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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2013 Sep 28;69(Pt 10):m562–m563. doi: 10.1107/S1600536813026172

Tetra­butyl­ammonium butyl­tetra­chlorido­stannate(IV)

Tidiane Diop a,*, Arie van der Lee b, Libasse Diop a
PMCID: PMC3790365  PMID: 24098187

Abstract

In the title compound, [N(C4H9)4][Sn(C4H9)Cl4], the SnIV atom of the stannate anion has a trigonal-bipyramidal coordination sphere by two Cl atoms and one butyl chain in the equatorial plane and by two Cl atoms in the apical positions. Two of the four butyl chains of the tetra­butyl­ammonium cation are partially disordered, each with refined site occupancies of 0.691 (6):0.309 (6). Weak C—H⋯Cl hydrogen-bonding inter­actions help to consolidate the crystal packing, as well as a short Cl⋯Cl inter­action of 3.295 (2) Å.

Related literature  

For general background to and applications of tin(IV) compounds, see: Evans & Karpel (1985 ▶); Davies et al. (2008 ▶). For related structures, see: Webster et al. (1976 ▶); Sow et al. (2010 ▶). For short Cl⋯Cl inter­actions in other chlorido­tin(IV) complexes, see: Brazeau et al. (2012 ▶); Cabon et al. (2010 ▶). For background to the weighting schemes used in the refinement, see: Prince (1982 ▶); Watkin (1994 ▶).graphic file with name e-69-0m562-scheme1.jpg

Experimental  

Crystal data  

  • (C16H36N)[Sn(C4H9)Cl4]

  • M r = 560.08

  • Triclinic, Inline graphic

  • a = 11.6933 (5) Å

  • b = 11.7463 (5) Å

  • c = 12.2301 (6) Å

  • α = 114.236 (5)°

  • β = 101.680 (4)°

  • γ = 104.123 (4)°

  • V = 1395.80 (14) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 1.30 mm−1

  • T = 175 K

  • 0.45 × 0.40 × 0.15 mm

Data collection  

  • Agilent Xcalibur (Sapphire3, Gemini) diffractometer

  • Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010 ▶) T min = 0.803, T max = 1.000

  • 18571 measured reflections

  • 6635 independent reflections

  • 5438 reflections with I > 2σ(I)

  • R int = 0.039

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.049

  • wR(F 2) = 0.088

  • S = 0.97

  • 6628 reflections

  • 254 parameters

  • 142 restraints

  • H-atom parameters constrained

  • Δρmax = 1.32 e Å−3

  • Δρmin = −1.00 e Å−3

Data collection: CrysAlis PRO (Agilent, 2010 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SUPERFLIP (Palatinus & Chapuis, 2007 ▶); program(s) used to refine structure: CRYSTALS (Betteridge et al., 2003 ▶); molecular graphics: OLEX2 (Dolomanov et al., 2009 ▶) and VESTA (Momma & Izumi, 2011 ▶); software used to prepare material for publication: CRYSTALS.

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536813026172/wm2766sup1.cif

e-69-0m562-sup1.cif (28.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813026172/wm2766Isup2.hkl

e-69-0m562-Isup2.hkl (415.5KB, hkl)

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

Table 1. Selected bond lengths (Å).

Sn1—C6 2.129 (5)
Sn1—Cl2 2.3390 (12)
Sn1—Cl3 2.3494 (14)
Sn1—Cl4 2.4812 (14)
Sn1—Cl5 2.5051 (14)

Table 2. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A D⋯A D—H⋯A
C15—H152⋯Cl4 0.96 2.81 3.752 (6) 167
C19—H191⋯Cl5i 0.96 2.88 3.837 (5) 171
C19—H192⋯Cl5ii 0.96 2.90 3.830 (5) 164

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

supplementary crystallographic information

1. Comment

The interest in new organotin(IV) derivatives is related to their applications in different fields: stabilization of polyvinyl chloride, treatments for glass surface, homogeneous catalysts, textile treatments and fungicidal properties (Evans & Karpel, 1985; Davies et al., 2008).

The asymmetric unit of the title compound, (N(C4H9)4)[Sn(C4H9)Cl4], is illustrated in Fig. 1. It consists of a tetrabutylammonium cation and a tetrachloridobutylstannate(IV) anion. The Sn(IV) atom is five-coordinated in a distorted trigonal-bipyramidal arrangement with Cl4 and Cl5 in the apical positions. Major bond angle deviations with respect to the ideal trigonal-bipyramidal coordination geometry appear to be related to the different sizes of the butyl group and the Cl atoms. Thus in the equitorial plane, the C6—Sn1—Cl2 angle (125.04 (15)°) is larger than the Cl2—Sn1—Cl3 angle (112.46 (6)°). The angle Cl4—Sn1—Cl5 is 175.24 (6)°, indicating a slight deviation from linearity. The local geometry at the Sn(IV) position in the title compound is thus similar to that in (Ph4As)[MeSnCl4] (Webster et al., 1976). The Sn—Cl distances, [2.3390 (12), 2.3494 (14), 2.4812 (14) and 2.5051 (14) Å], are slightly outside the range of the Sn—Cl distances [2.369 (4) and 2.400 (4) Å] observed in (n-Pr2NH2)[Sn(C2O4)Cl4] (Sow et al., 2010). The C—N—C angles of the cation are close to 109°, in agreement with the expected sp3 hybridization.

The packing of the structure is shown in Fig. 2. A short intermolecular Cl2···Cl2 interaction of 3.295 (2) Å is found between two SnBuCl4- anions related by an inversion center. Only two other non-disordered compounds containing chloridotin(IV) complexes have shorter Cl···Cl intermolecular interactions: 3.190 Å in [C33H25N3SnCl4]·CH2Cl2 (Brazeau et al., 2012); 3.288 Å in trans-[PdCl(SnCl3(2-PyPPh2)2)] (Cabon et al., 2010). In the title compound, cations and anions stack along the a-axis and are connected via weak C—H···Cl hydrogen-bonding interactions (Fig. 2). The stacks themselves are connected via weak Cl···Cl interactions and another C—H···Cl interaction as to form sheets parallel to the ab plane.

2. Experimental

Ethanolic solutions containing (NBu4)HSO4 (1.26 g, 4 mmol) and SnBuCl3 2.25 g, 8 mmol) were mixed and stirred at room temperature for more than 1 h. After removing the precipitate, the filtrate was allowed to evaporate to give colourless crystals of the title compound. The idealized overall reaction is: (NBu4)HSO4 + 2 SnBuCl3→ (NBu4)[SnBuCl4] + SnBuCl2HSO4

3. Refinement

Three reflections, (0 1 1), (1 0 0) and (1 1 1), were obstructed by the beam stop and were omitted from the refinement. Disorder is observed for the dibutyl ammonium ion. Two of the four butyl chains of the tetrabutylammonium cation are partially disordered and were refined with site occupancies of 0.691 (6):0.309 (6) for each chain. All equivalent disordered moieties were restrained to have similar geometries. The displacement parameters of disordered atoms C12, C121, C24 and C241 of the tetrabutylammonium cation were restrained to be approximately isotropic. The H atoms were initially refined with soft restraints on the bond lengths and angles to regularize their geometry (C—H in the range 0.93–0.98, Å) and Uiso(H) (in the range 1.2–1.5 times Ueq of the parent atom), after which the positions were refined with riding constraints.

Figures

Fig. 1.

Fig. 1.

The title compound with displacement ellipsoids drawn at the 30% probability level. H atoms are shown as spheres of arbitary radius. Only the major component of the disordered part of the tetrabutylammonium cation is drawn for the sake of clarity.

Fig. 2.

Fig. 2.

The packing of the structure viewed along the a axis in wireframe style. Intermolecular Cl···Cl interactions are drawn as dashed red lines and intermolecular C—H···Cl interactions as dashed blue lines.

Crystal data

(C16H36N)[Sn(C4H9)Cl4] Z = 2
Mr = 560.08 F(000) = 580.000
Triclinic, P1 Dx = 1.333 Mg m−3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 11.6933 (5) Å Cell parameters from 5275 reflections
b = 11.7463 (5) Å θ = 2.0–28.2°
c = 12.2301 (6) Å µ = 1.30 mm−1
α = 114.236 (5)° T = 175 K
β = 101.680 (4)° Plate, colourless
γ = 104.123 (4)° 0.45 × 0.40 × 0.15 mm
V = 1395.80 (14) Å3

Data collection

Agilent Xcalibur (Sapphire3, Gemini) diffractometer 6635 independent reflections
Radiation source: Enhance (Mo) X-ray Source 5438 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.039
Detector resolution: 16.0143 pixels mm-1 θmax = 29.2°, θmin = 1.9°
ω scans h = −15→16
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) k = −15→15
Tmin = 0.803, Tmax = 1.000 l = −16→16
18571 measured reflections

Refinement

Refinement on F2 Primary atom site location: iterative
Least-squares matrix: full Hydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.049 H-atom parameters constrained
wR(F2) = 0.088 Method, part 1, Chebychev polynomial, (Watkin, 1994, Prince, 1982) [weight] = 1.0/[A0*T0(x) + A1*T1(x) ··· + An-1]*Tn-1(x)] where Ai are the Chebychev coefficients listed below and x = F /Fmax Method = Robust Weighting (Prince, 1982) W = [weight] * [1-(deltaF/6*sigmaF)2]2 Ai are: 0.178E + 04 0.238E + 04 0.133E + 04 350. 47.8
S = 0.97 (Δ/σ)max = 0.001
6628 reflections Δρmax = 1.32 e Å−3
254 parameters Δρmin = −1.00 e Å−3
142 restraints

Special details

Experimental. The crystal was placed in the cold stream of an Oxford Cryosystems open-flow nitrogen cryostat (Cosier & Glazer, 1986) with a nominal stability of 0.1 K.Cosier, J. & Glazer, A·M., 1986. J. Appl. Cryst. 105–107.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq Occ. (<1)
Sn1 0.19913 (3) 0.15984 (3) 0.83567 (3) 0.0345
Cl2 0.07714 (13) 0.07249 (13) 0.93279 (13) 0.0501
Cl3 0.35953 (15) 0.36814 (14) 0.98257 (16) 0.0696
Cl4 0.34432 (13) 0.04890 (15) 0.87972 (15) 0.0554
Cl5 0.05658 (13) 0.28254 (14) 0.81078 (14) 0.0522
C6 0.1661 (6) 0.0700 (5) 0.6359 (5) 0.0528
C7 0.1672 (6) −0.0706 (6) 0.5700 (5) 0.0542
C8 0.0680 (6) −0.1742 (5) 0.5766 (5) 0.0541
C9 0.0661 (8) −0.3156 (6) 0.5062 (6) 0.0838
H91 0.0041 −0.3756 0.5178 0.1202*
H93 0.0471 −0.3436 0.4171 0.1200*
H92 0.1472 −0.3155 0.5410 0.1201*
H82 −0.0138 −0.1753 0.5366 0.0644*
H81 0.0801 −0.1504 0.6647 0.0641*
H72 0.1551 −0.0971 0.4805 0.0641*
H71 0.2490 −0.0689 0.6100 0.0640*
H61 0.2285 0.1287 0.6217 0.0612*
H62 0.0829 0.0638 0.5954 0.0613*
N10 0.7478 (4) 0.2479 (4) 0.9853 (4) 0.0392
C11 0.7451 (6) 0.1082 (5) 0.9094 (5) 0.0586
C12 0.6356 (7) −0.0102 (7) 0.8184 (7) 0.0540 0.691 (6)
C13 0.6825 (7) −0.1149 (7) 0.7370 (5) 0.0814
C14 0.7350 (7) −0.1247 (9) 0.6359 (7) 0.1001
H142 0.7377 −0.2109 0.5927 0.1750*
H141 0.8180 −0.0586 0.6779 0.1751*
H143 0.6843 −0.1054 0.5796 0.1750*
C15 0.6838 (5) 0.2475 (7) 1.0813 (5) 0.0657
C16 0.6844 (7) 0.3808 (9) 1.1736 (6) 0.0926
C17 0.6118 (8) 0.3602 (12) 1.2581 (7) 0.1457
C18 0.6068 (11) 0.4897 (14) 1.3521 (8) 0.2270
H182 0.5562 0.4628 1.4005 0.3500*
H183 0.6856 0.5485 1.4059 0.3500*
H181 0.5606 0.5205 1.3057 0.3500*
H172 0.6543 0.3240 1.3055 0.1789*
H171 0.5285 0.2957 1.2041 0.1789*
H161 0.7696 0.4436 1.2251 0.1170*
H162 0.6441 0.4184 1.1265 0.1170*
H151 0.7288 0.2166 1.1315 0.0782*
H152 0.5991 0.1855 1.0344 0.0781*
C19 0.8824 (5) 0.3421 (5) 1.0513 (5) 0.0448
C20 0.9606 (5) 0.3237 (6) 1.1534 (5) 0.0526
C21 1.0970 (6) 0.4119 (8) 1.1979 (6) 0.0762
C22 1.1793 (7) 0.3939 (9) 1.2977 (7) 0.1068
H221 1.2653 0.4435 1.3186 0.1650*
H223 1.1678 0.2998 1.2639 0.1650*
H222 1.1575 0.4216 1.3733 0.1649*
H212 1.1254 0.3905 1.1250 0.0922*
H211 1.1033 0.5062 1.2359 0.0922*
H201 0.9538 0.2311 1.1178 0.0639*
H202 0.9289 0.3467 1.2239 0.0643*
H191 0.9208 0.3319 0.9868 0.0541*
H192 0.8825 0.4319 1.0916 0.0543*
C23 0.6808 (7) 0.2893 (7) 0.9006 (5) 0.0727
C24 0.6979 (9) 0.2669 (10) 0.7805 (8) 0.0703 0.691 (6)
C25 0.5893 (8) 0.2945 (9) 0.7078 (7) 0.1069
C26 0.6013 (9) 0.2481 (10) 0.5815 (7) 0.1269
H262 0.5538 0.2733 0.5292 0.2270*
H261 0.6884 0.2824 0.5946 0.2270*
H263 0.5722 0.1505 0.5403 0.2270*
H241 0.7797 0.3319 0.8013 0.1187* 0.691 (6)
H242 0.6970 0.1809 0.7362 0.1187* 0.691 (6)
C121 0.7471 (16) 0.0365 (11) 0.7809 (10) 0.0577 0.309 (6)
C241 0.5625 (11) 0.2512 (19) 0.8044 (14) 0.0699 0.309 (6)
H121 0.5856 0.0133 0.7658 0.0975* 0.691 (6)
H122 0.5903 −0.0407 0.8624 0.0975* 0.691 (6)
H1211 0.8314 0.0601 0.7850 0.0600* 0.309 (6)
H1212 0.7041 0.0672 0.7270 0.0600* 0.309 (6)
H2411 0.5153 0.1542 0.7646 0.0600* 0.309 (6)
H2412 0.5081 0.2920 0.8470 0.0600* 0.309 (6)
H111 0.8000 0.1167 0.8633 0.0751* 0.691 (6)
H112 0.7805 0.0864 0.9717 0.0751* 0.691 (6)
H113 0.8166 0.1070 0.9614 0.0751* 0.309 (6)
H114 0.6711 0.0516 0.9086 0.0751* 0.309 (6)
H231 0.7030 0.3834 0.9501 0.0874* 0.691 (6)
H232 0.5937 0.2452 0.8808 0.0874* 0.691 (6)
H233 0.7374 0.2994 0.8564 0.0874* 0.309 (6)
H234 0.6878 0.3753 0.9619 0.0874* 0.309 (6)
H251 0.6031 0.3875 0.7471 0.1274* 0.691 (6)
H252 0.5094 0.2458 0.7040 0.1274* 0.691 (6)
H253 0.6697 0.3632 0.7582 0.1274* 0.309 (6)
H254 0.5284 0.3339 0.6994 0.1274* 0.309 (6)
H131 0.7456 −0.1166 0.7983 0.0974* 0.691 (6)
H132 0.6119 −0.1964 0.6969 0.0974* 0.691 (6)
H133 0.7157 −0.1461 0.7920 0.0974* 0.309 (6)
H134 0.5932 −0.1484 0.7118 0.0974* 0.309 (6)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Sn1 0.03730 (17) 0.03018 (15) 0.03305 (16) 0.00540 (12) 0.00836 (12) 0.01820 (12)
Cl2 0.0569 (8) 0.0525 (7) 0.0618 (8) 0.0205 (6) 0.0315 (7) 0.0408 (7)
Cl3 0.0570 (9) 0.0399 (7) 0.0734 (10) −0.0079 (6) −0.0061 (8) 0.0208 (7)
Cl4 0.0447 (7) 0.0638 (9) 0.0735 (10) 0.0213 (7) 0.0157 (7) 0.0484 (8)
Cl5 0.0568 (8) 0.0470 (7) 0.0678 (9) 0.0253 (6) 0.0236 (7) 0.0365 (7)
C6 0.074 (4) 0.048 (3) 0.038 (3) 0.015 (3) 0.018 (3) 0.027 (2)
C7 0.066 (4) 0.058 (3) 0.039 (3) 0.022 (3) 0.023 (3) 0.021 (3)
C8 0.067 (4) 0.045 (3) 0.044 (3) 0.019 (3) 0.017 (3) 0.017 (3)
C9 0.125 (7) 0.047 (4) 0.066 (4) 0.030 (4) 0.030 (4) 0.017 (3)
N10 0.042 (2) 0.049 (2) 0.041 (2) 0.0283 (18) 0.0206 (18) 0.0260 (17)
C11 0.100 (4) 0.042 (2) 0.039 (3) 0.031 (2) 0.021 (2) 0.0226 (18)
C12 0.065 (4) 0.058 (3) 0.050 (4) 0.039 (2) 0.016 (3) 0.029 (3)
C13 0.116 (5) 0.071 (3) 0.039 (3) 0.061 (4) 0.006 (3) 0.005 (2)
C14 0.082 (5) 0.106 (6) 0.078 (5) 0.027 (5) 0.018 (4) 0.024 (4)
C15 0.036 (3) 0.106 (5) 0.039 (3) 0.015 (3) 0.020 (2) 0.023 (3)
C16 0.080 (5) 0.151 (7) 0.042 (3) 0.086 (5) 0.023 (3) 0.019 (4)
C17 0.102 (7) 0.294 (15) 0.051 (4) 0.122 (9) 0.048 (5) 0.055 (7)
C18 0.222 (13) 0.43 (2) 0.053 (5) 0.270 (15) 0.051 (7) 0.047 (9)
C19 0.048 (3) 0.050 (3) 0.046 (3) 0.017 (2) 0.021 (2) 0.028 (2)
C20 0.051 (3) 0.075 (4) 0.049 (3) 0.036 (3) 0.022 (3) 0.035 (3)
C21 0.046 (3) 0.115 (6) 0.048 (3) 0.036 (4) 0.017 (3) 0.019 (4)
C22 0.064 (5) 0.139 (8) 0.088 (6) 0.060 (5) 0.003 (4) 0.028 (5)
C23 0.102 (4) 0.094 (4) 0.043 (3) 0.079 (4) 0.019 (3) 0.030 (3)
C24 0.096 (5) 0.079 (5) 0.079 (4) 0.053 (5) 0.047 (4) 0.056 (5)
C25 0.148 (6) 0.114 (6) 0.074 (4) 0.059 (5) 0.009 (4) 0.066 (4)
C26 0.131 (7) 0.154 (8) 0.068 (4) 0.077 (6) 0.004 (4) 0.029 (5)
C121 0.072 (7) 0.092 (4) 0.042 (4) 0.059 (6) 0.024 (5) 0.043 (4)
C241 0.063 (5) 0.069 (8) 0.102 (7) 0.042 (6) 0.017 (4) 0.059 (6)

Geometric parameters (Å, º)

Sn1—C6 2.129 (5) C17—H172 0.975
Sn1—Cl2 2.3390 (12) C17—H171 0.963
Sn1—Cl3 2.3494 (14) C18—H182 1.003
Sn1—Cl4 2.4812 (14) C18—H183 0.910
Sn1—Cl5 2.5051 (14) C18—H181 0.940
C6—C7 1.516 (7) C19—C20 1.516 (7)
C6—H61 0.971 C19—H191 0.964
C6—H62 0.969 C19—H192 0.963
C7—C8 1.505 (7) C20—C21 1.515 (8)
C7—H72 0.975 C20—H201 0.966
C7—H71 0.974 C20—H202 0.970
C8—C9 1.517 (7) C21—C22 1.515 (9)
C8—H82 0.976 C21—H212 0.972
C8—H81 0.965 C21—H211 0.986
C9—H91 0.957 C22—H221 0.951
C9—H93 0.957 C22—H223 0.970
C9—H92 0.957 C22—H222 0.956
N10—C11 1.505 (6) C23—C24 1.446 (7)
N10—C15 1.517 (6) C23—C241 1.450 (9)
N10—C19 1.501 (6) C23—H231 0.950
N10—C23 1.483 (6) C23—H232 0.950
C11—C12 1.447 (7) C23—H233 0.950
C11—C121 1.455 (9) C23—H234 0.950
C11—H111 0.950 C24—C25 1.578 (7)
C11—H112 0.950 C24—H241 0.974
C11—H113 0.950 C24—H242 0.925
C11—H114 0.950 C24—C241 1.648 (16)
C12—C13 1.532 (7) C24—H233 0.818
C12—C121 1.520 (16) C25—C26 1.462 (7)
C12—H121 0.950 C25—C241 1.523 (9)
C12—H122 0.939 C25—H251 0.950
C12—H114 0.963 C25—H252 0.950
C13—C14 1.465 (10) C25—H253 0.950
C13—C121 1.556 (9) C25—H254 0.950
C13—H131 0.950 C26—H262 0.946
C13—H132 0.950 C26—H261 0.952
C13—H133 0.950 C26—H263 0.975
C13—H134 0.954 C121—H1211 0.941
C14—H142 0.943 C121—H1212 0.983
C14—H141 0.954 C121—H111 0.985
C14—H143 0.952 C241—H2411 0.984
C15—C16 1.505 (9) C241—H2412 0.992
C15—H151 0.964 C241—H232 0.969
C15—H152 0.957 C241—H252 1.227
C16—C17 1.519 (10) H112—H113 0.499
C16—H161 0.969 H131—H133 0.395
C16—H162 0.975 H132—H134 0.626
C17—C18 1.508 (13)
Cl2—Sn1—Cl3 112.46 (6) N10—C19—H192 107.4
Cl2—Sn1—Cl4 88.66 (5) C20—C19—H192 107.4
Cl3—Sn1—Cl4 88.58 (6) H191—C19—H192 109.4
Cl2—Sn1—Cl5 88.99 (5) C19—C20—C21 109.9 (5)
Cl3—Sn1—Cl5 88.51 (6) C19—C20—H201 109.0
Cl4—Sn1—Cl5 175.24 (6) C21—C20—H201 108.7
Cl2—Sn1—C6 125.04 (15) C19—C20—H202 108.7
Cl3—Sn1—C6 122.42 (15) C21—C20—H202 110.6
Cl4—Sn1—C6 95.13 (16) H201—C20—H202 109.9
Cl5—Sn1—C6 89.61 (16) C20—C21—C22 111.7 (6)
Sn1—C6—C7 117.6 (3) C20—C21—H212 109.2
Sn1—C6—H61 107.8 C22—C21—H212 109.8
C7—C6—H61 108.6 C20—C21—H211 108.1
Sn1—C6—H62 106.8 C22—C21—H211 108.6
C7—C6—H62 105.9 H212—C21—H211 109.4
H61—C6—H62 110.0 C21—C22—H221 110.4
C6—C7—C8 114.0 (5) C21—C22—H223 109.3
C6—C7—H72 108.7 H221—C22—H223 108.2
C8—C7—H72 108.6 C21—C22—H222 111.2
C6—C7—H71 108.3 H221—C22—H222 109.5
C8—C7—H71 108.4 H223—C22—H222 108.1
H72—C7—H71 108.8 N10—C23—C24 122.5 (5)
C7—C8—C9 113.8 (5) N10—C23—C241 143.6 (8)
C7—C8—H82 108.0 C24—C23—C241 69.3 (7)
C9—C8—H82 106.9 N10—C23—H231 106.0
C7—C8—H81 109.5 C24—C23—H231 106.1
C9—C8—H81 108.9 C241—C23—H231 102.1
H82—C8—H81 109.6 N10—C23—H232 106.2
C8—C9—H91 109.6 C24—C23—H232 106.2
C8—C9—H93 109.9 H231—C23—H232 109.5
H91—C9—H93 109.6 N10—C23—H233 100.4
C8—C9—H92 108.2 C241—C23—H233 100.8
H91—C9—H92 109.5 H231—C23—H233 93.0
H93—C9—H92 109.9 H232—C23—H233 138.2
C11—N10—C15 107.9 (4) N10—C23—H234 100.2
C11—N10—C19 108.4 (4) C24—C23—H234 121.2
C15—N10—C19 111.0 (4) C241—C23—H234 100.2
C11—N10—C23 110.7 (4) H232—C23—H234 97.0
C15—N10—C23 109.5 (4) H233—C23—H234 109.5
C19—N10—C23 109.4 (4) C23—C24—C25 105.9 (6)
N10—C11—C12 126.8 (5) C23—C24—H241 106.6
N10—C11—C121 131.7 (6) C25—C24—H241 110.9
C12—C11—C121 63.1 (7) C23—C24—H242 110.2
N10—C11—H111 105.1 C25—C24—H242 113.5
C12—C11—H111 105.3 H241—C24—H242 109.5
N10—C11—H112 104.7 C23—C24—C241 55.5 (5)
C12—C11—H112 104.9 C25—C24—C241 56.3 (4)
C121—C11—H112 118.5 H241—C24—C241 143.5
H111—C11—H112 109.5 H242—C24—C241 106.8
N10—C11—H113 103.1 C25—C24—H233 132.3
C12—C11—H113 124.0 H241—C24—H233 71.0
C121—C11—H113 103.5 H242—C24—H233 109.8
H111—C11—H113 80.9 C241—C24—H233 92.9
N10—C11—H114 104.3 C24—C25—C26 101.9 (7)
C121—C11—H114 103.7 C24—C25—C241 64.2 (6)
H111—C11—H114 145.4 C26—C25—C241 144.2 (11)
H112—C11—H114 79.8 C24—C25—H251 110.9
H113—C11—H114 109.5 C26—C25—H251 110.8
C11—C12—C13 107.2 (6) C241—C25—H251 104.9
C11—C12—C121 58.7 (5) C24—C25—H252 111.8
C13—C12—C121 61.3 (5) C26—C25—H252 111.9
C11—C12—H121 108.2 C241—C25—H252 53.6
C13—C12—H121 109.7 H251—C25—H252 109.5
C121—C12—H121 90.6 C24—C25—H253 59.3
C11—C12—H122 109.3 C26—C25—H253 99.8
C13—C12—H122 112.0 C241—C25—H253 99.8
C121—C12—H122 158.8 H251—C25—H253 56.4
H121—C12—H122 110.4 H252—C25—H253 148.4
C13—C12—H114 128.6 C24—C25—H254 156.4
C121—C12—H114 98.6 C26—C25—H254 100.5
H121—C12—H114 117.7 C241—C25—H254 100.7
H122—C12—H114 69.2 H251—C25—H254 53.2
C12—C13—C14 131.8 (7) H252—C25—H254 65.8
C12—C13—C121 59.0 (6) H253—C25—H254 109.5
C14—C13—C121 79.8 (6) C25—C26—H262 113.7
C12—C13—H131 103.6 C25—C26—H261 106.8
C14—C13—H131 103.7 H262—C26—H261 111.5
C121—C13—H131 95.0 C25—C26—H263 107.0
C12—C13—H132 103.7 H262—C26—H263 108.9
C14—C13—H132 103.5 H261—C26—H263 108.6
C121—C13—H132 153.4 C13—C121—C12 59.8 (5)
H131—C13—H132 109.5 C13—C121—C11 105.6 (7)
C12—C13—H133 104.1 C12—C121—C11 58.2 (5)
C14—C13—H133 116.7 C13—C121—H1211 113.1
C121—C13—H133 116.3 C12—C121—H1211 156.6
H132—C13—H133 86.3 C11—C121—H1211 107.9
C12—C13—H134 68.6 C13—C121—H1212 113.8
C14—C13—H134 116.4 C12—C121—H1212 95.4
C121—C13—H134 116.2 C11—C121—H1212 108.9
H131—C13—H134 132.0 H1211—C121—H1212 107.4
H133—C13—H134 109.1 C13—C121—H111 134.7
C13—C14—H142 110.2 C12—C121—H111 98.5
C13—C14—H141 105.8 H1211—C121—H111 70.3
H142—C14—H141 110.2 H1212—C121—H111 107.1
C13—C14—H143 108.0 C25—C241—C23 108.6 (8)
H142—C14—H143 111.5 C25—C241—C24 59.5 (5)
H141—C14—H143 111.0 C23—C241—C24 55.2 (5)
N10—C15—C16 116.4 (6) C25—C241—H2411 112.5
N10—C15—H151 106.1 C23—C241—H2411 110.2
C16—C15—H151 106.8 C24—C241—H2411 106.2
N10—C15—H152 107.5 C25—C241—H2412 113.0
C16—C15—H152 109.5 C23—C241—H2412 108.9
H151—C15—H152 110.4 C24—C241—H2412 149.9
C15—C16—C17 109.1 (8) H2411—C241—H2412 103.4
C15—C16—H161 110.7 C25—C241—H232 149.0
C17—C16—H161 110.4 C24—C241—H232 91.9
C15—C16—H162 109.5 H2411—C241—H232 85.3
C17—C16—H162 109.1 H2412—C241—H232 85.2
H161—C16—H162 108.0 C23—C241—H252 147.1
C16—C17—C18 112.1 (11) C24—C241—H252 94.0
C16—C17—H172 107.9 H2411—C241—H252 87.8
C18—C17—H172 108.6 H2412—C241—H252 92.4
C16—C17—H171 108.2 H232—C241—H252 171.9
C18—C17—H171 110.7 C121—H111—C11 97.6
H172—C17—H171 109.2 C11—H112—H113 74.8
C17—C18—H182 104.3 C11—H113—H112 74.8
C17—C18—H183 110.3 C12—H114—C11 98.3
H182—C18—H183 110.4 C241—H232—C23 98.2
C17—C18—H181 108.0 C23—H233—C24 109.5
H182—C18—H181 107.6 C241—H252—C25 87.8
H183—C18—H181 115.7 C13—H131—H133 78.0
N10—C19—C20 116.1 (4) C13—H132—H134 71.2
N10—C19—H191 107.6 C13—H133—H131 78.0
C20—C19—H191 108.9 H132—H134—C13 70.5

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
C15—H152···Cl4 0.96 2.81 3.752 (6) 167
C19—H191···Cl5i 0.96 2.88 3.837 (5) 171
C19—H192···Cl5ii 0.96 2.90 3.830 (5) 164

Symmetry codes: (i) x+1, y, z; (ii) −x+1, −y+1, −z+2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: WM2766).

References

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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 datablock(s) global, I. DOI: 10.1107/S1600536813026172/wm2766sup1.cif

e-69-0m562-sup1.cif (28.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813026172/wm2766Isup2.hkl

e-69-0m562-Isup2.hkl (415.5KB, hkl)

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


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