Table 3.
2a2 | 2b | 2a3 | 2b | crystallography | |
---|---|---|---|---|---|
dielectric constant for PCM | 20.0 | 20.0 | 4.0 | 4.0 | |
energy (kcal/mol) | |||||
ΔE | 0.0 | 1.0 | 2.9 | 0.0 | |
ΔH | 0.0 | 1.2 | 2.7 | 0.0 | |
ΔG | 0.0 | 0.2 | 3.7 | 0.0 | |
bond length (Å) | |||||
Fe—O(1) | 2.065 | 2.366 | 2.058 | 2.376 | 2.1 |
O—O | 1.463 | 1.470 | 1.469 | 1.470 | 1.5 |
C2—O(2) | 1.518 | 1.504 | 1.501 | 1.505 | 1.4 |
Fe—O(C1) | 2.137 | 2.046 | 2.127 | 2.050 | 2.2 |
Fe—O(C2) | 1.990 | 1.997 | 2.005 | 2.000 | 2.3 |
C1—O | 1.279 | 1.278 | 1.280 | 1.276 | 1.3 |
C2—O | 1.370 | 1.363 | 1.369 | 1.361 | 1.5 |
C1—C2 | 1.531 | 1.530 | 1.532 | 1.531 | 1.5 |
C2(deviation from ring) | 0.380 | 0.385 | 0.380 | 0.385 | 0.46 |
hydrogen bonds (Å) | |||||
O(1)-H | 1.523 | 1.060 | 1.976 | 1.049 | — |
O(1)-N(His200) | 2.621 | 2.623 | 3.024 | 2.642 | 3.0 |
spin density | |||||
Fe | 4.03 | 3.99 | 4.00 | 3.98 | |
O(1) | 0.06 | 0.01 | 0.07 | 0.01 | |
O(2) | −0.02 | −0.02 | −0.01 | −0.02 | |
O2/O2H | 0.04 | −0.01 | 0.06 | −0.01 | |
C6(4NC) | −0.43 | −0.38 | −0.38 | −0.36 |
The numbering of atoms is shown in Figure 4.
Note that geometry optimization with ε = 4.0 was found to converge to 2b from both possible starting structures. Single-point energy using ε = 4.0 with thermal corrections with ε = 20.0 were performed to compare energetics of 2a and 2b below.
The optimized structure using ε = 4.0 with O(1)-N(His200) fixed. The energies relative to 2b optimized under the same condition as 2a and the thermal corrections with ε = 20.0 were applied to both 2a and 2b.