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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Nov 5;67(Pt 12):m1695–m1696. doi: 10.1107/S1600536811046150

trans-Carbonyl­chloridobis[tris­(4-meth­oxy­phen­yl)phosphane-κP]rhodium(I)

Stefan Warsink a,*, Andreas Roodt a
PMCID: PMC3238621  PMID: 22199512

Abstract

The title complex, [RhCl(C21H21O3P)2(CO)], is a rhodium analogue to Vaska’s complex with para-meth­oxy substituents on the six phosphan­yl–aryl units. Two independent mol­ecules are present in the unit cell, with their metal atoms both located on an inversion centre. This causes the chloride and carbonyl ligands to exhibit a positional disorder in a 0.5:0.5 ratio. The two RhI atoms exhibit a distorted square-planar geometry. There are a few weak intra­molecular C—H⋯X inter­actions (X = O, Cl). Inter­estingly, no significant inter­molecular inter­actions are found between the two independent mol­ecules.

Related literature

For background to Vaska’s complex, see: Angoletta (1959); Vaska & Di Luzio (1961). For related literature on rhodium Vaska complexes, see: Basson et al. (1990); Clarke et al. (2002); Kemp et al. (1995); Rheingold & Geib (1987); Roodt et al. (2003); Wilson et al. (2002). For similar complexes, see: Burgoyne et al. (2010), Meijboom et al. (2006), Monge et al. (1983); Otto et al. (1999). Synthetic details are given in McCleverty & Wilkinson (1990).graphic file with name e-67-m1695-scheme1.jpg

Experimental

Crystal data

  • [RhCl(C21H21O3P)2(CO)]

  • M r = 871.07

  • Triclinic, Inline graphic

  • a = 7.8350 (4) Å

  • b = 12.3151 (8) Å

  • c = 21.0591 (13) Å

  • α = 90.995 (2)°

  • β = 99.591 (2)°

  • γ = 101.220 (2)°

  • V = 1962.7 (2) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.64 mm−1

  • T = 100 K

  • 0.24 × 0.16 × 0.10 mm

Data collection

  • Bruker APEXII CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2004) T min = 0.887, T max = 0.937

  • 26016 measured reflections

  • 9327 independent reflections

  • 6401 reflections with I > 2σ(I)

  • R int = 0.098

Refinement

  • R[F 2 > 2σ(F 2)] = 0.052

  • wR(F 2) = 0.144

  • S = 1.04

  • 9327 reflections

  • 517 parameters

  • H-atom parameters constrained

  • Δρmax = 2.45 e Å−3

  • Δρmin = −1.17 e Å−3

Data collection: APEX2 (Bruker, 2005); cell refinement: SAINT-Plus (Bruker, 2004); data reduction: SAINT-Plus and XPREP (Bruker, 2004); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: Mercury (Macrae et al., 2008); software used to prepare material for publication: WinGX (Farrugia, 1999).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811046150/wm2548sup1.cif

e-67-m1695-sup1.cif (46.6KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811046150/wm2548Isup2.hkl

e-67-m1695-Isup2.hkl (447KB, hkl)

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

Table 1. Selected geometric parameters (Å, °).

Rh1—C1 1.699 (12)
Rh1—P1 2.3257 (10)
Rh1—Cl1 2.416 (5)
Rh2—C23 1.751 (11)
Rh2—P2 2.3321 (11)
Rh2—Cl2 2.410 (4)
C1—O1 1.157 (18)
C23—O5 1.171 (13)
C1—Rh1—P1 90.5 (4)
P1—Rh1—Cl1 91.20 (9)
C23—Rh2—P2 91.9 (4)
P2—Rh2—Cl2 92.06 (10)

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

D—H⋯A D—H H⋯A DA D—H⋯A
C14—H046⋯Cl1 0.95 2.81 3.191 (5) 105
C32—H021⋯Cl2 0.95 2.82 3.157 (5) 102
C8—H04A⋯Cl1i 0.98 2.73 3.693 (7) 169
C8—H04A⋯O1i 0.98 2.52 3.486 (18) 168

Symmetry code: (i) Inline graphic.

Acknowledgments

The authors thank SASOL, the South African NRF and THRIP and the University of the Free State Research Fund for financial support. The views expressed do not necessarily represent that of the NRF.

supplementary crystallographic information

Comment

Vaska's complex was first synthesized by Angoletta (1959) and later correctly formulated as trans-[IrCl(CO)(PPh3)2] (Vaska & Di Luzio, 1961). This compound has been used in various catalytic processes and it or its analogues are often employed as model compounds (Rheingold & Geib, 1987; Basson et al., 1990; Kemp et al., 1995; Roodt et al., 2003).

Various 'Vaska complexes' have been synthesized, exploring different metals but especially introducing different substituents on the phosphane ligands. These modifications have an impact on the steric hindrance around the metal (Clarke et al., 2002; Wilson et al., 2002), but in the case of para-substituted triaryl phosphanes the effect is purely electronic (Monge et al., 1983; Otto et al., 1999; Meijboom et al., 2006; Burgoyne et al., 2010). Since only limited data are available on this kind of complexes, we have prepared the rhodium analogue (I), [RhCl(C21H21O3P)2(CO)], bearing relatively electron-rich tri(para-methoxyphenyl)-phosphane ligands.

Two independent half-molecules are present in the asymmetric unit of compound (I), in each case with the RhI atoms located on inversion centres. The metal atoms display a distorted square planar geometry with the phosphane ligands located in mutual trans-positions (Fig. 1). Selected bond lenghts and angles are presented in Table 1.

The carbonyl moiety has a slightly bent geometry, with Rh—C—O angles of 173.2 (14)° and 176.8 (16)° for the two molecules, respectively. In solution infrared spectroscopy only one signal was observed for the carbonyl ligand at 1974 cm-1. Also in solid state infrared spectroscopy of the amorphous material, only one signal was observed at 1964 cm-1. Only when a crystalline sample was analysed, two signals were observed at 1956 and 1973 cm-1, showing the stretching vibrations of both the independent carbonyl ligands. In 31P NMR the signal for the phospine ligands was observed at 24.95 ppm with a JRh—P of 124.5 Hz, which is in line with analogous complexes.

The Rh—P bond lengths fall in the range of other, analogous rhodium Vaska complexes. In contrast, the bonds of the metal to the carbonyl and chlorido ligands are significantly influenced by the electron-donating phosphane ligands. The bond to the chlorido ligand is the longest reported for this kind of complexes bearing triaryl phosphanes. The same influence is also notably present in the bonding of the carbonyl ligand. Its bond to the rhodium atom is quite short, which indicates significant metal-to-ligand electron donation. As a consequence, the C—O bond is lengthened.

There are a few weak intramolecular C—H···X interactions (X = O, Cl), which are listed in Table 2. Interestingly, no intermolecular interactions are found between the two independent molecules.

Experimental

Compound (I) was synthesized by slowly adding 4 equivalents of tri(4-methoxyphenyl)phosphane to a dimethyl formamide solution of [RhCl(CO)2]2 (McCleverty & Wilkinson, 1990). The product was precipitated with ice water and isolated by filtration. Crystallization was performed by dissolving the complex in a small amount of dichloromethane which was then carefully layered with approximately 5 volumetric equivalents of hexane. The mixture was stored in a loosely closed vessel, from which yellow crystals precipitated.

Refinement

The aromatic and methyl H atoms were placed in geometrically idealized positions (C—H = 0.93–0.98) and constrained to ride on their parent atoms with Uiso(H) = 1.2Ueq(C) for aromatic protons and Uiso(H) = 1.5Ueq(C) for methyl protons. The disordered Cl and CO ligands were constrained to have occupancies of 0.5 at each of the two positions. The highest residual electron density was located 0.90 Å from Rh1 and was essentially meaningless. The deepest hole was located 1.00 Å from Rh1.

Figures

Fig. 1.

Fig. 1.

Molecular structure of (I), showing the unit cell to clarify the special positions of the two rhodium atoms. Displacement ellipsoids are drawn at the 50% probability level. H-atoms have been omitted for clarity [Symmetry code: (i) -x, 1 - y, 1 - z; (ii) -x, -y, -z].

Crystal data

[RhCl(C21H21O3P)2(CO)] Z = 2
Mr = 871.07 F(000) = 896
Triclinic, P1 Dx = 1.474 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 7.8350 (4) Å Cell parameters from 6500 reflections
b = 12.3151 (8) Å θ = 2.9–28.1°
c = 21.0591 (13) Å µ = 0.64 mm1
α = 90.995 (2)° T = 100 K
β = 99.591 (2)° Cuboid, yellow
γ = 101.220 (2)° 0.24 × 0.16 × 0.10 mm
V = 1962.7 (2) Å3

Data collection

Bruker APEXII CCD diffractometer 9327 independent reflections
Radiation source: sealed tube 6401 reflections with I > 2σ(I)
graphite Rint = 0.098
Detector resolution: 512 pixels mm-1 θmax = 28°, θmin = 2.0°
φ and ω scans h = −10→6
Absorption correction: multi-scan (SADABS; Bruker, 2004) k = −15→16
Tmin = 0.887, Tmax = 0.937 l = −27→27
26016 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)] = 0.052 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.144 H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0711P)2] where P = (Fo2 + 2Fc2)/3
9327 reflections (Δ/σ)max = 0.003
517 parameters Δρmax = 2.45 e Å3
0 restraints Δρmin = −1.17 e Å3

Special details

Experimental. The intensity data was collected on a Bruker X8 Apex II 4 K Kappa CCD diffractometer using an exposure time of 30 s/frame. A total of 1318 frames was collected with a frame width of 0.5° covering up to θ=28.00° with 98.3% completeness accomplished.
Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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 0.5 0.5 0.01620 (12)
Rh2 0 0 0 0.01681 (12)
P1 0.17881 (11) 0.45129 (8) 0.59018 (4) 0.0169 (2)
P2 0.19028 (11) 0.15093 (8) −0.03218 (4) 0.0169 (2)
C1 −0.0559 (14) 0.3657 (10) 0.4714 (6) 0.034 (3) 0.5
C2 0.3688 (4) 0.5602 (3) 0.62055 (16) 0.0169 (8)
C3 0.4759 (4) 0.6069 (3) 0.57726 (17) 0.0196 (8)
H023 0.4495 0.579 0.5336 0.023*
C4 0.6194 (4) 0.6927 (3) 0.59619 (18) 0.0210 (8)
H035 0.6927 0.7215 0.5663 0.025*
C5 0.6553 (5) 0.7363 (3) 0.65925 (19) 0.0228 (8)
C6 0.5486 (5) 0.6916 (3) 0.70302 (18) 0.0230 (8)
H030 0.5727 0.7214 0.7462 0.028*
C7 0.4080 (4) 0.6042 (3) 0.68391 (17) 0.0198 (8)
H047 0.3372 0.5738 0.7143 0.024*
C8 0.8885 (6) 0.8790 (4) 0.6380 (2) 0.0418 (12)
H04A 0.9481 0.8272 0.6187 0.063*
H04B 0.9769 0.9412 0.6604 0.063*
H04C 0.8091 0.9069 0.604 0.063*
C9 0.2703 (4) 0.3274 (3) 0.58447 (16) 0.0179 (8)
C10 0.4508 (4) 0.3317 (3) 0.58604 (16) 0.0184 (8)
H048 0.5295 0.4016 0.5905 0.022*
C11 0.5171 (5) 0.2356 (3) 0.58120 (17) 0.0221 (8)
H036 0.64 0.2404 0.5823 0.027*
C12 0.4043 (5) 0.1327 (3) 0.57470 (17) 0.0220 (8)
C13 0.2238 (5) 0.1265 (3) 0.57155 (18) 0.0233 (8)
H022 0.1452 0.0565 0.5662 0.028*
C14 0.1590 (4) 0.2230 (3) 0.57627 (17) 0.0222 (8)
H046 0.0355 0.2178 0.5739 0.027*
C15 0.3688 (6) −0.0645 (3) 0.5660 (2) 0.0342 (10)
H05J 0.3069 −0.0728 0.6029 0.051*
H05K 0.44 −0.1216 0.5657 0.051*
H05L 0.2822 −0.0724 0.5259 0.051*
C16 0.0517 (4) 0.4249 (3) 0.65485 (16) 0.0174 (8)
C17 0.0822 (4) 0.3493 (3) 0.70175 (17) 0.0212 (8)
H034 0.1791 0.3132 0.7026 0.025*
C18 −0.0271 (4) 0.3261 (3) 0.74719 (17) 0.0210 (8)
H033 −0.0038 0.2751 0.7793 0.025*
C19 −0.1717 (4) 0.3776 (3) 0.74576 (17) 0.0192 (8)
C20 −0.1985 (4) 0.4567 (3) 0.70120 (17) 0.0190 (8)
H043 −0.2924 0.4951 0.7016 0.023*
C21 −0.0880 (4) 0.4794 (3) 0.65610 (17) 0.0197 (8)
H014 −0.1077 0.5333 0.6254 0.024*
C22 −0.4399 (4) 0.3816 (4) 0.78430 (18) 0.0257 (9)
H04D −0.4143 0.4615 0.7948 0.039*
H04E −0.5113 0.3433 0.8143 0.039*
H04F −0.5052 0.3664 0.7401 0.039*
C23 −0.0457 (15) −0.0644 (11) −0.0774 (5) 0.020 (2) 0.5
C24 0.0810 (4) 0.2656 (3) −0.05056 (17) 0.0174 (8)
C25 0.1519 (4) 0.3536 (3) −0.08578 (17) 0.0196 (8)
H037 0.2597 0.353 −0.1006 0.024*
C26 0.0674 (4) 0.4416 (3) −0.09933 (17) 0.0184 (8)
H019 0.1175 0.5006 −0.1232 0.022*
C27 −0.0899 (4) 0.4437 (3) −0.07806 (17) 0.0170 (7)
C28 −0.1621 (4) 0.3576 (3) −0.04193 (17) 0.0195 (8)
H044 −0.2683 0.3594 −0.0262 0.023*
C29 −0.0769 (4) 0.2694 (3) −0.02936 (17) 0.0172 (8)
H017 −0.1276 0.2102 −0.0057 0.021*
C30 −0.1136 (5) 0.6129 (3) −0.12824 (19) 0.0253 (9)
H05D 0.0028 0.6508 −0.1055 0.038*
H05E −0.1928 0.6659 −0.1347 0.038*
H05F −0.102 0.5823 −0.1702 0.038*
C31 0.2855 (4) 0.1317 (3) −0.10391 (17) 0.0172 (8)
C32 0.1737 (4) 0.1092 (3) −0.16402 (17) 0.0196 (8)
H021 0.0512 0.1087 −0.1671 0.023*
C33 0.2403 (5) 0.0879 (3) −0.21875 (18) 0.0239 (9)
H026 0.1636 0.0744 −0.2593 0.029*
C34 0.4202 (5) 0.0860 (3) −0.21482 (18) 0.0225 (8)
C35 0.5329 (4) 0.1102 (3) −0.15605 (17) 0.0207 (8)
H016 0.6556 0.1114 −0.153 0.025*
C36 0.4641 (4) 0.1327 (3) −0.10139 (17) 0.0182 (8)
H041 0.5418 0.1493 −0.0612 0.022*
C37 0.6495 (6) 0.0500 (4) −0.2687 (2) 0.0389 (11)
H05A 0.727 0.1218 −0.2545 0.058*
H05B 0.6674 0.0277 −0.3116 0.058*
H05C 0.6775 −0.0058 −0.2382 0.058*
C38 0.3798 (4) 0.2067 (3) 0.03055 (17) 0.0178 (8)
C39 0.4737 (5) 0.1321 (3) 0.06249 (17) 0.0224 (8)
H031 0.4463 0.0563 0.0479 0.027*
C40 0.6072 (5) 0.1675 (3) 0.11553 (18) 0.0222 (8)
H054 0.6728 0.1167 0.136 0.027*
C41 0.6431 (4) 0.2766 (3) 0.13794 (17) 0.0187 (8)
C42 0.5510 (4) 0.3518 (3) 0.10570 (18) 0.0194 (8)
H018 0.5768 0.4274 0.1207 0.023*
C43 0.4228 (4) 0.3165 (3) 0.05225 (18) 0.0190 (8)
H032 0.3633 0.3686 0.03 0.023*
C44 0.8474 (5) 0.2447 (4) 0.22982 (19) 0.0304 (10)
H05G 0.7578 0.1861 0.2427 0.046*
H05H 0.922 0.2847 0.2684 0.046*
H05I 0.9207 0.2117 0.2047 0.046*
O1 −0.1082 (16) 0.2772 (11) 0.4481 (7) 0.034 (3) 0.5
O2 0.7890 (3) 0.8233 (2) 0.68280 (13) 0.0293 (7)
O3 0.4817 (3) 0.0430 (2) 0.57075 (13) 0.0283 (6)
O4 −0.2777 (3) 0.3427 (2) 0.78963 (12) 0.0237 (6)
O5 −0.085 (2) −0.1068 (14) −0.1294 (5) 0.037 (3) 0.5
O6 −0.1854 (3) 0.5247 (2) −0.09059 (12) 0.0209 (6)
O7 0.4683 (4) 0.0594 (3) −0.27137 (13) 0.0319 (7)
O8 0.7629 (3) 0.3197 (2) 0.19171 (12) 0.0231 (6)
Cl1 −0.0738 (4) 0.3106 (4) 0.4565 (2) 0.0283 (11) 0.5
Cl2 −0.0659 (5) −0.0881 (4) −0.10676 (18) 0.0247 (9) 0.5

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Rh1 0.01540 (18) 0.0208 (2) 0.0135 (2) 0.00573 (15) 0.00244 (14) 0.00556 (17)
Rh2 0.01738 (18) 0.0173 (2) 0.0175 (2) 0.00511 (15) 0.00556 (15) 0.00546 (17)
P1 0.0156 (4) 0.0228 (6) 0.0141 (4) 0.0068 (4) 0.0039 (3) 0.0060 (4)
P2 0.0165 (4) 0.0174 (5) 0.0181 (5) 0.0053 (4) 0.0043 (3) 0.0059 (4)
C1 0.025 (4) 0.048 (8) 0.023 (4) 0.003 (4) −0.010 (3) 0.010 (5)
C2 0.0161 (15) 0.021 (2) 0.0156 (17) 0.0075 (14) 0.0034 (13) 0.0050 (15)
C3 0.0186 (16) 0.025 (2) 0.0161 (17) 0.0070 (15) 0.0041 (13) −0.0002 (16)
C4 0.0189 (16) 0.024 (2) 0.0234 (19) 0.0066 (15) 0.0090 (14) 0.0037 (17)
C5 0.0221 (17) 0.021 (2) 0.027 (2) 0.0076 (15) 0.0029 (15) 0.0021 (17)
C6 0.0269 (18) 0.028 (2) 0.0158 (18) 0.0110 (16) 0.0020 (14) 0.0017 (16)
C7 0.0192 (16) 0.026 (2) 0.0171 (17) 0.0106 (15) 0.0051 (14) 0.0042 (16)
C8 0.034 (2) 0.033 (3) 0.055 (3) −0.0122 (19) 0.019 (2) −0.010 (2)
C9 0.0193 (16) 0.023 (2) 0.0124 (16) 0.0049 (14) 0.0043 (13) 0.0066 (15)
C10 0.0205 (16) 0.022 (2) 0.0131 (17) 0.0053 (14) 0.0023 (13) 0.0002 (15)
C11 0.0219 (17) 0.026 (2) 0.0200 (18) 0.0074 (15) 0.0047 (14) 0.0005 (17)
C12 0.0310 (19) 0.023 (2) 0.0154 (17) 0.0126 (16) 0.0066 (15) 0.0015 (16)
C13 0.0254 (17) 0.021 (2) 0.0231 (19) 0.0025 (15) 0.0059 (15) 0.0028 (17)
C14 0.0172 (16) 0.028 (2) 0.0224 (19) 0.0049 (15) 0.0058 (14) 0.0052 (17)
C15 0.044 (2) 0.020 (2) 0.043 (3) 0.0120 (19) 0.011 (2) 0.005 (2)
C16 0.0170 (15) 0.022 (2) 0.0160 (17) 0.0080 (14) 0.0059 (13) 0.0054 (15)
C17 0.0199 (16) 0.027 (2) 0.0188 (18) 0.0092 (15) 0.0023 (14) 0.0082 (17)
C18 0.0200 (16) 0.028 (2) 0.0177 (18) 0.0097 (15) 0.0030 (14) 0.0107 (16)
C19 0.0170 (15) 0.027 (2) 0.0153 (17) 0.0050 (15) 0.0060 (13) 0.0036 (16)
C20 0.0174 (15) 0.025 (2) 0.0181 (18) 0.0102 (15) 0.0060 (13) 0.0041 (16)
C21 0.0191 (16) 0.024 (2) 0.0175 (18) 0.0065 (15) 0.0034 (13) 0.0071 (16)
C22 0.0178 (16) 0.038 (3) 0.025 (2) 0.0091 (16) 0.0084 (15) 0.0062 (19)
C23 0.018 (4) 0.021 (6) 0.020 (6) 0.002 (4) 0.008 (5) 0.005 (5)
C24 0.0195 (16) 0.016 (2) 0.0179 (17) 0.0078 (14) 0.0021 (13) 0.0012 (15)
C25 0.0163 (15) 0.023 (2) 0.0228 (19) 0.0068 (14) 0.0086 (13) 0.0047 (16)
C26 0.0185 (15) 0.018 (2) 0.0209 (18) 0.0051 (14) 0.0075 (14) 0.0059 (16)
C27 0.0197 (16) 0.014 (2) 0.0195 (18) 0.0072 (14) 0.0046 (13) 0.0001 (15)
C28 0.0168 (15) 0.024 (2) 0.0215 (18) 0.0076 (14) 0.0088 (14) 0.0045 (16)
C29 0.0173 (15) 0.016 (2) 0.0200 (18) 0.0047 (14) 0.0055 (13) 0.0062 (15)
C30 0.0275 (18) 0.025 (2) 0.028 (2) 0.0104 (16) 0.0100 (16) 0.0112 (18)
C31 0.0203 (16) 0.0129 (19) 0.0197 (18) 0.0057 (14) 0.0037 (14) 0.0060 (15)
C32 0.0174 (15) 0.020 (2) 0.0217 (19) 0.0059 (14) 0.0023 (14) 0.0052 (16)
C33 0.0270 (18) 0.029 (2) 0.0160 (18) 0.0091 (16) −0.0015 (14) 0.0035 (17)
C34 0.0291 (18) 0.022 (2) 0.0185 (18) 0.0061 (16) 0.0088 (15) 0.0024 (16)
C35 0.0207 (16) 0.023 (2) 0.0202 (19) 0.0075 (15) 0.0062 (14) 0.0030 (16)
C36 0.0194 (15) 0.018 (2) 0.0187 (18) 0.0058 (14) 0.0042 (13) 0.0060 (15)
C37 0.037 (2) 0.057 (3) 0.030 (2) 0.018 (2) 0.0184 (19) −0.001 (2)
C38 0.0184 (15) 0.019 (2) 0.0161 (17) 0.0047 (14) 0.0032 (13) 0.0053 (15)
C39 0.0273 (18) 0.022 (2) 0.0194 (19) 0.0087 (16) 0.0037 (15) 0.0006 (16)
C40 0.0239 (17) 0.025 (2) 0.0198 (18) 0.0098 (16) 0.0029 (14) 0.0068 (17)
C41 0.0150 (15) 0.027 (2) 0.0165 (17) 0.0059 (14) 0.0070 (13) 0.0026 (16)
C42 0.0183 (15) 0.017 (2) 0.0246 (19) 0.0038 (14) 0.0081 (14) 0.0014 (16)
C43 0.0130 (14) 0.021 (2) 0.0252 (19) 0.0060 (14) 0.0070 (13) 0.0058 (16)
C44 0.031 (2) 0.038 (3) 0.022 (2) 0.0116 (18) −0.0023 (16) 0.0038 (19)
O1 0.025 (4) 0.048 (8) 0.023 (4) 0.003 (4) −0.010 (3) 0.010 (5)
O2 0.0238 (13) 0.0297 (18) 0.0314 (16) 0.0005 (12) 0.0029 (11) −0.0069 (13)
O3 0.0341 (14) 0.0233 (17) 0.0329 (16) 0.0137 (12) 0.0114 (12) 0.0018 (13)
O4 0.0215 (12) 0.0350 (17) 0.0199 (13) 0.0121 (11) 0.0102 (10) 0.0124 (12)
O5 0.050 (6) 0.043 (7) 0.019 (7) −0.001 (4) 0.012 (5) 0.004 (6)
O6 0.0208 (12) 0.0209 (15) 0.0264 (14) 0.0120 (10) 0.0095 (10) 0.0099 (12)
O7 0.0364 (15) 0.045 (2) 0.0190 (14) 0.0174 (14) 0.0089 (12) 0.0006 (13)
O8 0.0228 (12) 0.0276 (17) 0.0188 (13) 0.0068 (11) 0.0011 (10) 0.0009 (12)
Cl1 0.0235 (17) 0.031 (3) 0.026 (2) 0.0019 (17) −0.0072 (14) 0.002 (2)
Cl2 0.0301 (15) 0.026 (2) 0.017 (3) 0.0001 (14) 0.007 (2) 0.004 (2)

Geometric parameters (Å, °)

Rh1—C1 1.699 (12) C19—C20 1.385 (5)
Rh1—C1i 1.699 (13) C20—C21 1.385 (5)
Rh1—P1i 2.3257 (10) C20—H043 0.95
Rh1—P1 2.3257 (10) C21—H014 0.95
Rh1—Cl1 2.416 (5) C22—O4 1.431 (4)
Rh1—Cl1i 2.416 (5) C22—H04D 0.98
Rh2—C23 1.751 (11) C22—H04E 0.98
Rh2—C23ii 1.751 (11) C22—H04F 0.98
Rh2—P2ii 2.3321 (11) C23—Cl2 0.660 (9)
Rh2—P2 2.3321 (11) C23—O5 1.171 (13)
Rh2—Cl2 2.410 (4) C24—C29 1.392 (5)
Rh2—Cl2ii 2.410 (4) C24—C25 1.402 (5)
P1—C16 1.815 (3) C25—C26 1.386 (5)
P1—C2 1.817 (4) C25—H037 0.95
P1—C9 1.817 (4) C26—C27 1.384 (5)
P2—C24 1.804 (4) C26—H019 0.95
P2—C31 1.824 (4) C27—O6 1.363 (4)
P2—C38 1.827 (4) C27—C28 1.401 (5)
C1—Cl1 0.720 (12) C28—C29 1.388 (5)
C1—O1 1.157 (18) C28—H044 0.95
C2—C7 1.393 (5) C29—H017 0.95
C2—C3 1.397 (5) C30—O6 1.438 (4)
C3—C4 1.383 (5) C30—H05D 0.98
C3—H023 0.95 C30—H05E 0.98
C4—C5 1.387 (5) C30—H05F 0.98
C4—H035 0.95 C31—C36 1.389 (5)
C5—O2 1.365 (5) C31—C32 1.404 (5)
C5—C6 1.396 (5) C32—C33 1.383 (5)
C6—C7 1.382 (5) C32—H021 0.95
C6—H030 0.95 C33—C34 1.403 (5)
C7—H047 0.95 C33—H026 0.95
C8—O2 1.424 (5) C34—O7 1.361 (5)
C8—H04A 0.98 C34—C35 1.386 (5)
C8—H04B 0.98 C35—C36 1.395 (5)
C8—H04C 0.98 C35—H016 0.95
C9—C14 1.397 (5) C36—H041 0.95
C9—C10 1.400 (5) C37—O7 1.438 (5)
C10—C11 1.391 (5) C37—H05A 0.98
C10—H048 0.95 C37—H05B 0.98
C11—C12 1.386 (5) C37—H05C 0.98
C11—H036 0.95 C38—C43 1.379 (5)
C12—O3 1.367 (5) C38—C39 1.399 (5)
C12—C13 1.392 (5) C39—C40 1.396 (5)
C13—C14 1.388 (6) C39—H031 0.95
C13—H022 0.95 C40—C41 1.376 (6)
C14—H046 0.95 C40—H054 0.95
C15—O3 1.433 (5) C41—O8 1.370 (4)
C15—H05J 0.98 C41—C42 1.399 (5)
C15—H05K 0.98 C42—C43 1.378 (5)
C15—H05L 0.98 C42—H018 0.95
C16—C17 1.393 (5) C43—H032 0.95
C16—C21 1.394 (5) C44—O8 1.422 (4)
C17—C18 1.385 (5) C44—H05G 0.98
C17—H034 0.95 C44—H05H 0.98
C18—C19 1.399 (5) C44—H05I 0.98
C18—H033 0.95 O5—Cl2 0.511 (10)
C19—O4 1.363 (4)
C1—Rh1—C1i 180.000 (4) C17—C18—H033 120
C1—Rh1—P1i 89.5 (4) C19—C18—H033 120
C1i—Rh1—P1i 90.5 (4) O4—C19—C20 125.3 (3)
C1—Rh1—P1 90.5 (4) O4—C19—C18 115.1 (3)
C1i—Rh1—P1 89.5 (4) C20—C19—C18 119.6 (3)
P1i—Rh1—P1 180 C19—C20—C21 119.7 (3)
C1—Rh1—Cl1 1.9 (4) C19—C20—H043 120.1
C1i—Rh1—Cl1 178.1 (4) C21—C20—H043 120.1
P1i—Rh1—Cl1 88.80 (9) C20—C21—C16 121.3 (3)
P1—Rh1—Cl1 91.20 (9) C20—C21—H014 119.3
C1—Rh1—Cl1i 178.1 (4) C16—C21—H014 119.3
C1i—Rh1—Cl1i 1.9 (4) O4—C22—H04D 109.5
P1i—Rh1—Cl1i 91.20 (9) O4—C22—H04E 109.5
P1—Rh1—Cl1i 88.80 (9) H04D—C22—H04E 109.5
Cl1—Rh1—Cl1i 180.0000 (10) O4—C22—H04F 109.5
C23—Rh2—C23ii 180.0 (9) H04D—C22—H04F 109.5
C23—Rh2—P2ii 88.1 (4) H04E—C22—H04F 109.5
C23ii—Rh2—P2ii 91.9 (4) Cl2—C23—Rh2 177.8 (15)
C23—Rh2—P2 91.9 (4) O5—C23—Rh2 176.8 (16)
C23ii—Rh2—P2 88.1 (4) C29—C24—C25 117.9 (3)
P2ii—Rh2—P2 180.00 (5) C29—C24—P2 120.5 (3)
C23—Rh2—Cl2 0.6 (4) C25—C24—P2 121.6 (3)
C23ii—Rh2—Cl2 179.4 (4) C26—C25—C24 121.2 (3)
P2ii—Rh2—Cl2 87.94 (10) C26—C25—H037 119.4
P2—Rh2—Cl2 92.06 (10) C24—C25—H037 119.4
C23—Rh2—Cl2ii 179.4 (4) C27—C26—C25 120.1 (3)
C23ii—Rh2—Cl2ii 0.6 (4) C27—C26—H019 120
P2ii—Rh2—Cl2ii 92.06 (10) C25—C26—H019 120
P2—Rh2—Cl2ii 87.94 (10) O6—C27—C26 124.4 (3)
Cl2—Rh2—Cl2ii 180.0 (2) O6—C27—C28 115.7 (3)
C16—P1—C2 106.79 (17) C26—C27—C28 119.8 (3)
C16—P1—C9 103.67 (16) C29—C28—C27 119.4 (3)
C2—P1—C9 104.54 (16) C29—C28—H044 120.3
C16—P1—Rh1 109.09 (11) C27—C28—H044 120.3
C2—P1—Rh1 112.92 (11) C28—C29—C24 121.6 (3)
C9—P1—Rh1 118.87 (12) C28—C29—H017 119.2
C24—P2—C31 103.44 (16) C24—C29—H017 119.2
C24—P2—C38 104.95 (17) O6—C30—H05D 109.5
C31—P2—C38 104.75 (16) O6—C30—H05E 109.5
C24—P2—Rh2 111.46 (12) H05D—C30—H05E 109.5
C31—P2—Rh2 118.04 (12) O6—C30—H05F 109.5
C38—P2—Rh2 112.97 (11) H05D—C30—H05F 109.5
Cl1—C1—Rh1 173.6 (14) H05E—C30—H05F 109.5
O1—C1—Rh1 173.2 (14) C36—C31—C32 118.0 (3)
C7—C2—C3 118.0 (3) C36—C31—P2 122.7 (3)
C7—C2—P1 123.5 (3) C32—C31—P2 119.2 (3)
C3—C2—P1 118.3 (3) C33—C32—C31 120.6 (3)
C4—C3—C2 121.8 (3) C33—C32—H021 119.7
C4—C3—H023 119.1 C31—C32—H021 119.7
C2—C3—H023 119.1 C32—C33—C34 120.5 (3)
C3—C4—C5 119.4 (3) C32—C33—H026 119.8
C3—C4—H035 120.3 C34—C33—H026 119.8
C5—C4—H035 120.3 O7—C34—C35 125.4 (3)
O2—C5—C4 124.7 (3) O7—C34—C33 115.0 (3)
O2—C5—C6 115.7 (4) C35—C34—C33 119.6 (3)
C4—C5—C6 119.6 (4) C34—C35—C36 119.2 (3)
C7—C6—C5 120.4 (4) C34—C35—H016 120.4
C7—C6—H030 119.8 C36—C35—H016 120.4
C5—C6—H030 119.8 C31—C36—C35 122.0 (3)
C6—C7—C2 120.7 (3) C31—C36—H041 119
C6—C7—H047 119.6 C35—C36—H041 119
C2—C7—H047 119.6 O7—C37—H05A 109.5
O2—C8—H04A 109.5 O7—C37—H05B 109.5
O2—C8—H04B 109.5 H05A—C37—H05B 109.5
H04A—C8—H04B 109.5 O7—C37—H05C 109.5
O2—C8—H04C 109.5 H05A—C37—H05C 109.5
H04A—C8—H04C 109.5 H05B—C37—H05C 109.5
H04B—C8—H04C 109.5 C43—C38—C39 118.6 (3)
C14—C9—C10 117.3 (3) C43—C38—P2 123.0 (3)
C14—C9—P1 120.2 (3) C39—C38—P2 118.1 (3)
C10—C9—P1 122.5 (3) C40—C39—C38 120.9 (4)
C11—C10—C9 121.3 (4) C40—C39—H031 119.5
C11—C10—H048 119.4 C38—C39—H031 119.5
C9—C10—H048 119.4 C41—C40—C39 119.5 (3)
C12—C11—C10 120.2 (3) C41—C40—H054 120.2
C12—C11—H036 119.9 C39—C40—H054 120.2
C10—C11—H036 119.9 O8—C41—C40 124.9 (3)
O3—C12—C11 116.0 (3) O8—C41—C42 115.3 (4)
O3—C12—C13 124.4 (4) C40—C41—C42 119.7 (3)
C11—C12—C13 119.5 (4) C43—C42—C41 120.2 (4)
C14—C13—C12 119.8 (4) C43—C42—H018 119.9
C14—C13—H022 120.1 C41—C42—H018 119.9
C12—C13—H022 120.1 C42—C43—C38 121.0 (3)
C13—C14—C9 121.9 (3) C42—C43—H032 119.5
C13—C14—H046 119.1 C38—C43—H032 119.5
C9—C14—H046 119.1 O8—C44—H05G 109.5
O3—C15—H05J 109.5 O8—C44—H05H 109.5
O3—C15—H05K 109.5 H05G—C44—H05H 109.5
H05J—C15—H05K 109.5 O8—C44—H05I 109.5
O3—C15—H05L 109.5 H05G—C44—H05I 109.5
H05J—C15—H05L 109.5 H05H—C44—H05I 109.5
H05K—C15—H05L 109.5 C5—O2—C8 117.3 (3)
C17—C16—C21 118.3 (3) C12—O3—C15 117.2 (3)
C17—C16—P1 123.1 (3) C19—O4—C22 117.1 (3)
C21—C16—P1 118.5 (2) C27—O6—C30 116.2 (3)
C18—C17—C16 120.8 (3) C34—O7—C37 116.8 (3)
C18—C17—H034 119.6 C41—O8—C44 117.6 (3)
C16—C17—H034 119.6 O5—Cl2—C23 177 (2)
C17—C18—C19 120.0 (3) O5—Cl2—Rh2 176 (2)
C1—Rh1—P1—C16 −93.0 (4) C18—C19—C20—C21 3.7 (6)
C1i—Rh1—P1—C16 87.0 (4) C19—C20—C21—C16 −0.6 (6)
Cl1—Rh1—P1—C16 −94.75 (17) C17—C16—C21—C20 −2.3 (6)
Cl1i—Rh1—P1—C16 85.25 (17) P1—C16—C21—C20 175.0 (3)
C1—Rh1—P1—C2 148.5 (4) C31—P2—C24—C29 144.7 (3)
C1i—Rh1—P1—C2 −31.5 (4) C38—P2—C24—C29 −105.8 (3)
Cl1—Rh1—P1—C2 146.68 (16) Rh2—P2—C24—C29 16.9 (3)
Cl1i—Rh1—P1—C2 −33.32 (16) C31—P2—C24—C25 −35.9 (3)
C1—Rh1—P1—C9 25.5 (4) C38—P2—C24—C25 73.6 (3)
C1i—Rh1—P1—C9 −154.5 (4) Rh2—P2—C24—C25 −163.7 (3)
Cl1—Rh1—P1—C9 23.70 (16) C29—C24—C25—C26 −0.2 (5)
Cl1i—Rh1—P1—C9 −156.30 (16) P2—C24—C25—C26 −179.6 (3)
C23—Rh2—P2—C24 97.8 (4) C24—C25—C26—C27 −0.1 (6)
C23ii—Rh2—P2—C24 −82.2 (4) C25—C26—C27—O6 −177.9 (3)
Cl2—Rh2—P2—C24 97.21 (17) C25—C26—C27—C28 1.0 (6)
Cl2ii—Rh2—P2—C24 −82.79 (17) O6—C27—C28—C29 177.3 (3)
C23—Rh2—P2—C31 −21.7 (4) C26—C27—C28—C29 −1.7 (6)
C23ii—Rh2—P2—C31 158.3 (4) C27—C28—C29—C24 1.5 (6)
Cl2—Rh2—P2—C31 −22.28 (16) C25—C24—C29—C28 −0.5 (5)
Cl2ii—Rh2—P2—C31 157.72 (16) P2—C24—C29—C28 178.9 (3)
C23—Rh2—P2—C38 −144.3 (4) C24—P2—C31—C36 124.8 (3)
C23ii—Rh2—P2—C38 35.7 (4) C38—P2—C31—C36 15.1 (3)
Cl2—Rh2—P2—C38 −144.90 (17) Rh2—P2—C31—C36 −111.6 (3)
Cl2ii—Rh2—P2—C38 35.10 (17) C24—P2—C31—C32 −58.5 (3)
C16—P1—C2—C7 4.8 (3) C38—P2—C31—C32 −168.2 (3)
C9—P1—C2—C7 −104.6 (3) Rh2—P2—C31—C32 65.1 (3)
Rh1—P1—C2—C7 124.7 (3) C36—C31—C32—C33 0.5 (5)
C16—P1—C2—C3 −171.4 (3) P2—C31—C32—C33 −176.2 (3)
C9—P1—C2—C3 79.1 (3) C31—C32—C33—C34 1.4 (6)
Rh1—P1—C2—C3 −51.5 (3) C32—C33—C34—O7 177.3 (3)
C7—C2—C3—C4 1.4 (5) C32—C33—C34—C35 −2.6 (6)
P1—C2—C3—C4 177.8 (3) O7—C34—C35—C36 −178.0 (3)
C2—C3—C4—C5 −2.1 (6) C33—C34—C35—C36 1.9 (6)
C3—C4—C5—O2 −177.6 (3) C32—C31—C36—C35 −1.2 (5)
C3—C4—C5—C6 1.4 (6) P2—C31—C36—C35 175.4 (3)
O2—C5—C6—C7 179.2 (3) C34—C35—C36—C31 0.0 (6)
C4—C5—C6—C7 0.1 (6) C24—P2—C38—C43 −3.7 (3)
C5—C6—C7—C2 −0.9 (5) C31—P2—C38—C43 104.9 (3)
C3—C2—C7—C6 0.1 (5) Rh2—P2—C38—C43 −125.3 (3)
P1—C2—C7—C6 −176.1 (3) C24—P2—C38—C39 169.4 (3)
C16—P1—C9—C14 54.2 (3) C31—P2—C38—C39 −82.0 (3)
C2—P1—C9—C14 165.9 (3) Rh2—P2—C38—C39 47.8 (3)
Rh1—P1—C9—C14 −67.0 (3) C43—C38—C39—C40 0.5 (5)
C16—P1—C9—C10 −127.8 (3) P2—C38—C39—C40 −172.9 (3)
C2—P1—C9—C10 −16.0 (3) C38—C39—C40—C41 2.1 (5)
Rh1—P1—C9—C10 111.0 (3) C39—C40—C41—O8 175.8 (3)
C14—C9—C10—C11 −1.5 (5) C39—C40—C41—C42 −2.8 (5)
P1—C9—C10—C11 −179.6 (3) O8—C41—C42—C43 −177.8 (3)
C9—C10—C11—C12 0.0 (5) C40—C41—C42—C43 1.0 (5)
C10—C11—C12—O3 −179.6 (3) C41—C42—C43—C38 1.7 (5)
C10—C11—C12—C13 1.5 (5) C39—C38—C43—C42 −2.4 (5)
O3—C12—C13—C14 179.8 (3) P2—C38—C43—C42 170.6 (3)
C11—C12—C13—C14 −1.3 (5) C4—C5—O2—C8 5.7 (6)
C12—C13—C14—C9 −0.3 (6) C6—C5—O2—C8 −173.3 (4)
C10—C9—C14—C13 1.7 (5) C11—C12—O3—C15 178.2 (3)
P1—C9—C14—C13 179.8 (3) C13—C12—O3—C15 −2.9 (5)
C2—P1—C16—C17 −88.3 (4) C20—C19—O4—C22 7.5 (6)
C9—P1—C16—C17 21.8 (4) C18—C19—O4—C22 −171.7 (3)
Rh1—P1—C16—C17 149.4 (3) C26—C27—O6—C30 −0.4 (5)
C2—P1—C16—C21 94.6 (3) C28—C27—O6—C30 −179.3 (3)
C9—P1—C16—C21 −155.4 (3) C35—C34—O7—C37 3.5 (6)
Rh1—P1—C16—C21 −27.8 (3) C33—C34—O7—C37 −176.4 (3)
C21—C16—C17—C18 2.1 (6) C40—C41—O8—C44 −4.7 (5)
P1—C16—C17—C18 −175.1 (3) C42—C41—O8—C44 173.9 (3)
C16—C17—C18—C19 1.0 (6) O1—C1—Cl1—Rh1 132 (13)
C17—C18—C19—O4 175.4 (4) P1i—Rh1—Cl1—C1 −110 (11)
C17—C18—C19—C20 −3.9 (6) P1—Rh1—Cl1—C1 70 (11)
O4—C19—C20—C21 −175.5 (4)

Symmetry codes: (i) −x, −y+1, −z+1; (ii) −x, −y, −z.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C14—H046···Cl1 0.95 2.81 3.191 (5) 105.
C32—H021···Cl2 0.95 2.82 3.157 (5) 102.
C8—H04A···Cl1iii 0.98 2.73 3.693 (7) 169.
C8—H04A···O1iii 0.98 2.52 3.486 (18) 168.

Symmetry codes: (iii) −x+1, −y+1, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: WM2548).

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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/S1600536811046150/wm2548sup1.cif

e-67-m1695-sup1.cif (46.6KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811046150/wm2548Isup2.hkl

e-67-m1695-Isup2.hkl (447KB, hkl)

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


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