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Acta Cryst. (2008). E64, m1187    [ doi:10.1107/S1600536808023799 ]

Triclinic modification of di-n-butylbis(2-hydroxybenzoato-[kappa]2O1,O1')tin(IV)

R. Reisi, M. Misran, K. M. Lo and S. W. Ng

Abstract top

The Sn atom in the title compound, [Sn(C4H9)2(C7H5O3)2], is chelated by the carboxylate groups of 2-hydroxybenzoate liagnds, and exists in a six-coordinate skew-trapezoidal bipyramidal coordination geometry [C-Sn-C = 140.1 (3)°].

Comment top

Diorganotin dicarboxylates generally exist as monomeric molecules in which the carboxylate groups chelate in an anisobidentate manner (Tiekink, 1991; 1994). The R2Sn unit is bent, and the geometry at tin is described as being skew-trapezoidal bipyramidal (Ng et al., 1987). The title compound has been reported in a monoclinic form (Narula et al., 1992). This structure has one n-butyl group in a W conformation and the other in a U conformation. In the present triclinic modification (Scheme I, Fig. 1), both groups adopt a W conformation. Intramolecular O-H···O hydrogen bonds are noted (Table 1).

Related literature top

For the monoclinic modification, see: Narula et al. (1992). For a review of the structural chemistry of organotin carboxylates, see: Tiekink (1991, 1994). For a discussion of skew-trapezoidal bipyramidal diorganotin bis(chelates), see: Ng et al. (1987).

Experimental top

Dibutyltin oxide (2 g, 8 mmol) and salicylic acid (2.2 g, 16 mmol) were heated in toluene (100 ml) in a Dean-Stark water apparatus. Slow evaporation of the filtered solution yielded colorless crystals.

Refinement top

Carbon-bound H-atoms were placed in positions (C–H 0.95 to 0.99 Å) and were included in the refinement in the riding model approximation, with U(H) set to 1.2–1.5Ueq(C). The hydroxy H-atoms were similarly constrained (O–H 0.84 Å) but the hybridization of the oxygen atoms was assumed to be sp2.

The final difference Fourier map had a peak of 2.57 e Å-3 at 1.5 Å from the O5 and O6 atoms, and a deep hole of -1.40 e Å-3 at 1.5 Å from the H12 atom.

Computing details top

Data collection: APEX2 (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT (Bruker, 2007); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: X-SEED (Barbour, 2001); software used to prepare material for publication: publCIF (Westrip, 2008).

Figures top
[Figure 1] Fig. 1. Thermal ellipsoid plot (Barbour, 2001) plot of the triclinic form of [Sn(C4H9)2(C7H5O3] at the 50% probability level. Hydrogen atoms are drawn as spheres of arbitrary radius.
di-n-butylbis(2-hydroxybenzoato-κ2O1,O1')tin(IV) top
Crystal data top
[Sn(C4H9)2(C7H5O3)2]Z = 2
Mr = 507.13F000 = 516
Triclinic, P1Dx = 1.502 Mg m−3
Hall symbol: -P 1Mo Kα radiation
λ = 0.71073 Å
a = 9.1652 (2) ÅCell parameters from 6302 reflections
b = 11.2111 (2) Åθ = 2.5–27.7º
c = 12.2620 (2) ŵ = 1.17 mm−1
α = 94.759 (1)ºT = 100 (2) K
β = 106.872 (1)ºBlock, colorless
γ = 108.586 (1)º0.25 × 0.20 × 0.15 mm
V = 1121.24 (4) Å3
Data collection top
Bruker SMART APEX
diffractometer		5068 independent reflections
Radiation source: fine-focus sealed tube4633 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.034
T = 100(2) Kθmax = 27.5º
ω scansθmin = 1.8º
Absorption correction: Multi-scan
(SADABS; Sheldrick, 1996)		h = −11→7
Tmin = 0.758, Tmax = 0.844k = −14→14
11666 measured reflectionsl = −15→15
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.059H-atom parameters constrained
wR(F2) = 0.189  w = 1/[σ2(Fo2) + (0.0604P)2 + 8.6498P]
where P = (Fo2 + 2Fc2)/3
S = 1.18(Δ/σ)max = 0.001
5068 reflectionsΔρmax = 2.57 e Å−3
262 parametersΔρmin = −1.40 e Å−3
2 restraintsExtinction correction: none
Primary atom site location: structure-invariant direct methods
Crystal data top
[Sn(C4H9)2(C7H5O3)2]γ = 108.586 (1)º
Mr = 507.13V = 1121.24 (4) Å3
Triclinic, P1Z = 2
a = 9.1652 (2) ÅMo Kα
b = 11.2111 (2) ŵ = 1.17 mm−1
c = 12.2620 (2) ÅT = 100 (2) K
α = 94.759 (1)º0.25 × 0.20 × 0.15 mm
β = 106.872 (1)º
Data collection top
Bruker SMART APEX
diffractometer		5068 independent reflections
Absorption correction: Multi-scan
(SADABS; Sheldrick, 1996)		4633 reflections with I > 2σ(I)
Tmin = 0.758, Tmax = 0.844Rint = 0.034
11666 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0592 restraints
wR(F2) = 0.189H-atom parameters constrained
S = 1.18Δρmax = 2.57 e Å−3
5068 reflectionsΔρmin = −1.40 e Å−3
262 parameters
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Sn10.50157 (6)0.34322 (5)0.64132 (4)0.03511 (17)
O10.6039 (7)0.5445 (5)0.6922 (5)0.0424 (11)
O20.4303 (7)0.4748 (5)0.7850 (5)0.0495 (13)
O30.4148 (9)0.6313 (7)0.9462 (6)0.0687 (19)
H3O0.38020.55490.91110.103*
O40.6470 (6)0.3786 (5)0.5355 (4)0.0391 (11)
O50.5384 (8)0.1687 (6)0.5037 (5)0.0535 (14)
O60.5995 (9)0.0298 (5)0.3515 (6)0.0634 (18)
H6O0.54750.02760.39800.095*
C10.2603 (9)0.2912 (8)0.5242 (7)0.0452 (17)
H1A0.25220.36520.48730.054*
H1B0.24120.22010.46200.054*
C20.1264 (10)0.2505 (8)0.5755 (8)0.0512 (19)
H2A0.13540.32530.62960.061*
H2B0.01980.22430.51230.061*
C30.1281 (12)0.1422 (9)0.6398 (9)0.059 (2)
H3A0.22430.17380.71180.071*
H3B0.14100.07380.59110.071*
C4−0.0260 (15)0.0841 (11)0.6719 (11)0.077 (3)
H4A−0.01590.01500.71400.116*
H4B−0.12170.04960.60090.116*
H4C−0.03890.15070.72120.116*
C50.6353 (10)0.2839 (7)0.7842 (7)0.0429 (16)
H5A0.60760.30660.85340.051*
H5B0.60340.18950.76690.051*
C60.8165 (10)0.3455 (7)0.8106 (7)0.0423 (16)
H6A0.84730.43990.82590.051*
H6B0.84360.32150.74150.051*
C70.9178 (12)0.3068 (9)0.9151 (8)0.059 (2)
H7A0.89170.33180.98450.070*
H7B0.88610.21240.90030.070*
C81.0967 (13)0.3666 (13)0.9401 (10)0.079 (3)
H8A1.15470.34111.00930.118*
H8B1.12880.46020.95380.118*
H8C1.12450.33810.87360.118*
C90.5369 (9)0.5664 (7)0.7668 (6)0.0391 (15)
C100.5867 (10)0.6976 (7)0.8301 (6)0.0391 (15)
C110.5246 (11)0.7235 (8)0.9170 (7)0.0466 (18)
C120.5768 (15)0.8474 (9)0.9784 (8)0.066 (3)
H120.53440.86481.03750.079*
C130.6896 (18)0.9447 (9)0.9535 (11)0.085 (4)
H130.72371.02980.99490.102*
C140.7559 (19)0.9206 (9)0.8676 (11)0.091 (5)
H140.83610.98840.85220.109*
C150.7029 (12)0.7971 (8)0.8060 (8)0.053 (2)
H150.74570.77990.74710.064*
C160.6292 (8)0.2670 (7)0.4830 (6)0.0350 (14)
C170.7181 (8)0.2616 (7)0.4013 (6)0.0344 (14)
C180.6975 (10)0.1431 (7)0.3404 (7)0.0420 (16)
C190.7814 (12)0.1408 (9)0.2613 (7)0.052 (2)
H190.76490.06150.21630.063*
C200.8863 (13)0.2521 (10)0.2488 (8)0.061 (2)
H200.94410.24890.19640.074*
C210.9105 (12)0.3695 (9)0.3108 (8)0.056 (2)
H210.98490.44630.30200.067*
C220.8242 (9)0.3729 (7)0.3858 (7)0.0419 (16)
H220.83800.45320.42760.050*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Sn10.0326 (3)0.0370 (3)0.0356 (3)0.00980 (19)0.01499 (19)0.00458 (18)
O10.048 (3)0.040 (3)0.042 (3)0.015 (2)0.020 (2)0.006 (2)
O20.049 (3)0.045 (3)0.052 (3)0.010 (2)0.021 (3)0.006 (2)
O30.078 (5)0.059 (4)0.071 (4)0.009 (3)0.048 (4)0.003 (3)
O40.044 (3)0.038 (3)0.041 (3)0.014 (2)0.022 (2)0.006 (2)
O50.058 (4)0.046 (3)0.060 (4)0.010 (3)0.035 (3)0.010 (3)
O60.076 (4)0.036 (3)0.076 (4)0.006 (3)0.041 (4)−0.002 (3)
C10.041 (4)0.054 (4)0.039 (4)0.014 (3)0.013 (3)0.011 (3)
C20.040 (4)0.051 (5)0.065 (5)0.017 (4)0.020 (4)0.019 (4)
C30.055 (5)0.055 (5)0.077 (6)0.019 (4)0.034 (5)0.022 (5)
C40.080 (7)0.070 (7)0.098 (8)0.019 (6)0.062 (7)0.014 (6)
C50.050 (4)0.040 (4)0.039 (4)0.012 (3)0.019 (3)0.010 (3)
C60.048 (4)0.039 (4)0.041 (4)0.013 (3)0.017 (3)0.010 (3)
C70.063 (6)0.057 (5)0.054 (5)0.024 (4)0.011 (4)0.016 (4)
C80.056 (6)0.104 (9)0.074 (7)0.037 (6)0.008 (5)0.020 (6)
C90.042 (4)0.046 (4)0.034 (3)0.021 (3)0.014 (3)0.008 (3)
C100.049 (4)0.036 (3)0.032 (3)0.017 (3)0.011 (3)0.009 (3)
C110.057 (5)0.044 (4)0.044 (4)0.017 (4)0.024 (4)0.008 (3)
C120.099 (8)0.055 (5)0.054 (5)0.027 (5)0.043 (5)0.003 (4)
C130.136 (11)0.037 (5)0.086 (8)0.010 (6)0.068 (8)−0.001 (5)
C140.145 (12)0.038 (5)0.100 (9)0.007 (6)0.089 (9)0.002 (5)
C150.073 (6)0.044 (4)0.051 (5)0.017 (4)0.038 (4)0.009 (4)
C160.033 (3)0.040 (4)0.033 (3)0.013 (3)0.012 (3)0.007 (3)
C170.036 (3)0.041 (4)0.031 (3)0.017 (3)0.013 (3)0.008 (3)
C180.043 (4)0.039 (4)0.046 (4)0.013 (3)0.020 (3)0.008 (3)
C190.068 (6)0.055 (5)0.041 (4)0.026 (4)0.025 (4)0.003 (3)
C200.074 (6)0.082 (7)0.048 (5)0.039 (5)0.036 (5)0.018 (4)
C210.064 (6)0.059 (5)0.060 (5)0.023 (4)0.038 (5)0.028 (4)
C220.044 (4)0.043 (4)0.048 (4)0.020 (3)0.022 (3)0.016 (3)
Geometric parameters (Å, °) top
Sn1—C12.118 (8)C6—H6A0.9900
Sn1—C52.117 (8)C6—H6B0.9900
Sn1—O12.106 (5)C7—C81.485 (15)
Sn1—O22.561 (6)C7—H7A0.9900
Sn1—O42.090 (5)C7—H7B0.9900
Sn1—O52.645 (6)C8—H8A0.9800
O1—C91.288 (9)C8—H8B0.9800
O2—C91.259 (9)C8—H8C0.9800
O3—C111.348 (10)C9—C101.467 (10)
O3—H3O0.8400C10—C111.396 (11)
O4—C161.296 (8)C10—C151.395 (11)
O5—C161.247 (9)C11—C121.386 (12)
O6—C181.346 (9)C12—C131.368 (15)
O6—H6O0.8400C12—H120.9500
C1—C21.501 (11)C13—C141.408 (15)
C1—H1A0.9900C13—H130.9500
C1—H1B0.9900C14—C151.382 (12)
C2—C31.503 (12)C14—H140.9500
C2—H2A0.9900C15—H150.9500
C2—H2B0.9900C16—C171.472 (9)
C3—C41.534 (13)C17—C221.383 (10)
C3—H3A0.9900C17—C181.397 (10)
C3—H3B0.9900C18—C191.405 (11)
C4—H4A0.9800C19—C201.362 (14)
C4—H4B0.9800C19—H190.9500
C4—H4C0.9800C20—C211.382 (14)
C5—C61.503 (11)C20—H200.9500
C5—H5A0.9900C21—C221.382 (11)
C5—H5B0.9900C21—H210.9500
C6—C71.533 (11)C22—H220.9500
O4—Sn1—O182.3 (2)H6A—C6—H6B107.7
O4—Sn1—C5104.7 (3)C8—C7—C6113.3 (8)
O1—Sn1—C5102.1 (3)C8—C7—H7A108.9
O4—Sn1—C1104.1 (3)C6—C7—H7A108.9
O1—Sn1—C1108.7 (3)C8—C7—H7B108.9
C1—Sn1—C5140.1 (3)C6—C7—H7B108.9
O4—Sn1—O2137.44 (19)H7A—C7—H7B107.7
O1—Sn1—O255.25 (19)C7—C8—H8A109.5
C5—Sn1—O288.1 (3)C7—C8—H8B109.5
C1—Sn1—O289.0 (3)H8A—C8—H8B109.5
O4—Sn1—O553.64 (18)C7—C8—H8C109.5
O1—Sn1—O5135.77 (19)H8A—C8—H8C109.5
C5—Sn1—O587.8 (3)H8B—C8—H8C109.5
C1—Sn1—O587.5 (3)O2—C9—O1119.5 (7)
O2—Sn1—O5168.92 (18)O2—C9—C10120.8 (7)
C9—O1—Sn1102.7 (5)O1—C9—C10119.6 (7)
C9—O2—Sn182.4 (4)C11—C10—C15119.7 (7)
C11—O3—H3O120.0C11—C10—C9121.1 (7)
C16—O4—Sn1106.0 (4)C15—C10—C9119.2 (7)
C16—O5—Sn181.3 (4)O3—C11—C12117.1 (8)
C18—O6—H6O120.0O3—C11—C10122.6 (7)
C2—C1—Sn1116.0 (5)C12—C11—C10120.3 (8)
C2—C1—H1A108.3C13—C12—C11119.7 (9)
Sn1—C1—H1A108.3C13—C12—H12120.1
C2—C1—H1B108.3C11—C12—H12120.1
Sn1—C1—H1B108.3C12—C13—C14121.0 (9)
H1A—C1—H1B107.4C12—C13—H13119.5
C3—C2—C1114.3 (7)C14—C13—H13119.5
C3—C2—H2A108.7C15—C14—C13119.2 (9)
C1—C2—H2A108.7C15—C14—H14120.4
C3—C2—H2B108.7C13—C14—H14120.4
C1—C2—H2B108.7C14—C15—C10120.2 (8)
H2A—C2—H2B107.6C14—C15—H15119.9
C2—C3—C4114.0 (9)C10—C15—H15119.9
C2—C3—H3A108.8O5—C16—O4119.1 (6)
C4—C3—H3A108.8O5—C16—C17122.5 (7)
C2—C3—H3B108.8O4—C16—C17118.4 (6)
C4—C3—H3B108.8C22—C17—C18119.7 (7)
H3A—C3—H3B107.7C22—C17—C16120.5 (6)
C3—C4—H4A109.5C18—C17—C16119.9 (6)
C3—C4—H4B109.5O6—C18—C19117.5 (7)
H4A—C4—H4B109.5O6—C18—C17123.8 (7)
C3—C4—H4C109.5C19—C18—C17118.7 (7)
H4A—C4—H4C109.5C20—C19—C18120.2 (8)
H4B—C4—H4C109.5C20—C19—H19119.9
C6—C5—Sn1111.8 (5)C18—C19—H19119.9
C6—C5—H5A109.2C19—C20—C21121.5 (8)
Sn1—C5—H5A109.2C19—C20—H20119.2
C6—C5—H5B109.2C21—C20—H20119.2
Sn1—C5—H5B109.2C22—C21—C20118.6 (8)
H5A—C5—H5B107.9C22—C21—H21120.7
C5—C6—C7113.4 (7)C20—C21—H21120.7
C5—C6—H6A108.9C17—C22—C21121.3 (8)
C7—C6—H6A108.9C17—C22—H22119.4
C5—C6—H6B108.9C21—C22—H22119.4
C7—C6—H6B108.9
O4—Sn1—O1—C9179.6 (5)Sn1—O1—C9—O2−4.1 (8)
C5—Sn1—O1—C9−76.9 (5)Sn1—O1—C9—C10175.5 (5)
C1—Sn1—O1—C977.3 (5)O2—C9—C10—C113.9 (11)
O2—Sn1—O1—C92.1 (4)O1—C9—C10—C11−175.7 (7)
O5—Sn1—O1—C9−176.4 (4)O2—C9—C10—C15−178.8 (8)
O4—Sn1—O2—C9−5.8 (6)O1—C9—C10—C151.7 (11)
O1—Sn1—O2—C9−2.1 (4)C15—C10—C11—O3−178.5 (9)
C5—Sn1—O2—C9104.0 (5)C9—C10—C11—O3−1.2 (13)
C1—Sn1—O2—C9−115.8 (5)C15—C10—C11—C120.7 (13)
O5—Sn1—O2—C9172.4 (9)C9—C10—C11—C12178.0 (8)
O1—Sn1—O4—C16176.7 (5)O3—C11—C12—C13179.2 (11)
C5—Sn1—O4—C1676.2 (5)C10—C11—C12—C130.0 (17)
C1—Sn1—O4—C16−75.8 (5)C11—C12—C13—C14−1(2)
O2—Sn1—O4—C16179.8 (4)C12—C13—C14—C151(2)
O5—Sn1—O4—C160.2 (4)C13—C14—C15—C10−1(2)
O4—Sn1—O5—C16−0.2 (4)C11—C10—C15—C14−0.2 (15)
O1—Sn1—O5—C16−5.1 (6)C9—C10—C15—C14−177.6 (10)
C5—Sn1—O5—C16−110.3 (5)Sn1—O5—C16—O40.3 (6)
C1—Sn1—O5—C16109.4 (5)Sn1—O5—C16—C17−179.9 (7)
O2—Sn1—O5—C16−178.7 (9)Sn1—O4—C16—O5−0.4 (8)
O4—Sn1—C1—C2175.7 (6)Sn1—O4—C16—C17179.8 (5)
O1—Sn1—C1—C2−97.9 (6)O5—C16—C17—C22−176.5 (7)
C5—Sn1—C1—C240.6 (9)O4—C16—C17—C223.2 (10)
O2—Sn1—C1—C2−45.3 (6)O5—C16—C17—C182.4 (11)
O5—Sn1—C1—C2124.2 (6)O4—C16—C17—C18−177.9 (7)
Sn1—C1—C2—C3−55.4 (10)C22—C17—C18—O6178.7 (8)
C1—C2—C3—C4−169.0 (9)C16—C17—C18—O6−0.2 (12)
O4—Sn1—C5—C630.8 (6)C22—C17—C18—C19−2.3 (11)
O1—Sn1—C5—C6−54.3 (6)C16—C17—C18—C19178.8 (7)
C1—Sn1—C5—C6165.7 (5)O6—C18—C19—C20−177.9 (9)
O2—Sn1—C5—C6−108.1 (5)C17—C18—C19—C203.0 (13)
O5—Sn1—C5—C682.2 (5)C18—C19—C20—C21−1.5 (15)
Sn1—C5—C6—C7178.9 (6)C19—C20—C21—C22−0.7 (15)
C5—C6—C7—C8179.3 (9)C18—C17—C22—C210.1 (12)
Sn1—O2—C9—O13.3 (6)C16—C17—C22—C21179.0 (7)
Sn1—O2—C9—C10−176.3 (7)C20—C21—C22—C171.4 (13)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O3—H3o···O20.841.962.599 (9)132
O6—H6o···O50.842.002.626 (8)131
Table 1
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O3—H3o···O20.841.962.599 (9)132
O6—H6o···O50.842.002.626 (8)131
Acknowledgements top

We thank the University of Malaya for funding this study (SF022/2007 A, FS339/2008 A) and also for the purchase of the diffractometer.

references
References top

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