The projected dipole moment of the solvent µ r around the Na 2+ , Na 3+ , Cl 2-, and Cl 3-ions is shown in Fig. . For comparison, the µ r calculated from the Born model is also displayed, starting at d = 1 nm from the ion (where g(r) is close to 1) according to Eqs. ( ) and (30). Similarly to the case of the monovalent ions (Fig. ), the density profiles of the AdSoS systems are found to be in good agreement with the FG system (data not shown). It can be seen in Fig. that the short-range polarization of the FG and AdSoS systems match very well. However, in the SG and CG regions, the AdSoS water is slightly overpolarized, and this trend becomes more pronounced upon increasing the charge of the central ion. The scaling of the dipole moment with s 3/2 may explain an increased interaction of the scaled water with the ion. Nevertheless, the discrepancy remains small (< 5%), as the polarization decays to a significant degree in the FG region. The FG polarization, on the other hand, is in good agreement with the analytical Born polarization, and the residual discrepancies are likely due to the use of a cutoff. Different shades of blue correspond to different cutoffs.