“…( f 1 ) is the inhomogeneity of the magnetic field, H, on the bottom of the Petri dish, to be minimised as in [37] with a tolerance interval of ±10 A/m. Once (8) and (9) are solved, the H-field intensity can be computed from magnetic vector potential A in a straight forward way. Therefore the inhomogeneity of H in terms of the H-norm discrepancy, that is dimensionless, is evaluated on the bottom of the Petri dish on a fixed grid of points; ( f 2 ) is the sensitivity of f 1 with respect to the set of uncertain design variables shown in Table 2, evaluated according to (5), to be minimised; and ( f 3 ) is the end voltage (or current) when the inductor is supplied by applying a current (or a voltage, respectively).…”