Table 1. Formal charge binding energies and metal charges.
Men+ | BEPhCN | qf | BEDMMP | qf | BEDMMP–BEPhCN | Disp. (Calc)* | Disp. (Exp)† | Agreement‡ |
---|---|---|---|---|---|---|---|---|
Al3+ | −24.69 | 1.03 | −19.82 | 1.74 | 4.87 | No | Yes | No |
Fe3+ | −20.31 | 1.60 | −19.63 | 1.51 | 0.68 | No | Yes | No |
La3+ | −8.56 | 2.32 | −10.15 | 2.35 | −1.59 | Yes | Yes | Yes |
Cd2+ | −6.49 | 1.22 | −7.33 | 1.39 | −0.84 | Yes | No | No |
Co2+ | −6.88 | 0.87 | −7.72 | 1.22 | −0.84 | Yes | No | No |
Cu2+ | −9.88 | 0.81 | −8.52 | 1.31 | 1.36 | No | Yes | No |
Ni2+ | −7.66 | 0.86 | −8.26 | 1.23 | −0.60 | Yes | No | No |
Zn2+ | −6.81 | 1.34 | −8.17 | 1.27 | −1.36 | Yes | No | No |
Ag+ | −2.21 | 0.73 | −2.27 | 0.79 | −0.06 | No | No bind | No |
Na+ | −1.41 | 0.83 | −1.71 | 0.89 | −0.30 | Yes | No bind | No |
Binding energy [eV] and final metal charge (qf) for the minimum energy structures of Men+–PhCN and Men+–DMMP using the formal charge approach. Agreement regarding displacement events between theory and the original experiments was only seen in one of ten cases. After the follow-up experiments, agreement regarding displacement increased to three of ten cases (due to displacement of 5CB from Cd and Zn in the follow-up experiments).
*Computed displacement of PhCN by DMMP.
†Experimental displacement of PhCN by DMMP, from previous studies11.
‡Agreement between computed and experimental displacement. ‘No bind' indicates no homeotropic anchoring of the liquid crystal to the metal cation. Displacement is assumed to occur when BEDMMP−BEPhCN<−0.20 eV.