Ru3(CO)12 in Acidic Media
Inorganic Chemistry, Vol. 35, No. 25, 1996 7219
X-ray Structure Determinations. The crystals of [fac-Ru(OCOCF3)3-
(CO)3]Cs are colorless monoclinic prisms defined by the form {011}
closed by the pinacoid {100}. One of them was glued at the end of a
glass fiber and was mounted on a Siemens P4 automatic single-crystal
diffractometer, equipped with a graphite-monochromatized Mo KR
radiation. Cell parameters were calculated on the accurately centered
setting angles of 25 strong reflections with 12.5° e θ e 13°. Details
about the crystal parameters and intensity data collection are sum-
marized in the second column of Table 1. The Laue class was
established by an automatic procedure contained in the diffractometer
control program.12 A redundant set of data was collected to estimate
the collection accuracy. Three standard reflections measured every 97
measurements showed no decay in the crystal. The space group was
univocally established as P21/c on the basis of systematic absences.
The collected intensities were corrected for Lorentz and polarization
effects and for absorption by a Gaussian integration method.13 The
equivalent reflections present in the set were then merged resulting in
The final reliability parameters are shown in Table 1, where R1, wR2,
and S have the same meaning as in the preceeding column and w )
2
2
1/[σ2(Fo ) + (0.1454P)2 + 15.38P], where P ) [max(Fo ,0) + 2Fc2]/3.
The reliability appears acceptable considering the poor quality of the
crystal and the presence of disorder.
The crystals of [RuH(CO)2(py)3][BPh4] are colorless hexagonal
prisms closed by hexagonal bipyramids. One of them was glued at
the end of a glass fiber, and its diffraction pattern was studied on a
Weissenberg camera using Cu KR radiation (λ ) 1.541 78 Å). The
pattern showed well-shaped spots displaying hexagonal symmetry and
a very long c period. The systematic extinctions suggested a primitive
lattice with a 61 or 65 operator.
Accurate cell parameters and intensity data were collected on a
Nonius CAD4 single-crystal diffractometer equipped with graphite-
monochromatized Cu KR radiation. Crystal parameters and collection
details are summarized in the fourth column of Table 1. Collection of
three standard reflections every 97 measurements allowed one to
exclude any crystal decay. The collected data were corrected for
Lorentz and polarization effects and for absorption by using a ψ-scan
method. The structure was solved by standard Patterson and Fourier
methods in the P65 space group, and the absolute configuration of the
crystal was chosen on the basis of Flack index.14 The hydrogen atoms
were introduced in calculated positions and were allowed to ride on
the connected carbon atoms. The final reliability indexes obtained in
the last least-squares cycles, with all the heavy atoms with anisotropic
thermal parameters, are shown in the last column of Table 1, where w
an internal R value (Rint ) ∑|Fo2 - Fo (mean)|/∑(Fo )) of 0.022. The
structure was solved by the automatic Patterson method contained in
the SHELXTL2 program, and the molecule was completed by means
of the next Fourier map. Disorder in the positions of the CF3 groups
was suggested by electron density maps. The disorder was explained
as a statistical distribution of the trifluoroacetate groups on two different
conformations, and two different CF3 groups were introduced in each
position imposing the sums of occupancies equal to 1.
2
2
The final refinement cycles were made with anisotropic thermal
factors for Cs, Ru, O, and C atoms and isotropic for F atoms and
imposing geometrical constraints to the CF3 modifications. The final
reliability factors are showed in Table 1, where R1 ) ∑||Fo| - |Fc||/
2
2
) 1/[σ2(Fo ) + (0.0427P)2 + 0.09P] with P ) [max(Fo ,0) + 2Fc2]/3.
All calculations and drawings were performed by using the
SHELXTL13 program.
2
2
2
∑|Fo|, wR2 ) [w(Fo - Fc2)2/w(Fo )2]1/2, and w ) 1/[σ2 (Fo ) +
2
2
(0.0636P)2 + 12.34P], with P ) [max(Fo ,0) + 2Fc2]/3 and S ) [w(Fo
Results and Discussion
- Fc2)2/(N - P)]1/2
.
The crystals of {fac-Ru(OCOCF3)2(CO)3[(CH3)2CHOH]} (4) are
colorless milky, with a prismatic shape. Some of them were sealed
within glass capillaries under a nitrogen atmosphere and were examined
on a Siemens P4 single-crystal diffractometer. All the samples appeared
to be crystalline, but not one presented a good diffraction profile. In
fact some profiles appeared to be exceedingly large and some other
showed a depression in the central part of the profile as they
corresponded to two different single crystals slightly misaligned. The
third column of Table 1 summarizes the relevant crystal data and
intensity data collection details. Cell parameters were calculated from
the setting angles of 13 accurately centered strong reflections having
8.9° e θ e 9.6°. The choice of such a low value for max, here and in
the intensities collection, has been called for by the lack of intense
diffractions at high angles.
A redundant set of data was collected to verify, on merging, the
collection reliability. Three standard reflections measured every 97
measurements allowed one to exclude any crystal decay. The collected
data were corrected for Lorentz and polarization effects, but not for
absorption, since a scanning around the ψ angle of 5 intense reflections
showed a slight effect on the measured intensity.
The space group was univocally established as P21/c by systematic
extinctions, and the structure was solved by direct methods contained
in the TREF13 procedure. However, the two CF3 groups of the
trifluoroacetate ligands and two methyl groups of isopropyl alcohol
could not be reliably localized in a rather smeared electron density
that appeared on the Fourier map. We explained this fact with the
presence of disorder both in -CF3 and in -CH(CH3)2 groups. As in
the case of the cesium salt, we have introduced two distinct idealized
-CF3 groups in each expected position of trifluoroacetate ligand and
two different -CH(CH3)2 groups in the isopropyl alcohol, assuming a
total occupancy equal to 1 for each group. The atoms found in the
Fourier map were refined with anisotropic thermal factors, while
isotropic factors have been used for the disordered atoms that have
been introduced in geometrically calculated positions and have been
refined as rigid groups. The hydrogen atoms were not introduced.
Direct Detection of Intermediates during the CF3COOH-
Cocatalyzed WGSR. We recently evidenced that the nature
of conjugated base affects the acid-cocatalyzed WGSR promoted
by Rh4(CO)12.15 A role of the conjugated base is apparent also
in the case, examined here, of the Ru3(CO)12 precursor in H2O/
diglyme solution: by comparison of two strong acids, i.e.
sulfuric and triflic, as cocatalysts for the WGSR under the same
conditions, only the former resulted in activity. Moreover, by
the employment of CF3COOH as cocatalyst in the 8 M H2O/
diglyme medium ([Ru] ) 0.036 M, [CF3COOH] ) 0.5 M, PCO
) 0.8 atm, T ) 95 °C) the TOF(H2) (TOF(H2) ) mol of H2/
mol of Ru/day) was 3 and increased to 18 on adding CF3COOCs
in a 1/5 molar ratio with respect to the acid. Such a sharp
increase of TOF(H2) demonstrates the beneficial role of
CF3COO- and can be understood by considering that CF3COOH
behaves as a weak acid in the reaction medium (κa ) 2 × 10-2
at 25 °C).16 Therefore, the addition of CF3COOCs, although
only in a 1/5 molar ratio with respect to the acid, strongly
increases the concentration of its conjugated base.
Remarkably, the CF3COO- concentration also affects the
nature of the intermediate carbonyl complexes which accumulate
during WGSR. At the low CF3COO- concentration arising
from the dissociation of CF3COOH, only dimeric Ru(I) carbo-
nyls, namely a PCO-depending equilibrium mixture of Ru2[µ-
η2-OC(CF3)O]2(CO)6 (1a) and Ru2[µ-η2-OC(CF3)O]2(CO)4L2
(L ) H2O, diglyme) (1b),11 can be detected by IR analysis after
the early stages of catalysis (Figure 1a). When the CF3COO-
concentration is substantially increased by the addition of CF3-
COOCs, however, two new absorptions (νCO 2136 and 2065
(14) Flack, H. D. Acta Crystallogr. 1983, A39, 876.
(15) Fachinetti, G.; Fochi, G.; Funaioli, T. Inorg. Chem. 1994, 33, 1719.
(16) This value was determined by fitting the 19F NMR chemical shift data
of progressively diluted CF3COOH solutions (5 × 10-1 to 5 × 10-4
M, 25 °C) in diglyme containing 8 M H2O, to equation which describes
the dependence of the concentration Co on the measured chemical
shift (Dimicoli, J. L.; Helene, C. J. J. Chem. Soc. 1973, 95, 1036),
(12) XSCANS: X-ray Single Crystal Analysis System, rel. 2.1; Siemens
Analytical X-ray Instruments Inc.: Madison, WI, 1994.
(13) Sheldrick, G. M. SHELXTL-Plus, Rel. 5.03; Siemens Analytical X-ray
Instruments Inc.: Madison, WI, 1994.
affords the value of 2 × 10-2
.