A computational modeling of the protonation of corannulene at B3LYP/6-311G(d,p)//B3LYP/6-311G(d,p) and of the binding of lithium cations to corannulene at B3LYP/6-311G(d,p)//B3LYP/6-31G(d,p)has been performed. A proton attaches preferentially to one carbon atom, forming a
-complex. The isomerprotonated at the innermost (hub) carbon has the best total energy. Protonation at the outermost (rim) carbonand at the intermediate (bridgehead rim) carbon is less favorable by ca. 2 and 14 kcal mol
-1, respectively.Hydrogen-bridged isomers are transition states between the
-complexes; the corresponding activation energiesvary from 10 to 26 kcal mol
-1. With an empirical correction obtained from calculations on benzene, naphthalene,and azulene, the best estimate for the proton affinity of corannulene is 203 kcal mol
-1. The lithium cationpositions itself preferentially over a ring. There is a small energetic preference for the 6-ring over the 5-ringbinding (up to 2 kcal mol
-1) and of the convex face over the concave face (3-5 kcal mol
-1). The Li-bridgedcomplexes are transition states between the
-face complexes. Movement of the Li
+ cation over either face isfacile, and the activation energy does not exceed 6 kcal mol
-1 on the convex face and 2.2 kcal mol
-1 on theconcave face. In contrast, the transition of Li
+ around the corannulene edge involves a high activation
barrier(24 kcal mol
-1 with respect to the lowest energy
-face complex). An easier concave/convex transformationand vice versa is the bowl-to-bowl inversion with an activation energy of 7-12 kcal mol
-1. The computedbinding energy of Li
+ to corannulene is 44 kcal mol
-1. Calculations of the
7Li NMR chemical shifts andnuclear independent chemical shifts (NICS) have been performed to analyze the aromaticity of the corannulenerings and its changes upon protonation.