This organometallic system is particularly well suited for the
preparation of a single molecule nanomotor. Free rotation
around the ruthenium(II) centre allows movement of the
cyclopentadienyl upper platform (rotor) with respect to the
tripodal ligand (stator) which is intended to be deposited on a
surface after proper functionalisation. Work is underway to
control the direction of the rotation.
We thank the CNRS, the European Union and the University
of Toulouse for financial support and the French Ministry of
National Education for a fellowship to AC.
Notes and references
+
+
1
†
(
1: MS (DCI /NH
250 MHz, CD Cl
NMR (66 MHz, CDCl
3
): m/z 1037 (100%, [M+NH
): d (ppm) = 7.2–7.4 (m, 12H), 6.7–6.9 (m, 8H); 13C-
) d (ppm) = 147.74; 140.86; 134.00; 132.48; 132.06;
31.83; 131.74; 131.47; 131.41; 131.14; 129.09; 127.95; 122.45; 122.24;
4
] , calc 1037) ; H-NMR
2
2
3
1
1
(
+
+
22.15. 2: MS (DCI /NH
KBr/cm ) 2003, 2048 ; H-NMR (250 MHz, CD
3
1
): m/z 1096 (100%, [M+NH
4
] , calc 1096); IR
): d (ppm) = 7.2–7.3
21
2
Cl
2
Fig. 2 1H-NMR (CD
Cl , 250 MHz) spectra of 3 (bottom) compared to
2 2
3
3
13
(
AAABBA, 10H, J = 8.7 Hz), 6.8–6.9 (AAABBA, 10H, J = 8.7 Hz); C-
) d (ppm) = 196.40; 134.45; 132.22; 128.61; 124.03;
4Bo
Ru(cp)(Tp ) (top) at 25 °C.
NMR (66 MHz, CDCl
3
+
+
1
1
06.02. 3: MS (DCI /NH
NMR (250 MHz, CD Cl ): d (ppm) = 8.01 (dd, 3H, J = 8.6 Hz, J = 0.8
Hz), 7.86 (d, 3H, J = 0.8 Hz), 7.34–7.44 (m, 6H); 7.17–7.27 (m, 20H) ,
3
): m/z 1305 (100%, [M+H] , calc 1305) ; H-
1
The H-NMR spectrum of 3 (Fig. 2) shows that, just like in
3
4
2
2
the solid state, the two ligands also fit into each other in
solution. Compared to the spectrum with the non substituted
4
3
3
4
13
7.02 (ddd, 3H, J = 7.1 Hz, J = 6.9 Hz, J = 0.8 Hz); C-NMR (66 MHz,
CDCl ) d (ppm) = 143.60; 140.42; 135.27; 132.27; 130.78; 126.77; 123.07;
cyclopentadienyl ligand : Ru(cp)(Tp4Bo) which we have also
3
1
21.99; 120.70; 120.06; 111.58; 87.20. CV (V/SCE) ERuII/RuIII +0.78 rev.
synthesised, the spectrum of 3 shows striking differences.
Protons 1 and 2 (see numbering scheme on Fig. 3) are
significantly shielded from 8.62 to 7.86 ppm for protons 1 and
from 7.60 to 7.39 ppm for protons 2. This shielding is explained
by the location of these protons in the shielding cones of the p-
bromophenyl rings, evidencing the two ligands fitting into each
other. The rotational freedom of the cp ring has been evidenced
UV/Vis (CH Cl ): lmax (e) 295 (300 300), 311 (268 700), 396
2
2
=
(34 800).
1
2
Technomimetic Molecules part 1 see : G. Jimenez-Bueno and G.
Rapenne, Tetrahedron Lett., 2003, 44, 6261.
(a) T. C. Bedard and J. S. Moore, J. Am. Chem. Soc., 1995, 117, 10662;
(b) K. Tashiro, T. Fujiwara, K. Konishi and T. Aida, Chem. Commun.,
1998, 1121; (c) M. Ikeda, M. Takeuchi, S. Shinkai, F. Tani, Y. Naruta, S.
Sakamoto and K. Yamaguchi, Chem. Eur. J., 2002, 8, 5542.
S. Trofimenko, Scorpionates : The Coordination Chemistry of Poly-
pyrazolylborate Ligands, Imperial College Press, London, 1999.
R. S. Koefod and K. R. Mann, Inorg. Chem., 1991, 30, 541.
N. G. Connelly and I. Manners, J. Chem. Soc., Dalton Trans., 1989, 30,
1
by H-NMR since the three indazolyl groups are equivalent as
shown on Fig. 2. The p-bromophenyl rings are also free to
rotate, as evidenced by the chemical equivalence of the two
ortho protons (H ) and of the two meta protons (H ). These
o m
3
4
5
protons are referred to as an AAABBA spin system. Variable
1
temperature H-NMR from 290 °C to 120 °C did not show any
2
83–288.
significant differences in terms of equivalence of protons. The
rotation barrier could therefore not be measured and must be
6
(a) A. L. Rheingold, B. S. Haggerty, G. P. A. Yap and S. Trofimenko,
Inorg. Chem., 1997, 36, 5097; (b) C. Janiak, S. Temizdemir and S.
Dechert, Inorg. Chem. Commun., 2000, 3, 271.
2
1
low ( < 10 kcal.mol ).
If we confront these NMR data with the X-ray structure
which showed that the two ligands were interpenetrated, the
rotation of the cp ring should only be possible if the p-
bromophenyl groups tipped over to settle in the vacant spaces of
the tripodal ligand. In Fig. 3. is represented the secondary
rotation of the p-bromophenyl rings (action 2) induced by the
rotation of the upper cp ligand (action 1).
7 Crystal structure analysis of 3: orange prismatic crystals suitable for X-
ray analysis (0.344 3 0.197 3 0.087 mm) were obtained by dissolution
of the compound in benzene and slow liquid diffusion of methanol.
5 6 6 6
Crystal data for C56H36BBr N Ru·2C H : M, = 1460.51, orthorhombic,
space group Pbca, a = 14.271 (2), b = 21.144 (7), c = 40.875 (5), V =
3
23
21
1
2333 (5) Å , Z = 8, rcalc = 1.573 g cm , m(MoK
a
) = 3.48 mm
.
Data were collected on a Nonius KappaCCD diffractometer using MoK
a
graphite monochromated radiation (l = 0.71073 Å) at 298 K. A total of
3381 data was collected, 0° < q < 28.00°. The diffraction power of the
8
crystals was poor, only 2938 reflections having I > 3s(I), were used for
structure determination and refinement, 16% of the unique data was
observed. Only Ru and Br atoms were refined anisotropically. H atoms
were introduced as fixed contributors. The structure was solved using
direct methods and refined against ¡F¡. Absorption corrections were
applied. Large residual electron density peaks have been obtained in the
refinement which are located on the Ru atom. For all computations the
Brücker maXus software package8 was used. Final results : R(F) =
0
.088, Rw(F) = 0.139, GoF = 4.39. CCDC 207452. See http://
www.rsc.org/suppdata/cc/b3/b307577j/ for crystallographic data in .cif
or other electronic format.
8
S. Mackay, C. J. Gilmore, C. Edwards, N. Stewart and K. Shankland,
maXus, Computer program for the solution and refinement of crystal
structures; Nonius, Delft, The Netherlands; MacScience, Japan, the
University of Glasgow, 1999.
Fig. 3 Representation of the secondary rotation: the rotation of the upper cp
ligand (action 1) results in the paddles tipping over (action 2). The
1
numbering scheme for the H-NMR is also given.
CHEM. COMMUN., 2003, 2434–2435
2435