The termination of the current and the loss of runaway electrons following runaway current plateau formation during disruptions have been investigated in the JET, DIII-D and FTU tokamaks. Substantial conversion of magnetic energy into runaway kinetic energy, up to ~10 times the initial plateau runaway kinetic energy, has been inferred for the slowest current terminations. Both, modelling and experiment suggest that, in present devices, the efficiency of conversion into runaway kinetic energy is determined to a great extent by the characteristic runaway loss time, tdiff, and the resistive time of the residual ohmic plasma after the disruption, tres, increasing with the ratio tdiff /tres. It is predicted that, in large future devices such as ITER, the generation of runaways by the avalanche mechanism will play an important role, particularly for slow runaway discharge terminations, increasing substantially the amount of energy deposited by the runaways onto the plasma facing components by the conversion of magnetic energy of the runaway plasma into runaway kinetic energy. Estimates of the power fluxes on the beryllium plasma facing components during runaway termination in ITER indicate that for runaway currents of up to 2MA no melting of the componentsis expected. For larger runaway currents, minimization of the effects of runaway impact on the first wall requires a reduction of the kinetic energy of the runaway beam before termination and, in addition, high plasma density ne and low ohmic plasma resistance (long res) to prevent large conversion of magnetic into runaway kinetic energy during slow current terminations.