320
A.D. Burrows et al. / Journal of Organometallic Chemistry 573 (1999) 313–322
cm−1
.
FAB-MS+: m/6=949 {[M]+}, 822 {[Pd2
maining yellow powder was recrystallized from a
toluene/diethyl ether mixture and cooled slowly to
4°C (0.302 g, 89%). Some of these crystals were suit-
able for a single-crystal X-ray analysis. Anal. Calc.:
C, 63.0%; H, 5.3% (C59H56O3P2Pd2S requires: C,
63.2%; H, 5.0%). wmax/cm−1 1606 (CꢁO), 1195 (SO2),
1054 (SO2). lP ((CD3)2CO) 2.8 (s). FAB-MS+: m/6=
1120 {[M]+}, 822 {[Pd2(PBz3)2]+}, 731 {[Pd2(PBz3)
(PBz2)]+}.
(PBz3)2]+}, 731 {[Pd2(PBz3)(PBz2)]+}.
4.2.5. [Pd2(v-dba)(v-SO2)(PBz3)2] 5
PBz3 (184 mg, 0.60 mmol) was dissolved in toluene
(15 ml) and SO2 gas was bubbled through for 1 min.
This solution was then added to a solution of
[Pd2(dba)3].C6H6 (300 mg, 0.30 mmol) in toluene (25
ml), and SO2 gas bubbled through the solution for 10
min whereupon the colour of the solution had
changed from deep purple to red. The mixture was
stirred under an atmosphere of SO2 for a further 30
min to ensure completion of the reaction. The solvent
was removed under reduced pressure and the yellow-
red residue was washed with two successive 30 ml
portions of ethanol to remove the free dba. The re-
4.3. Crystallography
X-ray intensity data for compounds 1, 4 and 5
were collected on
a
Siemens P4 diffractometer
equipped with a Siemens LT2 low temperature device,
using graphite Mo–Kh radiation and a ꢀ−2q scan.
The crystal data, data collection and refinement are
summarised in Table 6. In all cases, three standard
reflections measured after every 97 reflections showed
no significant variation in intensity throughout data
collection. The data were corrected for Lorentz and
polarisation factors and absorption effects.
Table 5
˚
Selected bond lengths (A) and angles (°) for 5
˚
Bond lengths (A)
Pd(1)–Pd(2)
Pd(1)–P(1)
Pd(1)–C(11)
Pd(1)–C(12)
Pd(1)–S(1)
2.885(2)
2.325(4) Pd(2)–P(2)
2.232(13) Pd(2)–C(21)
2.334(13) Pd(2)–C(22)
2.246(4) Pd(2)–S(1)
1.458(11) S(1)–O(1)
1.84(2) P(2)–C(21A)
1.856(14) P(2)–C(21B)
1.82(2) P(2)–C(21C)
1.26(2) C(1)–C(11)
1.49(2) C(11)–C(12)
1.49(2) C(13)–C(14)
1.43(2) C(14)–C(15)
1.39(2) C(16)–C(17)
1.35(2) C(21)–C(22)
1.47(2)
2.335(4)
2.242(12)
2.35(2)
2.252(4)
1.473(10)
1.806(14)
1.838(14)
1.874(14)
1.42(2)
1.41(2)
1.38(2)
1.36(2)
1.45(2)
4.3.1. Structure solution and refinement [14]
The structures of compounds 1, 4 and 5 were
solved by direct methods which revealed nearly all the
non-hydrogen atoms and, in each case, the remaining
non-hydrogen atoms were located from subsequent
difference-Fourier syntheses. In the asymmetric unit
of 4, two molecular units were observed. In 1 and 5,
all the phenyl rings were constrained to refine as reg-
ular hexagons. In both cases, the phenyl hydrogen
atoms were placed in idealised position with displace-
ment parameters equal to 1.2 Ueq of the parent car-
bon atom of the phenyl groups. In 4, the methylene
hydrogen atoms were also placed in idealised geome-
try but their assigned displacement parameters were
equal to 1.5 Ueq of the parent carbon atom. For all
three compounds 1, 4 and 5, empirical absorption
corrections were applied to the data after initial refin-
ement with isotropic displacement parameters for all
atoms [15]. In 1, a total of 12 residual peaks, each ca.
S(1)–O(2)
P(1)–C(11A)
P(1)–C(11B)
P(1)–C(11C)
C(1)–O(11)
C(1)–C(21)
C(12)–C(13)
C(13)–C(18)
C(15)–C(16)
C(17)–C(18)
C(22)–C(23)
1.40(2)
Bond angles (°)
Pd(1)–S(1)–Pd(2)
O(2)–S(1)–Pd(1)
O(2)–S(1)–Pd(2)
P(1)–Pd(1)–Pd(2) 139.10(11) P(2)–Pd(2)–Pd(1)
S(1)–Pd(1)–Pd(2) 50.19(10) S(1)–Pd(2)–Pd(1)
C(11)–Pd(1)–Pd(2) 84.0(3)
C(12)–Pd(1)–Pd(2) 118.9(4)
C(11)–Pd(1)–S(1) 132.2(3)
79.80(12) O(2)–S(1)–O(1)
112.7(5)
117.4(4)
113.9(6)
O(1)–S(1)–Pd(1)
O(1)–S(1)–Pd(2)
116.9(4)
112.1(5)
140.25(11)
50.01(9)
83.7(4)
113.4(3)
133.5(4)
91.21(14)
159.4(4)
135.3(4)
101.8(4)
35.4(5)
C(21)–Pd(2)–Pd(1)
C(22)–Pd(2)–Pd(1)
C(21)–Pd(2)–S(1)
1 e A−3, in a planar disposition, were assigned as a
˚
severely disordered benzene ring, one of the solvent
molecules used in the reaction, this disorder accounts
for the poor diffraction by the crystal. In all cases, all
non-hydrogen atoms were assigned anisotropic dis-
placement parameters in the final cycles of full-matrix
least-squares refinement, based on F2.
S(1)–Pd(1)–P(1)
S(1)–Pd(1)–C(12) 168.0(4)
C(11)–Pd(1)–P(1) 134.1(3)
93.64(14) S(1)–Pd(2)–P(2)
S(1)–Pd(2)–C(22)
C(21)–Pd(2)–P(2)
P(2)–Pd(2)–C(22)
C(21)–Pd(2)–C(22)
C(22)–C(21)–Pd(2)
C(1)–C(21)–Pd(2)
C(21)–C(22)–Pd(2)
P(1)–Pd(1)–C(12)
98.3(3)
C(11)–Pd(1)–C(12) 35.9(5)
C(12)–C(11)–Pd(1) 76.0(8)
C(1)–C(11)–Pd(1) 89.8(9)
C(11)–C(12)–Pd(1) 68.1(7)
76.6(8)
96.1(8)
67.9(8)
C(23)–C(22)–Pd(2) 121.9(10) C(13)–C(12)–Pd(1)
C(11)–C(1)–C(21) 113.6(14) O(11)–C(1)–C(21)
O(11)–C(1)–C(11) 125.6(14) C(22)–C(21)–C(1)
C(12)–C(11)–C(1) 123.0(14) C(21)–C(22)–C(23)
C(11)–C(12)–C(13) 121.8(14)
115.1(9)
121(2)
125(2)
Acknowledgements
121.7(14)
We thank EPSRC for financial support and BP plc
for endowing D.M.P.M.’s chair.