Communications
Organometallics, Vol. 21, No. 5, 2002 781
31P spectra are observed at this temperature. When the
temperature is lowered, all resonances broaden, and
each of them eventually splits into two resonances with
ca. 2:1 relative intensities, except for the carbonyl
resonances, which exhibit a more complex behavior. The
relative intensities of the resonances assigned to each
of the two isomers change moderately with temperature,
so that the major isomer A is more abundant as the
temperature is lowered (ratio A:B ) 2.0 at 203 K, 2.2
at 188 K). From this we conclude that the minor isomer
B must be more abundant at room temperature, in
agreement with the averaged chemical shifts observed
at 291 K. In fact, from the averaged value of J (PC) of
the ipso carbon of PPh3, we can estimate a ratio A:B of
2:3 at 291 K.
Examination of the carbonyl resonances for 3a reveals
severe geometric differences between isomers. Isomer
B seems to have the symmetry of the hydrido complex
[Fe3(µ-H)(µ3,η2CtCtBu)(CO)9] (4) (see below), having an
AuPPh3 fragment bridging an Fe-Fe edge, as found for
[M3Au(µ3,η2-CtCtBu)(CO)9(PPh3)] (M ) Ru, Os).7,8 The
major isomer gives rise at 188 K to just two resonances
(2:1 intensity) and is consistent with the more sym-
metrical structure found for this compound in the
crystal, after allowing for rapid rotation of the Fe(CO)3
moieties of the cluster. The above proposal is consistent
with the spectroscopic properties of the alkyne reso-
nances. In fact, although chemical shifts for CR or Câ
are found in similar regions (around 185 or 140 ppm,
respectively), only the CR resonance of the major isomer
(181.3 ppm) exhibits P-C coupling (J PC ) 58 Hz).
Moreover, the large value of this coupling is fully
consistent with a carbon atom directly bonded to the
AuPPh3 fragment. Finally, the above assignment is also
consistent with the temperature dependence of the
equilibrium between isomers, as the isomer more abun-
dant at low temperature corresponds to that found in
the crystal.
F igu r e 1. View of compound 3a . Hydrogen atoms are
omitted for clarity. Selected bond lengths (Å) and angles
(deg): Fe(1b)-Fe(2), 2.702(8); Fe(1b)-Fe(3), 2.588(7);
Fe(2)-Fe(3), 2.476(2); Fe(1b)-Au(b), 2.672(8); Au(b)-C(1),
2.109(10); Fe(1b)-C(1), 1.808(9); Fe(2)-C(1), 2.027(8); Fe-
(3)-C(1), 2.001(9); Fe(2)-C(2b1), 1.92(4); Fe(3)-C(2b1),
2.054(16); C(1)-C(2b1), 1.348(18); C(1)-C(2b1)-C(2t),
137(2); Fe(1b)-Fe(3)-Fe(2), 64.44(18); Fe(2)-Fe(1b)-
Fe(3), 55.78(17); Fe(3)-Fe(2)-Fe(1b), 59.78(14); Fe(3)-
Fe(1b)-Au(b), 96.6(2); Fe(2)-Fe(1b)-Au(b), 91.4(2); C(1)-
Au(b)-P, 160.9(3); Fe(1b)-Au(b)-P, 156.6(3); Fe(1b)-
C(1)-Fe(3), 85.4(4); Fe(2)-C(1)-Fe(3), 75.9(3).
Sch em e 1
In all, the interconversion between isomers A and B
represents a reversible process of oxidative addition/
reductive elimination of an Au-C bond across a metal-
metal bond (Scheme 1). To our knowledge, this is the
first time that a process like that has been detected.3a,13
To gain further insight into the factors governing the
equilibrium between isomers for 3a , we have prepared
the related cluster [Fe3Au(µ4,η2-CtCtBu)(CO)9(PiPr3)]
(3b), which also exists in solution as a equilibrium
The coordination position of the gold fragment in 3a
is unexpected, as iron-gold clusters bearing one or more
AuPPh3 moieties usually display structures in which the
gold unit adopts either edge-bridging or face-capping
positions. Compound 3a appears to be the first example
of a mixed M3Au cluster (M ) Fe, Ru, Os) in which the
gold fragment displays this unexpected bonding mode.
As far as we know, [Fe2MAu2(µ4,η2-CtCPh)(CO)7-
(PPh3)2] (M ) Ir, Rh)11 are the only examples where a
similar coordination environment for the Au2(PPh3)2
unit has been previously observed. Moreover, it should
be noted that the structure of compound 3a contrasts
with those of the isoelectronic Ru and Os analogues
[M3Au(µ3,η2-CtCtBu)(CO)9(PPh3)],7,8 the latter having
the gold fragment bonded to the metal framework. Thus,
in a formal sense, replacement of Fe by Ru or Os favors
the oxidative cleavage of the Au-C(acetylide) bond.
In solution, 3a exists as an equilibrium mixture of
two isomers12 (labeled A and B in Scheme 1). Intercon-
version between isomers is fast at room temperature
(12) Data for 3a are as follows. 1H NMR: at 291 K in CDCl3 δ 7.61-
7.47 (m, 15H, C6H5), 1.57 (s, 9H, C(CH3)3); in CD2Cl2 at 223 K δ 7.70-
7.35 (m, 30H, C6H5), 1.54, 1.49 (2 × s, br, 2 × 9H, C(CH3)3). 13C{1H}
NMR in CD2Cl2 at 291 K: δ 214.2 (br, 6CO), 213.3 (br, 3CO), 134.3 (d,
J PC ) 14 Hz, C6H5), 132.4 (s, 4C(C6H5)), 129.8 (d, J PC ) 12 Hz, C6H5),
129.7 (d, J PC ) 55 Hz, 1C(C6H5)), 39.9 (s, C(CH3)3), 35.4 (s, CH3), alkynyl
signals are too broad to be observed. 31P{1H} NMR in CD2Cl2: at 291
K δ 50.6 (PPh3); at 223 K δ 52.2, 46.6 (PPh3). Data for isomer A are as
follows. 13C{1H} NMR in CD2Cl2 at 188 K: δ 214.9 (s, 6CO), 211.7 (s,
3CO), 181.3 (d, J PC ) 58 Hz, CR(CtCtBu)), 144.9 (s, Câ(CtCtBu)), 134.4
(d, J PC ) 14 Hz, C6H5), 132.8 (s, 4C(C6H5)), 129.9 (d, J PC ) 11 Hz, C6H5),
128.2 (d, J PC ) 59 Hz, 1C(C6H5)), 41.1 (s, C(CH3)3), 35.9 (s, CH3). Data
for isomer B are as follows. 13C{1H} NMR in CD2Cl2 at 188 K: δ 219.5
(s, 2CO), 216.7 (br, 2CO), 215.5 (s, CO), 211.7 (s, 2CO), 210.3 (s, 2CO),
193.4 (s, CR(CtCtBu)), 134.3 (d, J PC ) 15 Hz, C6H5), 132.0 (s, 4C(C6H5)),
130.9 (s, Câ(CtCtBu)), 130.2 (d, J PC ) 52 Hz (obtained from the
spectrum recorded at 223 K), 1C(C6H5)), 129.6 (d, J PC ) 11 Hz, C6H5),
38.5 (s, C(CH3)3), 33.5 (s, CH3).
1
on the NMR time scale, so that averaged H, 13C, and
(13) (a) Farrugia, L. J .; Orpen, A. G. In Metal Clusters in Chemistry;
Braunstein, P., Oro, L. A., Raithby, P., Eds.; Wiley-VCH: Weinheim,
Germany, 1999; Vol. 2, Chapter 3.4. (b) Dyson, P. J .In Metal Clusters
in Chemistry; Braunstein, P., Oro, L. A., Raithby, P., Eds.; Wiley-
VCH: Weinheim, Germany, 1999; Vol. 2, Chapter 3.5.
(10) Deabate, S.; Giordano, R.; Sappa, E. J . Cluster Sci. 1997, 8,
407.
(11) Bruce, M. I.; Koutsantonis, G. A.; Tiekink, E. R. T. J . Orga-
nomet. Chem. 1991, 408, 77.