Skip to main content
Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Jun 25;67(Pt 7):m984. doi: 10.1107/S1600536811023452

Bis(bicyclo­[2.2.1]hept-5-ene-2-carboxyl­ato)-1κ2 O,O′;4κ2 O,O′-di-μ2-chlorido-1:2κ2 Cl;3:4κ2 Cl-octa­methyl-1κ2 C,2κ2 C,3κ2 C,4κ2 C-di-μ3-oxido-1:2:3κ3 O;2:3:4κ3 O-tetra­tin(IV)

Yupo Ren a,*
PMCID: PMC3152064  PMID: 21836958

Abstract

In the title compound, [Sn4(CH3)8(C8H9O2)2Cl2O2], the tetra­nuclear complex mol­ecule has crystallographically imposed inversion symmetry. The coordination polyhedron about the two central Sn atoms is distorted trigonal–bipyramidal, whilst the two peripheral metal atoms bonded to the carboxyl­ate groups have a distorted octa­hedral coordination geometry. In the crystal, mol­ecules are connected by long Sn⋯O contacts [3.139 (11) Å], forming chains along [011].

Related literature

For the biological activity of organotin compounds, see: Dubey & Roy (2003). For a related structure, see: Li et al. (2006). graphic file with name e-67-0m984-scheme1.jpg

Experimental

Crystal data

  • [Sn4(CH3)8(C8H9O2)2Cl2O2]

  • M r = 972.24

  • Triclinic, Inline graphic

  • a = 9.3685 (12) Å

  • b = 9.8651 (13) Å

  • c = 9.9103 (15) Å

  • α = 109.779 (2)°

  • β = 96.340 (1)°

  • γ = 97.204 (1)°

  • V = 843.5 (2) Å3

  • Z = 1

  • Mo Kα radiation

  • μ = 3.12 mm−1

  • T = 298 K

  • 0.13 × 0.11 × 0.05 mm

Data collection

  • Siemens SMART CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996) T min = 0.687, T max = 0.860

  • 4366 measured reflections

  • 2915 independent reflections

  • 1818 reflections with I > 2σ(I)

  • R int = 0.024

Refinement

  • R[F 2 > 2σ(F 2)] = 0.047

  • wR(F 2) = 0.130

  • S = 1.02

  • 2915 reflections

  • 163 parameters

  • H-atom parameters constrained

  • Δρmax = 0.86 e Å−3

  • Δρmin = −0.64 e Å−3

Data collection: SMART (Siemens, 1996); cell refinement: SAINT (Siemens, 1996); 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.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811023452/rz2611sup1.cif

e-67-0m984-sup1.cif (17.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811023452/rz2611Isup2.hkl

e-67-0m984-Isup2.hkl (143KB, hkl)

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

Acknowledgments

The author thanks the National Natural Science Foundation of China (20971096) for financial support.

supplementary crystallographic information

Comment

In recent years, organotin compounds have attracted more and more attention due to their wide range of industrial applications and biological activities (Dubey & Roy, 2003). As a part of our ongoing investigations in this field, we have synthesized the title compound and present its crystal structure here.

The tetranuclear complex molecule of the title compound (Fig. 1) has crystallographically imposed inversion symmetry. The tin atoms have two different coordination modes, one atom (Sn2) is coordinated in a distorted trigonal-bipyramidal geometry by one µ3oxo oxygen atom and two methyl groups forming the equatorial plane, and by an µ3oxo oxygen atom and the chloride anion at the apices; the other tin metal (Sn1) has a distorted octahedral coordination geometry, with three O atoms and one Cl atom in equatorial positions and the axial position occupied by two methyl groups. The Sn—O bond distances involving the carboxylate group (Sn1—O2 = 2.115 (8) Å; Sn1—O3 = 2.699 (9) Å) are comparable to those found in a related organotin carboxylate (Li et al., 2006). The shortest Sn···Sn separation within the Sn4 core is 3.2898 (10) Å. In the crystal structure, complex molecules are connected by long Sn···O interaction (Sn1···O3i = 3.139 (11) Å; symmetry code: (i) 1-x, -y, 1-z) into one-dimensional chains parallel to the [011] direction (Fig. 2).

Experimental

The reaction was carried out under a nitrogen atmosphere. Bicyclo[2.2.1]heptane-2-carboxylic acid (1 mmol) and sodium ethoxide (1 mmol) were added to a stirred solution of benzene (30 ml) in a Schlenk flask After stirring the solution for 30 min, dimethyltin dichloride (2 mmol) was added and the reaction mixture was stirred for 12 h at room temperature. The resulting clear solution was evaporated under vacuum. The product was crystallized from a solution of diethyl ether to yield colourless crystals of the title compound suitable for X-ray analysis (yield: 76%). Anal. Calcd (%) for C24H42Cl2O6Sn4 (Mr = 972.33): C, 29.65; H, 4.35. Found (%): C, 29.47; H, 4.52.

Refinement

The H atoms were positioned geometrically, with C—H = 0.93–0.98 Å, and refined as riding on their parent atoms, with Uiso(H) = 1.2 Ueq(C) or 1.5 Ueq(C) for the methyl groups.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound, showing 50% probability displacement ellipsoids. H atoms have been omitted for clarity. Symmetry code: (A) 1-x, 1-y, 2-z.

Fig. 2.

Fig. 2.

View of the one-dimensional chain structure in the title compound.

Crystal data

[Sn4(CH3)8(C8H9O2)2Cl2O2] Z = 1
Mr = 972.24 F(000) = 468
Triclinic, P1 Dx = 1.914 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 9.3685 (12) Å Cell parameters from 1509 reflections
b = 9.8651 (13) Å θ = 2.2–25.2°
c = 9.9103 (15) Å µ = 3.12 mm1
α = 109.779 (2)° T = 298 K
β = 96.340 (1)° Block, colourless
γ = 97.204 (1)° 0.13 × 0.11 × 0.05 mm
V = 843.5 (2) Å3

Data collection

Siemens SMART CCD area-detector diffractometer 2915 independent reflections
Radiation source: fine-focus sealed tube 1818 reflections with I > 2σ(I)
graphite Rint = 0.024
φ and ω scans θmax = 25.0°, θmin = 2.2°
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) h = −6→11
Tmin = 0.687, Tmax = 0.860 k = −11→10
4366 measured reflections l = −11→11

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)] = 0.047 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.130 H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0634P)2] where P = (Fo2 + 2Fc2)/3
2915 reflections (Δ/σ)max = 0.001
163 parameters Δρmax = 0.86 e Å3
0 restraints Δρmin = −0.64 e Å3

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
Sn1 0.52583 (8) 0.20738 (8) 0.72575 (8) 0.0642 (3)
Sn2 0.34860 (7) 0.52430 (7) 0.91708 (7) 0.0541 (2)
Cl1 0.2281 (3) 0.7487 (4) 1.0584 (3) 0.0893 (9)
O1 0.5103 (6) 0.3891 (6) 0.8952 (6) 0.0567 (16)
O2 0.3315 (9) 0.2563 (10) 0.6371 (9) 0.104 (3)
O3 0.3517 (12) 0.0621 (12) 0.4673 (11) 0.123 (3)
C1 0.2708 (19) 0.160 (2) 0.5170 (19) 0.126 (6)
C2 0.114 (2) 0.312 (2) 0.436 (2) 0.147 (7)
H2 0.1241 0.4026 0.5205 0.177*
C3 0.1132 (19) 0.168 (2) 0.4573 (18) 0.137 (6)
H3 0.0508 0.1632 0.5294 0.164*
C4 0.042 (2) 0.057 (2) 0.3123 (19) 0.152 (7)
H4A 0.1041 −0.0144 0.2773 0.183*
H4B −0.0502 0.0065 0.3211 0.183*
C5 0.017 (2) 0.135 (2) 0.2080 (19) 0.139 (6)
H5 −0.0452 0.0854 0.1128 0.166*
C6 0.183 (2) 0.175 (2) 0.223 (2) 0.156 (7)
H6 0.2425 0.1242 0.1621 0.187*
C7 0.226 (2) 0.295 (2) 0.337 (2) 0.153 (7)
H7 0.3122 0.3604 0.3543 0.183*
C8 −0.0092 (18) 0.277 (2) 0.3130 (18) 0.140 (6)
H8A −0.0047 0.3524 0.2702 0.168*
H8B −0.1029 0.2657 0.3446 0.168*
C9 0.6728 (14) 0.2796 (14) 0.6114 (13) 0.101 (4)
H9A 0.7045 0.3833 0.6575 0.152*
H9B 0.6262 0.2576 0.5134 0.152*
H9C 0.7556 0.2311 0.6106 0.152*
C10 0.4421 (14) 0.0339 (13) 0.7839 (13) 0.095 (4)
H10A 0.4365 0.0689 0.8857 0.142*
H10B 0.5048 −0.0379 0.7639 0.142*
H10C 0.3464 −0.0094 0.7289 0.142*
C11 0.4013 (13) 0.6224 (13) 0.7674 (12) 0.086 (3)
H11A 0.3294 0.6805 0.7552 0.129*
H11B 0.4031 0.5479 0.6756 0.129*
H11C 0.4954 0.6837 0.8028 0.129*
C12 0.1694 (12) 0.3767 (14) 0.9197 (13) 0.098 (4)
H12A 0.1857 0.2786 0.8743 0.147*
H12B 0.0834 0.3910 0.8676 0.147*
H12C 0.1567 0.3928 1.0184 0.147*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Sn1 0.0789 (5) 0.0509 (5) 0.0573 (5) 0.0212 (4) 0.0060 (4) 0.0105 (4)
Sn2 0.0483 (4) 0.0559 (5) 0.0558 (4) 0.0153 (3) −0.0009 (3) 0.0177 (3)
Cl1 0.0721 (18) 0.088 (2) 0.092 (2) 0.0425 (15) −0.0049 (15) 0.0080 (17)
O1 0.057 (4) 0.052 (4) 0.056 (4) 0.028 (3) −0.001 (3) 0.009 (3)
O2 0.113 (7) 0.093 (7) 0.090 (6) 0.043 (5) −0.023 (5) 0.013 (5)
O3 0.142 (9) 0.113 (9) 0.091 (7) 0.039 (7) −0.028 (6) 0.016 (6)
C1 0.132 (14) 0.121 (14) 0.103 (12) 0.041 (11) −0.031 (10) 0.023 (11)
C2 0.154 (17) 0.134 (17) 0.121 (15) 0.047 (13) −0.017 (13) 0.009 (12)
C3 0.163 (16) 0.124 (15) 0.108 (13) 0.021 (12) −0.021 (11) 0.036 (12)
C4 0.157 (16) 0.137 (16) 0.131 (15) 0.024 (12) −0.027 (12) 0.022 (14)
C5 0.146 (16) 0.137 (16) 0.108 (13) 0.033 (12) −0.038 (11) 0.028 (12)
C6 0.147 (17) 0.154 (18) 0.122 (15) 0.036 (13) −0.005 (12) −0.002 (13)
C7 0.150 (17) 0.141 (18) 0.132 (16) 0.020 (13) −0.001 (14) 0.012 (14)
C8 0.141 (14) 0.138 (16) 0.124 (14) 0.065 (11) −0.025 (11) 0.025 (12)
C9 0.125 (11) 0.091 (10) 0.084 (9) 0.025 (8) 0.029 (8) 0.019 (8)
C10 0.109 (10) 0.075 (9) 0.093 (9) 0.009 (7) 0.003 (7) 0.028 (7)
C11 0.105 (9) 0.084 (9) 0.086 (8) 0.034 (7) 0.019 (7) 0.044 (7)
C12 0.080 (8) 0.089 (9) 0.111 (10) −0.002 (7) 0.009 (7) 0.026 (8)

Geometric parameters (Å, °)

Sn1—O1 2.034 (6) C4—C5 1.49 (2)
Sn1—C10 2.075 (11) C4—H4A 0.9700
Sn1—C9 2.082 (11) C4—H4B 0.9700
Sn1—O2 2.115 (8) C5—C8 1.51 (2)
Sn1—O3 2.699 (9) C5—C6 1.54 (2)
Sn1—Cl1i 2.848 (3) C5—H5 0.9800
Sn2—O1i 2.010 (5) C6—C7 1.31 (2)
Sn2—C12 2.088 (11) C6—H6 0.9300
Sn2—C11 2.096 (10) C7—H7 0.9300
Sn2—O1 2.122 (6) C8—H8A 0.9700
Sn2—Cl1 2.649 (3) C8—H8B 0.9700
Sn2—Sn2i 3.2898 (12) C9—H9A 0.9600
Cl1—Sn1i 2.848 (3) C9—H9B 0.9600
O1—Sn2i 2.010 (5) C9—H9C 0.9600
O2—C1 1.262 (16) C10—H10A 0.9600
O3—C1 1.300 (18) C10—H10B 0.9600
C1—C3 1.55 (2) C10—H10C 0.9600
C2—C8 1.494 (19) C11—H11A 0.9600
C2—C7 1.50 (2) C11—H11B 0.9600
C2—C3 1.51 (2) C11—H11C 0.9600
C2—H2 0.9800 C12—H12A 0.9600
C3—C4 1.50 (2) C12—H12B 0.9600
C3—H3 0.9800 C12—H12C 0.9600
O1—Sn1—C10 104.6 (4) C1—C3—H3 108.7
O1—Sn1—C9 105.3 (4) C5—C4—C3 108.8 (15)
C10—Sn1—C9 145.7 (5) C5—C4—H4A 109.9
O1—Sn1—O2 81.2 (3) C3—C4—H4A 109.9
C10—Sn1—O2 100.6 (4) C5—C4—H4B 109.9
C9—Sn1—O2 100.3 (5) C3—C4—H4B 109.9
O1—Sn1—O3 131.8 (3) H4A—C4—H4B 108.3
C10—Sn1—O3 85.5 (4) C4—C5—C8 98.8 (15)
C9—Sn1—O3 87.1 (4) C4—C5—C6 88.3 (13)
O2—Sn1—O3 50.6 (3) C8—C5—C6 97.7 (14)
O1—Sn1—Cl1i 74.13 (16) C4—C5—H5 121.6
C10—Sn1—Cl1i 86.0 (3) C8—C5—H5 121.6
C9—Sn1—Cl1i 86.2 (4) C6—C5—H5 121.6
O2—Sn1—Cl1i 155.3 (3) C7—C6—C5 107.2 (18)
O3—Sn1—Cl1i 154.0 (3) C7—C6—H6 126.4
O1i—Sn2—C12 114.6 (4) C5—C6—H6 126.4
O1i—Sn2—C11 111.7 (4) C6—C7—C2 109.9 (18)
C12—Sn2—C11 133.2 (5) C6—C7—H7 125.0
O1i—Sn2—O1 74.5 (3) C2—C7—H7 125.0
C12—Sn2—O1 99.8 (4) C2—C8—C5 102.3 (14)
C11—Sn2—O1 98.5 (4) C2—C8—H8A 111.3
O1i—Sn2—Cl1 79.31 (17) C5—C8—H8A 111.3
C12—Sn2—Cl1 91.0 (4) C2—C8—H8B 111.3
C11—Sn2—Cl1 91.0 (3) C5—C8—H8B 111.3
O1—Sn2—Cl1 153.80 (17) H8A—C8—H8B 109.2
O1i—Sn2—Sn2i 38.43 (16) Sn1—C9—H9A 109.5
C12—Sn2—Sn2i 111.3 (4) Sn1—C9—H9B 109.5
C11—Sn2—Sn2i 108.8 (3) H9A—C9—H9B 109.5
O1—Sn2—Sn2i 36.06 (15) Sn1—C9—H9C 109.5
Cl1—Sn2—Sn2i 117.74 (7) H9A—C9—H9C 109.5
Sn2—Cl1—Sn1i 81.42 (7) H9B—C9—H9C 109.5
Sn2i—O1—Sn1 125.1 (3) Sn1—C10—H10A 109.5
Sn2i—O1—Sn2 105.5 (3) Sn1—C10—H10B 109.5
Sn1—O1—Sn2 129.3 (3) H10A—C10—H10B 109.5
C1—O2—Sn1 113.3 (10) Sn1—C10—H10C 109.5
C1—O3—Sn1 83.5 (8) H10A—C10—H10C 109.5
O2—C1—O3 112.1 (13) H10B—C10—H10C 109.5
O2—C1—C3 117.7 (16) Sn2—C11—H11A 109.5
O3—C1—C3 130.1 (15) Sn2—C11—H11B 109.5
C8—C2—C7 92.7 (16) H11A—C11—H11B 109.5
C8—C2—C3 102.9 (15) Sn2—C11—H11C 109.5
C7—C2—C3 96.9 (16) H11A—C11—H11C 109.5
C8—C2—H2 119.7 H11B—C11—H11C 109.5
C7—C2—H2 119.7 Sn2—C12—H12A 109.5
C3—C2—H2 119.7 Sn2—C12—H12B 109.5
C4—C3—C2 103.5 (14) H12A—C12—H12B 109.5
C4—C3—C1 118.3 (17) Sn2—C12—H12C 109.5
C2—C3—C1 108.7 (15) H12A—C12—H12C 109.5
C4—C3—H3 108.7 H12B—C12—H12C 109.5
C2—C3—H3 108.7

Symmetry codes: (i) −x+1, −y+1, −z+2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: RZ2611).

References

  1. Dubey, S. K. & Roy, U. (2003). Appl. Organomet. Chem. 17, 3–8.
  2. Li, F.-H., Yin, H.-D., Sun, L., Zhao, Q. & Liu, W.-L. (2006). Acta Cryst. E62, m1117–m1118.
  3. Sheldrick, G. M. (1996). SADABS University of Göttingen, Germany.
  4. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  5. Siemens (1996). SMART and SAINT Siemens Analytical X-ray Instruments Inc., Madison, Wisconsin, USA.

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) I, global. DOI: 10.1107/S1600536811023452/rz2611sup1.cif

e-67-0m984-sup1.cif (17.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811023452/rz2611Isup2.hkl

e-67-0m984-Isup2.hkl (143KB, 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

RESOURCES