3D free boundary equilibrium computations have recently been used to model external kinks and edge harmonic oscillations (EHOs), comparing with linear MHD stability codes, and nonlinear analytic theory [Kleiner et al, PPCF 61 084005 (2019)]. In this study, results of the VMEC equilibrium code are compared further with nonlinear reduced MHD simulations, using the JOREK code, to investigate the extent to which the modelling approaches agree. For the simulated external kink, where the instability is dominated by a single toroidal harmonic, good agreement is found. The JOREK simulation is run with a low resistivity inside the plasma, and large resistivity outside, approximating the ideal MHD assumptions in VMEC. Assuming a more realistic resistivity, and including flows, the saturated state in JOREK and VMEC remain consistent. Modelling EHOs where multiple toroidal harmonics are linearly unstable, the saturated perturbation observed can differ in the dominant toroidal harmonic. On the ideal timescale, a n = 2 EHO is observed in JOREK, while the saturated perturbation predicted by VMEC is a n = 1 mode. Extending simulations into timescales where resistive effects can play a role, similar n = 1 perturbations can be found. The coupling of different linearly unstable toroidal harmonics in the JOREK simulation broadens the magnetic energy spectrum and ergodises the plasma edge region, resulting in a more localised pressure perturbation. These effects are not observed in VMEC, because closed magnetic flux surfaces are enforced. Despite these differences, the results of the two approaches are considered to be in reasonable agreement, even in this more advanced case.