Table 1. Two-State Thermodynamic Changes upon Cavity−Ligand Bindinga.
C,L | ξeq | ΔG | ΔH | − TΔS | ΔGW | ΔUCL | ΔULW | ΔUCW | ΔUWW |
---|---|---|---|---|---|---|---|---|---|
N,N | −0.345 | −16.5 | −29.1 | 12.6 | −10.5 | −6 (0) | 10(0) | 4(0) | −37 |
+,N | −0.085 | −2.3 | 11.7 | −14.0 | −1.2 | −1 (0) | 2(0) | 0(0) | 12 |
−,N | −0.105 | −3.4 | −3.0 | −0.4 | −1.4 | −2 (0) | 1(0) | −2 (−1) | 0 |
−,+ | −0.135 | −13.0 | −14.0 | 0.9 | 153.0 | −166 (−164) | 117(118) | 149(146) | −114 |
+,− | −0.035 | −6.1 | −16.8 | 10.7 | 123.9 | −130 (−128) | 80(81) | 121(119) | −88 |
N,+ | [ −0.195] | 12.9 | 45.8 | −32.9 | 15.9 | −3 (0) | 19(15) | −28 (0) | 57 |
N,− | [ −0.195] | 19.9 | 75.7 | −55.8 | 22.9 | −3 (0) | 34(29) | −35 (0) | 79 |
ξ values are in nm; thermodynamic data are in kJ mol−1. The electrostatic components of the interaction energies are reported in parentheses. Square brackets are used for arbitrary ξ values in the case of ligand rejection. Larger ξeq values for (+,N), (−,N), (−,+), and (+,−) are due to solvent-separated binding.