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Acta Cryst. (2007). E63, m2017    [ doi:10.1107/S1600536807030966 ]

cis-Dichloridobis(dimethoxyphenylphosphino)platinum(II)

A. M. Z. Slawin, P. G. Waddell and J. D. Woollins

Abstract top

The title compound, [PtCl2(C8H11O2P)2], resides on a crystallographic twofold rotation axis and adopts a cis-square-planar geometry. Molecules are linked by C-H...Cl interactions forming one-dimensional chains along the [010] direction.

Comment top

The title complex (I) is comparable to similar platinum dichloride complexes containing trimethoxy phosphite; [PtCl2(P(OMe)3)2] (Bao et al., 1987) and triphenyl phosphine [PtCl2(PPh3)2] (Fun et al., 2006). The central platinum atom in (I) can be seen to bear a closer resemblance to the triphenyl phosphine complex. These measurement are also similar when compared to the structure of the complex [PtCl2(P(OMe)Ph2)2] (Slawin et al., 2007) with the exception of the P—Pt—P bond angle which is unusually large.

Related literature top

For related literature on PtCl2L2 complexes, see: Bao et al. (1987); Fun et al. (2006); Slawin et al. (2007).

Experimental top

1 g (2.67 mmol) of PtCl2(COD) was dissolved in the minimum volume of dichloromethane in a round-bottomed flask. To this, 0.840 ml (5.34 mmol) of dimethylphenylphosphonite was added. The solution was then stirred for 0.5 h at room temperature. The product was precipitated via slow diffusion of hexane and was then filtered off and dried under vacuum, [PtCl2(P(OMe)2Ph)2] (1.86 mmol,ca 69%). 31P-{1H} NMR: δ 91.2 p.p.m. J{Pt—P} 4819 Hz.

Refinement top

All H atoms were included in calculated positions (C—H distances are 0.96 Å for methyl H atoms, 0.97 Å for methylene H atoms and 0.98 Å for methine H atoms) and were refined as riding atoms with Uiso(H) = 1.2 Ueq(parent atom, methylene and methine H atoms) or Uiso(H) = 1.5 Ueq(parent atom, methyl H atoms).

Computing details top

Data collection: SCXmini (Rigaku/MSC, 2006); cell refinement: PROCESS-AUTO (Rigaku, 1998); data reduction: PROCESS-AUTO; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: CrystalStructure (Rigaku/MSC, 2006); software used to prepare material for publication: CrystalStructure.

Figures top
[Figure 1] Fig. 1. The structure of (1) with displacement ellipsoids drawn at the 50% probability level, H atoms omitted for clarity.
cis-Dichloridobis(dimethoxyphenylphosphino)platinum(II) top
Crystal data top
[PtCl2(C8H11O2P)2]F000 = 1168
Mr = 606.27Dx = 1.967 Mg m3
Monoclinic, C2/cMo Kα radiation
λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 6759 reflections
a = 10.9734 (7) Åθ = 3.0–27.5º
b = 9.2290 (6) ŵ = 7.29 mm1
c = 20.7002 (14) ÅT = 125 (2) K
β = 102.398 (2)ºPrism, colourless
V = 2047.5 (2) Å30.20 × 0.16 × 0.07 mm
Z = 4
Data collection top
Rigaku SCXmini
diffractometer
1772 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.035
Monochromator: graphiteθmax = 25.3º
T = 125(2) Kθmin = 3.2º
ω scansh = 13→13
Absorption correction: multi-scan
(ABSCOR; Higashi, 1995)
k = 11→10
Tmin = 0.261, Tmax = 0.602l = 24→24
5869 measured reflectionsStandard reflections: ?
1869 independent reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.021H-atom parameters constrained
wR(F2) = 0.043  w = 1/[σ2(Fo2) + (0.0167P)2 + 0.5089P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max = 0.007
1869 reflectionsΔρmax = 0.62 e Å3
117 parametersΔρmin = 0.69 e Å3
Primary atom site location: structure-invariant direct methodsExtinction correction: none
Crystal data top
[PtCl2(C8H11O2P)2]V = 2047.5 (2) Å3
Mr = 606.27Z = 4
Monoclinic, C2/cMo Kα
a = 10.9734 (7) ŵ = 7.29 mm1
b = 9.2290 (6) ÅT = 125 (2) K
c = 20.7002 (14) Å0.20 × 0.16 × 0.07 mm
β = 102.398 (2)º
Data collection top
Rigaku SCXmini
diffractometer
1869 independent reflections
Absorption correction: multi-scan
(ABSCOR; Higashi, 1995)
1772 reflections with I > 2σ(I)
Tmin = 0.261, Tmax = 0.602Rint = 0.035
5869 measured reflectionsStandard reflections: ?
Refinement top
R[F2 > 2σ(F2)] = 0.021117 parameters
wR(F2) = 0.043H-atom parameters constrained
S = 1.07Δρmax = 0.62 e Å3
1869 reflectionsΔρmin = 0.69 e Å3
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > 2sigma(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R– factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Pt10.50000.40682 (2)0.25000.01234 (7)
Cl10.59209 (8)0.58930 (10)0.32480 (4)0.0204 (2)
P10.40029 (8)0.25413 (10)0.17390 (4)0.0141 (2)
C10.4614 (3)0.2496 (4)0.09966 (17)0.0156 (8)
C20.4028 (3)0.3176 (4)0.04180 (18)0.0217 (9)
H2A0.32640.36770.03970.026*
C30.4560 (3)0.3125 (5)0.01343 (19)0.0270 (10)
H3A0.41660.35980.05320.032*
C40.5671 (4)0.2379 (4)0.01014 (19)0.0300 (10)
H4A0.60270.23370.04810.036*
C50.6258 (4)0.1707 (5)0.0466 (2)0.0314 (10)
H5A0.70170.12000.04800.038*
C60.5744 (3)0.1764 (4)0.10287 (19)0.0244 (9)
H6A0.61580.13120.14280.029*
O10.3959 (2)0.0909 (2)0.19814 (12)0.0195 (6)
C70.3218 (4)0.0145 (4)0.15439 (19)0.0261 (9)
H7A0.23410.00590.15730.039*
H7B0.35180.11240.16760.039*
H7C0.32940.00370.10880.039*
O20.2590 (2)0.2966 (3)0.14365 (11)0.0170 (5)
C80.1756 (3)0.3272 (5)0.18759 (19)0.0266 (10)
H8A0.18040.24850.21980.040*
H8B0.08990.33530.16170.040*
H8C0.20010.41850.21090.040*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pt10.01451 (11)0.01079 (12)0.01187 (12)0.0000.00317 (8)0.000
Cl10.0245 (5)0.0150 (5)0.0195 (5)0.0003 (4)0.0004 (4)0.0036 (4)
P10.0172 (5)0.0127 (5)0.0125 (5)0.0014 (4)0.0033 (4)0.0006 (4)
C10.0178 (17)0.012 (2)0.017 (2)0.0047 (14)0.0040 (16)0.0026 (15)
C20.022 (2)0.023 (2)0.019 (2)0.0008 (16)0.0039 (18)0.0017 (17)
C30.031 (2)0.035 (3)0.012 (2)0.0028 (19)0.0005 (18)0.0011 (18)
C40.037 (2)0.036 (3)0.020 (2)0.003 (2)0.012 (2)0.0060 (19)
C50.023 (2)0.040 (3)0.034 (3)0.0069 (19)0.013 (2)0.001 (2)
C60.024 (2)0.027 (2)0.022 (2)0.0081 (17)0.0031 (18)0.0058 (18)
O10.0272 (13)0.0134 (14)0.0167 (14)0.0058 (11)0.0021 (11)0.0003 (11)
C70.040 (2)0.015 (2)0.022 (2)0.0068 (18)0.004 (2)0.0039 (17)
O20.0157 (12)0.0190 (15)0.0167 (14)0.0006 (10)0.0048 (11)0.0002 (11)
C80.022 (2)0.031 (3)0.030 (2)0.0002 (17)0.0135 (19)0.0001 (19)
Geometric parameters (Å, °) top
Pt1—P12.2190 (9)C4—C51.362 (5)
Pt1—P1i2.2190 (9)C4—H4A0.9500
Pt1—Cl12.3629 (9)C5—C61.400 (5)
Pt1—Cl1i2.3629 (9)C5—H5A0.9500
P1—O11.592 (2)C6—H6A0.9500
P1—O21.591 (2)O1—C71.453 (4)
P1—C11.804 (3)C7—H7A0.9800
C1—C21.382 (5)C7—H7B0.9800
C1—C61.402 (5)C7—H7C0.9800
C2—C31.392 (5)O2—C81.450 (4)
C2—H2A0.9500C8—H8A0.9800
C3—C41.388 (5)C8—H8B0.9800
C3—H3A0.9500C8—H8C0.9800
P1—Pt1—P1i101.16 (5)C5—C4—H4A119.5
P1—Pt1—Cl1173.78 (3)C3—C4—H4A119.5
P1i—Pt1—Cl184.90 (3)C4—C5—C6120.0 (4)
P1—Pt1—Cl1i84.90 (3)C4—C5—H5A120.0
P1i—Pt1—Cl1i173.78 (3)C6—C5—H5A120.0
Cl1—Pt1—Cl1i89.08 (4)C5—C6—C1119.3 (4)
O1—P1—O2105.34 (13)C5—C6—H6A120.3
O1—P1—C1106.75 (15)C1—C6—H6A120.3
O2—P1—C1100.32 (14)C7—O1—P1119.2 (2)
O1—P1—Pt1114.89 (10)O1—C7—H7A109.5
O2—P1—Pt1114.40 (10)O1—C7—H7B109.5
C1—P1—Pt1113.76 (11)H7A—C7—H7B109.5
C2—C1—C6120.1 (3)O1—C7—H7C109.5
C2—C1—P1122.6 (3)H7A—C7—H7C109.5
C6—C1—P1117.3 (3)H7B—C7—H7C109.5
C1—C2—C3119.8 (3)C8—O2—P1119.6 (2)
C1—C2—H2A120.1O2—C8—H8A109.5
C3—C2—H2A120.1O2—C8—H8B109.5
C4—C3—C2119.7 (4)H8A—C8—H8B109.5
C4—C3—H3A120.2O2—C8—H8C109.5
C2—C3—H3A120.2H8A—C8—H8C109.5
C5—C4—C3121.1 (4)H8B—C8—H8C109.5
P1i—Pt1—P1—O114.27 (10)P1—C1—C2—C3178.7 (3)
Cl1i—Pt1—P1—O1167.15 (11)C1—C2—C3—C40.6 (6)
P1i—Pt1—P1—O2136.32 (11)C2—C3—C4—C50.7 (6)
Cl1i—Pt1—P1—O245.10 (10)C3—C4—C5—C60.1 (7)
P1i—Pt1—P1—C1109.19 (13)C4—C5—C6—C11.1 (6)
Cl1i—Pt1—P1—C169.39 (13)C2—C1—C6—C51.3 (6)
O1—P1—C1—C2129.0 (3)P1—C1—C6—C5179.6 (3)
O2—P1—C1—C219.4 (3)O2—P1—O1—C746.7 (3)
Pt1—P1—C1—C2103.2 (3)C1—P1—O1—C759.3 (3)
O1—P1—C1—C652.7 (3)Pt1—P1—O1—C7173.6 (2)
O2—P1—C1—C6162.3 (3)O1—P1—O2—C875.5 (3)
Pt1—P1—C1—C675.1 (3)C1—P1—O2—C8173.8 (3)
C6—C1—C2—C30.4 (5)Pt1—P1—O2—C851.6 (3)
Symmetry codes: (i) −x+1, y, −z+1/2.
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
C7—H7B···Cl1ii0.982.823.778 (4)166
Symmetry codes: (ii) −x+1, y−1, −z+1/2.
Selected geometric parameters (Å, °) top
Pt1—P12.2190 (9)Pt1—Cl12.3629 (9)
P1—Pt1—P1i101.16 (5)P1i—Pt1—Cl184.90 (3)
P1—Pt1—Cl1173.78 (3)Cl1—Pt1—Cl1i89.08 (4)
Symmetry codes: (i) −x+1, y, −z+1/2.
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
C7—H7B···Cl1ii0.982.823.778 (4)166
Symmetry codes: (ii) −x+1, y−1, −z+1/2.
references
References top

Bao, Q.-B., Geib, S. J., Rheingold, A. L. & Brill, T. B. (1987). Inorg. Chem. 26, 3453–3458.

Fun, H.-K., Chantrapromma, S., Liu, Y.-C., Chen, Z.-F. & Liang, H. (2006). Acta Cryst. E62, m1252–m1254.

Higashi, T. (1995). ABSCOR. Rigaku Corporation, 3-9-12 Matsubara, Akishima, Tokyo 196-8666, Japan.

Rigaku (1998). PROCESS-AUTO. Rigaku Corporation, 3-9-12 Matsubara, Akishima, Tokyo 196-8666, Japan.

Rigaku/MSC (2006). Crystal Structure (Version 3.8) and SCXmini (Version 1.0). Rigaku/MSC, 9009 New Trails Drive, The Woodlands, TX 77381-5209, USA.

Sheldrick, G. M. (1997). SHELXL97. University of Göttingen, Germany.

Slawin, A. M. Z., Waddell, P. G. & Woollins, J. D. (2007). Acta Cryst. E63. Submitted.. Update?