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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Dec 4;67(Pt 1):m14. doi: 10.1107/S1600536810049706

cis-Dichloridotetra­kis­(trimethyl­phosphane-κP)ruthenium(II) benzene disolvate

Chen Fu a, Ting Bin Wen a,*
PMCID: PMC3050259  PMID: 21522541

Abstract

The title compound, cis-[RuCl2(C3H9P)4]·2C6H6, contains a complex mol­ecule with a crystallographic mirror plane passing through the RuII atom, the two cis-disposed Cl ligands and two P atoms of the two cis-disposed P(CH3)3 ligands. The RuII atom adopts a distorted octa­hedral RuCl2P4 coordination geometry with the two trans-disposed P atoms occupying the axial positions. The packing of the structure is accomplished through non-classical C—H⋯Cl hydrogen bonds between the benzene solvent mol­ecule and one of the Cl ligands.

Related literature

For general background to trans-[RuCl2(P(CH3)3)4], see: Csok et al. (2007 ▶); Gotzig et al. (1985 ▶); Hartwig et al. (1991 ▶); Hirano et al. (2010 ▶); Kohlmann & Werner (1993 ▶). For a related structure, see: Joo et al. (1994 ▶).graphic file with name e-67-00m14-scheme1.jpg

Experimental

Crystal data

  • [RuCl2(C3H9P)4]·2C6H6

  • M r = 632.47

  • Orthorhombic, Inline graphic

  • a = 17.6243 (15) Å

  • b = 18.1889 (19) Å

  • c = 9.4610 (11) Å

  • V = 3032.9 (5) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.92 mm−1

  • T = 173 K

  • 0.18 × 0.12 × 0.06 mm

Data collection

  • Oxford Diffraction Gemini S Ultra diffractometer

  • Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2008 ▶) T min = 0.949, T max = 1.000

  • 14352 measured reflections

  • 3550 independent reflections

  • 1653 reflections with I > 2σ(I)

  • R int = 0.148

Refinement

  • R[F 2 > 2σ(F 2)] = 0.058

  • wR(F 2) = 0.081

  • S = 0.82

  • 3550 reflections

  • 139 parameters

  • H-atom parameters constrained

  • Δρmax = 0.97 e Å−3

  • Δρmin = −0.57 e Å−3

Data collection: CrysAlis CCD (Oxford Diffraction, 2008 ▶); cell refinement: CrysAlis RED (Oxford Diffraction, 2008 ▶); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810049706/wm2431sup1.cif

e-67-00m14-sup1.cif (17.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810049706/wm2431Isup2.hkl

e-67-00m14-Isup2.hkl (174.2KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Selected bond lengths (Å).

Ru1—P1 2.2690 (19)
Ru1—P2 2.297 (2)
Ru1—P3 2.3819 (14)
Ru1—Cl1 2.479 (2)
Ru1—Cl2 2.5038 (19)

Table 2. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A D⋯A D—H⋯A
C4S—H4SA⋯Cl2 0.93 2.83 3.710 (5) 159

Acknowledgments

The authors acknowledge financial support from the Young Talent Project of Department of Science & Technology of Fujian Province (grant No. 2007 F3095).

supplementary crystallographic information

Comment

The ruthenium(II) complex trans-[RuCl2(PMe3)4], which can be readily prepared from the reaction of RuCl2(PPh3)3 with PMe3 in hexane at room temperature (Gotzig et al., 1985), has proved to be a useful precursor for a wide variety of ruthenium compounds (Hartwig et al., 1991; Kohlmann & Werner, 1993; Csok et al., 2007; Hirano et al., 2010). However, its geometrical isomer, cis-[RuCl2(PMe3)4], has not been reported yet. During our preparation of ruthenium compounds with phosphine ligands using trans-[RuCl2(PMe3)4] as the starting material, we found that the trans-isomer slowly isomerizes to the cis-isomer, the structure of which we report here as the benzene disolvate.

As shown in Fig.1, the structure of the title complex possesses a crystallographic mirror plane passing through the RuII atom, the two cis-disposed Cl ligands and the two P atoms as well as two C atoms of the two cis-disposed PMe3 ligands. Thus the asymmetric unit of the structure contains half of a molecule. The RuII atom adopts a distorted octahedral geometry with the two trans-disposed P atoms occupying the axial positions. The bond lengths of the two axial Ru—P bonds (2.3819 (14) Å), which are actually image-related, are slightly longer than those of the two equatorial Ru—P bonds which are trans to the Cl ligands (2.2690 (19) and 2.297 (2) Å, respectively). The two Ru—Cl bond lengths are 2.479 (2) and 2.5038 (19) Å, respectively, while the Cl(1)—Ru(1)—Cl(2) bond angle is 86.20 (7)°. These geometric values are similar to those reported for the only example of a sructurally characterized monodentate tetrakis(phosphine)-cis-dichlorido-ruthenium(II) complex, viz. [cis-RuCl2(PTA)4] (PTA = 1,3,5-triaza-7-phospha-adamantane-κP); 2.488 (2) and 2.503 (2) Å, 84.2 (1) °; Joo et al., 1994).

The packing of the structure (Fig. 2) is accomplished through non-classical C—H···Cl hydrogen bonds between the benzene solvent molecule and one of the Cl ligands (Table 2).

Experimental

Route A: To a solution of RuCl2(PPh3)3 (0.25 g, 0.24 mmol) in toluene (8 ml) under nitrogen atmosphere was added PMe3 (0.27 ml, 2.5 mmol) and the resulting yellow solution was refluxed for 20 h. The solvent was removed under vacuum, and the solid residue was washed with n-hexane, and dried under vacuum to afford a white solid. Yield: 90 mg, 80%. Route B: A solution of trans-[RuCl2(PMe3)4] (100 mg, 0.21 mmol) in benzene (5 ml) was refluxed for 12 h under nitrogen atmosphere. After the solution was cooled to ambient temperature, a white solid was precipitated, which was collected by filtration, washed with n-hexane, and dried under vacuum. Yield: 72 mg, 72%. Crystals suitable for X-ray analysis were obtained from standing a solution of trans-[RuCl2(PMe3)4] in benzene at room temperature for 2 weeks.

Refinement

The benzene solvent molecule was treated as a rigid body. All non-hydrogen atoms were refined anisotropically. The hydrogen atoms were positioned geometrically (C—H = 0.96 or 0.93 Å for methyl or phenyl H atoms, respectively) and were included in the refinement in the riding model approximation. The displacement parameters of methyl H atoms were set to 1.5Ueq(C), while those of the phenyl H atoms were set to 1.2Ueq(C). In the final Fourier map the highest peak is 0.04 Å from atom Ru1 and the deepest hole is 0.71 Å from atom Ru1.

Figures

Fig. 1.

Fig. 1.

The coordination of the RuII atom in the structure of cis-[RuCl2(P(CH3)3)4] with the atom labelling and displacement ellipsoids drawn at the 30% probability level. H atoms have been omitted for clarity. [Symmetry code: (A) x, -y+1/2, z.]

Fig. 2.

Fig. 2.

The packing diagram of the structure viewed down the c axis, showing the non-classical C—H···Cl hydrogen bonds between the benzene solvent molecule and one of the Cl ligands of the complex molecule.

Crystal data

[RuCl2(C3H9P)4]·2C6H6 F(000) = 1320
Mr = 632.47 Dx = 1.385 Mg m−3
Orthorhombic, Pnma Mo Kα radiation, λ = 0.7107 Å
Hall symbol: -P 2ac 2n Cell parameters from 1376 reflections
a = 17.6243 (15) Å θ = 2.3–28.9°
b = 18.1889 (19) Å µ = 0.92 mm−1
c = 9.4610 (11) Å T = 173 K
V = 3032.9 (5) Å3 Block, colorless
Z = 4 0.18 × 0.12 × 0.06 mm

Data collection

Oxford Diffraction Gemini S Ultra diffractometer 3550 independent reflections
Radiation source: Enhance (Mo) X-ray Source 1653 reflections with I > 2σ(I)
graphite Rint = 0.148
Detector resolution: 16.1930 pixels mm-1 θmax = 27.5°, θmin = 2.3°
ω scans h = −22→21
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2008) k = −23→22
Tmin = 0.949, Tmax = 1.000 l = −10→12
14352 measured reflections

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.058 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.081 H-atom parameters constrained
S = 0.82 w = 1/[σ2(Fo2) + (0.0104P)2] where P = (Fo2 + 2Fc2)/3
3550 reflections (Δ/σ)max = 0.003
139 parameters Δρmax = 0.97 e Å−3
0 restraints Δρmin = −0.57 e Å−3

Special details

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 > σ(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)

x y z Uiso*/Ueq
Ru1 0.54358 (3) 0.2500 0.30360 (7) 0.01803 (17)
Cl1 0.47805 (10) 0.2500 0.0718 (2) 0.0308 (6)
Cl2 0.41377 (9) 0.2500 0.4111 (2) 0.0347 (6)
P1 0.66211 (10) 0.2500 0.2100 (2) 0.0221 (5)
P2 0.57932 (10) 0.2500 0.5371 (2) 0.0233 (6)
P3 0.53321 (8) 0.37973 (7) 0.27518 (17) 0.0273 (4)
C11 0.6660 (4) 0.2500 0.0209 (8) 0.032 (2)
H11A 0.7178 0.2500 −0.0104 0.049*
H11B 0.6408 0.2069 −0.0142 0.049*
C12 0.7266 (2) 0.3256 (2) 0.2488 (6) 0.0303 (17)
H12A 0.7740 0.3175 0.2015 0.045*
H12B 0.7350 0.3282 0.3489 0.045*
H12C 0.7047 0.3709 0.2165 0.045*
C21 0.6769 (3) 0.2500 0.5976 (8) 0.036 (2)
H21A 0.6785 0.2500 0.6990 0.055*
H21B 0.7020 0.2069 0.5623 0.055*
C22 0.5445 (3) 0.3255 (3) 0.6447 (6) 0.057 (2)
H22A 0.5627 0.3200 0.7397 0.086*
H22B 0.4900 0.3252 0.6447 0.086*
H22C 0.5624 0.3713 0.6065 0.086*
C31 0.5557 (3) 0.4150 (3) 0.1015 (6) 0.0368 (16)
H31A 0.5499 0.4675 0.1010 0.055*
H31B 0.5221 0.3936 0.0331 0.055*
H31C 0.6072 0.4027 0.0781 0.055*
C32 0.4370 (2) 0.4140 (3) 0.2916 (7) 0.0447 (18)
H32A 0.4369 0.4664 0.2789 0.067*
H32B 0.4177 0.4023 0.3837 0.067*
H32C 0.4056 0.3916 0.2208 0.067*
C33 0.5837 (3) 0.4488 (3) 0.3798 (6) 0.046 (2)
H33A 0.5700 0.4971 0.3476 0.069*
H33B 0.6374 0.4420 0.3690 0.069*
H33C 0.5703 0.4436 0.4776 0.069*
C1S 0.2535 (3) 0.4577 (2) 0.8727 (8) 0.069 (3)
H1SA 0.2273 0.4919 0.9273 0.082*
C2S 0.3127 (4) 0.4177 (4) 0.9316 (4) 0.073 (3)
H2SA 0.3263 0.4251 1.0255 0.088*
C3S 0.3518 (2) 0.3667 (3) 0.8500 (8) 0.068 (3)
H3SA 0.3915 0.3399 0.8894 0.081*
C4S 0.3316 (3) 0.3557 (2) 0.7096 (8) 0.059 (2)
H4SA 0.3578 0.3215 0.6550 0.071*
C5S 0.2724 (3) 0.3957 (3) 0.6507 (4) 0.059 (2)
H5SA 0.2589 0.3883 0.5567 0.071*
C6S 0.23327 (19) 0.4467 (3) 0.7323 (8) 0.064 (3)
H6SA 0.1936 0.4735 0.6929 0.076*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Ru1 0.0145 (3) 0.0200 (3) 0.0196 (4) 0.000 −0.0017 (4) 0.000
Cl1 0.0333 (12) 0.0318 (13) 0.0275 (14) 0.000 −0.0146 (10) 0.000
Cl2 0.0154 (11) 0.0489 (14) 0.0398 (15) 0.000 −0.0001 (10) 0.000
P1 0.0212 (10) 0.0254 (12) 0.0197 (14) 0.000 0.0015 (11) 0.000
P2 0.0181 (11) 0.0330 (14) 0.0187 (14) 0.000 0.0012 (10) 0.000
P3 0.0230 (8) 0.0249 (8) 0.0339 (11) 0.0015 (7) −0.0029 (8) −0.0031 (8)
C11 0.029 (5) 0.036 (6) 0.032 (6) 0.000 0.012 (4) 0.000
C12 0.026 (3) 0.029 (3) 0.036 (5) 0.002 (3) 0.003 (3) 0.000 (3)
C21 0.023 (5) 0.073 (7) 0.013 (5) 0.000 −0.004 (4) 0.000
C22 0.059 (4) 0.081 (5) 0.032 (4) 0.027 (4) −0.006 (4) −0.018 (4)
C31 0.048 (4) 0.027 (3) 0.035 (4) −0.003 (3) −0.002 (3) 0.008 (3)
C32 0.039 (4) 0.031 (3) 0.064 (5) 0.009 (3) −0.008 (4) −0.001 (4)
C33 0.039 (4) 0.033 (4) 0.066 (6) −0.007 (3) 0.003 (3) −0.013 (4)
C1S 0.085 (6) 0.053 (6) 0.067 (7) −0.029 (5) 0.050 (5) −0.019 (6)
C2S 0.099 (7) 0.091 (8) 0.029 (5) −0.066 (5) −0.019 (5) 0.026 (6)
C3S 0.039 (4) 0.063 (6) 0.101 (9) −0.009 (4) −0.006 (5) 0.041 (6)
C4S 0.056 (5) 0.026 (4) 0.097 (8) −0.004 (3) 0.049 (5) −0.009 (5)
C5S 0.087 (6) 0.059 (6) 0.033 (5) −0.050 (4) −0.003 (5) 0.007 (5)
C6S 0.035 (4) 0.037 (5) 0.119 (10) −0.007 (3) 0.010 (5) 0.029 (6)

Geometric parameters (Å, °)

Ru1—P1 2.2690 (19) C22—H22B 0.9600
Ru1—P2 2.297 (2) C22—H22C 0.9600
Ru1—P3i 2.3819 (14) C31—H31A 0.9600
Ru1—P3 2.3819 (14) C31—H31B 0.9600
Ru1—Cl1 2.479 (2) C31—H31C 0.9600
Ru1—Cl2 2.5038 (19) C32—H32A 0.9600
P1—C11 1.790 (8) C32—H32B 0.9600
P1—C12 1.821 (4) C32—H32C 0.9600
P1—C12i 1.821 (4) C33—H33A 0.9600
P2—C21 1.812 (6) C33—H33B 0.9600
P2—C22 1.816 (5) C33—H33C 0.9600
P2—C22i 1.816 (5) C1S—C2S 1.3900
P3—C31 1.808 (5) C1S—C6S 1.3900
P3—C32 1.813 (4) C1S—H1SA 0.9300
P3—C33 1.831 (5) C2S—C3S 1.3900
C11—H11A 0.9600 C2S—H2SA 0.9300
C11—H11B 0.9598 C3S—C4S 1.3900
C12—H12A 0.9600 C3S—H3SA 0.9300
C12—H12B 0.9600 C4S—C5S 1.3900
C12—H12C 0.9600 C4S—H4SA 0.9300
C21—H21A 0.9600 C5S—C6S 1.3900
C21—H21B 0.9599 C5S—H5SA 0.9300
C22—H22A 0.9600 C6S—H6SA 0.9300
P1—Ru1—P2 97.07 (8) H21A—C21—H21B 109.5
P1—Ru1—P3i 91.52 (4) P2—C22—H22A 109.5
P2—Ru1—P3i 97.45 (4) P2—C22—H22B 109.5
P1—Ru1—P3 91.52 (4) H22A—C22—H22B 109.5
P2—Ru1—P3 97.45 (4) P2—C22—H22C 109.5
P3i—Ru1—P3 164.31 (8) H22A—C22—H22C 109.5
P1—Ru1—Cl1 94.79 (8) H22B—C22—H22C 109.5
P2—Ru1—Cl1 168.14 (7) P3—C31—H31A 109.5
P3i—Ru1—Cl1 82.20 (4) P3—C31—H31B 109.5
P3—Ru1—Cl1 82.20 (4) H31A—C31—H31B 109.5
P1—Ru1—Cl2 179.01 (9) P3—C31—H31C 109.5
P2—Ru1—Cl2 81.94 (7) H31A—C31—H31C 109.5
P3i—Ru1—Cl2 88.61 (4) H31B—C31—H31C 109.5
P3—Ru1—Cl2 88.61 (4) P3—C32—H32A 109.5
Cl1—Ru1—Cl2 86.20 (7) P3—C32—H32B 109.5
C11—P1—C12 100.2 (2) H32A—C32—H32B 109.5
C11—P1—C12i 100.2 (2) P3—C32—H32C 109.5
C12—P1—C12i 98.0 (3) H32A—C32—H32C 109.5
C11—P1—Ru1 115.2 (2) H32B—C32—H32C 109.5
C12—P1—Ru1 119.71 (17) P3—C33—H33A 109.5
C12i—P1—Ru1 119.71 (17) P3—C33—H33B 109.5
C21—P2—C22 98.3 (2) H33A—C33—H33B 109.5
C21—P2—C22i 98.3 (2) P3—C33—H33C 109.5
C22—P2—C22i 98.3 (4) H33A—C33—H33C 109.5
C21—P2—Ru1 124.3 (3) H33B—C33—H33C 109.5
C22—P2—Ru1 116.5 (2) C2S—C1S—C6S 120.0
C22i—P2—Ru1 116.5 (2) C2S—C1S—H1SA 120.0
C31—P3—C32 99.3 (3) C6S—C1S—H1SA 120.0
C31—P3—C33 98.1 (3) C3S—C2S—C1S 120.0
C32—P3—C33 99.9 (2) C3S—C2S—H2SA 120.0
C31—P3—Ru1 115.93 (18) C1S—C2S—H2SA 120.0
C32—P3—Ru1 113.76 (17) C2S—C3S—C4S 120.0
C33—P3—Ru1 125.57 (19) C2S—C3S—H3SA 120.0
P1—C11—H11A 110.1 C4S—C3S—H3SA 120.0
P1—C11—H11B 109.1 C3S—C4S—C5S 120.0
H11A—C11—H11B 109.5 C3S—C4S—H4SA 120.0
P1—C12—H12A 109.5 C5S—C4S—H4SA 120.0
P1—C12—H12B 109.5 C6S—C5S—C4S 120.0
H12A—C12—H12B 109.5 C6S—C5S—H5SA 120.0
P1—C12—H12C 109.5 C4S—C5S—H5SA 120.0
H12A—C12—H12C 109.5 C5S—C6S—C1S 120.0
H12B—C12—H12C 109.5 C5S—C6S—H6SA 120.0
P2—C21—H21A 110.1 C1S—C6S—H6SA 120.0
P2—C21—H21B 109.1

Symmetry codes: (i) x, −y+1/2, z.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C4S—H4SA···Cl2i 0.93 2.83 3.710 (5) 159.

Symmetry codes: i.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: WM2431).

References

  1. Csok, Z., Gandum, C., Rissanen, K., Tuzi, A. & Rodrigues, J. (2007). J. Organomet. Chem. 692, 5263–5271.
  2. Gotzig, J., Werner, R. & Werner, H. (1985). J. Organomet. Chem. 290, 99–114.
  3. Hartwig, J. F., Bergman, R. G. & Andersen, R. A. (1991). Organometallics, 10, 3344–3362.
  4. Hirano, M., Togashi, S., Ito, M., Sakaguchi, Y., Komine, N. & Komiya, S. (2010). Organometallics, 29, 3146–3159.
  5. Joo, F., Kannisto, M., Katho, A., Reibenspies, J., Daigle, D. & Darensbourg, D. (1994). Inorg. Chem. 33, 200–208.
  6. Kohlmann, W. & Werner, H. (1993). Z. Naturforsch. Teil B, 48, 1499–1511.
  7. Oxford Diffraction (2008). CrysAlis CCD and CrysAlis RED Oxford Diffraction Ltd, Yarnton, England.
  8. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810049706/wm2431sup1.cif

e-67-00m14-sup1.cif (17.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810049706/wm2431Isup2.hkl

e-67-00m14-Isup2.hkl (174.2KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

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