supplementary materials


Acta Cryst. (2007). E63, m1904    [ doi:10.1107/S1600536807027912 ]

mer-Trichloridotris(dimethyl sulfide-[kappa]S)rhodium(III)

A. Abbasi, M. Habibian and M. Sandström

Abstract top

The title compound, [RhCl3(C2H6S)3], exists as discrete molecules in which the RhIII atom is coordinated by three S atoms from the dimethyl sulfide molecules and three Cl atoms in a mer-octahedral configuration.

Comment top

One aim of the current study is to investigate the nature of Rh—S bonds and to make a comparison with analogous compounds such as the sulfoxide complexes (Abbasi, et al., 2006; Calligaris, 2004; Alessio, 2004). Interest in the use of the dimethyl sulfide ligand arises from its involvement in the homogeneous hydrogenation of olefinic substrates (James et al. 1968).

The rhodium(III) ion is octahedrally coordinated by the sulfur atoms of the three dimethyl sulfide molecules, and three chlorine atoms in a mer octahedral configuration (Fig. 1). The Rh—S bond distance in for the sulfur trans to the chlorine [2.328 (1) Å] is longer than that cis to the chlorine [2.283 (1) Å], which indicates strongr π-back bonding from metal to sulfur (Abbasi et al., 2006).

Related literature top

For the related dimethyl sulfoxide compound, see Abbasi et al. (2006).

For related literature, see: Alessio (2004); Calligaris (2004); James et al. (1968).

Experimental top

The compound was synthesized by dissolving rhodium(III) chloride (Aldrich, 98%) in excess of dimethyl sulfide (Merck, 99%) at 343 K followed by a 12 h reflux. The mixture was then cooled to room temperature. Crystals were obtained after the evaporation of the solvent.

Refinement top

The Flack parameter was refined from 1283 Friedel pairs.

The H atoms are in calculated positions and constrained to ride on the parent C atoms with the C—H distance 0.96 Å and Uiso(H) = 1.5 Ueq(C).

Computing details top

Data collection: IPDS Software (Stoe & Cie, 1997); cell refinement: IPDS Software; data reduction: IPDS Software; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: DIAMOND (Brandenburg, 1999); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. Molecular structure of (I), shown with 50% probability displacement ellipsoids. H atoms are shown with arbitrary radii.
mer-Trichloridotris(dimethyl sulfide-κS)rhodium(III) top
Crystal data top
[RhCl3(C2H6S)3]F000 = 792
Mr = 395.64Dx = 1.812 Mg m3
Orthorhombic, P212121Mo Kα radiation
λ = 0.71073 Å
Hall symbol: P 2ac 2abCell parameters from 7089 reflections
a = 7.9835 (10) Åθ = 2.1–26.7º
b = 13.312 (2) ŵ = 2.12 mm1
c = 13.6450 (18) ÅT = 290 (2) K
V = 1450.1 (3) Å3Needle, brown
Z = 40.2 × 0.1 × 0.1 mm
Data collection top
Stoe IPDS II
diffractometer
3037 independent reflections
Radiation source: fine-focus sealed tube2965 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.016
T = 290(2) Kθmax = 26.7º
Area detector, φ oscillation scansθmin = 2.1º
Absorption correction: numerical
(X-RED; Stoe & Cie, 1997)
h = 8→10
Tmin = 0.693, Tmax = 0.793k = 16→14
7089 measured reflectionsl = 17→17
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.017  w = 1/[σ2(Fo2) + (0.0163P)2 + 0.5475P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.039(Δ/σ)max = 0.001
S = 1.08Δρmax = 0.28 e Å3
3037 reflectionsΔρmin = 0.24 e Å3
118 parametersExtinction correction: none
Primary atom site location: structure-invariant direct methodsAbsolute structure: Flack (1983), with 1283 Friedel pairs
Secondary atom site location: difference Fourier mapFlack parameter: 0.02 (3)
Crystal data top
[RhCl3(C2H6S)3]V = 1450.1 (3) Å3
Mr = 395.64Z = 4
Orthorhombic, P212121Mo Kα
a = 7.9835 (10) ŵ = 2.12 mm1
b = 13.312 (2) ÅT = 290 (2) K
c = 13.6450 (18) Å0.2 × 0.1 × 0.1 mm
Data collection top
Stoe IPDS II
diffractometer
3037 independent reflections
Absorption correction: numerical
(X-RED; Stoe & Cie, 1997)
2965 reflections with I > 2σ(I)
Tmin = 0.693, Tmax = 0.793Rint = 0.016
7089 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.017H-atom parameters constrained
wR(F2) = 0.039Δρmax = 0.28 e Å3
S = 1.08Δρmin = 0.24 e Å3
3037 reflectionsAbsolute structure: Flack (1983), with 1283 Friedel pairs
118 parametersFlack parameter: 0.02 (3)
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 > 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) top
xyzUiso*/Ueq
Rh10.27392 (2)0.830500 (13)0.232940 (12)0.03469 (5)
S10.15639 (11)0.67291 (6)0.20553 (5)0.05978 (18)
S20.15091 (10)0.88897 (5)0.08792 (5)0.05395 (17)
S30.40313 (9)0.78043 (5)0.38115 (4)0.04733 (15)
Cl10.04246 (9)0.86245 (7)0.33444 (5)0.0681 (2)
Cl20.38670 (10)0.98917 (5)0.27322 (5)0.06140 (18)
Cl30.50634 (10)0.79376 (7)0.13543 (5)0.0654 (2)
C110.2440 (5)0.6116 (2)0.1013 (3)0.0790 (10)
H11A0.36000.59720.11340.095*
H11B0.23430.65450.04510.095*
H11C0.18480.55000.08940.095*
C120.0530 (4)0.6866 (3)0.1598 (3)0.0839 (12)
H12A0.12090.71940.20820.101*
H12B0.09880.62150.14560.101*
H12C0.05120.72630.10100.101*
C210.2849 (7)0.9835 (2)0.0363 (2)0.0870 (13)
H21A0.38850.95330.01610.104*
H21B0.30701.03420.08460.104*
H21C0.23081.01350.01930.104*
C220.0265 (6)0.9645 (4)0.1181 (3)0.1057 (16)
H22A0.11150.92320.14720.127*
H22B0.06970.99520.05960.127*
H22C0.00641.01590.16360.127*
C310.3508 (5)0.6535 (3)0.4118 (2)0.0690 (9)
H31A0.23350.64920.42680.083*
H31B0.41490.63270.46780.083*
H31C0.37600.61050.35730.083*
C320.6223 (4)0.7626 (3)0.3596 (3)0.0796 (11)
H32A0.67220.82550.34130.096*
H32B0.63770.71480.30780.096*
H32C0.67460.73810.41830.096*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Rh10.03557 (8)0.04055 (8)0.02795 (7)0.00209 (7)0.00126 (6)0.00432 (6)
S10.0891 (5)0.0511 (3)0.0391 (3)0.0230 (4)0.0130 (3)0.0006 (3)
S20.0735 (5)0.0478 (3)0.0406 (3)0.0079 (3)0.0169 (3)0.0056 (3)
S30.0523 (4)0.0567 (4)0.0330 (3)0.0014 (3)0.0059 (3)0.0039 (3)
Cl10.0431 (4)0.1089 (7)0.0523 (4)0.0039 (4)0.0116 (3)0.0301 (4)
Cl20.0819 (5)0.0494 (3)0.0530 (3)0.0191 (3)0.0068 (4)0.0064 (3)
Cl30.0523 (4)0.0961 (6)0.0478 (3)0.0098 (4)0.0156 (3)0.0042 (4)
C110.089 (3)0.0612 (17)0.087 (2)0.0176 (19)0.029 (2)0.0321 (16)
C120.064 (2)0.105 (3)0.083 (2)0.036 (2)0.0082 (17)0.033 (2)
C210.143 (4)0.066 (2)0.0520 (17)0.012 (2)0.005 (2)0.0160 (14)
C220.101 (3)0.123 (4)0.094 (3)0.060 (3)0.034 (3)0.019 (3)
C310.084 (2)0.072 (2)0.0515 (16)0.0090 (17)0.0111 (15)0.0156 (15)
C320.0433 (16)0.121 (3)0.075 (2)0.0062 (18)0.0167 (16)0.011 (2)
Geometric parameters (Å, °) top
Rh1—S12.3283 (8)C12—H12A0.9600
Rh1—Cl32.3350 (7)C12—H12B0.9600
Rh1—S22.3422 (7)C12—H12C0.9600
Rh1—Cl12.3481 (7)C21—H21A0.9600
Rh1—Cl22.3609 (7)C21—H21B0.9600
Rh1—S32.3660 (7)C21—H21C0.9600
S1—C111.782 (3)C22—H22A0.9600
S1—C121.793 (4)C22—H22B0.9600
S2—C221.785 (4)C22—H22C0.9600
S2—C211.795 (4)C31—H31A0.9600
S3—C321.790 (3)C31—H31B0.9600
S3—C311.790 (3)C31—H31C0.9600
C11—H11A0.9600C32—H32A0.9600
C11—H11B0.9600C32—H32B0.9600
C11—H11C0.9600C32—H32C0.9600
S1—Rh1—Cl392.29 (3)S1—C12—H12A109.5
S1—Rh1—S289.70 (3)S1—C12—H12B109.5
Cl3—Rh1—S285.49 (3)H12A—C12—H12B109.5
S1—Rh1—Cl186.60 (3)S1—C12—H12C109.5
Cl3—Rh1—Cl1177.97 (3)H12A—C12—H12C109.5
S2—Rh1—Cl196.21 (3)H12B—C12—H12C109.5
S1—Rh1—Cl2175.67 (3)S2—C21—H21A109.5
Cl3—Rh1—Cl290.97 (3)S2—C21—H21B109.5
S2—Rh1—Cl293.40 (3)H21A—C21—H21B109.5
Cl1—Rh1—Cl290.04 (3)S2—C21—H21C109.5
S1—Rh1—S393.40 (3)H21A—C21—H21C109.5
Cl3—Rh1—S394.68 (3)H21B—C21—H21C109.5
S2—Rh1—S3176.89 (3)S2—C22—H22A109.5
Cl1—Rh1—S383.68 (3)S2—C22—H22B109.5
Cl2—Rh1—S383.50 (3)H22A—C22—H22B109.5
C11—S1—C1297.72 (17)S2—C22—H22C109.5
C11—S1—Rh1112.51 (13)H22A—C22—H22C109.5
C12—S1—Rh1109.86 (14)H22B—C22—H22C109.5
C22—S2—C2199.7 (2)S3—C31—H31A109.5
C22—S2—Rh1108.98 (15)S3—C31—H31B109.5
C21—S2—Rh1108.32 (13)H31A—C31—H31B109.5
C32—S3—C3198.14 (19)S3—C31—H31C109.5
C32—S3—Rh1108.87 (12)H31A—C31—H31C109.5
C31—S3—Rh1111.35 (10)H31B—C31—H31C109.5
S1—C11—H11A109.5S3—C32—H32A109.5
S1—C11—H11B109.5S3—C32—H32B109.5
H11A—C11—H11B109.5H32A—C32—H32B109.5
S1—C11—H11C109.5S3—C32—H32C109.5
H11A—C11—H11C109.5H32A—C32—H32C109.5
H11B—C11—H11C109.5H32B—C32—H32C109.5
Table 1
Selected geometric parameters (Å)
top
Rh1—S12.3283 (8)S1—C111.782 (3)
Rh1—Cl32.3350 (7)S1—C121.793 (4)
Rh1—S22.3422 (7)S2—C221.785 (4)
Rh1—Cl12.3481 (7)S2—C211.795 (4)
Rh1—Cl22.3609 (7)S3—C321.790 (3)
Rh1—S32.3660 (7)S3—C311.790 (3)
Acknowledgements top

This work was supported by a grant from the University of Tehran.

references
References top

Abbasi, A., Azizi, F., Eriksson, L. & Sandström, M. (2006). Acta Cryst. E62, m2651–m2652.

Alessio, E. (2004). Chem. Rev. 104, 4203–4242.

Brandenburg, K. (1999). DIAMOND. Version 2.1e. Crystal Impact GbR, Bonn, Germany. [Please check year - Version 2.1e normally in 2001, and 2.1c in 1999]

Calligaris, M. (2004). Coord. Chem. Rev. 248, 351–375.

Flack, H. D. (1983). Acta Cryst. A39, 876–881.

James, B. R., Ng, F. T. T. & Rempel, G. L. (1968). Inorg. Nucl. Chem. Lett. 4, 197–199.

Oxford Diffraction (2003). CrysAlis CCD and CrysAlis RED. Versions 1.171.29.2. Oxford Diffraction Ltd, Abingdon, Oxfordshire, England. [Reference not cited - may it be removed?]

Sheldrick, G. M. (1997). SHELXS97 and SHELXL97. University of Göttingen, Germany.

Stoe & Cie (1997). IPDS Software (Version 2.87) and X-RED (Version 1.09). Stoe & Cie GmbH, Darmstadt, Germany.