metal-organic compounds
μ-n-butyrato-κ2O:O′)bis[chloridorhenium(III)](Re—Re)
of tetrakis(aDepartment of Chemistry, St. Francis Xavier University, PO Box 5000, Antigonish, Nova Scotia, B2G 2W5, Canada, and bDepartment of Chemistry, Queen's University, Kingston, Ontario, K7L 3N6, Canada
*Correspondence e-mail: maquino@stfx.ca
With an inversion center at the mid-point of the two ReIII atoms, the title compound, [Re2Cl2{O2C(CH2)2CH3}4], exhibits a paddle-wheel or lantern-type structure with four n-butyrate groups bridging two ReIII atoms in a syn–syn fashion. The axial chloride ligands together with the Re—Re quadruple bond [2.2330 (3) Å] complete an essentially octahedral geometry around each ReIII atom. There is little distortion, with an Re—Re—Cl bond angle of 176.18 (3)° and typical cis-O—Re—O bond angles ranging from 89.39 (11) to 90.68 (11)°. There are two molecules in the and no significant intermolecular interactions were noticed between molecules in the crystal.
Keywords: crystal structure; dirhenium core; butyrate bridging ligand.
CCDC reference: 1023523
1. Related literature
For the synthesis and structure of five related structures, see: Taha & Wilkinson (1963); Calvo et al. (1969); Collins et al. (1979); Lydon et al. (2003).
2. Experimental
2.1. Crystal data
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2.3. Refinement
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Data collection: APEX2 (Bruker, 2010); cell SAINT (Bruker, 2010); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.
Supporting information
CCDC reference: 1023523
10.1107/S1600536814020273/wm5055sup1.cif
contains datablocks I, New_Global_Publ_Block. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536814020273/wm5055Isup2.hkl
This compund was prepared following a method analogous to the procedure used by Taha & Wilkinson (1963). Rhenium trichloride (1.25 g, 4.27 mmol) was reacted with 13 ml of butyric acid and 0.5 ml of butyric anhydride at 423 K, with stirring, under a steady stream of nitrogen for five days. The dark solution was removed from heat and allowed to cool overnight. The brown product was collected via suction filtration and washed with a 50 ml portion of petroleum ether. The product was dried in vacuo for 24 hours and then re-crystallized from dichloromethane. Yield = 0.481g, (56.9 %).
Data collection: APEX2 (Bruker, 2010); cell
SAINT (Bruker, 2010); data reduction: SAINT (Bruker, 2010); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).[Re2(C4H7O2)4Cl2] | F(000) = 744 |
Mr = 791.68 | Dx = 2.241 Mg m−3 |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2yn | Cell parameters from 3188 reflections |
a = 6.7292 (4) Å | θ = 3.7–27.1° |
b = 12.0367 (8) Å | µ = 10.57 mm−1 |
c = 14.6737 (9) Å | T = 180 K |
β = 99.262 (1)° | Needle, orange |
V = 1173.0 (1) Å3 | 0.30 × 0.06 × 0.06 mm |
Z = 2 |
Bruker APEXII CCD diffractometer | 2277 independent reflections |
Radiation source: fine-focus sealed tube | 2077 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.016 |
ϕ and ω scans | θmax = 26.0°, θmin = 3.7° |
Absorption correction: multi-scan (SADABS; Bruker, 2010) | h = −8→7 |
Tmin = 0.144, Tmax = 0.570 | k = −12→14 |
4625 measured reflections | l = −18→18 |
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)] = 0.019 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.049 | H-atom parameters constrained |
S = 1.06 | w = 1/[σ2(Fo2) + (0.0278P)2 + 0.2053P] where P = (Fo2 + 2Fc2)/3 |
2277 reflections | (Δ/σ)max = 0.005 |
129 parameters | Δρmax = 0.90 e Å−3 |
0 restraints | Δρmin = −1.32 e Å−3 |
[Re2(C4H7O2)4Cl2] | V = 1173.0 (1) Å3 |
Mr = 791.68 | Z = 2 |
Monoclinic, P21/n | Mo Kα radiation |
a = 6.7292 (4) Å | µ = 10.57 mm−1 |
b = 12.0367 (8) Å | T = 180 K |
c = 14.6737 (9) Å | 0.30 × 0.06 × 0.06 mm |
β = 99.262 (1)° |
Bruker APEXII CCD diffractometer | 2277 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2010) | 2077 reflections with I > 2σ(I) |
Tmin = 0.144, Tmax = 0.570 | Rint = 0.016 |
4625 measured reflections |
R[F2 > 2σ(F2)] = 0.019 | 0 restraints |
wR(F2) = 0.049 | H-atom parameters constrained |
S = 1.06 | Δρmax = 0.90 e Å−3 |
2277 reflections | Δρmin = −1.32 e Å−3 |
129 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
Re1 | 0.91824 (2) | 0.559012 (11) | 1.039538 (10) | 0.02050 (7) | |
Cl1 | 0.71261 (17) | 0.68750 (8) | 1.12219 (8) | 0.0397 (3) | |
O1 | 0.7020 (4) | 0.57529 (19) | 0.92707 (18) | 0.0254 (6) | |
O2 | 0.8665 (4) | 0.45750 (19) | 0.84940 (19) | 0.0256 (6) | |
O3 | 0.7697 (4) | 0.42938 (19) | 1.08438 (19) | 0.0243 (6) | |
O4 | 0.9312 (4) | 0.31123 (19) | 1.00486 (18) | 0.0241 (6) | |
C1 | 0.7167 (6) | 0.5223 (3) | 0.8532 (3) | 0.0253 (8) | |
C2 | 0.5652 (6) | 0.5386 (3) | 0.7691 (3) | 0.0308 (9) | |
H2A | 0.4565 | 0.5877 | 0.7838 | 0.037* | |
H2B | 0.5045 | 0.4661 | 0.7486 | 0.037* | |
C3 | 0.6593 (7) | 0.5899 (4) | 0.6916 (3) | 0.0451 (12) | |
H3A | 0.7561 | 0.5366 | 0.6719 | 0.054* | |
H3B | 0.5526 | 0.6040 | 0.6380 | 0.054* | |
C4 | 0.7670 (9) | 0.6974 (5) | 0.7202 (5) | 0.083 (2) | |
H4A | 0.8092 | 0.7325 | 0.6662 | 0.125* | |
H4B | 0.8857 | 0.6821 | 0.7666 | 0.125* | |
H4C | 0.6761 | 0.7474 | 0.7464 | 0.125* | |
C5 | 0.8023 (6) | 0.3306 (3) | 1.0595 (3) | 0.0247 (8) | |
C6 | 0.6899 (6) | 0.2376 (3) | 1.0943 (3) | 0.0338 (10) | |
H6A | 0.5453 | 0.2464 | 1.0688 | 0.041* | |
H6B | 0.7037 | 0.2445 | 1.1623 | 0.041* | |
C7 | 0.7539 (7) | 0.1221 (3) | 1.0718 (3) | 0.0333 (9) | |
H7A | 0.8978 | 0.1111 | 1.0975 | 0.040* | |
H7B | 0.7373 | 0.1126 | 1.0040 | 0.040* | |
C8 | 0.6260 (8) | 0.0359 (3) | 1.1127 (3) | 0.0426 (11) | |
H8A | 0.6674 | −0.0389 | 1.0974 | 0.064* | |
H8B | 0.4836 | 0.0470 | 1.0871 | 0.064* | |
H8C | 0.6449 | 0.0445 | 1.1800 | 0.064* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Re1 | 0.02322 (11) | 0.02022 (10) | 0.02042 (10) | 0.00156 (6) | 0.01068 (7) | 0.00100 (5) |
Cl1 | 0.0449 (6) | 0.0377 (5) | 0.0419 (6) | 0.0105 (5) | 0.0232 (5) | −0.0039 (5) |
O1 | 0.0283 (15) | 0.0278 (13) | 0.0217 (14) | 0.0015 (11) | 0.0092 (12) | 0.0030 (10) |
O2 | 0.0294 (16) | 0.0275 (13) | 0.0222 (14) | 0.0013 (11) | 0.0108 (12) | −0.0003 (10) |
O3 | 0.0256 (15) | 0.0252 (13) | 0.0243 (14) | −0.0007 (10) | 0.0105 (12) | 0.0029 (10) |
O4 | 0.0267 (14) | 0.0235 (13) | 0.0238 (13) | −0.0025 (11) | 0.0086 (11) | −0.0006 (11) |
C1 | 0.027 (2) | 0.0276 (18) | 0.024 (2) | −0.0031 (16) | 0.0112 (17) | 0.0024 (15) |
C2 | 0.029 (2) | 0.041 (2) | 0.024 (2) | 0.0023 (18) | 0.0081 (17) | 0.0013 (17) |
C3 | 0.034 (3) | 0.071 (3) | 0.033 (2) | 0.015 (2) | 0.012 (2) | 0.021 (2) |
C4 | 0.063 (4) | 0.095 (5) | 0.084 (5) | −0.027 (4) | −0.010 (3) | 0.060 (4) |
C5 | 0.0217 (19) | 0.0284 (19) | 0.0246 (19) | −0.0020 (16) | 0.0058 (15) | 0.0014 (15) |
C6 | 0.035 (2) | 0.031 (2) | 0.039 (2) | −0.0015 (18) | 0.0177 (19) | 0.0082 (17) |
C7 | 0.038 (2) | 0.025 (2) | 0.038 (2) | −0.0064 (17) | 0.011 (2) | 0.0019 (17) |
C8 | 0.048 (3) | 0.031 (2) | 0.049 (3) | −0.012 (2) | 0.012 (2) | 0.0063 (19) |
Re1—O2i | 2.008 (3) | C3—C4 | 1.509 (7) |
Re1—O3 | 2.019 (2) | C3—H3A | 0.9900 |
Re1—O4i | 2.025 (2) | C3—H3B | 0.9900 |
Re1—O1 | 2.026 (3) | C4—H4A | 0.9800 |
Re1—Re1i | 2.2330 (3) | C4—H4B | 0.9800 |
Re1—Cl1 | 2.5135 (9) | C4—H4C | 0.9800 |
O1—C1 | 1.275 (5) | C5—C6 | 1.487 (5) |
O2—C1 | 1.283 (4) | C6—C7 | 1.508 (5) |
O2—Re1i | 2.008 (3) | C6—H6A | 0.9900 |
O3—C5 | 1.273 (4) | C6—H6B | 0.9900 |
O4—C5 | 1.294 (4) | C7—C8 | 1.531 (5) |
O4—Re1i | 2.025 (2) | C7—H7A | 0.9900 |
C1—C2 | 1.482 (6) | C7—H7B | 0.9900 |
C2—C3 | 1.520 (6) | C8—H8A | 0.9800 |
C2—H2A | 0.9900 | C8—H8B | 0.9800 |
C2—H2B | 0.9900 | C8—H8C | 0.9800 |
O2i—Re1—O3 | 89.39 (11) | C4—C3—H3B | 109.2 |
O2i—Re1—O4i | 90.26 (10) | C2—C3—H3B | 109.2 |
O3—Re1—O4i | 179.64 (11) | H3A—C3—H3B | 107.9 |
O2i—Re1—O1 | 179.70 (10) | C3—C4—H4A | 109.5 |
O3—Re1—O1 | 90.68 (11) | C3—C4—H4B | 109.5 |
O4i—Re1—O1 | 89.67 (10) | H4A—C4—H4B | 109.5 |
O2i—Re1—Re1i | 90.42 (7) | C3—C4—H4C | 109.5 |
O3—Re1—Re1i | 89.36 (7) | H4A—C4—H4C | 109.5 |
O4i—Re1—Re1i | 90.55 (7) | H4B—C4—H4C | 109.5 |
O1—Re1—Re1i | 89.29 (7) | O3—C5—O4 | 120.7 (3) |
O2i—Re1—Cl1 | 92.90 (8) | O3—C5—C6 | 118.9 (3) |
O3—Re1—Cl1 | 88.76 (8) | O4—C5—C6 | 120.4 (3) |
O4i—Re1—Cl1 | 91.34 (7) | C5—C6—C7 | 116.1 (3) |
O1—Re1—Cl1 | 87.40 (8) | C5—C6—H6A | 108.3 |
Re1i—Re1—Cl1 | 176.18 (3) | C7—C6—H6A | 108.3 |
C1—O1—Re1 | 120.0 (2) | C5—C6—H6B | 108.3 |
C1—O2—Re1i | 119.6 (2) | C7—C6—H6B | 108.3 |
C5—O3—Re1 | 120.7 (2) | H6A—C6—H6B | 107.4 |
C5—O4—Re1i | 118.7 (2) | C6—C7—C8 | 109.9 (4) |
O1—C1—O2 | 120.7 (4) | C6—C7—H7A | 109.7 |
O1—C1—C2 | 120.3 (3) | C8—C7—H7A | 109.7 |
O2—C1—C2 | 119.0 (3) | C6—C7—H7B | 109.7 |
C1—C2—C3 | 111.3 (4) | C8—C7—H7B | 109.7 |
C1—C2—H2A | 109.4 | H7A—C7—H7B | 108.2 |
C3—C2—H2A | 109.4 | C7—C8—H8A | 109.5 |
C1—C2—H2B | 109.4 | C7—C8—H8B | 109.5 |
C3—C2—H2B | 109.4 | H8A—C8—H8B | 109.5 |
H2A—C2—H2B | 108.0 | C7—C8—H8C | 109.5 |
C4—C3—C2 | 112.3 (4) | H8A—C8—H8C | 109.5 |
C4—C3—H3A | 109.2 | H8B—C8—H8C | 109.5 |
C2—C3—H3A | 109.2 | ||
O2i—Re1—O1—C1 | 13 (19) | Re1i—O2—C1—O1 | −0.9 (5) |
O3—Re1—O1—C1 | −89.7 (3) | Re1i—O2—C1—C2 | 176.6 (2) |
O4i—Re1—O1—C1 | 90.2 (3) | O1—C1—C2—C3 | 115.7 (4) |
Re1i—Re1—O1—C1 | −0.3 (3) | O2—C1—C2—C3 | −61.7 (5) |
Cl1—Re1—O1—C1 | −178.4 (3) | C1—C2—C3—C4 | −55.2 (5) |
O2i—Re1—O3—C5 | −90.7 (3) | Re1—O3—C5—O4 | −0.1 (5) |
O4i—Re1—O3—C5 | −77 (17) | Re1—O3—C5—C6 | 179.9 (3) |
O1—Re1—O3—C5 | 89.0 (3) | Re1i—O4—C5—O3 | 0.5 (5) |
Re1i—Re1—O3—C5 | −0.3 (3) | Re1i—O4—C5—C6 | −179.5 (3) |
Cl1—Re1—O3—C5 | 176.4 (3) | O3—C5—C6—C7 | −172.7 (4) |
Re1—O1—C1—O2 | 0.8 (5) | O4—C5—C6—C7 | 7.2 (6) |
Re1—O1—C1—C2 | −176.6 (2) | C5—C6—C7—C8 | 179.5 (4) |
Symmetry code: (i) −x+2, −y+1, −z+2. |
Re1—O2i | 2.008 (3) | Re1—O1 | 2.026 (3) |
Re1—O3 | 2.019 (2) | Re1—Cl1 | 2.5135 (9) |
Re1—O4i | 2.025 (2) |
Symmetry code: (i) −x+2, −y+1, −z+2. |
Acknowledgements
The authors thank NSERC (Canada) for financial support.
References
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