Abstract
In the title compound, trans-[RhCl(C20H17P)2(CO)], the RhI atom is situated on a center of symmetry, resulting in a statistical 1:1 disorder of the chloride [Rh—Cl = 2.383 (2) Å] and carbonyl [Rh—C = 1.752 (7) Å] ligands. The distorted trans square-planar environment is completed by two P atoms [Rh—P = 2.3251 (4) Å] from two diphenyl(4-vinylphenyl)phosphane ligands. The vinyl group is disordered over two sets of sites in a 0.668 (10):0.332 (10) ratio. The crystal packing exhibits weak C—H⋯Cl and C—H⋯O hydrogen bonds and π–π interactions between the phenyl rings of neighbouring molecules, with a centroid–centroid distance of 3.682 (2) Å.
Related literature
For a review of rhodium Vaska {trans-[RhCl(CO)(PR
3)2]} compounds, see: Roodt et al. (2003 ▶). For related compounds, see: Angoletta (1959 ▶); Vaska & Di Luzio (1961 ▶); Chen et al. (1991 ▶); Kuwabara & Bau (1994 ▶); Otto et al. (2000 ▶); Otto (2001 ▶); Meijboom et al. (2005 ▶).
Experimental
Crystal data
[RhCl(C20H17P)2(CO)]
M r = 742.98
Triclinic,
a = 9.9030 (4) Å
b = 9.9310 (4) Å
c = 10.4150 (4) Å
α = 85.727 (2)°
β = 68.475 (2)°
γ = 62.295 (2)°
V = 837.85 (6) Å3
Z = 1
Cu Kα radiation
μ = 6.01 mm−1
T = 100 K
0.10 × 0.08 × 0.06 mm
Data collection
Bruker APEXII CCD diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2007 ▶) T min = 0.107, T max = 0.402
11163 measured reflections
2941 independent reflections
2850 reflections with I > 2σ(I)
R int = 0.026
Refinement
R[F 2 > 2σ(F 2)] = 0.024
wR(F 2) = 0.057
S = 1.04
2941 reflections
232 parameters
6 restraints
H-atom parameters constrained
Δρmax = 0.46 e Å−3
Δρmin = −0.27 e Å−3
Data collection: APEX2 (Bruker, 2007 ▶); cell refinement: SAINT-Plus (Bruker, 2007 ▶); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: DIAMOND (Brandenburg & Putz, 2005 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶).
Supplementary Material
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812013669/cv5270sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812013669/cv5270Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| C9B—H9B1⋯O01i | 0.93 | 2.54 | 3.205 (11) | 129 |
| C14—H14⋯Cl1ii | 0.93 | 2.79 | 3.660 (3) | 157 |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
Financial assistance from the South African National Research Foundation (SA NRF), the Research Fund of the University of Johannesburg, TESP and SASOL is gratefully acknowledged. Mr S. Enus is acknowledged for the synthesis of this compound.
supplementary crystallographic information
Comment
The original Vaska complex, trans-[IrCl(CO)(PPh3)2], was first reported in 1959 (Angoletta, 1959), but later correctly formulated by Vaska in 1961 (Vaska & Di Luzio, 1961) . This class of symmetrical square-planar complexes often crystallizes with the metal atom on a crystallographic inversion centre of symmetry, thus imposing a disordered packing arrangement (Otto, 2001;Otto et al., 2000; Chen et al.,1991; Kuwabara & Bau, 1994).These Vaska type complexes are useful model complexes and provide several probing methods, e.g. NMR and IR, to investigate the steric and electronic effects of novel group 15 ligands (Roodt et al., 2003).
Here we report the title compound, the i>trans-[RhClL2(CO)](L = diphenyl(4-vinylphenyl)phosphane) complex crystallizes in the triclinic space group, P-1.The crystal structure of the title compound (Fig.1) shows the expected square planar geometry with the phosphane ligands trans to each other. The RhI atom is situated on a center of symmetry, resulting in a statistical 1:1 disorder of the chlorido [Rh—Cl 2.383 (2) Å] and carbonyl [Rh—C 1.752 (7) Å] ligands. The distorted trans square-planar environment is completed by two P atoms [Rh—P 2.3251 (4) Å] from two L ligands. The vinyl group is disordered over two sets of sites in a 0.668 (10):0.332 (10) ratio. The J coupling of (Rh-P) is 128 Hz which is in agreement with the coupling constants for other rhodium Vaska type complexes of this nature (Meijboom et al., 2005). The C01–Rh1–P2 angle of 92.99 (17) ° and the P2–Rh1–Cl1 of 94.46 (3) ° exemplifies the deviation from the ideal 90 ° square planar geometry.
The crystal packing exhibits weak intermolecular C—H···Cl and C—H···O hydrogen bonds (Table 1). There is a π–π interaction between the neighbouring phenyl ring centroids of C16-C21 and C16-C21 (2-x,1-y,1-z), respectively with the centroid-centroid distance of 3.682 (2) Å.
Experimental
Diphenylphosphinostyrene (0.15 g, 0.51 mmol) was dissolved in acetone (6 cm3). A solution of dichlorotetracarbonyldirhodium(I) (0.04 g, 0.13 mmol) in acetone was added to the phosphine solution. The mixture was stirred for 5 minutes, slow evaporation of the solvent afforded the title compound as a yellow crystalline solid. Spectroscopic analysis:31P{H} NMR (CDCl3, 161.99 MHz, p.p.m.): 46.42 [d, 1J(Rh—P) = 179.81 Hz]; IR ν(CO): 1957.96 cm-1; (CD2Cl2) ν(CO): 1977.04 cm-1.
Refinement
The H atoms were placed in geometrically idealized positions (C—H bonds of 0.95–0.98 /%A) and constrained to ride on their parent atoms with Uiso(H) = 1.2Ueq(C).
Figures
Fig. 1.
The molecular structure of the title compound showing the atomic numbering and 50% probability displacement ellipsoids [symmetry code: (i) (1 - x, 1 - y, 1 - z)].
Crystal data
| [RhCl(C20H17P)2(CO)] | Z = 1 |
| Mr = 742.98 | F(000) = 380 |
| Triclinic, P1 | Dx = 1.473 Mg m−3 |
| Hall symbol: -P 1 | Cu Kα radiation, λ = 1.54178 Å |
| a = 9.9030 (4) Å | Cell parameters from 8410 reflections |
| b = 9.9310 (4) Å | θ = 4.6–66.3° |
| c = 10.4150 (4) Å | µ = 6.01 mm−1 |
| α = 85.727 (2)° | T = 100 K |
| β = 68.475 (2)° | Rectangular, yellow |
| γ = 62.295 (2)° | 0.10 × 0.08 × 0.06 mm |
| V = 837.85 (6) Å3 |
Data collection
| Bruker APEXII CCD diffractometer | 2941 independent reflections |
| Radiation source: fine-focus sealed tube | 2850 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.026 |
| φ and ω scans | θmax = 66.3°, θmin = 4.6° |
| Absorption correction: multi-scan (SADABS; Bruker, 2007) | h = −11→7 |
| Tmin = 0.107, Tmax = 0.402 | k = −11→11 |
| 11163 measured reflections | l = −12→12 |
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)] = 0.024 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.057 | H-atom parameters constrained |
| S = 1.04 | w = 1/[σ2(Fo2) + (0.0256P)2 + 0.5512P] where P = (Fo2 + 2Fc2)/3 |
| 2941 reflections | (Δ/σ)max = 0.001 |
| 232 parameters | Δρmax = 0.46 e Å−3 |
| 6 restraints | Δρmin = −0.27 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 | Occ. (<1) | |
| Rh1 | 0.5 | 0.5 | 0.5 | 0.02293 (9) | |
| Cl1 | 0.34866 (19) | 0.7717 (2) | 0.55041 (12) | 0.0329 (3) | 0.5 |
| C01 | 0.6149 (7) | 0.2999 (8) | 0.4747 (5) | 0.0330 (14)* | 0.5 |
| O01 | 0.6932 (5) | 0.1680 (6) | 0.4511 (4) | 0.0393 (13)* | 0.5 |
| P2 | 0.71286 (5) | 0.50159 (5) | 0.30681 (4) | 0.02055 (12) | |
| C2 | 0.7589 (2) | 0.3785 (2) | 0.15917 (19) | 0.0239 (4) | |
| C3 | 0.9177 (3) | 0.2746 (2) | 0.0745 (2) | 0.0305 (4) | |
| H3 | 1.0063 | 0.2629 | 0.0949 | 0.037* | |
| C4 | 0.9461 (3) | 0.1880 (3) | −0.0400 (2) | 0.0412 (5) | |
| H4 | 1.0536 | 0.1179 | −0.0942 | 0.049* | |
| C5 | 0.8188 (4) | 0.2033 (3) | −0.0755 (2) | 0.0431 (6) | |
| C6 | 0.6589 (3) | 0.3064 (3) | 0.0108 (3) | 0.0421 (6) | |
| H6 | 0.5708 | 0.3183 | −0.0103 | 0.05* | |
| C7 | 0.6284 (3) | 0.3916 (2) | 0.1273 (2) | 0.0331 (4) | |
| H7 | 0.5206 | 0.4578 | 0.1843 | 0.04* | |
| C10 | 0.6760 (2) | 0.6851 (2) | 0.23862 (19) | 0.0224 (4) | |
| C11 | 0.6826 (2) | 0.7072 (2) | 0.1032 (2) | 0.0253 (4) | |
| H11 | 0.7081 | 0.6263 | 0.0436 | 0.03* | |
| C12 | 0.6512 (3) | 0.8499 (2) | 0.0569 (2) | 0.0327 (4) | |
| H12 | 0.6555 | 0.8642 | −0.0335 | 0.039* | |
| C13 | 0.6137 (3) | 0.9700 (2) | 0.1445 (3) | 0.0379 (5) | |
| H13 | 0.591 | 1.0657 | 0.1137 | 0.045* | |
| C14 | 0.6097 (3) | 0.9485 (2) | 0.2788 (2) | 0.0346 (5) | |
| H14 | 0.5864 | 1.0292 | 0.3374 | 0.042* | |
| C15 | 0.6406 (2) | 0.8070 (2) | 0.3253 (2) | 0.0277 (4) | |
| H15 | 0.6377 | 0.793 | 0.4153 | 0.033* | |
| C16 | 0.9104 (2) | 0.4379 (2) | 0.32389 (18) | 0.0226 (4) | |
| C17 | 0.9552 (3) | 0.3347 (2) | 0.4169 (2) | 0.0297 (4) | |
| H17 | 0.8835 | 0.299 | 0.4721 | 0.036* | |
| C18 | 1.1066 (3) | 0.2846 (2) | 0.4277 (2) | 0.0335 (4) | |
| H18 | 1.1369 | 0.2139 | 0.4888 | 0.04* | |
| C19 | 1.2126 (2) | 0.3398 (2) | 0.3477 (2) | 0.0316 (4) | |
| H19 | 1.3137 | 0.3065 | 0.3553 | 0.038* | |
| C20 | 1.1679 (2) | 0.4442 (3) | 0.2569 (2) | 0.0314 (4) | |
| H20 | 1.2384 | 0.4822 | 0.2042 | 0.038* | |
| C21 | 1.0179 (2) | 0.4927 (2) | 0.2438 (2) | 0.0274 (4) | |
| H21 | 0.9891 | 0.562 | 0.1814 | 0.033* | |
| C8A | 0.8768 (8) | 0.0979 (6) | −0.2041 (5) | 0.0314 (11) | 0.668 (10) |
| H8A | 0.9865 | 0.0231 | −0.2409 | 0.038* | 0.668 (10) |
| C9A | 0.7794 (5) | 0.1079 (5) | −0.2647 (4) | 0.0441 (14) | 0.668 (10) |
| H9A1 | 0.6693 | 0.1819 | −0.2295 | 0.053* | 0.668 (10) |
| H9A2 | 0.8198 | 0.041 | −0.3433 | 0.053* | 0.668 (10) |
| C9B | 0.9234 (11) | 0.0621 (10) | −0.2909 (12) | 0.043 (3) | 0.332 (10) |
| H9B1 | 1.0259 | 0.0295 | −0.2862 | 0.051* | 0.332 (10) |
| H9B2 | 0.916 | 0.0272 | −0.3672 | 0.051* | 0.332 (10) |
| C8B | 0.7895 (13) | 0.1573 (11) | −0.1898 (8) | 0.028 (2) | 0.332 (10) |
| H8B | 0.6847 | 0.1928 | −0.1903 | 0.034* | 0.332 (10) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Rh1 | 0.01987 (12) | 0.02210 (12) | 0.02175 (12) | −0.01035 (8) | −0.00276 (8) | 0.00663 (7) |
| Cl1 | 0.0272 (6) | 0.0269 (8) | 0.0345 (6) | −0.0141 (6) | 0.0001 (4) | 0.0063 (6) |
| P2 | 0.0190 (2) | 0.0228 (2) | 0.0180 (2) | −0.01070 (18) | −0.00469 (17) | 0.00582 (17) |
| C2 | 0.0292 (9) | 0.0246 (9) | 0.0233 (9) | −0.0173 (8) | −0.0107 (8) | 0.0098 (7) |
| C3 | 0.0334 (10) | 0.0332 (11) | 0.0265 (10) | −0.0203 (9) | −0.0065 (8) | 0.0024 (8) |
| C4 | 0.0518 (14) | 0.0439 (13) | 0.0288 (11) | −0.0326 (11) | −0.0013 (10) | −0.0035 (9) |
| C5 | 0.0767 (17) | 0.0471 (13) | 0.0270 (11) | −0.0487 (13) | −0.0171 (11) | 0.0118 (10) |
| C6 | 0.0690 (16) | 0.0469 (13) | 0.0488 (13) | −0.0451 (13) | −0.0427 (13) | 0.0280 (11) |
| C7 | 0.0363 (11) | 0.0316 (11) | 0.0426 (12) | −0.0208 (9) | −0.0216 (9) | 0.0135 (9) |
| C10 | 0.0172 (8) | 0.0230 (9) | 0.0246 (9) | −0.0103 (7) | −0.0051 (7) | 0.0061 (7) |
| C11 | 0.0225 (9) | 0.0273 (9) | 0.0248 (9) | −0.0127 (7) | −0.0069 (7) | 0.0052 (7) |
| C12 | 0.0315 (10) | 0.0335 (11) | 0.0308 (10) | −0.0154 (9) | −0.0114 (8) | 0.0146 (8) |
| C13 | 0.0359 (11) | 0.0251 (10) | 0.0481 (13) | −0.0151 (9) | −0.0119 (10) | 0.0133 (9) |
| C14 | 0.0317 (10) | 0.0264 (10) | 0.0405 (12) | −0.0146 (8) | −0.0061 (9) | −0.0009 (8) |
| C15 | 0.0247 (9) | 0.0302 (10) | 0.0249 (9) | −0.0135 (8) | −0.0050 (7) | 0.0028 (8) |
| C16 | 0.0229 (9) | 0.0241 (9) | 0.0182 (8) | −0.0094 (7) | −0.0067 (7) | −0.0001 (7) |
| C17 | 0.0337 (10) | 0.0297 (10) | 0.0298 (10) | −0.0168 (8) | −0.0144 (8) | 0.0077 (8) |
| C18 | 0.0373 (11) | 0.0304 (10) | 0.0371 (11) | −0.0133 (9) | −0.0230 (9) | 0.0086 (9) |
| C19 | 0.0273 (10) | 0.0353 (11) | 0.0315 (10) | −0.0109 (8) | −0.0142 (8) | −0.0023 (8) |
| C20 | 0.0274 (10) | 0.0418 (12) | 0.0266 (10) | −0.0184 (9) | −0.0088 (8) | 0.0028 (8) |
| C21 | 0.0271 (9) | 0.0344 (10) | 0.0213 (9) | −0.0149 (8) | −0.0096 (8) | 0.0056 (8) |
| C8A | 0.032 (2) | 0.030 (2) | 0.029 (3) | −0.0122 (19) | −0.010 (2) | 0.0010 (17) |
| C9A | 0.044 (2) | 0.045 (2) | 0.038 (2) | −0.0152 (17) | −0.0148 (16) | −0.0073 (17) |
| C9B | 0.046 (6) | 0.048 (5) | 0.033 (6) | −0.018 (4) | −0.016 (4) | −0.004 (4) |
| C8B | 0.023 (4) | 0.029 (4) | 0.031 (4) | −0.010 (4) | −0.011 (3) | −0.002 (3) |
Geometric parameters (Å, º)
| Rh1—C01i | 1.752 (7) | C12—C13 | 1.377 (3) |
| Rh1—C01 | 1.752 (7) | C12—H12 | 0.93 |
| Rh1—P2 | 2.3251 (4) | C13—C14 | 1.388 (3) |
| Rh1—P2i | 2.3251 (4) | C13—H13 | 0.93 |
| Rh1—Cl1i | 2.383 (2) | C14—C15 | 1.383 (3) |
| Rh1—Cl1 | 2.383 (2) | C14—H14 | 0.93 |
| C01—O01 | 1.158 (7) | C15—H15 | 0.93 |
| P2—C2 | 1.8205 (19) | C16—C17 | 1.389 (3) |
| P2—C10 | 1.8266 (18) | C16—C21 | 1.395 (3) |
| P2—C16 | 1.8298 (18) | C17—C18 | 1.389 (3) |
| C2—C3 | 1.388 (3) | C17—H17 | 0.93 |
| C2—C7 | 1.396 (3) | C18—C19 | 1.387 (3) |
| C3—C4 | 1.387 (3) | C18—H18 | 0.93 |
| C3—H3 | 0.93 | C19—C20 | 1.377 (3) |
| C4—C5 | 1.380 (4) | C19—H19 | 0.93 |
| C4—H4 | 0.93 | C20—C21 | 1.389 (3) |
| C5—C6 | 1.396 (4) | C20—H20 | 0.93 |
| C5—C8B | 1.473 (8) | C21—H21 | 0.93 |
| C5—C8A | 1.518 (6) | C8A—C9A | 1.299 (8) |
| C6—C7 | 1.387 (3) | C8A—H8A | 0.93 |
| C6—H6 | 0.93 | C9A—H9A1 | 0.93 |
| C7—H7 | 0.93 | C9A—H9A2 | 0.93 |
| C10—C15 | 1.392 (3) | C9B—C8B | 1.311 (15) |
| C10—C11 | 1.393 (3) | C9B—H9B1 | 0.93 |
| C11—C12 | 1.392 (3) | C9B—H9B2 | 0.93 |
| C11—H11 | 0.93 | C8B—H8B | 0.93 |
| C01i—Rh1—C01 | 180.0000 (10) | C12—C11—C10 | 120.20 (19) |
| C01i—Rh1—P2 | 92.99 (17) | C12—C11—H11 | 119.9 |
| C01—Rh1—P2 | 87.01 (17) | C10—C11—H11 | 119.9 |
| C01i—Rh1—P2i | 87.01 (17) | C13—C12—C11 | 120.2 (2) |
| C01—Rh1—P2i | 92.99 (17) | C13—C12—H12 | 119.9 |
| P2—Rh1—P2i | 180.00 (2) | C11—C12—H12 | 119.9 |
| C01i—Rh1—Cl1i | 175.46 (17) | C12—C13—C14 | 120.06 (19) |
| C01—Rh1—Cl1i | 4.54 (17) | C12—C13—H13 | 120 |
| P2—Rh1—Cl1i | 85.54 (3) | C14—C13—H13 | 120 |
| P2i—Rh1—Cl1i | 94.46 (3) | C15—C14—C13 | 119.9 (2) |
| C01i—Rh1—Cl1 | 4.54 (17) | C15—C14—H14 | 120.1 |
| C01—Rh1—Cl1 | 175.46 (17) | C13—C14—H14 | 120.1 |
| P2—Rh1—Cl1 | 94.46 (3) | C14—C15—C10 | 120.72 (19) |
| P2i—Rh1—Cl1 | 85.54 (3) | C14—C15—H15 | 119.6 |
| Cl1i—Rh1—Cl1 | 180.00 (6) | C10—C15—H15 | 119.6 |
| O01—C01—Rh1 | 176.7 (5) | C17—C16—C21 | 119.13 (17) |
| C2—P2—C10 | 103.30 (8) | C17—C16—P2 | 120.51 (15) |
| C2—P2—C16 | 105.19 (8) | C21—C16—P2 | 120.36 (14) |
| C10—P2—C16 | 102.16 (8) | C16—C17—C18 | 120.31 (19) |
| C2—P2—Rh1 | 110.70 (6) | C16—C17—H17 | 119.8 |
| C10—P2—Rh1 | 116.84 (6) | C18—C17—H17 | 119.8 |
| C16—P2—Rh1 | 117.12 (6) | C19—C18—C17 | 120.11 (19) |
| C3—C2—C7 | 118.24 (19) | C19—C18—H18 | 119.9 |
| C3—C2—P2 | 123.22 (15) | C17—C18—H18 | 119.9 |
| C7—C2—P2 | 118.52 (16) | C20—C19—C18 | 119.90 (18) |
| C4—C3—C2 | 120.8 (2) | C20—C19—H19 | 120 |
| C4—C3—H3 | 119.6 | C18—C19—H19 | 120 |
| C2—C3—H3 | 119.6 | C19—C20—C21 | 120.27 (19) |
| C5—C4—C3 | 121.7 (2) | C19—C20—H20 | 119.9 |
| C5—C4—H4 | 119.2 | C21—C20—H20 | 119.9 |
| C3—C4—H4 | 119.2 | C20—C21—C16 | 120.26 (18) |
| C4—C5—C6 | 117.4 (2) | C20—C21—H21 | 119.9 |
| C4—C5—C8B | 140.7 (5) | C16—C21—H21 | 119.9 |
| C6—C5—C8B | 101.4 (5) | C9A—C8A—C5 | 122.6 (5) |
| C4—C5—C8A | 113.1 (3) | C9A—C8A—H8A | 118.7 |
| C6—C5—C8A | 129.4 (3) | C5—C8A—H8A | 118.7 |
| C7—C6—C5 | 121.6 (2) | C8A—C9A—H9A1 | 120 |
| C7—C6—H6 | 119.2 | C8A—C9A—H9A2 | 120 |
| C5—C6—H6 | 119.2 | H9A1—C9A—H9A2 | 120 |
| C6—C7—C2 | 120.3 (2) | C8B—C9B—H9B1 | 120 |
| C6—C7—H7 | 119.9 | C8B—C9B—H9B2 | 120 |
| C2—C7—H7 | 119.9 | H9B1—C9B—H9B2 | 120 |
| C15—C10—C11 | 118.91 (17) | C9B—C8B—C5 | 114.4 (8) |
| C15—C10—P2 | 118.66 (14) | C9B—C8B—H8B | 122.8 |
| C11—C10—P2 | 122.43 (15) | C5—C8B—H8B | 122.8 |
| C01i—Rh1—P2—C2 | −126.99 (17) | Rh1—P2—C10—C15 | 59.78 (15) |
| C01—Rh1—P2—C2 | 53.01 (17) | C2—P2—C10—C11 | 1.31 (17) |
| Cl1i—Rh1—P2—C2 | 48.71 (7) | C16—P2—C10—C11 | 110.36 (15) |
| Cl1—Rh1—P2—C2 | −131.29 (7) | Rh1—P2—C10—C11 | −120.47 (14) |
| C01i—Rh1—P2—C10 | −9.16 (17) | C15—C10—C11—C12 | −1.2 (3) |
| C01—Rh1—P2—C10 | 170.84 (17) | P2—C10—C11—C12 | 179.06 (15) |
| Cl1i—Rh1—P2—C10 | 166.53 (7) | C10—C11—C12—C13 | 0.1 (3) |
| Cl1—Rh1—P2—C10 | −13.47 (7) | C11—C12—C13—C14 | 1.0 (3) |
| C01i—Rh1—P2—C16 | 112.47 (17) | C12—C13—C14—C15 | −1.1 (3) |
| C01—Rh1—P2—C16 | −67.53 (17) | C13—C14—C15—C10 | 0.1 (3) |
| Cl1i—Rh1—P2—C16 | −71.84 (7) | C11—C10—C15—C14 | 1.1 (3) |
| Cl1—Rh1—P2—C16 | 108.16 (7) | P2—C10—C15—C14 | −179.15 (15) |
| C10—P2—C2—C3 | 99.98 (17) | C2—P2—C16—C17 | −96.18 (16) |
| C16—P2—C2—C3 | −6.79 (18) | C10—P2—C16—C17 | 156.22 (16) |
| Rh1—P2—C2—C3 | −134.20 (15) | Rh1—P2—C16—C17 | 27.23 (17) |
| C10—P2—C2—C7 | −78.41 (16) | C2—P2—C16—C21 | 83.97 (16) |
| C16—P2—C2—C7 | 174.82 (15) | C10—P2—C16—C21 | −23.63 (17) |
| Rh1—P2—C2—C7 | 47.41 (16) | Rh1—P2—C16—C21 | −152.63 (13) |
| C7—C2—C3—C4 | 1.0 (3) | C21—C16—C17—C18 | −1.3 (3) |
| P2—C2—C3—C4 | −177.38 (16) | P2—C16—C17—C18 | 178.86 (16) |
| C2—C3—C4—C5 | 1.1 (3) | C16—C17—C18—C19 | 1.3 (3) |
| C3—C4—C5—C6 | −1.9 (3) | C17—C18—C19—C20 | −0.3 (3) |
| C3—C4—C5—C8B | 168.8 (5) | C18—C19—C20—C21 | −0.9 (3) |
| C3—C4—C5—C8A | −180.0 (2) | C19—C20—C21—C16 | 0.9 (3) |
| C4—C5—C6—C7 | 0.6 (3) | C17—C16—C21—C20 | 0.2 (3) |
| C8B—C5—C6—C7 | −173.4 (3) | P2—C16—C21—C20 | −179.99 (15) |
| C8A—C5—C6—C7 | 178.3 (3) | C4—C5—C8A—C9A | −171.1 (3) |
| C5—C6—C7—C2 | 1.5 (3) | C6—C5—C8A—C9A | 11.1 (5) |
| C3—C2—C7—C6 | −2.3 (3) | C8B—C5—C8A—C9A | −5.9 (6) |
| P2—C2—C7—C6 | 176.19 (15) | C4—C5—C8B—C9B | 6.1 (10) |
| C2—P2—C10—C15 | −178.44 (14) | C6—C5—C8B—C9B | 177.7 (6) |
| C16—P2—C10—C15 | −69.39 (16) | C8A—C5—C8B—C9B | −15.6 (5) |
Symmetry code: (i) −x+1, −y+1, −z+1.
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C9B—H9B1···O01ii | 0.93 | 2.54 | 3.205 (11) | 129 |
| C14—H14···Cl1iii | 0.93 | 2.79 | 3.660 (3) | 157 |
Symmetry codes: (ii) −x+2, −y, −z; (iii) −x+1, −y+2, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: CV5270).
References
- Angoletta, M. (1959). Gazz. Chim. Ital. 89, 2359–2361.
- Brandenburg, K. & Putz, H. (2005). DIAMOND Crystal Impact GbR, Bonn, Germany.
- Bruker (2007). APEX2, SAINT-Plus and SADABS Bruker AXS Inc., Madison, Wisconsin, USA.
- Chen, Y.-J., Wang, J.-C. & Wang, Y. (1991). Acta Cryst. C47, 2441–2442.
- Farrugia, L. J. (1999). J. Appl. Cryst. 32, 837–838.
- Kuwabara, E. & Bau, R. (1994). Acta Cryst. C50, 1409–1411.
- Meijboom, R., Muller, A. & Roodt, A. (2005). Acta Cryst. E61, m1283–m1285.
- Otto, S. (2001). Acta Cryst. C57, 793–795. [DOI] [PubMed]
- Otto, S., Roodt, A. & Smith, J. (2000). Inorg. Chim. Acta, 303, 295–299.
- Roodt, A., Otto, S. & Steyl, G. (2003). Coord. Chem. Rev. 245, 121–137.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Vaska, L. & Di Luzio, J. W. (1961). J. Am. Chem. Soc. 83, 2784–2785.
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812013669/cv5270sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812013669/cv5270Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

