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. Author manuscript; available in PMC: 2014 Aug 6.
Published in final edited form as: Annu Rev Biophys. 2013;42:121–142. doi: 10.1146/annurev-biophys-083012-130318

Figure 6. Simple model system illustrating weak entropy-enthalpy compensation.

Figure 6

An idealized protein and ligand interact via a Morse potential that is strengthened or weakened to simulate ligand modifications. (a) Intermolecular Morse potential U(r) = De[1−ea(rr0)]2, with r0 = 2.8 Å, a = 1/(0.5 Å), and well depth De varying from 2–10 kcal/mol. (b) Potential of mean force F(r) = U(r)−kBT ln4πr2 between protein and ligand as a function of intermolecular distance r for temperature T = 25 C. (c) Standard entropic (TΔS) and enthalpic (ΔH) contributions to the binding free energy for different well depths De, computed from classical statistical mechanics. Note that, while some entropy-enthalpy compensation is apparent, it is not linear.