C. Sravani et al. / Polyhedron 62 (2013) 169–178
171
[15] refining on F2. Packing diagrams were produced using the pro-
gram PovRay and graphic interface X-seed [16]. All non-H atoms
were refined anisotropically. All the hydrogen atoms, except the
amino hydrogens H1A and H1B, were included in idealized posi-
tions in a riding model with Uiso set at 1.2 or 1.5 times those of
the parent atoms. H1A and H1B were located by difference Fourier
methods and refined independently with a simple bond length
constraint. The structure was refined successfully with R = 0.0238.
(CCDC number 900110) [16]: C28H16O13P2PtRu4, M.w.t = 1221.
72 g molꢀ1, monoclinic, space group P21/c, a = 9.4382(2) Å, b =
11.4153(3) Å, c = 31.4264(6) Å, = 90°, = 95.801(2)°, = 90°, V = 33
68.54(13) Å3, Z = 4, calcd = 2.409 Mg/m3, T = 173(2) K, = 6.048 m
mꢀ1, F(000) = 2288, crystal size 0.15 ꢁ 0.14 ꢁ 0.14 mm3. Intensity
data were collected with a Nonius Kappa CCD diffractometer.
94236 reflections, 6393 independent (Rint = 0.0519), multi-scan
the GAUSSIAN basis set of the same size [19]. This combination of ba-
sis set and functional has been used successfully in previous stud-
ies of Pt and Ru complexes [20,21] Geometry optimizations were
performed without any symmetry constraints and the relative
energies were compared taking into account the total number of
molecules present. The convergence criteria for these optimiza-
tions consisted of the following threshold values: 1 ꢁ 10ꢀ5 Ha for
energy; 0.002 Ha Åꢀ1 for gradient and 0.005 Å for displacement
convergence, while a self-consistent field density convergence
threshold of 1 ꢁ 10ꢀ6 Ha was specified. All optimized geometries
were subjected to a full frequency analysis at the same level of the-
ory (GGA/PW91/DNP) to verify the nature of the stationary points.
Equilibrium geometries were characterized by the absence of
imaginary frequencies.
The phenyl substituents on the bis-phosphino ligand contain a
large number of atoms which contribute little to the electronic
structure of these complexes, and consequently they were replaced
by H atoms in the calculations to reduce the computational de-
mands of the system.
absorption correction
(SADABS), structure solution using direct
methods (SHELXS-97), structure refinement on F2 using full-matrix
least-squares procedures (SHELXL-97), R1 = 0.0238 [I > 2(I)], wR2
= 0.0449 (all data), GOF = 1.194, max./min. residual electron
density = 0.929/ꢀ0.686 e Åꢀ3 [17].1
2.2. Synthetic methodology
2.1.8. Crystallographic data for the compound [Pt2Ru(CO)2
2.2.1. Preparation of [PtRu2(CO)8(dppp)] (5)
(l-CO)3(PPh3)3] (13)
2 (256 mg, 0.3433 mmol) and [Ru3(CO)12] (220 mg, 0.3441
mmol) were dissolved in 10 mL of toluene. The reaction mixture
was then heated to 80 °C in a closed flask under reduced pressure
for 8 h. A dark colored solution was formed. The reaction was mon-
itored by 31P NMR until the completion of the reaction. All the vol-
atiles were removed by a high vacuum pump and the residue was
dissolved in 5 mL of CH2Cl2 and added to the top of a silica gel col-
umn. An orange red band was collected by eluting with a solvent
mixture of 4:1 CH2Cl2: n-hexane. The product was obtained as a
bright orange red solid (5). Yield: 319 mg (90%). M.p.: 166–
169 °C (dec.). Anal. Calc. for C35H26O8P2PtRu2 (1034.88): C, 40.67;
(CCDC number 671765) [14]: C59H45P3Ru1Pt2O5, M.w.t = 14
18 g molꢀ1, triclinic, space group P1, a = 12.5217(1) Å, b = 13.4675
(1) Å, c = 15.6595(1) Å, = 85.026(1)°, = 77.121(1)°, = 72.026(1)°,
V = 2448.23(3) Å3, Z = 2, calcd = 1.924 Mg/m3, T = 113 (2) K, = 6.15
5 mmꢀ1, F(000) = 1368, 5.70 < 2 < 51.83, (Mo k) = 0.71073 Å, crys-
tal size 0.14 ꢁ 0.18 ꢁ 0.18 mm3. Intensity data were collected [17]
with a Nonius Kappa CCD diffractometer. 61236 reflections, 9276
independent (Rint = 0.0315), multi-scan absorption correction
ꢀ
(
SADABS), structure solution using direct methods (SHELXS-97),
structure refinement on F2 using full-matrix least-squares proce-
dures (SHELXL-97), R1 = 0.0195 [I > 2(I)], wR2 = 0.0420 (all data),
GOF = 1.102, max./min. residual electron density = 0.693/
H, 2.54. Found: C, 40.48; H, 2.92%. IR (m
CO/cmꢀ1) in CH2Cl2:
2066 m, 2023vs, 1997sh, 1983s, 1960sh. 1H NMR (CDCl3) d: 6.85–
7.73 (m, 20H, Ph), 1.84–2.40 (m, 6H, P–CH2); 31P NMR (CDCl3) d:
8.35 (JPt–P = 3079 Hz). Mass Data, m/z: 1034.9 [M]+; 607.1
[(dppp)Pt]+.
ꢀ0.583 e Åꢀ3
.
2.1.9. Crystallographic data for the compound PtRu2(CO)6(l-dppm)2]
(14)
(CCDC number 670301) [14]: C56H44O6P4PtRu2ꢂ2(C6H6), M.w.t =
1490.24 g molꢀ1, monoclinic, space group P21/c, a = 15.8482(10) Å,
b = 19.7322(12) Å, c = 18.9112(12) Å, = 94.072(3)°, V = 5899.0(6)
Åꢀ3, Z = 4, calcd = 1.678 Mg/m3, T = 100(2) K, F(000) = 2952, 3.30
< 2 < 105.98, (Mo k) = 0.71073 Å, crystal size 0.33 ꢁ 0.30 ꢁ 0.19
mm3. Intensity data were collected [14] with a Bruker KAPPA APEX
II diffractometer. 258672 reflections, independent reflections
66042 [Rint = 0.0657], multi-scan absorption correction (SADABS),
structure solution using direct methods (SHELXS-97), structure
refinement on F2 using full-matrix least-squares procedures
2.2.2. Preparation of [PtRu2(CO)8(dppe)] (6)
3 (225 mg, 0.3075 mmol) and [Ru3(CO)12] (200 mg, 0.3128
mmol) were dissolved in 10 mL of toluene and then the mixture
was heated to 80 °C in a closed flask under reduced pressure for
8 h. A similar work-up procedure was used as mentioned above
to isolate an orange red solid (6). Yield: 244 mg (78%). M.p.: 85–
90 °C (dec.). Anal. Calc. for C34H24O8P2PtRu2 (1019.72): C, 40.05;
H, 2.37. Found: C, 40.79; H, 2.44. IR (m
CO/cmꢀ1) in CH2Cl2: 2063s,
2025s, 1978br, 1953m. 1H NMR (CDCl3) d: 7.34–7.98 (m, 20H,
Ph), 1.92–2.20 (m, 4H, P–CH2); 31P {1H} NMR (CDCl3) d: 61.3
(JPt–P = 3117 Hz). Mass Data, m/z: 1019.7 [M]+, 593.1 [Pt(dppe)]+.
(
SHELXL-97), R1 = 0.0395 [I > 2(I)], wR2 = 0.0629 (36020 reflections),
GOF = 1.225 max./min. transmission = 0.5965/0.4343 e Åꢀ3
.
2.2.3. Preparation of [PtRu4(CO)13(l4-PCH2CH2CH2PPh2)] (5a)
2.1.10. Computational details
All calculations were carried out using the DMol3 density func-
tional theory (DFT) code as implemented in the Accelrys Material
StudioÒ 5.0 software package [17]. The non-local generalized gra-
dient approximation (GGA) using the PW91 exchange–correlation
functional was used for geometry optimizations in all cases [18].
A double numeric, polarized split valence (DNP) basis set was used
in this study with a DFT semi-core pseudo potential to account for
relativistic effects in Ru and Pt. The size of the DNP basis set is
comparable to GAUSSIAN 6-31G⁄⁄, but the DNP is more accurate than
2 (186 mg, 0.2494 mmol) and [Ru3(CO)12] (164 mg, 0.2565
mmol) were dissolved in 10 mL of toluene. The reaction mixture
was then heated to 80 °C in a closed flask under reduced pressure
for 3 days. An intense red colored solution was formed. The 31P
NMR spectrum of the crude reaction mixture indicated the forma-
tion of 5 as a major product at 8.35 ppm (JPt–P = 3079 Hz) and a
new doublet at 13.2 ppm (JPt–P = 3126 Hz). All the volatiles were
removed by a high vacuum pump and the residue was dissolved
in 5 mL of CH2Cl2 and added to the top of a silica gel column. An
orange red band was collected by eluting with a solvent mixture
of 4:1 CH2Cl2:n-hexane. The major product, a bright orange red so-
lid (5), was obtained in 72% yield and isolated as mentioned above.
Then using CH2Cl2:n-hexane (10:1) as the eluant, an intense green
1
Crystallographic data have been deposited at the CCDC, 12 Union Road,
Cambridge CB2 1EZ, UK and copies can be obtained on request, free of charge, by
quoting the publication citation and the deposition number 670301.