In the case of the NR-in-BLG and NR-in-POPC systems (Fig. ), the deviation between the (converged) induced potentials produced using models A, B, and C relative to model D is 0.002 and -0.005 au, respectively, corresponding to 0.05 and -0.14 eV. The induced potentials increase gradually with the cutoff distance for both NR systems, leveling out after around 40 Å. The different requirements observed for the PNP systems versus the NR systems in terms of the cutoff distance for the induced potentials are in line with the findings of Beerepoot et al. The induced potentials obtained from models A and B are almost identical at all cutoff distances, which strengthens the assertion that model B does not produce improved induced dipoles compared to model A. Regarding the permanent potentials, we also observe some large changes in the NR systems due to the inclusion of ions. In the case of NR-in-BLG, it is the inclusion of sodium ions, thus causing a gradual increase, while in the NR-in-POPC system, it is the inclusion of potassium and chloride ions, which thus results in oscillations. Again there is no apparent effect on the induced potentials.