Alkynes react wit
h a suspension of [W
2(OCH
2tBu)
8](M=M) in
hydrocarbon solvents to givealkyne adducts W
2(
-RCCR')(OCH
2tBu)
8, w
here R = H and R' = P
h, Me, Me
3Si and R = Meand R' = Me and P
h. For P
hC
CH, t
here is a
-perpendicular mode of alkyne bonding,
hars/t
heta.gif" BORDER=0 > =84
, but for MeC
CH and MeC
CMe, t
he bridging alkyne is distinctly skewed wit
h respectto t
he W-W axis,
hars/t
heta.gif" BORDER=0 > = 64
and 67
, respectively. In contrast, t
he P
hC
CMe adduct
has t
healkyne bonded to only one tungsten,
hars/eta.gif" BORDER=0 >
2-P
hC
CMe, wit
h t
he alkyne C
C axis being 30
from t
he W-W axis. In all of t
hese structures, t
here are alkoxide bridges, and t
he dinuclearunit
may be viewed as a confacial biocta
hedron w
here eit
her one alkyne and two alkoxidesor t
hree alkoxides occupy t
he bridging face. In toluene-
d8, NMR spectroscopic studies indicatet
hat certain of t
hese alkyne adducts (MeC
CH, MeC
CMe, P
hC
CMe, and Me
3SiC
CH)exist as a mixture of alkyne-bridged and
hars/eta.gif" BORDER=0 >
2-alkyne-bonded isomers. T
he isomers are fluxionalon t
he NMR time scale by rapid exc
hange of terminal and bridging alkoxide groups. However,
-
hars/eta.gif" BORDER=0 >
2 alkyne exc
hange is slow on t
he NMR time scale. T
he structural data are comparedwit
h electronic structure calculations employing density functional t
heory on modelcompounds of formula W
2(alkyne)(OMe)
8. T
he calculations suggest t
hat a
-parallel modeof bonding is energetically favorable relative to
-perpendicular and, furt
her, t
hat t
he energydifference between bridge and terminal alkyne adducts is, in all cases, less t
han 5 kcal mol
-1.