Fig. 2 Computed atomic charges in 2a9.
In conclusion, we have shown that the reaction between
(C6F5)2BOH and organonitriles leads to the formation of
heterocyclic compounds with a BOBOCN ring, the atoms being
held together by a combination of covalent and dative bonds. This
discovery is an exciting manifestation of the multi-functionality of
(C6F5)2BOH, i.e. Lewis and Brønsted acidity as well as Lewis
basicity, which allows a multitude of reactions, such as protona-
tions, Lewis acid–base interactions, H-bonding and the formation
of covalent bonds. We are currently investigating the mechanism
of formation of these heterocycles and their reactivity.
Fig. 1 The molecular structure of one (A) of the two independent
molecules present in the crystals of 2a.
We are grateful to the EPSRC for support (GR/R92042/01).
˚
the boron atom B(19) that lies ca. 0.64 A out of the plane of the
˚
other five atoms (which are again coplanar to within ca. 0.06 A).
Notes and references
There are no statistically significant differences in the equivalent
bond lengths within the central six-membered rings of the two
independent molecules, and the pattern of bonding is similar to
that seen in the related compound I (Table 1).13 The bonds in I are
{ Selected analytical data. 2a: Mp: 130–133 uC. 1H-NMR (CDCl3):
7.90 (m, OH), 7.56 (br. s, NH), 2.53 (s, CH3). 11B-NMR (CDCl3):
2.3 (OBO), 21.2 (NBO). 19F-NMR (CDCl3): 2137.3 (d, 4F, 3JFF = 12 Hz,
o), 2137.5 (d, 4F, o), 2153.1 (t, 2F, 3JFF = 20 Hz, p), 2153.4 (t, 2F, 3JFF
=
˚
all longer than in 2a (on average, by ca. 0.03 A), presumably a
20 Hz, p), 2161.0 (td, 4F, 3JFF = 12 Hz, 3JFF = 21 Hz, m), 2161.9 (td, 4F,
3JFF = 12 Hz, 3JFF = 21 Hz, m). MS-EI (m/z): 765 [M]+, 598 [M 2 (C6F5)]+,
430 [M 2 (C6F5)2H]+. Anal.: Found (Calc.): C, 40.79 (40.83); H, 0.64
(0.66); N, 1.89 (1.83). 2b: 11B NMR (CDCl3): 1.6, 23.2. 19F NMR
(CDCl3): 2134.3 (4F, o), 2134.9 (4F, o), 2157.4 (2F, p), 2157.6 (2F, p),
2165.6 (8F, m). 2c: 11B NMR (CDCl3): 0.7, 21.8. 19F NMR (CDCl3):
2133.6 (4F, o), 2134.0 (4F, o), 2155.8 (2F, p), 2160.0 (2F, p), 2163.9 (8F,
consequence of the change from phenyl to pentafluorophenyl
groups and the increased Lewis acidity of the boron centres in 2a.
The amide C–O and C–N distances seen here in 2a are the same as
˚
each other (at ca. 1.30 A) in contrast to the ca. 0.1 A difference
˚
˚
˚
[C–O ca. 1.23 A, C–N ca. 1.33 A] seen in simple acyclic amides,
indicating a significant contribution from the canonical form as
shown in Eq. 2.
¯
m). Crystal data for 2a: C26H5B2F20NO2, M = 764.93, triclinic, P1 (no. 2), a
˚
= 10.7737(6), b = 14.0513(7), c = 18.8781(10) A, a = 97.147(4), b =
3
˚
96.075(4), c = 104.631(5)u, V = 2715.5(2) A , Z = 4 (2 independent
molecules), Dc = 1.871 g cm23, m(Cu-Ka) = 1.939 mm21, T = 173 K,
colourless blocks, Oxford Diffraction Xcalibur PX Ultra diffractometer;
10017 independent measured reflections, F2 refinement, R1 = 0.046, wR2 =
0.127, 8953 independent observed absorption-corrected reflections [|Fo| >
4s(|Fo|), 2hmax = 142u], 938 parameters. CCDC 288347. For crystal-
lographic data in CIF or other electronic format see DOI: 10.1039/
b516262a
In order to obtain further insight into the type of bonding in this
unusual heterocycle, the formation of 2a was modelled with DFT
calculations.§ As can be seen in Table 1, the bond lengths of the
optimised structure 2a9 are in very good agreement with
the experimental data. Irrespective of the starting geometry for
the calculations, A or B, the optimised structure 2a9 has geometry
B, which indicates that this geometry is probably thermodynami-
cally favoured whereas geometry A arises from crystal packing
§ All calculations were performed at the B3LYP level of theory20–22 and
6-31G(d) basis set23,24 using the Gaussian03 suite of programs.25 Structures
have been fully optimised under no symmetry constraints and confirmed as
minima by frequency analysis.
…
effects in the solid state (F p interactions). Natural bond orbital
analysis (NBO)15–19 reveals a CLN double bond, a covalent
polarised C–O bond and highly ionic B–O and B–N bonds.
The computed atomic charges, as shown in Fig. 2, are consistent
with a highly ionic mode of bonding and confirm the proposed
bonding description with significant positive charge on the carbon
and boron centres and negative charge on the oxygen and nitrogen
centres.
1 R. D. Chambers and T. Chivers, J. Chem. Soc., 1965, 3933–3939.
2 K. Ishihara, H. Kurihara and H. Yamamoto, J. Org. Chem., 1997, 62,
5664–5665.
3 K. Ishihara, H. Kurihara and H. Yamamoto, Synlett, 1997, 597–599.
4 R. Kratzer, (Basell Polyolefins), DE10059717, 2001.
5 H. Bohnen and U. Hahn, (Aventis R&T GmbH), WO0017208, 2000.
6 I. Ikeno, H. Mitsui, T. Iida and T. Moriguchi, (Nippon Shokubai Co.),
WO0244185, 2002.
7 J. Schottek and C. Fritze, (Targor), DE10009714, 2001.
8 K. Takei, K. Mizuta, M. Aoki and K. Takebe, (Nippon Shokubai Co.
Ltd.), JP2004265785, 2004.
Table 1 Selected bond lengths in 2a, I and 2a9
9 T. Beringhelli, G. D’Alfonso, D. Donghi, D. Maggioni, P. Mercandelli
and A. Sironi, Organometallics, 2003, 22, 1588–1590.
10 T. Beringhelli, G. D’Alfonso, D. Donghi, D. Maggioni, P. Mercandelli
and A. Sironi, Organometallics, 2004, 23, 5493–5502.
11 G. J. P. Britovsek, J. Ugolotti and A. J. P. White, Organometallics, 2005,
24, 1685–1691.
12 H. Jacobsen, H. Berke, S. Doering, G. Kehr, G. Erker, R. Froehlich
and O. Meyer, Organometallics, 1999, 18, 1724–1735.
13 H. Ho¨pfl, V. Barba, G. Vargas, N. Farfan, R. Santillan and D. Castillo,
Chem. Heterocycl. Compd., 1999, 35, 912–927.
2a
I
2a9
CLN
NAB
B–O
OAB
B–O
O–C
1.296(3)
1.539(3)
1.523(2)
1.529(2)
1.503(2)
1.295(2)
1.342(7)
1.612(8)
1.553(7)
1.558(8)
1.532(7)
1.325(6)
1.308
1.562
1.527
1.542
1.499
1.293
1296 | Chem. Commun., 2006, 1295–1297
This journal is ß The Royal Society of Chemistry 2006