Download citation
Download citation
link to html
The crystal structure determination of the title compound, [Sn(C4H9)2(C8F4O4)]n, revealed an infinite polymeric chain in the solid state. The Sn atom is in a distorted sixfold coordination between bicapped tetrahedral and skew-bipyramidal.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807006940/kp2085sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807006940/kp2085Isup2.hkl
Contains datablock I

CCDC reference: 640405

Key indicators

  • Single-crystal X-ray study
  • T = 298 K
  • Mean [sigma](C-C) = 0.014 Å
  • R factor = 0.055
  • wR factor = 0.184
  • Data-to-parameter ratio = 14.3

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT125_ALERT_4_C No _symmetry_space_group_name_Hall Given ....... ? PLAT220_ALERT_2_C Large Non-Solvent C Ueq(max)/Ueq(min) ... 3.00 Ratio PLAT342_ALERT_3_C Low Bond Precision on C-C bonds (x 1000) Ang ... 14
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 3 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 1 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Computing details top

Data collection: SMART (Bruker, 1999); cell refinement: SMART; data reduction: SAINT (Bruker, 1999); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997a); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997a); molecular graphics: SHELXTL (Sheldrick, 1997b); software used to prepare material for publication: SHELXTL.

catena-Poly[[dibutyltin(IV)]-µ-3,4,5,6-tetrafluorobenzene-1,2-dicarboxylato- κ4O1,O1':O2,O2'] top
Crystal data top
[Sn(C4H9)2(C8F4O4)]F(000) = 928
Mr = 468.99Dx = 1.663 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 9.8470 (17) ÅCell parameters from 3138 reflections
b = 17.733 (3) Åθ = 2.2–25.6°
c = 11.146 (2) ŵ = 1.42 mm1
β = 105.732 (3)°T = 298 K
V = 1873.3 (6) Å3Block, colourless
Z = 40.23 × 0.21 × 0.15 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
3238 independent reflections
Radiation source: fine-focus sealed tube2125 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.033
φ and ω scansθmax = 25.0°, θmin = 2.2°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 511
Tmin = 0.736, Tmax = 0.815k = 2121
9445 measured reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.055Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.184H-atom parameters constrained
S = 1.00 w = 1/[σ2(Fo2) + (0.121P)2 + 0.7607P]
where P = (Fo2 + 2Fc2)/3
3238 reflections(Δ/σ)max < 0.001
226 parametersΔρmax = 0.97 e Å3
376 restraintsΔρmin = 1.22 e Å3
Special details top

Experimental. The elemental analyses were performed with PERKIN ELMER MODEL 2400 SERIES II.

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) top
xyzUiso*/Ueq
Sn10.53223 (7)0.19966 (3)0.14262 (5)0.0682 (3)
F10.3152 (7)0.0370 (3)0.2338 (5)0.1068 (19)
F20.1551 (7)0.1018 (3)0.3641 (6)0.1124 (19)
F30.1259 (6)0.0376 (3)0.5742 (6)0.1044 (18)
F40.2610 (7)0.0900 (3)0.6573 (5)0.1004 (18)
O10.4000 (6)0.1622 (3)0.2470 (4)0.0653 (13)
O20.5585 (7)0.0710 (3)0.2748 (5)0.0831 (16)
O30.5552 (6)0.1795 (3)0.5122 (5)0.0715 (14)
O40.3898 (7)0.2097 (3)0.6020 (5)0.0747 (15)
C10.4561 (10)0.0987 (5)0.2964 (7)0.0700 (14)
C20.3763 (9)0.0620 (4)0.3786 (6)0.0630 (15)
C30.3062 (9)0.0040 (4)0.3392 (7)0.0701 (16)
C40.2217 (9)0.0372 (4)0.4045 (7)0.0733 (17)
C50.2073 (9)0.0040 (5)0.5108 (8)0.0712 (16)
C60.2767 (9)0.0609 (4)0.5513 (7)0.0683 (16)
C70.3607 (8)0.0950 (4)0.4875 (6)0.0596 (15)
C80.4430 (10)0.1659 (4)0.5342 (7)0.0650 (15)
C90.7078 (11)0.2375 (6)0.2756 (10)0.098 (2)
H9A0.71050.29210.28100.118*
H9B0.71390.21630.35700.118*
C100.8273 (12)0.2053 (7)0.2183 (13)0.121 (3)
H10A0.81200.15210.19960.146*
H10B0.82630.23180.14180.146*
C110.9663 (12)0.2172 (8)0.3142 (14)0.139 (3)
H11A0.96940.18820.38880.167*
H11B0.97870.27010.33680.167*
C121.0845 (16)0.1906 (9)0.2558 (19)0.179 (6)
H12A1.17500.20260.31120.268*
H12B1.07420.21580.17750.268*
H12C1.07750.13710.24250.268*
C130.4925 (10)0.1354 (5)0.0233 (9)0.0896 (19)
H13A0.47030.16970.09380.108*
H13B0.57820.10880.02440.108*
C140.3719 (9)0.0775 (5)0.0410 (8)0.0891 (19)
H14A0.37140.04550.11170.107*
H14B0.38910.04570.03240.107*
C150.2331 (10)0.1137 (6)0.0617 (10)0.104 (2)
H15A0.21890.14820.13150.124*
H15B0.23170.14300.01150.124*
C160.1109 (12)0.0563 (8)0.0883 (12)0.140 (4)
H16A0.02290.08260.10210.210*
H16B0.12270.02310.01820.210*
H16C0.11130.02740.16110.210*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Sn10.0944 (5)0.0617 (4)0.0577 (4)0.0113 (3)0.0365 (3)0.0098 (2)
F10.178 (6)0.072 (3)0.071 (3)0.011 (3)0.034 (3)0.024 (2)
F20.127 (5)0.072 (3)0.120 (4)0.035 (3)0.003 (4)0.001 (3)
F30.101 (4)0.104 (4)0.121 (4)0.014 (3)0.050 (3)0.031 (3)
F40.153 (5)0.098 (4)0.072 (3)0.016 (3)0.067 (3)0.003 (3)
O10.091 (4)0.056 (3)0.054 (3)0.013 (3)0.030 (3)0.017 (2)
O20.109 (4)0.075 (3)0.079 (4)0.024 (3)0.048 (3)0.011 (3)
O30.082 (4)0.073 (3)0.064 (3)0.010 (3)0.027 (3)0.009 (3)
O40.101 (4)0.067 (3)0.063 (3)0.008 (3)0.035 (3)0.017 (2)
C10.099 (3)0.065 (3)0.052 (2)0.002 (3)0.030 (2)0.004 (2)
C20.090 (3)0.052 (3)0.047 (3)0.002 (3)0.018 (3)0.007 (2)
C30.096 (3)0.056 (3)0.055 (3)0.001 (3)0.016 (3)0.002 (3)
C40.093 (4)0.057 (3)0.063 (3)0.004 (3)0.009 (3)0.009 (3)
C50.089 (4)0.060 (3)0.065 (3)0.004 (3)0.022 (3)0.012 (3)
C60.091 (4)0.064 (3)0.054 (3)0.003 (3)0.025 (3)0.007 (3)
C70.086 (3)0.051 (3)0.043 (3)0.000 (3)0.019 (3)0.005 (2)
C80.093 (3)0.056 (3)0.050 (3)0.001 (3)0.025 (3)0.001 (3)
C90.112 (4)0.094 (4)0.089 (4)0.010 (4)0.027 (4)0.013 (4)
C100.133 (5)0.111 (5)0.114 (5)0.005 (4)0.021 (4)0.010 (4)
C110.146 (6)0.131 (6)0.130 (6)0.008 (5)0.020 (5)0.006 (5)
C120.148 (10)0.191 (11)0.184 (11)0.031 (9)0.021 (10)0.000 (9)
C130.116 (4)0.087 (4)0.071 (3)0.008 (4)0.036 (3)0.004 (3)
C140.119 (4)0.085 (4)0.063 (3)0.001 (4)0.023 (3)0.005 (3)
C150.128 (5)0.109 (5)0.074 (4)0.002 (4)0.027 (4)0.001 (4)
C160.150 (8)0.149 (7)0.105 (7)0.014 (7)0.009 (6)0.005 (6)
Geometric parameters (Å, º) top
Sn1—C92.061 (11)C9—H9A0.9700
Sn1—O12.075 (5)C9—H9B0.9700
Sn1—O4i2.100 (6)C10—C111.506 (14)
Sn1—C132.117 (9)C10—H10A0.9700
Sn1—O22.690 (5)C10—H10B0.9700
F1—C31.337 (9)C11—C121.553 (15)
F2—C41.335 (9)C11—H11A0.9700
F3—C51.343 (9)C11—H11B0.9700
F4—C61.335 (9)C12—H12A0.9600
O1—C11.308 (9)C12—H12B0.9600
O2—C11.204 (10)C12—H12C0.9600
O3—C81.219 (10)C13—C141.541 (11)
O4—C81.290 (10)C13—H13A0.9700
O4—Sn1ii2.100 (6)C13—H13B0.9700
C1—C21.506 (11)C14—C151.470 (11)
C2—C31.369 (11)C14—H14A0.9700
C2—C71.393 (10)C14—H14B0.9700
C3—C41.377 (12)C15—C161.543 (12)
C4—C51.365 (12)C15—H15A0.9700
C5—C61.352 (11)C15—H15B0.9700
C6—C71.370 (10)C16—H16A0.9600
C7—C81.510 (11)C16—H16B0.9600
C9—C101.589 (13)C16—H16C0.9600
C9—Sn1—O1103.5 (3)C11—C10—C9107.1 (10)
C9—Sn1—O4i106.7 (3)C11—C10—H10A110.3
O1—Sn1—O4i83.2 (2)C9—C10—H10A110.3
C9—Sn1—C13136.4 (4)C11—C10—H10B110.3
O1—Sn1—C13108.8 (3)C9—C10—H10B110.3
O4i—Sn1—C13105.6 (3)H10A—C10—H10B108.6
C9—Sn1—O286.8 (3)C10—C11—C12107.5 (12)
O1—Sn1—O253.40 (19)C10—C11—H11A110.2
O4i—Sn1—O2136.6 (2)C12—C11—H11A110.2
C13—Sn1—O289.4 (3)C10—C11—H11B110.2
C1—O1—Sn1104.7 (5)C12—C11—H11B110.2
C1—O2—Sn178.6 (4)H11A—C11—H11B108.5
C8—O4—Sn1ii103.5 (6)C11—C12—H12A109.5
O2—C1—O1123.2 (7)C11—C12—H12B109.5
O2—C1—C2123.2 (7)H12A—C12—H12B109.5
O1—C1—C2113.5 (7)C11—C12—H12C109.5
C3—C2—C7118.2 (7)H12A—C12—H12C109.5
C3—C2—C1118.4 (7)H12B—C12—H12C109.5
C7—C2—C1123.1 (7)C14—C13—Sn1115.1 (6)
F1—C3—C2120.5 (7)C14—C13—H13A108.5
F1—C3—C4118.1 (7)Sn1—C13—H13A108.5
C2—C3—C4121.4 (7)C14—C13—H13B108.5
F2—C4—C5120.4 (8)Sn1—C13—H13B108.5
F2—C4—C3120.0 (8)H13A—C13—H13B107.5
C5—C4—C3119.6 (8)C15—C14—C13112.4 (8)
F3—C5—C6121.4 (8)C15—C14—H14A109.1
F3—C5—C4118.9 (8)C13—C14—H14A109.1
C6—C5—C4119.7 (8)C15—C14—H14B109.1
F4—C6—C5117.1 (7)C13—C14—H14B109.1
F4—C6—C7121.3 (7)H14A—C14—H14B107.9
C5—C6—C7121.6 (7)C14—C15—C16112.7 (9)
C6—C7—C2119.4 (7)C14—C15—H15A109.1
C6—C7—C8122.2 (7)C16—C15—H15A109.1
C2—C7—C8118.3 (7)C14—C15—H15B109.1
O3—C8—O4122.3 (7)C16—C15—H15B109.1
O3—C8—C7121.7 (7)H15A—C15—H15B107.8
O4—C8—C7116.0 (8)C15—C16—H16A109.5
C10—C9—Sn199.4 (7)C15—C16—H16B109.5
C10—C9—H9A111.9H16A—C16—H16B109.5
Sn1—C9—H9A111.9C15—C16—H16C109.5
C10—C9—H9B111.9H16A—C16—H16C109.5
Sn1—C9—H9B111.9H16B—C16—H16C109.5
H9A—C9—H9B109.6
Symmetry codes: (i) x, y+1/2, z1/2; (ii) x, y+1/2, z+1/2.
 

Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds