Literature DB >> 23723767

Diacetatodi-tert-butyltin(IV).

Martin Reichelt1, Hans Reuter.   

Abstract

The title compound, [Sn(C4H9)2(CH3COO)2], was synthesized in order to study the influence of large organic groups on the mol-ecular structure of diorganotin di-acetates. The title compound exhibits the same structure type as other diorganotin(IV) di-acetates characterized by an unsymmetrical bidentate bonding mode of the two acetate groups to tin. The influence of the t-butyl groups on this mol-ecular structure is expressed in two significant differences: tin-carbon bond lengths are much more longer than in the other di-acetates, as are the additional inter-actions of the acetate groups with the tin atom. Inter-molecular inter-actions are restricted to C-H⋯O ones similar to those in the other di-acetates, giving rise to a chain-like arrangement of the molecules with the tin atoms and acetate groups in the propagation plane.

Entities:  

Year:  2013        PMID: 23723767      PMCID: PMC3647801          DOI: 10.1107/S1600536813009185

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For background to diorganotin(IV) carboxyl­ates, see: Tiekink (1991 ▶) and to diorganotin(IV) di­acetates, see: Alcock et al. (1992 ▶); Lockhart et al. (1987 ▶); Mistry et al. (1995 ▶).

Experimental

Crystal data

[Sn(C4H9)2(C2H3O2)2] M = 351.00 Monoclinic, a = 6.1039 (3) Å b = 15.3928 (7) Å c = 15.9601 (8) Å β = 95.462 (2)° V = 1492.74 (12) Å3 Z = 4 Mo Kα radiation μ = 1.71 mm−1 T = 100 K 0.14 × 0.06 × 0.04 mm

Data collection

Bruker APEXII CCD diffractometer Absorption correction: multi-scan (SADABS; Bruker, 2009 ▶) T min = 0.791, T max = 0.939 76636 measured reflections 3590 independent reflections 2980 reflections with I > 2σ(I) R int = 0.081

Refinement

R[F 2 > 2σ(F 2)] = 0.023 wR(F 2) = 0.046 S = 1.04 3590 reflections 167 parameters H-atom parameters constrained Δρmax = 0.59 e Å−3 Δρmin = −0.51 e Å−3 Data collection: APEX2 (Bruker, 2009 ▶); cell refinement: SAINT (Bruker, 2009 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: DIAMOND (Brandenburg, 2006 ▶) and Mercury (Macrae et al., 2008 ▶); software used to prepare material for publication: SHELXTL (Sheldrick, 2008 ▶). Click here for additional data file. Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536813009185/aa2086sup1.cif Click here for additional data file. Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813009185/aa2086Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
[Sn(C4H9)2(C2H3O2)2]F(000) = 712
Mr = 351.00Dx = 1.562 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 6480 reflections
a = 6.1039 (3) Åθ = 2.6–25.7°
b = 15.3928 (7) ŵ = 1.71 mm1
c = 15.9601 (8) ÅT = 100 K
β = 95.462 (2)°Block, colourless
V = 1492.74 (12) Å30.14 × 0.06 × 0.04 mm
Z = 4
Bruker APEXII CCD diffractometer3590 independent reflections
Radiation source: fine-focus sealed tube2980 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.081
φ and ω scansθmax = 28.0°, θmin = 1.8°
Absorption correction: multi-scan (SADABS; Bruker, 2009)h = −8→8
Tmin = 0.791, Tmax = 0.939k = −20→19
76636 measured reflectionsl = −21→21
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.023H-atom parameters constrained
wR(F2) = 0.046w = 1/[σ2(Fo2) + (0.0133P)2 + 1.0511P] where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max = 0.002
3590 reflectionsΔρmax = 0.59 e Å3
167 parametersΔρmin = −0.51 e Å3
0 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.00201 (16)
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.
xyzUiso*/Ueq
Sn10.19140 (2)0.295768 (9)0.285075 (8)0.01333 (6)
C110.0432 (3)0.20445 (14)0.19231 (13)0.0162 (4)
C12−0.1709 (3)0.24192 (16)0.14968 (14)0.0257 (5)
H12A−0.23740.20010.10850.031 (2)*
H12B−0.13960.29620.12110.031 (2)*
H12C−0.27300.25340.19220.031 (2)*
C130.2095 (4)0.18975 (15)0.12781 (13)0.0216 (5)
H13A0.34850.16890.15660.031 (2)*
H13B0.23500.24450.09900.031 (2)*
H13C0.15150.14640.08650.031 (2)*
C14−0.0036 (4)0.11881 (15)0.23553 (14)0.0259 (5)
H14A−0.11280.12850.27580.031 (2)*
H14B0.13270.09660.26540.031 (2)*
H14C−0.06090.07640.19320.031 (2)*
C210.0894 (3)0.38924 (14)0.37595 (12)0.0161 (4)
C22−0.0723 (4)0.34722 (15)0.43092 (14)0.0245 (5)
H22A−0.11800.39000.47130.030 (2)*
H22B−0.00110.29800.46140.030 (2)*
H22C−0.20160.32670.39530.030 (2)*
C230.2995 (4)0.41692 (15)0.42919 (14)0.0243 (5)
H23A0.26260.45910.47170.030 (2)*
H23B0.40140.44350.39280.030 (2)*
H23C0.36890.36590.45720.030 (2)*
C24−0.0185 (4)0.46712 (15)0.33009 (14)0.0249 (5)
H24A−0.15020.44810.29500.030 (2)*
H24B0.08520.49360.29440.030 (2)*
H24C−0.06010.50980.37130.030 (2)*
O110.4677 (2)0.22581 (9)0.33641 (9)0.0198 (3)
O120.1995 (3)0.18113 (10)0.40892 (10)0.0251 (4)
C150.3940 (4)0.17649 (14)0.39399 (13)0.0203 (5)
C160.5546 (4)0.11407 (16)0.43777 (14)0.0265 (5)
H16A0.52820.10990.49730.037 (4)*
H16B0.70490.13470.43330.037 (4)*
H16C0.53570.05670.41140.037 (4)*
O210.4416 (2)0.36282 (9)0.23048 (9)0.0178 (3)
O220.1404 (2)0.41038 (10)0.15759 (9)0.0231 (3)
C250.3440 (4)0.40733 (13)0.16819 (13)0.0185 (5)
C260.4899 (4)0.45081 (15)0.11080 (14)0.0240 (5)
H26A0.51600.41140.06460.038 (4)*
H26B0.63060.46560.14230.038 (4)*
H26C0.41880.50390.08790.038 (4)*
U11U22U33U12U13U23
Sn10.01484 (8)0.01307 (8)0.01231 (8)0.00027 (6)0.00240 (5)−0.00084 (6)
C110.0158 (10)0.0177 (11)0.0156 (10)−0.0010 (8)0.0038 (8)−0.0048 (8)
C120.0162 (11)0.0342 (14)0.0260 (12)0.0018 (10)−0.0017 (9)−0.0072 (10)
C130.0222 (11)0.0235 (13)0.0194 (11)−0.0006 (9)0.0037 (9)−0.0078 (9)
C140.0294 (13)0.0220 (12)0.0276 (12)−0.0095 (10)0.0089 (10)−0.0041 (10)
C210.0153 (10)0.0166 (11)0.0167 (10)0.0006 (8)0.0028 (8)−0.0051 (8)
C220.0249 (12)0.0239 (13)0.0265 (12)0.0005 (10)0.0128 (10)−0.0036 (10)
C230.0246 (12)0.0266 (13)0.0216 (12)−0.0006 (10)0.0018 (9)−0.0093 (9)
C240.0303 (13)0.0204 (12)0.0246 (12)0.0065 (10)0.0057 (10)−0.0020 (9)
O110.0211 (8)0.0180 (8)0.0199 (8)0.0020 (6)−0.0005 (6)0.0035 (6)
O120.0273 (9)0.0222 (9)0.0263 (9)0.0039 (7)0.0055 (7)0.0017 (7)
C150.0286 (13)0.0147 (11)0.0166 (11)0.0014 (9)−0.0025 (9)−0.0031 (8)
C160.0337 (13)0.0229 (12)0.0221 (12)0.0072 (10)−0.0024 (10)0.0049 (10)
O210.0192 (8)0.0172 (8)0.0174 (7)−0.0003 (6)0.0046 (6)0.0027 (6)
O220.0226 (9)0.0267 (9)0.0202 (8)0.0019 (7)0.0028 (6)0.0013 (6)
C250.0279 (12)0.0137 (11)0.0147 (10)−0.0021 (9)0.0055 (9)−0.0036 (8)
C260.0304 (13)0.0215 (13)0.0209 (12)−0.0012 (10)0.0076 (10)0.0030 (9)
Sn1—O212.1001 (14)C22—H22B0.9800
Sn1—O112.1002 (14)C22—H22C0.9800
Sn1—C112.175 (2)C23—H23A0.9800
Sn1—C212.176 (2)C23—H23B0.9800
C11—C141.527 (3)C23—H23C0.9800
C11—C121.528 (3)C24—H24A0.9800
C11—C131.530 (3)C24—H24B0.9800
C12—H12A0.9800C24—H24C0.9800
C12—H12B0.9800O11—C151.304 (3)
C12—H12C0.9800O12—C151.235 (3)
C13—H13A0.9800C15—C161.497 (3)
C13—H13B0.9800C16—H16A0.9800
C13—H13C0.9800C16—H16B0.9800
C14—H14A0.9800C16—H16C0.9800
C14—H14B0.9800O21—C251.304 (3)
C14—H14C0.9800O22—C251.239 (3)
C21—C241.522 (3)C25—C261.495 (3)
C21—C221.525 (3)C26—H26A0.9800
C21—C231.530 (3)C26—H26B0.9800
C22—H22A0.9800C26—H26C0.9800
O21—Sn1—O1179.93 (6)C21—C22—H22B109.5
O21—Sn1—C11107.88 (7)H22A—C22—H22B109.5
O11—Sn1—C11101.58 (7)C21—C22—H22C109.5
O21—Sn1—C21102.54 (7)H22A—C22—H22C109.5
O11—Sn1—C21110.43 (7)H22B—C22—H22C109.5
C11—Sn1—C21138.97 (7)C21—C23—H23A109.5
C14—C11—C12109.77 (18)C21—C23—H23B109.5
C14—C11—C13109.93 (18)H23A—C23—H23B109.5
C12—C11—C13110.51 (17)C21—C23—H23C109.5
C14—C11—Sn1109.51 (14)H23A—C23—H23C109.5
C12—C11—Sn1109.99 (14)H23B—C23—H23C109.5
C13—C11—Sn1107.09 (13)C21—C24—H24A109.5
C11—C12—H12A109.5C21—C24—H24B109.5
C11—C12—H12B109.5H24A—C24—H24B109.5
H12A—C12—H12B109.5C21—C24—H24C109.5
C11—C12—H12C109.5H24A—C24—H24C109.5
H12A—C12—H12C109.5H24B—C24—H24C109.5
H12B—C12—H12C109.5C15—O11—Sn1104.81 (13)
C11—C13—H13A109.5O12—C15—O11120.3 (2)
C11—C13—H13B109.5O12—C15—C16123.1 (2)
H13A—C13—H13B109.5O11—C15—C16116.6 (2)
C11—C13—H13C109.5C15—C16—H16A109.5
H13A—C13—H13C109.5C15—C16—H16B109.5
H13B—C13—H13C109.5H16A—C16—H16B109.5
C11—C14—H14A109.5C15—C16—H16C109.5
C11—C14—H14B109.5H16A—C16—H16C109.5
H14A—C14—H14B109.5H16B—C16—H16C109.5
C11—C14—H14C109.5C25—O21—Sn1106.07 (13)
H14A—C14—H14C109.5O22—C25—O21120.25 (19)
H14B—C14—H14C109.5O22—C25—C26123.21 (19)
C24—C21—C22109.65 (17)O21—C25—C26116.51 (19)
C24—C21—C23110.46 (18)C25—C26—H26A109.5
C22—C21—C23110.65 (17)C25—C26—H26B109.5
C24—C21—Sn1109.79 (13)H26A—C26—H26B109.5
C22—C21—Sn1110.17 (14)C25—C26—H26C109.5
C23—C21—Sn1106.07 (13)H26A—C26—H26C109.5
C21—C22—H22A109.5H26B—C26—H26C109.5
D—H···AD—HH···AD···AD—H···A
C12—H12C···O21i0.982.543.362 (3)142
C22—H22C···O11i0.982.653.584 (3)160
C16—H16C···O22ii0.982.693.636 (3)163
C16—H16A···O22iii0.982.603.518 (3)155
Table 1

Selected bond lengths (Å)

Sn1—O212.1001 (14)
Sn1—O112.1002 (14)
Sn1—C112.175 (2)
Sn1—C212.176 (2)
O11—C151.304 (3)
O12—C151.235 (3)
O21—C251.304 (3)
O22—C251.239 (3)
Table 2

Hydrogen-bond geometry (Å, °)

D—H⋯A D—HH⋯A DA D—H⋯A
C12—H12C⋯O21i 0.982.543.362 (3)142
C22—H22C⋯O11i 0.982.653.584 (3)160
C16—H16C⋯O22ii 0.982.693.636 (3)163
C16—H16A⋯O22iii 0.982.603.518 (3)155

Symmetry codes: (i) ; (ii) ; (iii) .

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