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In the title compound, [Pt(C18H15P)(C28H28P2S)]­(ClO4)2·­C3H6O or [Pt(PPh3)(PSP)](ClO4)2·CH3COCH3, where PSP is the potentially tridentate chelate ligand bis(2-di­phenyl­phosphinoethyl) sulfide, all three donor groups of the PSP ligand are coordinated to the central Pt atom, with Pt—P = 2.310 (1) Å and Pt—S = 2.343 (1) Å. The fourth coordination site is occupied by the P donor of the tri­phenyl­phosphine ligand [Pt—P = 2.289 (1) Å]. The complex cation has exact mirror symmetry, with the S atom, the Pt atom and the P atom of the PPh3 ligand in the mirror plane. The Pt atom has a distorted square-planar coordination geometry. A π–π interaction is present between the phenyl rings of the PPh3 ligand and the terminal –PPh2 group of the PSP chelate.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270102009186/gg1116sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270102009186/gg1116Isup2.hkl
Contains datablock I

CCDC reference: 192943

Comment top

A range of platinum complexes of phosphinothioether chelate ligands have been found to serve as efficient catalysts in homogeneous hydrogenation, carbonylation and asymmetric allylic alkylation reactions (Bayón et al., 1999; Dilworth et al., 1995; Sugama et al., 2001). In addition, the synthesis and characterization of PtII complexes of mixed P,S polydentate chelate ligands, these being acyclic or macrocyclic ligands, have attracted significant attention (Andreasen et al., 1999; Connolly et al., 1997; Kyba et al., 1987; Siah et al., 1994). The systematic geometric variation of the respective P and S donors within these ligands has provided insight into the trans influence of chelated phosphines on chelated thioethers and vice versa.

In the current investigation by us of the relationship between structure and reactivity of tridentately chelated PtII complexes, several complexes of the tridentate phosphinothioether chelate ligand PSP have been prepared and characterized (Andreasen et al., 1999; Andreasen; 2000). Two of these PtII—PSP complexes, [Pt(PSP)Cl]ClO4 and [Pt(PSP)I]I, have been characterized by X-ray diffraction (Andreasen et al., 1999). We present here the X-ray structure of a third such complex, the title compound, (I). \sch

Complex (I) contains PPh3 trans to the central thioether chelate donor; the molecular structure of the cation of (I) is shown in Fig. 1. The three donors of the PSP chelate ligand, the S and the two tertiary phosphine groups, are all coordinated to the Pt atom, forming two five-membered chelate rings, with the PPh3 donor occupying the fourth coordination site. The [Pt(PSP)(PPh3)]2+ cation has exact mirror symmetry with atoms S, Pt and P1 of the PPh3 ligand in the mirror plane.

The coordination sphere of the [Pt(PSP)(PPh3)]2+ cation is tetrahedrally distorted from planar geometry, with the two PSP P atoms (P2 and P2') deviating by 0.075 Å to the one side of the least-squares plane through the S and P donor atoms, while the remaining two donors, i.e. the PSP S and the PPh3 P1, are located on the opposite side of this plane at 0.085 and 0.064 Å, respectively. The Pt atom is 0.04 Å from the plane on the same side as the S and PPh3 P atoms. This tetrahedral distortion is, however, less pronounced than that in the [Pt(PSP)Cl]+ and [Pt(PSP)I]+ complexes.

In addition to the two ClO4- counter-anions, which are centred 4.950 (2) and 6.422 (2) Å from the closest Pt atom, a molecule of acetone has co-crystallized in (I). This acetone solvate is located close to the PPh3 group, with a shortest distance to a phenyl ring C atom for O7···C26 of 3.293 (5) Å.

The P1—Pt—S bond angle of 178.29 (4)° is close to the ideal value of 180°, while the P2—Pt—P2' angle of 161.57 (5)° is significantly bent. The large steric demand of the PPh3 group is indicated by the large cis P—Pt—P angles between the –PPh2 and the PPh3 groups; P1—Pt—P2 is 98.79 (2)°, exceeding the reported cis P—Pt—I angles in the [Pt(PSP)I]+ cation, in spite of the fact that I is likewise a sterically demanding ligand. The cis P—Pt—P angles for (I) are, however, not unusual in complexes having two non-chelated mutually cis phosphine ligands (Battan et al., 1999). This steric crowding is illustrated further by the smallest P—Pt—S angles [P2—Pt—S 81.30 (2)°] yet observed in the five-membered chelate ring of PtII—PSP complexes.

The mirror plane of the cation in (I) results in equal Pt—P bond lengths [Pt—P2 2.310 (1) Å] and this Pt—P distance is within the normal range observed for two mutually trans –PPh2 donors (Andreasen et al., 1999; Siah et al., 1994). The Pt—S bond length in (I) [Pt—S 2.343 (1) Å] is approximately 0.09 Å longer than the Pt—S bonds in the PtII—PSP salts [Pt(PSP)Cl]ClO4 and [Pt(PSP)I]I, which is in line with the larger trans influence of the PPh3 donor compared with Cl or I. Only scant information is available on bond distances in PtII complexes having the trans S—Pt-PPh3 motif, with S being both a monodentate thioether ligand and a part of a chelate system; one example is [Pt({iPrS(CH2)3}2S)(PPh3)](BF4)2 [{iPrS(CH2)3}2S is 2,12-dimethyl-3,7,11-trithiatridecane, C12H26S3; Loeb & Mansfield, 1996]. The Pt—S distance in (I) is similar to the values for chelated thioether donors in the trans position both to PPh3 in [Pt({iPrS(CH2)3}2S)(PPh3)]2+ (Loeb & Mansfield, 1996) and to intraligand –PPh2 donors (Connolly et al., 1997).

The Pt—P bond length in (I) to the coordinated PPh3 ligand [Pt—P1 2.289 (1) Å] is significantly shorter than the reported Pt-PPh3 distance of 2.332 (2) Å in [Pt({iPrS(CH2)3}2S)(PPh3)]2+, where the PPh3 donor is also positioned trans to a chelated thioether group. The latter length, however, is longer than the Pt—P distance in trans-[PtI2(PPh3)2] [2.318 (2) Å; Boag et al., 1991]. This is remarkable, since it is generally accepted that the trans influence of PPh3 is greater than that of a thioether group (Connolly et al., 1997).

In (I), the PPh3 phenyl ring C21—C26 and the phenyl ring C41—C46 of PSP are positioned so that they are approximately slipped-parallel and only tilted by 3°, with a C21···C41 separation of 3.370 (5) Å for the two Cipso atoms. This magnitude is similar to the calculated optimum distance of 3.5 Å obtained for slipped-parallel benzene dimers, as reported in a recent computational calculation by Tsuzuki et al. (2002). This indicates that a ππ interaction may exist between the phenyl rings of PPh3 and PSP, and the C21···C41 distance is in the range reported for overlap between arene moieties (Breu et al., 1997; Fanizzi et al., 1994).

Experimental top

Compound (I) was prepared as previously reported by Andreasen et al. (1999). Colourless crystals suitable for single-crystal X-ray diffraction were grown by slow diffusion of diethyl ether into an acetone/methanolic solution of (I).

Refinement top

The H atoms were kept fixed at calculated positions, with C—H = 0.95 Å and Uiso(H) = 1.2Ueq for the atoms to which they were attached. Refinement of (I) in the centrosymmetric space group Pnma gave very elongated displacement ellipsoids for atom C1. This elongation could either result from disorder or from a wrong choice of space group. Solving and refining the structure in the polar space group Pna21 gave many non-positive definite displacement ellipsoids and refinement of the polarity gave a Rogers factor (Rogers, 1981) close to zero instead of ±1, indicating that the structure was non-polar. The structure was therefore refined in Pnma with C1 split over two sites, C1A and C1B, each with 50% site occupancy.

Computing details top

Data collection: SMART (Siemens, 1995); cell refinement: SAINT (Siemens, 1995); data reduction: SAINT; program(s) used to solve structure: SIR97 (Altomare et al., 1996) and KRYSTAL (Hazell, 1995); program(s) used to refine structure: modified ORFLS (Busing et al., 1962) and KRYSTAL; molecular graphics: ORTEPIII (Burnett & Johnson, 1996) and KRYSTAL; software used to prepare material for publication: KRYSTAL.

Figures top
[Figure 1] Fig. 1. A view of the cation of (I) showing the labelling of the non-H atoms. Displacement ellipsoids are shown at the 50% probability level and H atoms have been omitted for clarity [symmetry code: (i) x, 1/2 - y, z].
[Bis(2-diphenylphosphinoethyl) sulfide-κ3P,S,P'](triphenylphosphine- κP)platinum(II) diperchlorate acetone solvate top
Crystal data top
[Pt(C28H28P2S)(C18H15P)](ClO4)2·C3H6OF(000) = 2352
Mr = 1172.84Dx = 1.621 Mg m3
Orthorhombic, PnmaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2nCell parameters from 8192 reflections
a = 15.698 (3) Åθ = 2.0–30.4°
b = 15.337 (3) ŵ = 3.23 mm1
c = 19.957 (4) ÅT = 120 K
V = 4804.9 (16) Å3Octahedron, colourless
Z = 40.26 × 0.24 × 0.24 mm
Data collection top
Siemens SMART CCD area-detector
diffractometer
7613 independent reflections
Radiation source: X-ray tube5723 reflections with I > 3σ(I)
Graphite monochromatorRint = 0.054
ω rotation scans with narrow framesθmax = 30.5°, θmin = 2.0°
Absorption correction: integration
XPREP (Siemens, 1995)
h = 1621
Tmin = 0.448, Tmax = 0.594k = 2222
41330 measured reflectionsl = 2724
Refinement top
Refinement on F0 constraints
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.032 w = 1/{[σcs(F2) + 1.03F2]1/2-|F|}2
wR(F2) = 0.036(Δ/σ)max < 0.001
S = 0.99Δρmax = 1.3 (2) e Å3
5723 reflectionsΔρmin = 1.5 (2) e Å3
329 parametersExtinction correction: B-C type 1 Lorentzian isotropic (Becker & Coppens, 1974)
0 restraintsExtinction coefficient: 88 (9)
Crystal data top
[Pt(C28H28P2S)(C18H15P)](ClO4)2·C3H6OV = 4804.9 (16) Å3
Mr = 1172.84Z = 4
Orthorhombic, PnmaMo Kα radiation
a = 15.698 (3) ŵ = 3.23 mm1
b = 15.337 (3) ÅT = 120 K
c = 19.957 (4) Å0.26 × 0.24 × 0.24 mm
Data collection top
Siemens SMART CCD area-detector
diffractometer
7613 independent reflections
Absorption correction: integration
XPREP (Siemens, 1995)
5723 reflections with I > 3σ(I)
Tmin = 0.448, Tmax = 0.594Rint = 0.054
41330 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0320 restraints
wR(F2) = 0.036H-atom parameters constrained
S = 0.99Δρmax = 1.3 (2) e Å3
5723 reflectionsΔρmin = 1.5 (2) e Å3
329 parameters
Special details top

Refinement. Sfls: F calc weight full matrix

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Pt0.31948 (1)0.250000.02781 (1)0.0127 (1)
S0.36778 (8)0.250000.08328 (6)0.0178 (6)
P10.26818 (7)0.250000.13518 (6)0.0114 (6)
P20.33400 (6)0.39869 (7)0.01321 (5)0.0202 (5)
C1A0.4141 (5)0.3558 (6)0.1004 (4)0.026 (4)0.50
C1B0.4633 (5)0.3169 (6)0.0710 (4)0.030 (4)0.50
C20.4331 (3)0.4059 (3)0.0353 (2)0.035 (2)
C110.3505 (3)0.25000.1982 (2)0.015 (2)
C120.4356 (3)0.25000.1782 (3)0.021 (3)
C130.5008 (4)0.25000.2257 (3)0.032 (3)
C140.4797 (4)0.25000.2935 (3)0.031 (3)
C150.3959 (4)0.25000.3135 (3)0.027 (3)
C160.3312 (3)0.25000.2663 (2)0.019 (2)
C210.2009 (2)0.3447 (2)0.1518 (2)0.015 (2)
C220.2140 (2)0.4011 (3)0.2053 (2)0.022 (2)
C230.1617 (3)0.4729 (3)0.2147 (2)0.028 (2)
C240.0961 (3)0.4900 (3)0.1698 (2)0.027 (2)
C250.0834 (2)0.4348 (3)0.1161 (2)0.025 (2)
C260.1352 (2)0.3626 (3)0.1066 (2)0.020 (2)
C310.2549 (3)0.4423 (3)0.0432 (2)0.027 (2)
C320.1854 (3)0.3925 (3)0.0631 (2)0.028 (2)
C330.1287 (3)0.4239 (4)0.1112 (2)0.041 (3)
C340.1423 (3)0.5049 (4)0.1391 (2)0.043 (3)
C350.2105 (4)0.5556 (3)0.1189 (2)0.041 (3)
C360.2668 (3)0.5242 (3)0.0715 (2)0.035 (3)
C410.3489 (2)0.4748 (3)0.0814 (2)0.023 (2)
C420.4181 (3)0.4610 (3)0.1250 (2)0.025 (2)
C430.4319 (3)0.5175 (3)0.1775 (2)0.031 (2)
C440.3787 (3)0.5882 (3)0.1874 (2)0.032 (2)
C450.3103 (3)0.6029 (3)0.1444 (2)0.034 (2)
C460.2957 (3)0.5456 (3)0.0915 (2)0.028 (2)
Cl10.63190 (9)0.250000.06144 (8)0.0301 (8)
Cl20.93226 (9)0.250000.21850 (7)0.0274 (7)
O10.5796 (2)0.1738 (2)0.0657 (2)0.050 (2)
O20.6888 (4)0.25000.1167 (4)0.102 (6)
O30.6820 (5)0.25000.0029 (4)0.080 (5)
O40.8527 (3)0.25000.1856 (3)0.053 (3)
O50.9969 (4)0.25000.1713 (3)0.132 (9)
O60.9389 (4)0.1760 (3)0.2598 (3)0.087 (4)
O71.0280 (3)0.25000.0058 (2)0.044 (3)
C30.9535 (4)0.25000.0183 (3)0.030 (3)
C40.9046 (4)0.1675 (4)0.0265 (3)0.048 (3)
H1Aa0.37530.38880.12680.031*0.50
H1Ab0.46570.34800.12450.031*0.50
H1Ba0.48900.32950.11300.037*0.50
H1Bb0.50300.28710.04330.037*0.50
H2a0.44680.46500.04470.042*0.50
H2b0.47890.37960.01160.042*0.50
H2a'0.42530.44870.06910.042*0.50
H2b'0.47710.42400.00570.042*0.50
H120.44920.25000.13180.026*
H130.55880.25000.21200.038*
H140.52360.25000.32620.037*
H150.38230.25000.35990.033*
H160.27340.25000.28040.023*
H220.25930.39030.23570.026*
H230.17070.51050.25190.034*
H240.06020.53930.17610.032*
H250.03870.44640.08530.030*
H260.12610.32520.06930.024*
H320.17640.33670.04370.034*
H330.08120.38980.12470.049*
H340.10450.52610.17240.052*
H350.21860.61200.13760.049*
H360.31400.55890.05820.042*
H420.45510.41280.11820.030*
H430.47830.50790.20710.037*
H440.38880.62680.22370.038*
H450.27400.65160.15110.040*
H460.24900.55520.06210.034*
H4a0.84690.17690.01410.057*
H4b0.92860.12360.00120.057*
H4c0.90700.14940.07200.057*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pt0.0111 (1)0.0160 (1)0.0109 (1)0.00000.0006 (1)0.0000
S0.0156 (6)0.0252 (7)0.0125 (5)0.00000.0012 (4)0.0000
P10.0100 (5)0.0122 (6)0.0119 (5)0.00000.0005 (4)0.0000
P20.0262 (5)0.0191 (5)0.0153 (4)0.0059 (4)0.0010 (3)0.0033 (3)
C1A0.029 (4)0.031 (5)0.018 (4)0.003 (4)0.011 (3)0.003 (3)
C1B0.020 (4)0.048 (6)0.023 (4)0.009 (4)0.006 (3)0.005 (4)
C20.042 (2)0.036 (2)0.026 (2)0.018 (2)0.013 (2)0.002 (2)
C110.013 (2)0.014 (2)0.018 (2)0.0000.002 (2)0.000
C120.019 (2)0.019 (3)0.026 (3)0.0000.002 (2)0.000
C130.016 (3)0.040 (4)0.040 (4)0.0000.008 (2)0.000
C140.032 (3)0.030 (3)0.031 (3)0.0000.019 (3)0.000
C150.038 (3)0.023 (3)0.021 (3)0.0000.013 (2)0.000
C160.023 (3)0.018 (3)0.017 (2)0.0000.003 (2)0.000
C210.013 (1)0.014 (2)0.019 (2)0.002 (1)0.003 (1)0.001 (1)
C220.023 (2)0.024 (2)0.019 (2)0.005 (2)0.001 (1)0.001 (2)
C230.037 (2)0.020 (2)0.028 (2)0.006 (2)0.003 (2)0.005 (2)
C240.024 (2)0.024 (2)0.032 (2)0.008 (2)0.007 (2)0.000 (2)
C250.020 (2)0.023 (2)0.031 (2)0.003 (2)0.001 (2)0.005 (2)
C260.016 (2)0.022 (2)0.022 (2)0.000 (1)0.001 (1)0.002 (2)
C310.041 (2)0.025 (2)0.014 (2)0.001 (2)0.002 (1)0.002 (2)
C320.029 (2)0.032 (2)0.024 (2)0.009 (2)0.000 (2)0.007 (2)
C330.030 (2)0.058 (3)0.033 (2)0.014 (2)0.002 (2)0.009 (2)
C340.048 (3)0.058 (4)0.023 (2)0.027 (3)0.001 (2)0.012 (2)
C350.070 (3)0.030 (3)0.022 (2)0.013 (2)0.003 (2)0.010 (2)
C360.059 (3)0.026 (2)0.021 (2)0.001 (2)0.003 (2)0.005 (2)
C410.029 (2)0.021 (2)0.020 (2)0.008 (2)0.001 (1)0.002 (2)
C420.028 (2)0.026 (2)0.022 (2)0.008 (2)0.002 (2)0.002 (2)
C430.029 (2)0.044 (3)0.020 (2)0.014 (2)0.001 (2)0.001 (2)
C440.038 (2)0.033 (3)0.024 (2)0.014 (2)0.006 (2)0.006 (2)
C450.042 (3)0.029 (2)0.030 (2)0.002 (2)0.002 (2)0.004 (2)
C460.034 (2)0.024 (2)0.026 (2)0.002 (2)0.003 (2)0.002 (2)
Cl10.0175 (6)0.0410 (9)0.0318 (8)0.00000.0017 (5)0.0000
Cl20.0253 (7)0.0395 (9)0.0173 (6)0.00000.0034 (5)0.0000
O10.026 (2)0.040 (2)0.083 (3)0.003 (2)0.001 (2)0.011 (2)
O20.059 (4)0.145 (8)0.101 (6)0.0000.061 (4)0.000
O30.084 (5)0.071 (5)0.087 (5)0.0000.052 (4)0.000
O40.031 (2)0.088 (5)0.040 (3)0.0000.014 (2)0.000
O50.029 (3)0.327 (14)0.040 (4)0.0000.013 (3)0.000
O60.117 (5)0.047 (3)0.096 (4)0.018 (3)0.044 (3)0.022 (3)
O70.034 (2)0.066 (4)0.033 (2)0.0000.020 (2)0.000
C30.032 (3)0.040 (4)0.016 (3)0.0000.005 (2)0.000
C40.057 (3)0.051 (3)0.035 (2)0.017 (3)0.008 (2)0.005 (3)
Geometric parameters (Å, º) top
Pt—P12.289 (1)Cl1—O11.431 (4)
Pt—P22.310 (1)Cl1—O31.408 (6)
Pt—P2i2.310 (1)Cl1—O21.418 (6)
Pt—S2.343 (1)Cl2—O41.411 (5)
P1—C111.804 (5)Cl2—O51.385 (6)
P1—C211.826 (4)Cl2—O61.407 (4)
P2—C311.805 (4)O7—C31.196 (7)
P2—C411.809 (4)C3—C41.489 (6)
P2—C21.835 (4)C3—C4i1.489 (6)
S—C1A1.810 (9)C1A—H1Aa0.950
S—C1Ai1.810 (9)C1A—H1Ab0.950
S—C1B1.834 (8)C1B—H1Ba0.950
S—C1Bi1.834 (8)C1B—H1Bb0.950
C1A—C1B1.139 (12)C2—H2a0.950
C1A—C21.540 (9)C2—H2b0.950
C1B—C21.612 (10)C2—H2a'0.950
C11—C121.394 (7)C2—H2b'0.950
C11—C161.391 (7)C12—H120.950
C12—C131.396 (8)C13—H130.950
C13—C141.393 (9)C14—H140.950
C14—C151.375 (9)C15—H150.950
C15—C161.386 (7)C16—H160.950
C21—C221.390 (5)C22—H220.950
C21—C261.397 (5)C23—H230.950
C22—C231.387 (6)C24—H240.950
C23—C241.390 (6)C25—H250.950
C24—C251.381 (6)C26—H260.950
C25—C261.388 (5)C32—H320.950
C31—C321.389 (6)C33—H330.950
C31—C361.390 (6)C34—H340.950
C32—C331.396 (6)C35—H350.950
C33—C341.377 (8)C36—H360.950
C34—C351.383 (8)C42—H420.950
C35—C361.381 (7)C43—H430.950
C41—C421.407 (5)C44—H440.950
C41—C461.385 (6)C45—H450.950
C42—C431.378 (6)C46—H460.950
C43—C441.382 (7)C4—H4a0.950
C44—C451.392 (6)C4—H4b0.950
C45—C461.393 (6)C4—H4c0.950
P1—Pt—P298.79 (2)O6—Cl2—O6i107.6 (4)
P1—Pt—P2i98.79 (2)O7—C3—C4121.8 (3)
P2—Pt—P2i161.57 (5)C4—C3—C4i116.4 (6)
S—Pt—P1178.29 (5)S—C1A—H1Aa109.0
S—Pt—P281.30 (2)S—C1A—H1Ab109.0
S—Pt—P2i81.30 (2)S—C1B—H1Ba110.1
Pt—P1—C11113.6 (2)S—C1B—H1Bb110.1
Pt—P1—C21111.9 (1)H1Aa—C1A—H1Ab109.5
Pt—P1—C21i111.9 (1)C2—C1A—H1Aa109.0
Pt—P2—C31112.1 (1)C2—C1A—H1Ab109.0
Pt—P2—C41123.7 (1)H1Ba—C1B—H1Bb109.5
Pt—P2—C2102.1 (2)C2—C1B—H1Ba110.1
Pt—S—C1A108.0 (2)C2—C1B—H1Bb110.1
Pt—S—C1Ai108.0 (2)H2a—C2—H2b109.5
Pt—S—C1B98.0 (3)C1A—C2—H2a110.7
Pt—S—C1Bi98.0 (3)C1A—C2—H2b110.7
C1A—S—C1Bi101.5 (4)C1B—C2—H2a'107.9
C11—P1—C21106.7 (1)C1B—C2—H2b'107.9
C21—P1—C21i105.3 (2)C11—C12—H12119.7
C31—P2—C41108.6 (2)C13—C12—H12119.7
C2—P2—C31103.4 (2)C12—C13—H13120.5
C2—P2—C41104.3 (2)C14—C13—H13120.5
S—C1A—C2111.5 (5)C13—C14—H14119.6
S—C1B—C2107.0 (5)C15—C14—H14119.6
P2—C2—C1A104.5 (4)C14—C15—H15119.9
P2—C2—C1B115.6 (4)C16—C15—H15119.9
C12—C11—C16119.3 (5)C15—C16—H16119.9
P1—C11—C16121.6 (4)C11—C16—H16119.9
P1—C11—C12119.1 (4)C21—C22—H22119.6
C11—C12—C13120.5 (5)C23—C22—H22119.6
C12—C13—C14119.0 (5)C22—C23—H23120.0
C13—C14—C15120.7 (5)C24—C23—H23120.0
C14—C15—C16120.2 (6)C23—C24—H24120.3
C11—C16—C15120.3 (5)C25—C24—H24120.3
C22—C21—C26118.9 (3)C24—C25—H25119.6
P1—C21—C22123.3 (3)C26—C25—H25119.6
P1—C21—C26117.8 (3)C25—C26—H26120.0
C21—C22—C23120.7 (3)C21—C26—H26120.0
C22—C23—C24120.1 (4)C31—C32—H32119.8
C23—C24—C25119.4 (4)C33—C32—H32119.8
C24—C25—C26120.8 (4)C32—C33—H33120.3
C21—C26—C25120.1 (4)C34—C33—H33120.3
C32—C31—C36119.1 (4)C33—C34—H34119.7
P2—C31—C32120.9 (3)C35—C34—H34119.7
P2—C31—C36119.8 (3)C36—C35—H35120.1
C31—C32—C33120.5 (4)C34—C35—H35120.1
C32—C33—C34119.4 (5)C35—C36—H36119.7
C33—C34—C35120.7 (4)C31—C36—H36119.7
C34—C35—C36119.9 (4)C41—C42—H42120.1
C31—C36—C35120.5 (5)C43—C42—H42120.1
C42—C41—C46119.6 (4)C42—C43—H43119.8
P2—C41—C46122.5 (3)C44—C43—H43119.8
P2—C41—C42117.9 (3)C43—C44—H44119.8
C41—C42—C43119.8 (4)C45—C44—H44119.8
C42—C43—C44120.5 (4)C44—C45—H45120.3
C43—C44—C45120.3 (4)C46—C45—H45120.3
C44—C45—C46119.5 (4)C41—C46—H46119.8
C41—C46—C45120.3 (4)C45—C46—H46119.8
O1—Cl1—O1i109.6 (3)H4a—C4—H4b109.5
O1—Cl1—O2108.3 (3)H4a—C4—H4c109.5
O1—Cl1—O3111.7 (2)C3—C4—H4a109.5
O2—Cl1—O3107.0 (5)H4b—C4—H4c109.5
O4—Cl2—O5109.4 (4)C3—C4—H4b109.5
O4—Cl2—O6109.8 (3)C3—C4—H4c109.4
O5—Cl2—O6110.1 (3)
Symmetry code: (i) x, y+1/2, z.

Experimental details

Crystal data
Chemical formula[Pt(C28H28P2S)(C18H15P)](ClO4)2·C3H6O
Mr1172.84
Crystal system, space groupOrthorhombic, Pnma
Temperature (K)120
a, b, c (Å)15.698 (3), 15.337 (3), 19.957 (4)
V3)4804.9 (16)
Z4
Radiation typeMo Kα
µ (mm1)3.23
Crystal size (mm)0.26 × 0.24 × 0.24
Data collection
DiffractometerSiemens SMART CCD area-detector
diffractometer
Absorption correctionIntegration
XPREP (Siemens, 1995)
Tmin, Tmax0.448, 0.594
No. of measured, independent and
observed [I > 3σ(I)] reflections
41330, 7613, 5723
Rint0.054
(sin θ/λ)max1)0.714
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.032, 0.036, 0.99
No. of reflections5723
No. of parameters329
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)1.3 (2), 1.5 (2)

Computer programs: SMART (Siemens, 1995), SAINT (Siemens, 1995), SAINT, SIR97 (Altomare et al., 1996) and KRYSTAL (Hazell, 1995), modified ORFLS (Busing et al., 1962) and KRYSTAL, ORTEPIII (Burnett & Johnson, 1996) and KRYSTAL, KRYSTAL.

Selected geometric parameters (Å, º) top
Pt—P12.289 (1)S—C1A1.810 (9)
Pt—P22.310 (1)S—C1B1.834 (8)
Pt—S2.343 (1)
P1—Pt—P298.79 (2)S—Pt—P281.30 (2)
P2—Pt—P2i161.57 (5)S—Pt—P2i81.30 (2)
S—Pt—P1178.29 (5)
Symmetry code: (i) x, y+1/2, z.
 

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