results sh
ow how the shape of a magnetic modon depends on its 'signature' (magne
tic flux profile), and that these magnetic modons are unexpectedly uns
table to nonsymmetric perturbations. Diffusion can change the topology
of the field through a reconnection process and separate the two magn
etic eddies. We further show that the analogous Euler flow (or modon)
behaves similar to a perturbed Hill's vortex.