7036 Inorganic Chemistry, Vol. 35, No. 24, 1996
Huang et al.
C19H42Cl2OP2Ru. RuCl2(CO)L2 has two rotamers at temperature <
-30 °C; the 31P chemical shifts are 38.5 and 37.8 ppm with a ratio of
1:0.7 at -70 °C.
Table 1. Crystallographic Data for
[PtBu2MeH][Ru2Cl5(CO)2(PtBu2Me)2]
formula C29H63Cl5O2P3Ru2
fw ) 916.14
space group: P21/a
trans,trans,trans-RuCl2(CO)2(PtBu2Me)2 and cis,cis,trans-RuCl2-
(CO)2(PtBu2Me)2. In an NMR tube with a Teflon stopcock, 10 mg of
RuCl2(CO)(PtBu2Me)2 was dissolved in toluene-d8. After three freeze-
pump-thaw cycles, 1 atm of CO was introduced, and the brown
solution changed to light yellow within the time of mixing. 31P{1H}
NMR: 42.05 ppm (trans isomer). 1H NMR: 1.47 (vt, N ) 5.7 Hz, 6
H, PCH3), 1.35 (vt, N ) 12.3 Hz, 36 H, PCCH3) ppm. IR: ν(CO) )
1981 cm-1. The solution was then kept at 80 °C in an oil bath for 2
h, during which the solution became colorless. 31P{1H} NMR: 44.8
ppm (cis, trans isomer). 1H NMR: 1.65 (vt, N ) 8.1 Hz, 6 H, PCH3),
1.29 (vt, N ) 12 Hz, 36 H, PCCH3) ppm. IR: ν(CO) ) 2029, 1964
T ) -173 °C
a ) 16.418(2) Å
b ) 12.578(2) Å
c ) 20.044(3) Å
â ) 103.38(1)°
V ) 4026.69 Å3
Z ) 4
λ ) 0.710 69 Åa
Fcalc ) 1.511 g cm-3
µ ) 12.1 cm-1
R(Fo)b ) 0.0583
Rw(Fo)c ) 0.0601
a Graphite monochromator. b R ) ∑||Fo| - |Fc||/∑|Fo|. c Rw
)
2
[∑w(|Fo| - |Fc|)2/∑w|Fo| ]1/2 where w ) 1/σ2(|Fo|).
Table 2. Selected Distances (Å) and Angles (deg) for
[PtBu2MeH][Ru2Cl5(CO)2(PtBu2Me)2]
cm-1
.
[HPtBu2Me][Ru2Cl5(CO)2(PtBu2Me)2]. A Schlenk flask was charged
with RuCl2(CO)(PtBu2Me)2 (50 mg; 0.096 mmol) and toluene (5 mL).
After three freeze-pump-thaw cycles, 0.096 mmol of HCl gas was
condensed (-196 °C) into the flask via a gas manifold. The solution
was warmed to room temperature, and some white precipitate formed.
The solution was filtered, and the solid was washed with toluene. The
combined toluene solution was evaporated to dryness, and the residue
was recrystallized from CH2Cl2 and ether to give red crystals. Anal.
Calc (found) for C29H63Cl5O2P3Ru2: C, 38.02 (37.78); H, 6.93 (7.01).
31P{1H} NMR (C6D6): 64.3, 62.5, 28.7 ppm. 1H NMR (C6D6), ppm:
for the cation 0.94 (d, JHP ) 15.3 Hz, PCCH3), 1.54 (d, JHP ) 9.3 Hz,
PCH3); for the major anion isomer 1.43 (d, JHP ) 12.9 Hz, PCCH3),
1.45 (d, JHP ) 12.9 Hz, PCCH3), 1.48 (d, JHP ) 6.6 Hz, PCH3); for the
Distances
Ru(1)-Ru(2)
Ru(1)-Cl(3)
Ru(1)-Cl(4)
Ru(1)-Cl(5)
Ru(1)-Cl(6)
Ru(1)-P(9)
Ru(1)-C(7)
Ru(2)-Cl(3)
Ru(2)-Cl(4)
3.2988(10)
2.4264(22)
2.5144(25)
2.4857(21)
2.359(3)
2.3389(25)
1.858(12)
2.4205(22)
2.4996(23)
Ru(2)-Cl(5)
Ru(2)-Cl(19)
Ru(2)-P(22)
Ru(2)-C(20)
O(8)-C(7)
O(21)-C(20)
P(32)-Cl(19)
P(32)-Cl(4)
2.4890(22)
2.3952(27)
2.3453(23)
1.828(11)
1.088(14)
1.142(14)
3.857(3)
4.176(3)
Angles
Cl(3)-Ru(1)-Cl(4)
Cl(3)-Ru(1)-Cl(5)
80.33(8) Cl(3)-Ru(2)-P(22)
97.06(8)
98.8(3)
79.18(8)
90.13(8)
81.26(7) Cl(3)-Ru(2)-C(20)
minor anion isomer 1.37 (d, JHP ) 12.9 Hz, PCCH3), 1.51 (d, JHP
12.2 Hz, PCCH3), 1.61 (d, JHP ) 5.4 Hz, PCH3). IR (C6D6): ν(CO) )
1948, 1957 (sh) (weak) cm-1
)
Cl(3)-Ru(1)-Cl(6) 167.40(10) Cl(4)-Ru(2)-Cl(5)
Cl(3)-Ru(1)-P(9)
Cl(3)-Ru(1)-C(7)
Cl(4)-Ru(1)-Cl(5)
Cl(4)-Ru(1)-Cl(6)
Cl(4)-Ru(1)-P(9)
Cl(4)-Ru(1)-C(7)
Cl(5)-Ru(1)-Cl(6)
Cl(5)-Ru(1)-P(9)
Cl(5)-Ru(1)-C(7)
Cl(6)-Ru(1)-P(9)
Cl(6)-Ru(1)-C(7)
P(9)-Ru(1)-C(7)
Cl(3)-Ru(2)-Cl(4)
Cl(3)-Ru(2)-Cl(5)
99.10(8) Cl(4)-Ru(2)-Cl(19)
97.5(4)
Cl(4)-Ru(2)-P(22) 177.25(8)
.
78.96(8) Cl(4)-Ru(2)-C(20)
87.81(11) Cl(5)-Ru(2)-Cl(19)
92.1(4)
91.18(9)
Search for Intermediates by Low-Temperature Reactions. Typi-
cal method: An NMR tube was charged with RuHCl(CO)(PtBu2Me)2
(10 mg; 0.020 mmol) and toluene-d8 (0.5 mL). It was degassed by
three freeze-pump-thaw cycles. One equivalent of HCl gas was
introduced at -196 °C, and the tube was flame-sealed. The sealed
tube was kept in a dry ice-acetone bath with most of the tube immersed
in the bath. After the tube was shaken several times to allow mixing
of the gas and liquid, it was transferred to a precooled NMR probe.
Certain low-temperature experiments seeking to detect an adduct
between H2 and RuCl2(CO)L2 gave artifactual results due to formation
of an adduct with H2O impurity. This adduct, at -27 ppm in its 31P
178.27(8) Cl(5)-Ru(2)-P(22) 102.19(8)
91.4(4)
Cl(5)-Ru(2)-C(20) 171.1(4)
92.37(9) Cl(19)-Ru(2)-P(22) 92.23(8)
102.59(8) Cl(19)-Ru(2)-C(20) 87.4(3)
170.3(4)
92.87(10) Ru(1)-Cl(3)-Ru(2)
86.9(4)
87.1(4)
P(22)-Ru(2)-C(20)
86.6(4)
85.78(7)
82.28(7)
83.07(6)
177.4(11)
Ru(1)-Cl(4)-Ru(2)
Ru(1)-Cl(5)-Ru(2)
80.75(8) Ru(1)-C(7)-O(8)
81.31(7) Ru(2)-C(20)-O(21) 175.2(10)
1
Cl(3)-Ru(2)-Cl(19) 169.10(9)
NMR, showed a temperature-dependent H NMR signal in the range
3.14-3.42 ppm for the water protons. In contrast, dry sources of H2
gave no change in the 31P NMR spectrum in the temperature range
-50 to -120 °C (in Freons).
correction was applied (range 0.71-0.91). The structure was solved
by locating the Ru atoms in the best E map from MULTAN-78. The
remaining non-hydrogen atoms were located in successive iterations
of least-squares refinement followed by difference Fourier calculations.
Following initial refinement, many of the hydrogen atoms were evident,
at least one on each methyl group. Hydrogen atoms were then
introduced in fixed idealized positions and assigned a thermal parameter
of 1.0 plus the isotropic equivalent of the parent atom. During the
refinement, abnormally short C-O distances were noticed in the two
carbonyl groups (C(7)-O(8) and C(20)-O(21)), as well as elongated
thermal ellipsoids on the carbon atoms in these groups. A disorder
between CO and Cl was suspected and resolved. At the predominantly
CO site, the disorder is 85% CO and 15% Cl for Cl(42) and Cl(43). A
similar disorder would then be expected at the terminal Cl sites (Cl(6)
and Cl(19)); however, it was not possible to observe the 15% C and O
positions in a difference map computed after the occupancy of the Cl
atoms had been refined to approximately 85%. The final cycles of
full-matrix least-squares refinement were then completed using aniso-
tropic thermal parameters on non-hydrogen atoms, except for C(7),
O(8), C(20), O(21), Cl(42), and Cl(43), which were refined with
isotropic thermal parameters. Hydrogen atoms were fixed, and the final
R(F) was 0.058 for the full unique data. The final difference map was
essentially featureless, the largest peak was 1.33 e/Å3 in the vicinity of
Ru(1), and the deepest hole was -1.35 e/Å3. The results of the structure
determination are shown in Table 2 and Figure 1.
Reaction of RuCl2(CO)(PtBu2Me)2 with 0.5 equiv of HCl. To a
benzene solution of 10 mg of RuCl2(CO)(PtBu2Me)2 was added 0.01
mmol of HCl gas. The color changed from brown to orange. 31P{1H}
NMR: 64.3, 62.6 ([Ru2Cl5(CO)2(PtBu2Me)2]-) 22.0 ppm (coalesced
peak of [HPtBu2Me]+ and PtBu2Me).
Reaction of RuCl2(CO)(PtBu2Me)2 with H2 in the Presence of
NEt3. Into a degassed benzene solution of 10 mg of RuCl2(CO)-
(PtBu2Me)2 and 3 µL of NEt3 was introduced 1 atm of H2. After
mixing,
a
white precipitate formed. 31P{1H} NMR showed
RuHCl(CO)(PtBu2Me)2 as the only phosphine-containing product (50.1
1
ppm); this was further confirmed by H NMR.
X-ray Structure Determination of [HPtBu2Me][Ru2Cl5(CO)2-
(PtBu2Me)2]. A suitable single crystal (plate) was selected from the
bulk sample using inert-atmosphere handling techniques (nitrogen-filled
glovebag).7 The crystal was attached to a glass fiber using silicone
grease and then transferred to a goniostat where it was cooled to -173
°C for characterization and data collection. A systematic search of
selected regions of reciprocal space yielded a set of reflections which
exhibited 2/m diffraction symmetry. The systematic extinctions of h0l
for h ) 2n + 1 and of 0k0 for k ) 2n + 1 uniquely identified the
space group as P21/a (No. 14). This choice was confirmed by the
subsequent solution and refinement of the structure. Data collection
(6 < 2θ < 45°) was undertaken as detailed in Table 1; an absorption
Reaction of RuCl2(CO)(PtBu2Me)2 with PhCCH. To a benzene
solution of 10 mg (0.02 mmol) of RuCl2(CO)(PtBu2Me)2 was added 3
µL (0.02 mmol) of PhCCH. After 5 min at room temperature, 31P{1H}
(7) Huffman, J. C.; Lewis, L. N.; Caulton, K. G. Inorg. Chem. 1980, 19,
2755.