Brandt et al.
known to use electrostatic interactions, hydrophobic
interactions, hydrogen bonds, and dispersion interactions
in combination with repulsive steric interactions to
specifically bind and transform a substrate.13 In asym-
metric catalysis a chiral ligand is commonly used in place
of a protein to differentiate between two prochiral faces
via repulsive steric interactions. In some cases though,
enantioselection is realized by stabilization of one of the
diastereomeric transition states by attractive inter-
actions. One such well-known example is the Sharpless
asymmetric dihydroxylation that partly relies on attrac-
tive interactions between aromatic moieties. This inter-
action could, according to the participating molecular
fragments and the geometry of the transition state, be
referred to as π-stacking.14 The importance of arene-arene
interactions as well as alkyl-arene interactions is still a
matter of debate.15
In the case of ruthenium-catalyzed asymmetric trans-
fer hydrogenation Van Leeuwen et al.10 suggest that
steric hindrance is the major factor determining the
enantioselectivity. To the contrary, Noyori et al. earlier
proposed that the selectivity is due to an attractive CH/π
interaction between the aryl of the substrate and the
arene in the catalyst.11,16 On the basis of MP2 and B3LYP
calculations, this interaction is suggested to be dominated
by electrostatic forces together with a nonnegligible
charge-transfer component. This proposal nicely rational-
izes why aliphatic ketones are poor substrates and that
electron-withdrawing substituents on acetophenone sub-
strates decrease the enantiomeric excess. For the catalyst
derived from an amino alcohol and [RuCl2(hexameth-
ylbenzene)]2, a stabilizing electrostatic attraction between
C(sp3)H/π is proposed. Again quantum chemical calcula-
tions show that the hydrogens of the methyl groups of
the hexamethylbenzene have net positive charge.
F IGURE 1. 2-Azanorbornyl-3-methanol ligands 1 and 2.
calculations using the polarized continuum model (PCM),17
a great improvement in the correlation between predicted
and experimental enantioselectivity was achieved. Thus,
we arrived at a conclusion very different from those of
Van Leeuwen and Noyori, namely, that electrostatics and
sterics, well taken care of by our DFT calculations, could
not be the main contributors to the enantioselectivity.
In this paper we have studied in detail the impact of
electrostatics and sterics on enantioselectivity, trying to
form a consensus picture of the origin of the enantio-
selectivity in the ruthenium-catalyzed transfer hydroge-
nation.
We have earlier reported that ligands 1 and 2 are
excellent ligands in the ruthenium-catalyzed asymmetric
transfer hydrogenation of aromatic ketones (Figure 1).
Here, we present our conclusions on the origin of the
enantioselectivities achieved in the reactions using these
ligands.
Com p u ta tion a l Meth od s
Geometries of all substrates were calculated using the
Gaussian electronic structure program,18 using B3LYP,19
a
density functional based on a hybrid functional, together with
the double-ú quality basis set LANL2DZ.20 The basis set
involve the use of d95 for C, N, O, and H. Atomic charge
distributions were thereafter fitted to the electrostatic poten-
tial at points selected according to the CHelpG21 scheme using
the procedure implemented in Gaussian 98. This was done
using the B3LYP/6-311+G(d,p) wave functions at the B3LYP/
LANL2DZ geometries. For the 3-substituted substrates, there
are two alternative conformations relating to the position of
the substituent relative to the acetyl group. In this work we
report data from the s-trans conformations. The s-cis confor-
mations were also investigated, but no significant differences
were detected. The sum of the calculated charges of the six
heavy atoms in the aromatic ring of the substrate were used
as a measure of the charge distribution of the aromatic ring.
To assess the performance of B3LYP in terms of predicting
relative enantioselectivities between substrates with different
charge distribution, we performed transition state calculations
using two different substrates, acetophenone and 2,3,4,5,6-
In the first published quantum chemical investigation
of the reaction,8 we concluded that gas-phase density
functional theory calculations (B3LYP) are not able to
reproduce the degree of enantioselection experienced in
the reaction. In this approach, two major forces are
neglected, namely, the dispersion interaction between
catalyst and substrate and the effect of the solvent.
Taking this latter effect into account by performing
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