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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Dec 11;67(Pt 1):m56. doi: 10.1107/S1600536810050713

Butyl­trichlorido{2-[(diisopropyl­ammonio)­meth­yl]phen­yl}tin(IV) dichloro­methane monosolvate

Adina Rotar a,*, Richard A Varga a, Malgorzata Staninska a
PMCID: PMC3050250  PMID: 21522574

Abstract

The title compound, [Sn(C4H9)(C13H21N)Cl3]·CH2Cl2, was obtained by recrystallization of [2-(diisopropyl­amino­meth­yl)phen­yl]tin(IV) butyl dichloride from a CH2Cl2/n-hexane mixture (1:4 v/v) in the presence of ambient moisture. Partial hydrolysis led to the title compound, the hydro­chloric acid adduct of the dichloride, having a penta­coordinated Sn atom with a trigonal–bipyramidal C2SnCl3 core. The N atom of the 2-[(diisopropyl­ammonio)­meth­yl]phenyl ligand forms a strong intra­molecular N—H⋯Cl hydrogen bond, resulting in a zwitterionic species, [2-(iPr2HN+CH2)C6H4]SnBuCl3 −·CH2Cl2. Disorder was found in the n-butyl group, which was refined as disordered over three positions, with site occupancies of 0.22 (1), 0.51 (1) and 0.27 (2).

Related literature

For related tin(IV) compounds, see: Varga et al. (2001 ▶, 2005 ▶, 2006 ▶); Varga & Silvestru (2007 ▶); Rotar et al. (2007 ▶, 2009 ▶); Rotar, Schuermann et al. (2008 ▶); Rotar, Varga & Silvestru (2008 ▶); Švec et al. (2010 ▶).graphic file with name e-67-00m56-scheme1.jpg

Experimental

Crystal data

  • [Sn(C4H9)(C13H21N)Cl3]·CH2Cl2

  • M r = 558.39

  • Triclinic, Inline graphic

  • a = 10.654 (8) Å

  • b = 11.093 (9) Å

  • c = 12.406 (10) Å

  • α = 115.594 (13)°

  • β = 100.767 (15)°

  • γ = 97.176 (15)°

  • V = 1263.5 (17) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 1.54 mm−1

  • T = 297 K

  • 0.45 × 0.20 × 0.18 mm

Data collection

  • Bruker SMART APEX CCD area-detector diffractometer

  • Absorption correction: multi-scan (Bruker, 2000 ▶) T min = 0.544, T max = 0.769

  • 9126 measured reflections

  • 4416 independent reflections

  • 3122 reflections with I > 2σ(I)

  • R int = 0.074

Refinement

  • R[F 2 > 2σ(F 2)] = 0.076

  • wR(F 2) = 0.213

  • S = 1.02

  • 4416 reflections

  • 257 parameters

  • 40 restraints

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 1.43 e Å−3

  • Δρmin = −0.73 e Å−3

Data collection: SMART (Bruker, 2000 ▶); cell refinement: SAINT-Plus (Bruker, 2001 ▶); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: DIAMOND (Brandenburg & Putz, 2006 ▶); software used to prepare material for publication: publCIF (Westrip, 2010 ▶).

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810050713/zl2332sup1.cif

e-67-00m56-sup1.cif (26.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810050713/zl2332Isup2.hkl

e-67-00m56-Isup2.hkl (216.3KB, hkl)

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

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A D⋯A D—H⋯A
N1—H1⋯Cl2 0.86 (1) 2.37 (7) 3.208 (8) 165 (8)

Acknowledgments

This work was supported by the Romanian Ministry of Education and Research (PD 443/2010/AR). AR gratefully acknowledges the assistance of PhD student Ioana Barbul and Dr Ciprian Raţ in the two-dimensional NMR experiments. We thank the National Center for X-ray Diffraction (Babes-Bolyai University, Cluj-Napoca) collecting the diffraction data.

supplementary crystallographic information

Comment

During our work on hypercoordinated organotin(IV) compounds with [2-(R2NCH2)C6H4]Sn fragments (Varga et al., 2001, 2005, 2006, Rotar et al., 2007, 2008, 2009) the title compound was isolated.

In an attempt to obtain single-crystals of the dichloride [2-(iPr2NCH2)C6H4]SnBuCl2 (1), recrystallization from a CH2Cl2/n-hexane mixture (1:4) in the presence of air afforded the HCl adduct 1.HCl.CH2Cl2. The nitrogen atom of the LCN ligand [LCN = 2-(diisopropylaminomethyl)phenyl] is protonated and a new Sn—Cl bond is simultaneously formed, thus leading to the formation of a zwitterionic species, [2-(iPr2HN+CH2)C6H4]SnBuCl3–.CH2Cl2. The presence of the HCl is probably due to partial hydrolysis of the diorganotin(IV) dihalide in the presence of ambient moisture from air.

The central tin atom is pentacoordinated with a distorted trigonal bipyramidal geometry (Fig. 1). The axial positions are occupied by two chlorine atoms [Cl1—Sn1—Cl2 = 178.50 (7)°], while the two carbon atoms from the two organic groups and a chlorine atom are placed in equatorial positions. The angles in the equatorial C2SnCl system are situated in the range between 97.4 (13) and 145.8 (14) °, showing a strong deviation from the ideal value of 120°. The Cl2 atom forms a strong intramolecular hydrogen bond with H1 from the nitrogen atom [Cl2···H1 = 2.37 (7) Å].

Disorder was found in the n-butyl group. This was resolved over three positions with the components of the disorder having site a occupancy ratio of 0.21 (1):0.51 (2):0.27 (2) (see Refinement section; Fig. 2).

Experimental

A solution of BuLi in hexane (10.5 ml, 1.6M, 20% excess) was added dropwise to a stirred solution of 2-(N,N-diisopropylaminomethyl)benzene bromide (3.7 g, 13.7 mmol) in 100 ml of anhydrous hexane at room temperature under argon using Schlenk techniques. The reaction mixture was refluxed under stirring for four hours and then allowed to reach room temperature. The obtained liquid product was added dropwise under stirring to a cooled (195 K, -78°C) solution of BuSnCl3 (1.8 ml, 11 mmol) in 50 ml of anhydrous hexane. After the organolithiun compound was added, the reaction mixture was stirred for 1 h at 195 K (-78°C), then overnight to reach room temperature. The solvent was removed in vacuo. The oily residue was recrystallized from CH2Cl2/n-hexane, in presence of air moisture, resulting in the isolation of [2-(iPr2HN+CH2)C6H4]SnBuCl3–. CH2Cl2 (1.67 g, 32.9%).

1H NMR (300 MHz, CDCl3, 293.5K): 0.98 t (3H, SnCH2CH2CH2CH3, 3JHH = 7.3 Hz), 1.28 d (6HA, NCH(CH3)2, 3JHH = 6.7 Hz), 1.47 d (6HB, NCH(CH3)2, 3JHH = 6.8 Hz), 1.52 s (2H, SnCH2CH2CH2CH3, 3JHH = 7.4 Hz), 2.01 quin (2H, SnCH2CH2CH2CH3, 3JHH = 8.2 Hz), 2.23 t (2H, SnCH2CH2CH2CH3, 3JHH = 8.1, 2JSnH = 81.4 Hz), 3.50 H (2H, NCH(CH3)2, 3JHH = 6.5 Hz), 3.96 d (2H, –CH2–, 3JHH = 4.3 Hz), 7.49m (2H, H4,5, C6H4), 7.65m (1H, H3, C6H4), 7.71m (1H, H6, C6H4), 9.22 s,br (1H, NH).

13C NMR (75.4 MHz, CDCl3, 293.5K): 13.68 s (SnCH2CH2CH2CH3, 4JSnC = 7.8 Hz), 18.73 s (NCH(CH3)2 [B]), 19.11 s (NCH(CH3)2 [A]), 25.95 s (SnCH2CH2CH2CH3, 3JSnC = 130.6 Hz), 27.47 s (SnCH2CH2CH2CH3, 2JSnC = 51.1 Hz), 37.40 s,br (SnCH2CH2CH2CH3), 51.07 s (-CH2–), 52.90 s (NCH(CH3)2), 129.71 s (C5, C6H4, 3JSnC 51.1 = Hz), 129.86 s (C4, C6H4, 4JSnC = 16.3 Hz), 132.15 s (C1, C6H4), 134.77 s (C3, C6H4, 3JSnC = 61.8 Hz), 136.11 s (C6, C6H4, 2JSnC = 80.1 Hz), 154.98 s (C2, C6H4).

Refinement

All hydrogen atoms were placed in calculated positions using a riding model, with C—H = 0.93–0.98 Å and with Uiso= 1.2 or 1.5Ueq (C) for H. The methyl groups were allowed to rotate but not to tip. The H1 atom bonded to N1 was found in a difference map and refined with a restrained N—H distance of 0.86 (1) Å.

The n-butyl group was found to be severly disordered. Attempts to refine the chain as disordered over two moieties (with appropriate distance restraints for the C—C bonds) did not give satisfactory results with ADPs of neighboring atoms being icompatible even after application of severe restraints for the thermal ellipsoids. Disorder over three moieties allowed to avoid these problems. In the final refinement the butyl chain was refined as disordered over three sites with equivalent bonds from the disordered components restrained to have similar lengths length. The same Uij parameters were used for atom C14/C14B/C14C, C15/C15B/C15C, C16/C16B/C16C and C17/C17B/C17C, leading to refined site occupancies of 0.21 (1):0.51 (2):0.27 (2).

Figures

Fig. 1.

Fig. 1.

View of the title compound showing the atom-numbering scheme and the intramolecular hydrogen bond (black dashed line) with only the major component for the disordered n-butyl group. Displacement ellipsoids are drawn at the 30% probability level and H atoms as spheres of arbitrary radii.

Fig. 2.

Fig. 2.

View of the disordered n-butyl group showing the atom-numbering scheme (major component with grey and the two minor components with white). Displacement ellipsoids are drawn at the 30% probability level (H atoms were omitted for clarity).

Crystal data

[Sn(C4H9)(C13H21N)Cl3]·CH2Cl2 Z = 2
Mr = 558.39 F(000) = 564
Triclinic, P1 Dx = 1.468 Mg m−3
Hall symbol: -p 1 Mo Kα radiation, λ = 0.71073 Å
a = 10.654 (8) Å Cell parameters from 1665 reflections
b = 11.093 (9) Å θ = 2.4–20.1°
c = 12.406 (10) Å µ = 1.54 mm−1
α = 115.594 (13)° T = 297 K
β = 100.767 (15)° Block, colourless
γ = 97.176 (15)° 0.45 × 0.20 × 0.18 mm
V = 1263.5 (17) Å3

Data collection

Bruker SMART APEX CCD area-detector diffractometer 4416 independent reflections
Radiation source: fine-focus sealed tube 3122 reflections with I > 2σ(I)
graphite Rint = 0.074
phi and ω scans θmax = 25.0°, θmin = 2.0°
Absorption correction: multi-scan (Bruker, 2000) h = −12→12
Tmin = 0.544, Tmax = 0.769 k = −13→13
9126 measured reflections l = −14→14

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)] = 0.076 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.213 H atoms treated by a mixture of independent and constrained refinement
S = 1.02 w = 1/[σ2(Fo2) + (0.1038P)2 + 0.0754P] where P = (Fo2 + 2Fc2)/3
4416 reflections (Δ/σ)max = 0.008
257 parameters Δρmax = 1.43 e Å−3
40 restraints Δρmin = −0.73 e Å−3

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 Occ. (<1)
C1 0.4960 (8) 0.7632 (8) 0.8171 (7) 0.0490 (19)
C2 0.4078 (8) 0.8089 (8) 0.8876 (7) 0.052 (2)
C3 0.4102 (10) 0.7820 (10) 0.9900 (7) 0.068 (3)
H3 0.3545 0.8145 1.0401 0.082*
C4 0.4950 (11) 0.7076 (11) 1.0147 (9) 0.079 (3)
H4 0.4942 0.6882 1.0804 0.095*
C5 0.5813 (11) 0.6613 (11) 0.9442 (10) 0.080 (3)
H5 0.6392 0.6124 0.9626 0.096*
C6 0.5798 (10) 0.6891 (10) 0.8458 (9) 0.070 (3)
H6 0.6369 0.6570 0.7973 0.084*
C7 0.3141 (8) 0.8942 (8) 0.8704 (7) 0.054 (2)
H7A 0.3545 0.9547 0.8424 0.065*
H7B 0.2999 0.9514 0.9501 0.065*
C8 0.1153 (9) 0.6964 (9) 0.7985 (8) 0.061 (2)
H8 0.1822 0.6500 0.8175 0.073*
C9 0.0569 (11) 0.7551 (12) 0.9098 (10) 0.093 (3)
H9A 0.1267 0.8024 0.9852 0.139*
H9B 0.0012 0.6814 0.9118 0.139*
H9C 0.0064 0.8181 0.9019 0.139*
C10 0.0112 (9) 0.5909 (11) 0.6802 (9) 0.084 (3)
H10A −0.0587 0.6325 0.6632 0.126*
H10B −0.0232 0.5140 0.6910 0.126*
H10C 0.0501 0.5602 0.6119 0.126*
C11 0.0904 (9) 0.8991 (10) 0.7562 (8) 0.067 (2)
H11 0.0007 0.8537 0.7457 0.080*
C12 0.1211 (12) 1.0427 (11) 0.8664 (10) 0.098 (4)
H12A 0.1148 1.0351 0.9395 0.147*
H12B 0.0593 1.0926 0.8498 0.147*
H12C 0.2084 1.0905 0.8791 0.147*
C13 0.0929 (13) 0.9059 (15) 0.6384 (10) 0.109 (4)
H13A 0.0260 0.9499 0.6199 0.163*
H13B 0.0769 0.8145 0.5716 0.163*
H13C 0.1773 0.9575 0.6483 0.163*
C14 0.571 (6) 0.712 (5) 0.490 (3) 0.065 (6) 0.22
H14A 0.5530 0.6136 0.4589 0.078* 0.22
H14B 0.5079 0.7296 0.4342 0.078* 0.22
C15 0.702 (6) 0.754 (8) 0.477 (7) 0.089 (8) 0.22
H15A 0.7620 0.7795 0.5565 0.107* 0.22
H15B 0.7010 0.8400 0.4735 0.107* 0.22
C16 0.772 (6) 0.681 (6) 0.384 (5) 0.124 (10) 0.22
H16A 0.8528 0.7432 0.3967 0.148* 0.22
H16B 0.7955 0.6044 0.3948 0.148* 0.22
C17 0.686 (9) 0.632 (10) 0.258 (7) 0.127 (10) 0.22
H17A 0.6103 0.6701 0.2635 0.191* 0.22
H17B 0.6587 0.5331 0.2181 0.191* 0.22
H17C 0.7333 0.6591 0.2105 0.191* 0.22
C14B 0.587 (10) 0.664 (4) 0.511 (7) 0.065 (6) 0.51
H14C 0.6522 0.6240 0.5402 0.078* 0.51
H14D 0.5129 0.5900 0.4515 0.078* 0.51
C15B 0.644 (4) 0.733 (3) 0.446 (3) 0.089 (8) 0.51
H15C 0.7198 0.8063 0.5038 0.107* 0.51
H15D 0.5797 0.7743 0.4161 0.107* 0.51
C16B 0.684 (4) 0.634 (3) 0.340 (4) 0.124 (10) 0.51
H16C 0.7401 0.5852 0.3687 0.148* 0.51
H16D 0.6065 0.5662 0.2783 0.148* 0.51
C17B 0.755 (3) 0.699 (4) 0.280 (3) 0.127 (10) 0.51
H17D 0.6927 0.7125 0.2216 0.191* 0.51
H17E 0.8077 0.6408 0.2368 0.191* 0.51
H17F 0.8104 0.7862 0.3418 0.191* 0.51
C14C 0.600 (19) 0.687 (6) 0.512 (13) 0.065 (6) 0.27
H14E 0.6634 0.6401 0.5342 0.078* 0.27
H14F 0.5301 0.6190 0.4404 0.078* 0.27
C15C 0.663 (7) 0.794 (6) 0.486 (5) 0.089 (8) 0.27
H15E 0.7464 0.8457 0.5474 0.107* 0.27
H15F 0.6072 0.8569 0.4877 0.107* 0.27
C16C 0.685 (6) 0.724 (4) 0.360 (5) 0.124 (10) 0.27
H16E 0.6005 0.6957 0.3002 0.148* 0.27
H16F 0.7398 0.7924 0.3497 0.148* 0.27
C17C 0.744 (8) 0.603 (6) 0.324 (7) 0.127 (10) 0.27
H17G 0.6755 0.5202 0.2812 0.191* 0.27
H17H 0.7975 0.6054 0.3965 0.191* 0.27
H17I 0.7974 0.6042 0.2696 0.191* 0.27
C18 0.7688 (13) 0.2311 (16) 0.7029 (15) 0.131 (6)
H18A 0.7283 0.1506 0.7073 0.157*
H18B 0.7266 0.2221 0.6226 0.157*
Cl1 0.75445 (19) 0.9363 (2) 0.79244 (19) 0.0594 (6)
Cl2 0.2839 (2) 0.6520 (2) 0.5385 (2) 0.0644 (6)
Cl3 0.4604 (2) 0.9945 (2) 0.65829 (19) 0.0549 (5)
Cl4 0.7400 (7) 0.3745 (6) 0.8168 (7) 0.234 (4)
Cl5 0.9241 (6) 0.2338 (7) 0.7127 (7) 0.214 (3)
N1 0.1814 (7) 0.8103 (7) 0.7781 (6) 0.0557 (18)
H1 0.197 (8) 0.773 (8) 0.707 (4) 0.067*
Sn1 0.52253 (6) 0.79582 (6) 0.66440 (5) 0.0525 (3)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.039 (5) 0.055 (5) 0.045 (4) 0.004 (4) 0.005 (4) 0.020 (4)
C2 0.043 (5) 0.055 (5) 0.047 (4) 0.010 (4) 0.004 (4) 0.017 (4)
C3 0.069 (6) 0.091 (7) 0.047 (5) 0.012 (5) 0.016 (4) 0.035 (5)
C4 0.096 (8) 0.100 (8) 0.074 (6) 0.043 (7) 0.026 (6) 0.064 (6)
C5 0.081 (8) 0.090 (7) 0.090 (7) 0.035 (6) 0.004 (6) 0.063 (6)
C6 0.072 (7) 0.070 (6) 0.076 (6) 0.035 (5) 0.025 (5) 0.034 (5)
C7 0.044 (5) 0.058 (5) 0.043 (4) 0.011 (4) 0.010 (4) 0.009 (4)
C8 0.047 (5) 0.066 (5) 0.067 (5) 0.005 (4) 0.019 (4) 0.029 (5)
C9 0.075 (8) 0.103 (8) 0.086 (7) −0.008 (6) 0.015 (6) 0.042 (7)
C10 0.052 (6) 0.086 (7) 0.078 (7) −0.007 (5) 0.005 (5) 0.017 (6)
C11 0.045 (5) 0.077 (6) 0.080 (6) 0.020 (5) 0.017 (5) 0.037 (5)
C12 0.094 (9) 0.075 (7) 0.100 (8) 0.049 (6) 0.010 (7) 0.017 (6)
C13 0.110 (10) 0.158 (12) 0.091 (8) 0.076 (9) 0.029 (7) 0.075 (9)
C14 0.087 (17) 0.046 (13) 0.066 (7) 0.035 (16) 0.034 (9) 0.019 (12)
C15 0.09 (2) 0.09 (2) 0.062 (19) 0.00 (2) 0.042 (19) 0.004 (15)
C16 0.15 (3) 0.081 (18) 0.16 (2) 0.004 (19) 0.10 (2) 0.06 (2)
C17 0.16 (3) 0.14 (3) 0.095 (16) 0.04 (2) 0.038 (18) 0.060 (18)
C14B 0.087 (17) 0.046 (13) 0.066 (7) 0.035 (16) 0.034 (9) 0.019 (12)
C15B 0.09 (2) 0.09 (2) 0.062 (19) 0.00 (2) 0.042 (19) 0.004 (15)
C16B 0.15 (3) 0.081 (18) 0.16 (2) 0.004 (19) 0.10 (2) 0.06 (2)
C17B 0.16 (3) 0.14 (3) 0.095 (16) 0.04 (2) 0.038 (18) 0.060 (18)
C14C 0.087 (17) 0.046 (13) 0.066 (7) 0.035 (16) 0.034 (9) 0.019 (12)
C15C 0.09 (2) 0.09 (2) 0.062 (19) 0.00 (2) 0.042 (19) 0.004 (15)
C16C 0.15 (3) 0.081 (18) 0.16 (2) 0.004 (19) 0.10 (2) 0.06 (2)
C17C 0.16 (3) 0.14 (3) 0.095 (16) 0.04 (2) 0.038 (18) 0.060 (18)
C18 0.094 (10) 0.156 (13) 0.208 (16) 0.038 (9) 0.044 (10) 0.139 (13)
Cl1 0.0326 (11) 0.0740 (13) 0.0603 (12) 0.0032 (10) 0.0069 (9) 0.0261 (11)
Cl2 0.0525 (14) 0.0652 (13) 0.0581 (12) 0.0074 (11) 0.0045 (10) 0.0194 (11)
Cl3 0.0529 (13) 0.0512 (11) 0.0716 (13) 0.0172 (10) 0.0157 (10) 0.0374 (10)
Cl4 0.316 (10) 0.177 (5) 0.300 (8) 0.125 (6) 0.220 (8) 0.120 (5)
Cl5 0.163 (5) 0.303 (7) 0.364 (8) 0.147 (5) 0.150 (5) 0.264 (7)
N1 0.045 (4) 0.066 (4) 0.052 (4) 0.016 (4) 0.016 (3) 0.022 (4)
Sn1 0.0492 (4) 0.0576 (4) 0.0541 (4) 0.0190 (3) 0.0164 (3) 0.0262 (3)

Geometric parameters (Å, °)

C1—C6 1.385 (12) C15—H15B 0.9700
C1—C2 1.396 (11) C16—C17 1.48 (2)
C1—Sn1 2.137 (8) C16—H16A 0.9700
C2—C3 1.421 (11) C16—H16B 0.9700
C2—C7 1.506 (12) C17—H17A 0.9600
C3—C4 1.376 (13) C17—H17B 0.9600
C3—H3 0.9300 C17—H17C 0.9600
C4—C5 1.380 (14) C14B—C15B 1.483 (18)
C4—H4 0.9300 C14B—Sn1 2.137 (12)
C5—C6 1.380 (13) C14B—H14C 0.9700
C5—H5 0.9300 C14B—H14D 0.9700
C6—H6 0.9300 C15B—C16B 1.490 (18)
C7—N1 1.524 (11) C15B—H15C 0.9700
C7—H7A 0.9700 C15B—H15D 0.9700
C7—H7B 0.9700 C16B—C17B 1.479 (18)
C8—N1 1.509 (11) C16B—H16C 0.9700
C8—C10 1.529 (12) C16B—H16D 0.9700
C8—C9 1.537 (14) C17B—H17D 0.9600
C8—H8 0.9800 C17B—H17E 0.9600
C9—H9A 0.9600 C17B—H17F 0.9600
C9—H9B 0.9600 C14C—C15C 1.48 (2)
C9—H9C 0.9600 C14C—Sn1 2.139 (16)
C10—H10A 0.9600 C14C—H14E 0.9700
C10—H10B 0.9600 C14C—H14F 0.9700
C10—H10C 0.9600 C15C—C16C 1.49 (2)
C11—C13 1.500 (13) C15C—H15E 0.9700
C11—C12 1.527 (13) C15C—H15F 0.9700
C11—N1 1.535 (11) C16C—C17C 1.48 (2)
C11—H11 0.9800 C16C—H16E 0.9700
C12—H12A 0.9600 C16C—H16F 0.9700
C12—H12B 0.9600 C17C—H17G 0.9600
C12—H12C 0.9600 C17C—H17H 0.9600
C13—H13A 0.9600 C17C—H17I 0.9600
C13—H13B 0.9600 C18—Cl5 1.632 (14)
C13—H13C 0.9600 C18—Cl4 1.721 (16)
C14—C15 1.481 (19) C18—H18A 0.9700
C14—Sn1 2.141 (18) C18—H18B 0.9700
C14—H14A 0.9700 Cl1—Sn1 2.547 (3)
C14—H14B 0.9700 Cl2—Sn1 2.608 (3)
C15—C16 1.485 (19) Cl3—Sn1 2.406 (3)
C15—H15A 0.9700 N1—H1 0.857 (10)
C6—C1—C2 119.4 (8) H17B—C17—H17C 109.5
C6—C1—Sn1 113.1 (6) C15B—C14B—Sn1 114.6 (19)
C2—C1—Sn1 127.5 (6) C15B—C14B—H14C 108.6
C1—C2—C3 118.7 (8) Sn1—C14B—H14C 108.6
C1—C2—C7 125.5 (8) C15B—C14B—H14D 108.6
C3—C2—C7 115.7 (8) Sn1—C14B—H14D 108.6
C4—C3—C2 119.8 (9) H14C—C14B—H14D 107.6
C4—C3—H3 120.1 C14B—C15B—C16B 111 (2)
C2—C3—H3 120.1 C14B—C15B—H15C 109.5
C3—C4—C5 121.5 (9) C16B—C15B—H15C 109.5
C3—C4—H4 119.3 C14B—C15B—H15D 109.5
C5—C4—H4 119.3 C16B—C15B—H15D 109.5
C6—C5—C4 118.5 (9) H15C—C15B—H15D 108.1
C6—C5—H5 120.7 C17B—C16B—C15B 113 (3)
C4—C5—H5 120.7 C17B—C16B—H16C 108.9
C5—C6—C1 122.1 (9) C15B—C16B—H16C 108.9
C5—C6—H6 119.0 C17B—C16B—H16D 108.9
C1—C6—H6 119.0 C15B—C16B—H16D 108.9
C2—C7—N1 114.1 (7) H16C—C16B—H16D 107.7
C2—C7—H7A 108.7 C16B—C17B—H17D 109.5
N1—C7—H7A 108.7 C16B—C17B—H17E 109.5
C2—C7—H7B 108.7 H17D—C17B—H17E 109.5
N1—C7—H7B 108.7 C16B—C17B—H17F 109.5
H7A—C7—H7B 107.6 H17D—C17B—H17F 109.5
N1—C8—C10 110.1 (7) H17E—C17B—H17F 109.5
N1—C8—C9 110.6 (8) C15C—C14C—Sn1 105 (3)
C10—C8—C9 111.8 (8) C15C—C14C—H14E 110.8
N1—C8—H8 108.1 Sn1—C14C—H14E 110.8
C10—C8—H8 108.1 C15C—C14C—H14F 110.9
C9—C8—H8 108.1 Sn1—C14C—H14F 110.9
C8—C9—H9A 109.5 H14E—C14C—H14F 108.9
C8—C9—H9B 109.5 C14C—C15C—C16C 108 (4)
H9A—C9—H9B 109.5 C14C—C15C—H15E 110.2
C8—C9—H9C 109.5 C16C—C15C—H15E 110.2
H9A—C9—H9C 109.5 C14C—C15C—H15F 110.1
H9B—C9—H9C 109.5 C16C—C15C—H15F 110.1
C8—C10—H10A 109.5 H15E—C15C—H15F 108.5
C8—C10—H10B 109.5 C17C—C16C—C15C 121 (5)
H10A—C10—H10B 109.5 C17C—C16C—H16E 107.0
C8—C10—H10C 109.5 C15C—C16C—H16E 107.0
H10A—C10—H10C 109.5 C17C—C16C—H16F 107.0
H10B—C10—H10C 109.5 C15C—C16C—H16F 107.0
C13—C11—C12 111.4 (10) H16E—C16C—H16F 106.8
C13—C11—N1 110.8 (8) C16C—C17C—H17G 109.5
C12—C11—N1 112.6 (7) C16C—C17C—H17H 109.5
C13—C11—H11 107.2 H17G—C17C—H17H 109.5
C12—C11—H11 107.2 C16C—C17C—H17I 109.5
N1—C11—H11 107.2 H17G—C17C—H17I 109.5
C11—C12—H12A 109.5 H17H—C17C—H17I 109.5
C11—C12—H12B 109.5 Cl5—C18—Cl4 114.1 (10)
H12A—C12—H12B 109.5 Cl5—C18—H18A 108.7
C11—C12—H12C 109.5 Cl4—C18—H18A 108.7
H12A—C12—H12C 109.5 Cl5—C18—H18B 108.7
H12B—C12—H12C 109.5 Cl4—C18—H18B 108.7
C11—C13—H13A 109.5 H18A—C18—H18B 107.6
C11—C13—H13B 109.5 C8—N1—C7 114.9 (7)
H13A—C13—H13B 109.5 C8—N1—C11 114.1 (7)
C11—C13—H13C 109.5 C7—N1—C11 113.3 (7)
H13A—C13—H13C 109.5 C8—N1—H1 108 (6)
H13B—C13—H13C 109.5 C7—N1—H1 105 (6)
C15—C14—Sn1 123 (4) C11—N1—H1 100 (6)
C15—C14—H14A 106.6 C14B—Sn1—C1 126.9 (17)
Sn1—C14—H14A 106.6 C14B—Sn1—C14C 7(3)
C15—C14—H14B 106.6 C1—Sn1—C14C 132 (3)
Sn1—C14—H14B 106.6 C14B—Sn1—C14 19 (2)
H14A—C14—H14B 106.5 C1—Sn1—C14 145.8 (14)
C14—C15—C16 132 (5) C14C—Sn1—C14 15 (5)
C14—C15—H15A 104.4 C14B—Sn1—Cl3 116.5 (18)
C16—C15—H15A 104.4 C1—Sn1—Cl3 116.5 (2)
C14—C15—H15B 104.4 C14C—Sn1—Cl3 111 (3)
C16—C15—H15B 104.4 C14—Sn1—Cl3 97.4 (13)
H15A—C15—H15B 105.6 C14B—Sn1—Cl1 93 (3)
C17—C16—C15 109 (7) C1—Sn1—Cl1 89.0 (2)
C17—C16—H16A 109.9 C14C—Sn1—Cl1 89 (5)
C15—C16—H16A 109.9 C14—Sn1—Cl1 95.1 (16)
C15—C16—H16B 109.9 Cl3—Sn1—Cl1 90.96 (9)
H16A—C16—H16B 108.3 C14B—Sn1—Cl2 88 (3)
C16—C17—H17A 109.5 C1—Sn1—Cl2 89.5 (2)
C16—C17—H17B 109.5 C14C—Sn1—Cl2 92 (5)
H17A—C17—H17B 109.5 C14—Sn1—Cl2 86.3 (16)
C16—C17—H17C 109.5 Cl3—Sn1—Cl2 89.46 (9)
H17A—C17—H17C 109.5 Cl1—Sn1—Cl2 178.50 (7)
C6—C1—C2—C3 2.3 (12) C15B—C14B—Sn1—C1 −158 (5)
Sn1—C1—C2—C3 −176.8 (6) C15B—C14B—Sn1—C14 29 (6)
C6—C1—C2—C7 177.9 (8) C15B—C14B—Sn1—Cl3 26 (8)
Sn1—C1—C2—C7 −1.2 (12) C15B—C14B—Sn1—Cl1 −67 (7)
C1—C2—C3—C4 −2.4 (13) C15B—C14B—Sn1—Cl2 114 (7)
C7—C2—C3—C4 −178.4 (9) C6—C1—Sn1—C14B 30 (4)
C2—C3—C4—C5 1.8 (16) C2—C1—Sn1—C14B −151 (4)
C3—C4—C5—C6 −1.0 (17) C6—C1—Sn1—C14C 24 (7)
C4—C5—C6—C1 0.9 (16) C2—C1—Sn1—C14C −157 (7)
C2—C1—C6—C5 −1.5 (14) C6—C1—Sn1—C14 34 (3)
Sn1—C1—C6—C5 177.7 (8) C2—C1—Sn1—C14 −147 (3)
C1—C2—C7—N1 88.7 (10) C6—C1—Sn1—Cl3 −154.2 (6)
C3—C2—C7—N1 −95.6 (8) C2—C1—Sn1—Cl3 25.0 (8)
Sn1—C14—C15—C16 154 (8) C6—C1—Sn1—Cl1 −63.6 (6)
C14—C15—C16—C17 52 (13) C2—C1—Sn1—Cl1 115.5 (7)
Sn1—C14B—C15B—C16B −179 (5) C6—C1—Sn1—Cl2 116.6 (6)
C14B—C15B—C16B—C17B −174 (6) C2—C1—Sn1—Cl2 −64.2 (7)
Sn1—C14C—C15C—C16C −164 (7) C15C—C14C—Sn1—C1 −147 (7)
C14C—C15C—C16C—C17C −47 (12) C15C—C14C—Sn1—C14 54 (9)
C10—C8—N1—C7 −160.6 (7) C15C—C14C—Sn1—Cl3 31 (13)
C9—C8—N1—C7 75.3 (9) C15C—C14C—Sn1—Cl1 −60 (11)
C10—C8—N1—C11 66.2 (9) C15C—C14C—Sn1—Cl2 121 (11)
C9—C8—N1—C11 −57.9 (10) C15—C14—Sn1—C14B −91 (12)
C2—C7—N1—C8 49.8 (9) C15—C14—Sn1—C1 −101 (6)
C2—C7—N1—C11 −176.6 (7) C15—C14—Sn1—C14C −72 (18)
C13—C11—N1—C8 −126.3 (9) C15—C14—Sn1—Cl3 86 (6)
C12—C11—N1—C8 108.2 (9) C15—C14—Sn1—Cl1 −5(6)
C13—C11—N1—C7 99.7 (9) C15—C14—Sn1—Cl2 175 (6)
C12—C11—N1—C7 −25.8 (11)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1···Cl2 0.86 (1) 2.37 (7) 3.208 (8) 165 (8)

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: ZL2332).

References

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  2. Bruker (2000). SMART and SADABS Bruker AXS Inc., Madison, Wisconsin, USA.
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  10. Varga, R. A., Rotar, A., Schuermann, M., Jurkschat, K. & Silvestru, C. (2006). Eur. J. Inorg. Chem. 7, 1475–1486.
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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810050713/zl2332sup1.cif

e-67-00m56-sup1.cif (26.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810050713/zl2332Isup2.hkl

e-67-00m56-Isup2.hkl (216.3KB, 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

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