Angewandte
Chemie
Calculations of the natural bond orbital (NBO)-based
partial atomic charges,[8] show a negative charge of ꢀ0.54 on
the lithiated carbon atom at the ortho position of aniline, and
there is no significant change in this charge upon coordination
of the nitrogen center with BH3 or BF3 (Figure 1).[7b] Even
charged hydrogen atoms (Li···H1 = 1.92 , Li···H2 = 1.92 ),
ꢀ
which results in high ellipticity of the Li B bond (e = 2.74).
From the NBO and AIM analyses described above, and
the geometry shown in Figure 1, we infer that in case of BH3
the primary electrostatic interaction of Li+ is with the
negatively charged boron atom, which brings two hydrogen
atoms close to the Li center causing a greater spatial require-
ꢀ
ment for this bond. In contrast, with BF3 even a single Li F
bond can, because of its strength, provide effective stabiliza-
tion and this results in a six-membered chelation ring with less
crowding around lithium (cf. X = F and X = H; Figure 1); this
may also be additionally relevant for the solvated moieties.
The dichotomy in BH3 and BF3 bonding to Li can not only
help to explain the superior effectiveness of BF3 in promoting
lithiations, but also explain the gross variations in crystal
structure of LiBH4 (Li···B = 2.47-2.54 , Li···H = 1.98, 2.02,
2.15 ) and LiBF4 (F-Li = 1.85 ).[10–12]
In conclusion we have shown that, in principle, BF3
complexation methodology can be extended to directed
ortho metalations and thereby improve the poor ability of
the dimethyl amino group in DoMꢀs to exceed the directing
ability of even chloro and methoxy groups. The DFT
computations are in line with the experimental findings on
the comparative reactivity and regioselectivity of the reaction,
and clearly indicate that chelation of lithium by BX3
coordinated to a nitrogen center (CIPE) has an important
role; an aspect largely ignored in earlier mechanistic consid-
erations on BX3 acceleration of alkyl lithium reactions.[3,4]
Interestingly, in the lithiated intermediates complexed to
BH3, tridentate chelation of Li+ is indicated, whereas a two-
ꢀ
center F Li bond, with characteristics remarkably similar to
Figure 1. 3D-structures of the lithiated intermediates (23) and the
transition states (22TS) that lead to their formation. The important
partial atomic charges are also shown. a) 23 (X=H): the Li atom is
bonded to the B atom with a bond length of 2.21 ꢀ, b) 23 (X=F): the
Li atom is bonded to the F atom with a bond length of 1.80-ꢀ,
c) transition-state 22 (X=H): the Li–B bond length is 2.27 ꢀ, and
d) transition-state 22 (X=F): the Li–F bond length is 1.82 ꢀ.
ꢀ
those of the C Li bond, is seen in the corresponding BF3
complexes. In view of the recent demonstration of the
acceleration of metathesis by chelation of ruthenium to an
aryl fluorine,[13] the effect of BF3 on transition-metal-medi-
ated reactions of heteroatom-containing substrates also needs
to be explored, and if successful it can have an impact on the
scope of this chemistry.[14]
within the known limitations of the method,[8] this result is
surprising, as well as contrary to apriori assumptions;[3] this
suggests a more important role for dipole interactions and
lithium chelation. In contrast, there is clear indication of a
strong interaction between the fluorine and lithium atoms
based on the computations of lithiated intermediate 23 (X =
F). Although one may tend to consider the lithium–carbon
bond as the primary bond, there is, in terms of an atoms in
molecule (AIM) analysis,[9] a six-membered ring critical point
Received: December 28, 2007
Revised: March 16, 2008
Published online: May 16, 2008
Keywords: anilines · boron · density functional calculations ·
.
lithiation · metalation
1939, 61, 106; b) G. Wittig, G. Fuhrmann, Chem. Ber. 1940, 73,
1197.
ꢀ
ꢀ
in 23 and a remarkable similarity between the Li F and Li C
bonds in terms of charge (C = ꢀ0.56, F = ꢀ0.62, Li = 0.90),
ꢀ
ꢀ
ꢀ
bond length (C Li = 2.01 , F Li = 1.80 ), 1 (C Li = 0.039,
[2] a) H. W. Gschwend, H. R. Rodriguez, Org. React. 1979, 26, 1;
on ortho lithiation see: N. J. R. Von Eikema Hommes, P. v. R.
Schleyer, Tetrahedron 1994, 50, 5903; e) A.-M. Sapre, P. v. R.
Schleyer, Lithium Chemistry; A theoretical and experimental
overview, Wiley, New York, 1995.
2
ꢀ
ꢀ
ꢀ
ꢀ
F Li = 0.036), 5 1 (C Li = 0.19, F Li = 0.29), and e (C Li =
ꢀ
0.02, F Li = 0.02). AIM computations on the solvate,
23·2Me2O, give essentially similar results, including a six-
membered ring critical point with the expected decrease in
electron density of the Li bonds to F and C (see the
Supporting Information). In comparison, in the lithiated
BH3 complex of 23 (X = H) there is a five-membered ring
critical point with Li···B distance of 2.21 (charge Li = 0.89,
B = ꢀ0.23). Lithium is also in contact with two weakly
Kessar, P. Singh, K. N. Singh, A. Kaur, P. Venugopalan, P. V.
Angew. Chem. Int. Ed. 2008, 47, 4703 –4706
ꢀ 2008 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim