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. Author manuscript; available in PMC: 2012 Mar 16.
Published in final edited form as: J Am Chem Soc. 2011 Feb 22;133(10):3570–3581. doi: 10.1021/ja109904u

Table 3.

Experimental (ΔGoexpt) and computed (ΔGocalc) binding free energies for CB[7] with bicyclo[2.2.2]octane guests, along with computed free energy breakdowns. Published: our prior calculations7. Corrected: current calculations with corrected (finer) finite-difference Poisson-Boltzmann (FDPB) grids. Academic vdW: current calculations with corrected FDPB grids and academic Lennard-Jones parameters (see text). Academic vdW/Commercial radii: current calculations with corrected FDPB grids, academic Lennard-Jones parameters, and dielectric cavity radii based upon commercial Lennard-Jones σ values. Δ(U+W): change in Boltzmann-averaged total potential and solvation energy. −TΔSocfg: configurational entropy contribution to binding free energy. Mean energy changes: Boltzmann-averaged energy contributions from the various potential and solvation energy contributions, as follows. ΔUvdW: van der Waals energy; ΔUC: Coulombic energy; ΔWel: electrostatic (PB) solvation energy; ΔEel: sum of ΔUC and ΔWel; ΔUval: valence (bond-stretch, angle-bend, and dihedral) energy; ΔWnp: nonpolar salvation energy.

Mean Energy Changes
ΔGoexpt ΔGocalc Δ(U+W) TΔSocfg ΔUvdW ΔUC ΔWel ΔEel ΔUval ΔWnp
Published
B2 −13.4 −12.8 −29.6 16.8 −34.6 −8.1 14.3 6.2 1.4 −2.7
B5 −19.5 −25.6 −37.6 12.0 −31.8 −162.1 155.3 −6.8 3.8 −2.7
B11 −20.6 −19.9 −41.4 21.5 −42.0 −241.1 232.0 −9.1 13.5 −3.8
Corrected
B2 −13.4 −12.0 −29.4 17.4 −34.3 −8.2 14.5 6.3 1.2 −2.6
B5 −19.5 −23.1 −37.6 14.5 −31.3 −163.3 156.7 −6.6 3.0 −2.7
B11 −20.6 −22.4 −38.2 15.7 −37.6 −227.5 226.4 −1.1 3.9 −3.2
Academic vdW
B2 −13.4 −12.4 −29.6 17.2 −32.9 −8.2 14.1 5.9 0.2 −2.7
B5 −19.5 −23.7 −38.5 14.8 −30.3 −155.1 146.9 −8.2 2.8 −2.8
B11 −20.6 −22.9 −38.7 15.8 −35.7 −219.2 216.2 −3.0 3.3 −3.2
Academic vdW/Commercial Radii
B2 −13.4 −11.9 −28.0 16.1 −33.0 −7.2 14.7 7.5 0.2 −2.7
B5 −19.5 −17.8 −31.5 13.7 −30.6 −153.3 152.9 −0.4 2.2 −2.8
B11 −20.6 −16.1 −30.0 14.0 −35.7 −219.2 225.9 6.8 2.1 −3.2
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