T.M. Becker et al. / Journal of Organometallic Chemistry 629 (2001) 165–170
169
from The Director, CCDC, 12 Union Road, Cam-
bridge CB2 1EZ, UK (fax: +44-1233-336-033; e-mail:
ac.uk). Structure factors are available upon request
from the authors.
Acknowledgements
CCD data was collected through the Ohio Crystallo-
graphic Consortium, funded by the Ohio Board of
Regents 1995 Investment Fund (CAP-075) located at
the University of Toledo, Instrumentation Center in
A&S, Toledo, OH 43606.
Fig. 2. Calculated bond angles and bond distance for Li+(H2O): FLi.
References
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To gain further insight of this rather unusual bond-
ing motif, we have examined the model complex Li+
(H2O):FLi, in which Mn(1) (Fig. 1) has been replaced
by Li, and Mn(2) (Fig. 1) by Li+. The optimized
structure of this model complex (see Fig. 2) has features
that are quite similar to those observed experimentally
for 2. When Li+ is bonded to one H2O molecule, the
hydrated ion Li+:H2O has C26 symmetry, with Li+
positioned at the negative end of the water dipole
moment vector. Thus, this species is stabilized by strong
electrostatic attractions. In the model complex Li+
(H2O):FLi, Li+ is similarly bonded to the oxygen.
Because the proton-donor in the model complex is a
cationic species, the O···F distance is very short, at
,
2.443 A, and the O–H···F hydrogen bond is essentially
linear. In addition, the O–F–Li angle is very large at
168°. This orientation does not provide the best orien-
tation for a directed lone pair on F participating in the
hydrogen bond. Rather, in small cationic complexes the
orientation of the proton acceptor molecule tends to
favor a head-to-tail alignment of the bond dipole mo-
ment of the proton donor ion with the dipole moment
of the proton acceptor molecule. In the model complex,
the hydrogen bonded O–H bond of water is lengthened
+
,
,
considerably, from 0.968A in Li (H2O) to 1.028 A in
Li+(H2O):FLi. All of these structural characteristics are
consistent with the presence of a very strong O–H···F
hydrogen bond, which has a computed MP2/aug’-cc-
pVTZ binding energy (DEe) of −38.7 kcal mol−1, and
a binding enthalpy (DH°) of −37.6 kcal mol−1
.
[19] D.E. Woon, T.H. Dunning Jr, J. Chem. Phys. 98 (1993) 1358.
[20] M.J. Frisch, G.W. Trucks, H.B. Schlegel, G.E. Scuseria, M.A.
Robb, J.R. Cheeseman, V.G. Zakrzewski, J.A. Montgomery Jr.,
R.E. Stratmann, J.C. Burant, S. Dapprich, J.M. Millam, A.D.
Daniels, K.N. Kudin, M.C. Strain, O. Farkas, J. Tomasi, V.
Barone, M. Cossi, R. Cammi, B. Mennucci, C. Pomelli, C.
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Cui, K. Morokuma, D.K. Malick, A.D. Rabuck, K.
Raghavachari, J.B. Foresman, J. Cioslowski, J.V. Ortiz, A.G.
4. Supplementary material
Crystallographic data (excluding structure factors)
for the structural analysis have been deposited with the
Cambridge Crystallographic Data Centre, CCDC no.
156936. Copies of this information may be obtained