Abstract
The asymmetric unit of the title compound, (C6H7ClN)4[SnCl6]Cl2, comprises two 4-chloroanilinium cations, half of an [SnCl6]2− anion and a Cl− anion. The SnIV atom, located on a special position on a twofold rotation axis, exhibits an octahedral environment. In the crystal, molecules are linked by N—H⋯Cl hydrogen bonds between the 4-chloroanilinium cations, [SnCl6]2− anions and Cl− anions.
Related literature
For general background to ferroelectric metal-organic frameworks, see: Ye et al. (2009 ▶); Fu et al. (2007 ▶). For phase transitions in ferroelectric materials, see: Zhang et al. (2008 ▶); Zhao et al. (2008 ▶); Ye et al. (2006 ▶).
Experimental
Crystal data
(C6H7ClN)4[SnCl6]Cl2
M r = 916.59
Monoclinic,
a = 27.855 (6) Å
b = 7.2061 (14) Å
c = 21.895 (4) Å
β = 125.03 (3)°
V = 3598.8 (18) Å3
Z = 4
Mo Kα radiation
μ = 1.63 mm−1
T = 293 K
0.20 × 0.20 × 0.20 mm
Data collection
Rigaku SCXmini diffractometer
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005 ▶) T min = 0.715, T max = 0.730
17870 measured reflections
4122 independent reflections
3581 reflections with I > 2σ(I)
R int = 0.031
Refinement
R[F 2 > 2σ(F 2)] = 0.030
wR(F 2) = 0.067
S = 1.10
4122 reflections
188 parameters
H-atom parameters constrained
Δρmax = 0.44 e Å−3
Δρmin = −0.46 e Å−3
Data collection: CrystalClear (Rigaku, 2005 ▶); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: DIAMOND (Brandenburg & Putz, 2005 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812021666/kp2409sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812021666/kp2409Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Selected bond lengths (Å).
| Cl3—Sn1 | 2.4205 (11) |
| Cl4—Sn1 | 2.4076 (7) |
| Cl5—Sn1 | 2.4356 (7) |
Table 2. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N1—H1A⋯Cl5i | 0.89 | 2.64 | 3.522 (2) | 172 |
| N1—H1A⋯Cl3i | 0.89 | 2.98 | 3.424 (2) | 112 |
| N1—H1B⋯Cl6ii | 0.89 | 2.25 | 3.123 (3) | 165 |
| N1—H1C⋯Cl6iii | 0.89 | 2.26 | 3.120 (3) | 162 |
| N2—H2A⋯Cl3iv | 0.89 | 2.75 | 3.455 (2) | 137 |
| N2—H2A⋯Cl4v | 0.89 | 2.79 | 3.567 (2) | 147 |
| N2—H2A⋯Cl4iv | 0.89 | 2.92 | 3.344 (3) | 111 |
| N2—H2B⋯Cl6vi | 0.89 | 2.20 | 3.085 (3) | 175 |
| N2—H2C⋯Cl5vii | 0.89 | 2.61 | 3.424 (3) | 153 |
Symmetry codes: (i)
; (ii)
; (iii)
; (iv)
; (v)
; (vi)
; (vii)
.
Acknowledgments
The authors are grateful to the starter fund of Southeast University, Nanjing, People’s Republic of China.
supplementary crystallographic information
Comment
The study of ferroelectric materials has received much attention; some of them have predominantly dielectric–ferroelectric performance (Ye et al., 2006; Fu et al., 2007; Zhao et al. 2008; Zhang et al., 2008; Ye et al., 2009). As a part of our work to obtain potential ferroelectric phase-transition material, we report herein on the crystal structure of title compound. Unluckily, the title compound has no dielectric anomalies in the temperature range 93–453 K, suggesting that it might be only a paraelectric.
The asymmetric unit of the title compound is shown in Fig. 1 and Sn-Cl bonds are listed in Table 1. The crystal packing (Fig. 2) is stabilised by intermolecular N—H···Cl hydrogen bonds between the [C6H7ClN]+cations and SnCl62–anions and Cl- anions (Table 2).
Experimental
For the preparation of the title compound, the water solution of the hydrochloric acid (10 mmol) was added to the ethanol solution of the 4-chlorobenzenamine(10 mmol), then the water solution of the SnCl4(5 mmol) was added into a reaction mixture. The resulting precipitate was filtered. Colourless crystals suitable for X-ray analysis were formed after several weeks by slow evaporation of the solvent at room temperature.
Refinement
Positional parameters of all the H atoms bonded to C atoms were calculated geometrically and were allowed to ride on the C atoms to which they are bonded, with Uiso(H) = 1.2Ueq(C) and Uiso(H) = 1.5Ueq(C) for the methyl group. The other H bonded to N atoms were calculated geometrically and were allowed to ride on the N atoms with Uiso(H) = 1.5Ueq(O).
Figures
Fig. 1.
The molecular structure of the title compound with the atomic numbering scheme. Displacement ellipsoids are drawn at the 30% probability level.[The suffix A denotes the symmetry code: 2-x y 1/2 - z.]
Fig. 2.
Crystal packing of the title compound. Dashed lines indicate hydrogen bonds.
Crystal data
| (C6H7ClN)4[SnCl6]Cl2 | F(000) = 1816 |
| Mr = 916.59 | Dx = 1.692 Mg m−3 |
| Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -C 2yc | Cell parameters from 4122 reflections |
| a = 27.855 (6) Å | θ = 3.4–27.5° |
| b = 7.2061 (14) Å | µ = 1.63 mm−1 |
| c = 21.895 (4) Å | T = 293 K |
| β = 125.03 (3)° | Prism, colourless |
| V = 3598.8 (18) Å3 | 0.20 × 0.20 × 0.20 mm |
| Z = 4 |
Data collection
| Rigaku SCXmini diffractometer | 4122 independent reflections |
| Radiation source: fine-focus sealed tube | 3581 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.031 |
| Detector resolution: 13.6612 pixels mm-1 | θmax = 27.5°, θmin = 3.4° |
| CCD_Profile_fitting scans | h = −36→35 |
| Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | k = −9→9 |
| Tmin = 0.715, Tmax = 0.730 | l = −28→28 |
| 17870 measured reflections |
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)] = 0.030 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.067 | H-atom parameters constrained |
| S = 1.10 | w = 1/[σ2(Fo2) + (0.0236P)2 + 4.0429P] where P = (Fo2 + 2Fc2)/3 |
| 4122 reflections | (Δ/σ)max = 0.002 |
| 188 parameters | Δρmax = 0.44 e Å−3 |
| 0 restraints | Δρmin = −0.46 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 | ||
| C1 | 0.12061 (12) | 0.1500 (4) | 0.12876 (15) | 0.0503 (6) | |
| C2 | 0.13487 (13) | 0.0639 (4) | 0.08532 (16) | 0.0540 (7) | |
| H2 | 0.1066 | −0.0001 | 0.0425 | 0.065* | |
| C3 | 0.19188 (13) | 0.0738 (4) | 0.10633 (16) | 0.0535 (7) | |
| H3 | 0.2025 | 0.0155 | 0.0779 | 0.064* | |
| C4 | 0.23257 (12) | 0.1696 (4) | 0.16906 (17) | 0.0507 (7) | |
| C5 | 0.21803 (13) | 0.2551 (5) | 0.21162 (17) | 0.0632 (8) | |
| H5 | 0.2463 | 0.3194 | 0.2544 | 0.076* | |
| C6 | 0.16093 (14) | 0.2459 (5) | 0.19102 (17) | 0.0661 (9) | |
| H6 | 0.1503 | 0.3047 | 0.2195 | 0.079* | |
| C7 | 0.39010 (11) | 0.0792 (3) | 0.05568 (13) | 0.0401 (5) | |
| C8 | 0.38139 (12) | −0.0100 (3) | −0.00526 (14) | 0.0470 (6) | |
| H8 | 0.4121 | −0.0253 | −0.0103 | 0.056* | |
| C9 | 0.32612 (14) | −0.0767 (4) | −0.05904 (15) | 0.0556 (7) | |
| H9 | 0.3192 | −0.1366 | −0.1010 | 0.067* | |
| C10 | 0.28179 (12) | −0.0544 (4) | −0.05054 (16) | 0.0554 (7) | |
| C11 | 0.29063 (13) | 0.0384 (5) | 0.00988 (18) | 0.0634 (8) | |
| H11 | 0.2597 | 0.0554 | 0.0144 | 0.076* | |
| C12 | 0.34538 (13) | 0.1062 (4) | 0.06368 (16) | 0.0559 (7) | |
| H12 | 0.3519 | 0.1694 | 0.1049 | 0.067* | |
| Cl1 | 0.21316 (4) | −0.14614 (15) | −0.11590 (6) | 0.0983 (3) | |
| Cl2 | 0.30443 (4) | 0.17986 (14) | 0.19641 (6) | 0.0843 (3) | |
| Cl3 | 0.94108 (3) | 0.11974 (9) | 0.11503 (3) | 0.04947 (16) | |
| Cl4 | 1.06231 (3) | −0.11341 (9) | 0.25190 (4) | 0.04712 (15) | |
| Cl5 | 1.06027 (3) | 0.36499 (8) | 0.24919 (4) | 0.04846 (15) | |
| Cl6 | 0.02508 (4) | 0.72478 (14) | 0.05762 (5) | 0.0808 (3) | |
| N1 | 0.05994 (11) | 0.1377 (4) | 0.10653 (15) | 0.0707 (8) | |
| H1A | 0.0577 | 0.1853 | 0.1423 | 0.106* | |
| H1B | 0.0488 | 0.0193 | 0.0993 | 0.106* | |
| H1C | 0.0365 | 0.2010 | 0.0645 | 0.106* | |
| N2 | 0.44908 (10) | 0.1413 (3) | 0.11539 (12) | 0.0525 (5) | |
| H2A | 0.4466 | 0.2420 | 0.1370 | 0.079* | |
| H2B | 0.4692 | 0.1682 | 0.0964 | 0.079* | |
| H2C | 0.4674 | 0.0515 | 0.1492 | 0.079* | |
| Sn1 | 1.0000 | 0.12149 (3) | 0.2500 | 0.03220 (7) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0478 (15) | 0.0652 (17) | 0.0503 (15) | −0.0127 (13) | 0.0353 (13) | −0.0134 (13) |
| C2 | 0.0628 (18) | 0.0596 (17) | 0.0540 (16) | −0.0140 (14) | 0.0419 (15) | −0.0158 (13) |
| C3 | 0.0664 (18) | 0.0497 (15) | 0.0680 (18) | −0.0019 (13) | 0.0524 (17) | −0.0038 (13) |
| C4 | 0.0492 (15) | 0.0470 (15) | 0.0678 (18) | 0.0016 (12) | 0.0405 (15) | 0.0108 (13) |
| C5 | 0.0535 (17) | 0.075 (2) | 0.0566 (17) | −0.0164 (15) | 0.0292 (15) | −0.0175 (15) |
| C6 | 0.0631 (19) | 0.086 (2) | 0.0632 (19) | −0.0188 (17) | 0.0446 (17) | −0.0322 (17) |
| C7 | 0.0448 (13) | 0.0332 (12) | 0.0393 (12) | 0.0021 (10) | 0.0223 (11) | 0.0041 (9) |
| C8 | 0.0551 (16) | 0.0395 (13) | 0.0508 (15) | 0.0061 (11) | 0.0329 (13) | 0.0027 (11) |
| C9 | 0.072 (2) | 0.0416 (14) | 0.0429 (14) | −0.0030 (13) | 0.0270 (15) | −0.0031 (11) |
| C10 | 0.0507 (16) | 0.0471 (15) | 0.0483 (15) | −0.0062 (12) | 0.0167 (13) | 0.0083 (12) |
| C11 | 0.0526 (17) | 0.074 (2) | 0.071 (2) | 0.0020 (15) | 0.0404 (17) | 0.0082 (17) |
| C12 | 0.0602 (18) | 0.0636 (18) | 0.0546 (16) | 0.0014 (14) | 0.0392 (15) | −0.0034 (14) |
| Cl1 | 0.0635 (5) | 0.0962 (7) | 0.0859 (7) | −0.0256 (5) | 0.0140 (5) | 0.0026 (5) |
| Cl2 | 0.0541 (5) | 0.0922 (6) | 0.1164 (8) | 0.0013 (4) | 0.0548 (5) | 0.0153 (6) |
| Cl3 | 0.0565 (4) | 0.0537 (4) | 0.0338 (3) | 0.0105 (3) | 0.0233 (3) | 0.0055 (3) |
| Cl4 | 0.0442 (3) | 0.0433 (3) | 0.0505 (3) | 0.0109 (3) | 0.0252 (3) | −0.0019 (3) |
| Cl5 | 0.0575 (4) | 0.0401 (3) | 0.0623 (4) | −0.0089 (3) | 0.0428 (3) | −0.0001 (3) |
| Cl6 | 0.0672 (5) | 0.1076 (7) | 0.0878 (6) | −0.0289 (5) | 0.0563 (5) | −0.0438 (5) |
| N1 | 0.0547 (15) | 0.110 (2) | 0.0647 (16) | −0.0254 (14) | 0.0443 (14) | −0.0329 (15) |
| N2 | 0.0499 (13) | 0.0521 (13) | 0.0477 (12) | 0.0004 (10) | 0.0234 (11) | −0.0010 (10) |
| Sn1 | 0.04091 (13) | 0.02673 (11) | 0.03437 (12) | 0.000 | 0.02476 (10) | 0.000 |
Geometric parameters (Å, º)
| C1—C6 | 1.356 (4) | C9—H9 | 0.9300 |
| C1—C2 | 1.372 (4) | C10—C11 | 1.373 (4) |
| C1—N1 | 1.468 (3) | C10—Cl1 | 1.732 (3) |
| C2—C3 | 1.378 (4) | C11—C12 | 1.374 (4) |
| C2—H2 | 0.9300 | C11—H11 | 0.9300 |
| C3—C4 | 1.364 (4) | C12—H12 | 0.9300 |
| C3—H3 | 0.9300 | Cl3—Sn1 | 2.4205 (11) |
| C4—C5 | 1.359 (4) | Cl4—Sn1 | 2.4076 (7) |
| C4—Cl2 | 1.731 (3) | Cl5—Sn1 | 2.4356 (7) |
| C5—C6 | 1.383 (4) | N1—H1A | 0.8900 |
| C5—H5 | 0.9300 | N1—H1B | 0.8900 |
| C6—H6 | 0.9300 | N1—H1C | 0.8900 |
| C7—C12 | 1.368 (4) | N2—H2A | 0.8900 |
| C7—C8 | 1.371 (3) | N2—H2B | 0.8900 |
| C7—N2 | 1.464 (3) | N2—H2C | 0.8900 |
| C8—C9 | 1.381 (4) | Sn1—Cl4i | 2.4076 (7) |
| C8—H8 | 0.9300 | Sn1—Cl3i | 2.4205 (11) |
| C9—C10 | 1.360 (4) | Sn1—Cl5i | 2.4356 (7) |
| C6—C1—C2 | 121.7 (3) | C12—C11—H11 | 120.1 |
| C6—C1—N1 | 119.7 (2) | C7—C12—C11 | 118.9 (3) |
| C2—C1—N1 | 118.6 (2) | C7—C12—H12 | 120.5 |
| C1—C2—C3 | 118.8 (3) | C11—C12—H12 | 120.5 |
| C1—C2—H2 | 120.6 | C1—N1—H1A | 109.5 |
| C3—C2—H2 | 120.6 | C1—N1—H1B | 109.5 |
| C4—C3—C2 | 119.6 (3) | H1A—N1—H1B | 109.5 |
| C4—C3—H3 | 120.2 | C1—N1—H1C | 109.5 |
| C2—C3—H3 | 120.2 | H1A—N1—H1C | 109.5 |
| C5—C4—C3 | 121.2 (3) | H1B—N1—H1C | 109.5 |
| C5—C4—Cl2 | 119.0 (2) | C7—N2—H2A | 109.5 |
| C3—C4—Cl2 | 119.9 (2) | C7—N2—H2B | 109.5 |
| C4—C5—C6 | 119.6 (3) | H2A—N2—H2B | 109.5 |
| C4—C5—H5 | 120.2 | C7—N2—H2C | 109.5 |
| C6—C5—H5 | 120.2 | H2A—N2—H2C | 109.5 |
| C1—C6—C5 | 119.1 (3) | H2B—N2—H2C | 109.5 |
| C1—C6—H6 | 120.5 | Cl4i—Sn1—Cl4 | 90.65 (4) |
| C5—C6—H6 | 120.5 | Cl4i—Sn1—Cl3 | 89.91 (3) |
| C12—C7—C8 | 121.7 (2) | Cl4—Sn1—Cl3 | 89.67 (3) |
| C12—C7—N2 | 118.7 (2) | Cl4i—Sn1—Cl3i | 89.67 (3) |
| C8—C7—N2 | 119.6 (2) | Cl4—Sn1—Cl3i | 89.91 (3) |
| C7—C8—C9 | 118.7 (3) | Cl3—Sn1—Cl3i | 179.40 (3) |
| C7—C8—H8 | 120.6 | Cl4i—Sn1—Cl5 | 178.18 (2) |
| C9—C8—H8 | 120.6 | Cl4—Sn1—Cl5 | 90.77 (3) |
| C10—C9—C8 | 119.9 (3) | Cl3—Sn1—Cl5 | 88.97 (3) |
| C10—C9—H9 | 120.1 | Cl3i—Sn1—Cl5 | 91.46 (3) |
| C8—C9—H9 | 120.1 | Cl4i—Sn1—Cl5i | 90.77 (3) |
| C9—C10—C11 | 121.0 (3) | Cl4—Sn1—Cl5i | 178.18 (2) |
| C9—C10—Cl1 | 120.0 (2) | Cl3—Sn1—Cl5i | 91.46 (3) |
| C11—C10—Cl1 | 119.0 (3) | Cl3i—Sn1—Cl5i | 88.97 (3) |
| C10—C11—C12 | 119.7 (3) | Cl5—Sn1—Cl5i | 87.82 (4) |
| C10—C11—H11 | 120.1 | ||
| C6—C1—C2—C3 | 0.8 (5) | C12—C7—C8—C9 | −1.1 (4) |
| N1—C1—C2—C3 | −179.5 (3) | N2—C7—C8—C9 | 176.5 (2) |
| C1—C2—C3—C4 | −0.5 (4) | C7—C8—C9—C10 | −0.5 (4) |
| C2—C3—C4—C5 | 0.3 (5) | C8—C9—C10—C11 | 1.9 (4) |
| C2—C3—C4—Cl2 | 179.1 (2) | C8—C9—C10—Cl1 | −177.3 (2) |
| C3—C4—C5—C6 | −0.3 (5) | C9—C10—C11—C12 | −1.6 (5) |
| Cl2—C4—C5—C6 | −179.1 (3) | Cl1—C10—C11—C12 | 177.6 (2) |
| C2—C1—C6—C5 | −0.8 (5) | C8—C7—C12—C11 | 1.4 (4) |
| N1—C1—C6—C5 | 179.5 (3) | N2—C7—C12—C11 | −176.2 (3) |
| C4—C5—C6—C1 | 0.5 (5) | C10—C11—C12—C7 | 0.0 (5) |
Symmetry code: (i) −x+2, y, −z+1/2.
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1A···Cl5ii | 0.89 | 2.64 | 3.522 (2) | 172 |
| N1—H1A···Cl3ii | 0.89 | 2.98 | 3.424 (2) | 112 |
| N1—H1B···Cl6iii | 0.89 | 2.25 | 3.123 (3) | 165 |
| N1—H1C···Cl6iv | 0.89 | 2.26 | 3.120 (3) | 162 |
| N2—H2A···Cl3v | 0.89 | 2.75 | 3.455 (2) | 137 |
| N2—H2A···Cl4vi | 0.89 | 2.79 | 3.567 (2) | 147 |
| N2—H2A···Cl4v | 0.89 | 2.92 | 3.344 (3) | 111 |
| N2—H2B···Cl6vii | 0.89 | 2.20 | 3.085 (3) | 175 |
| N2—H2C···Cl5viii | 0.89 | 2.61 | 3.424 (3) | 153 |
Symmetry codes: (ii) x−1, y, z; (iii) x, y−1, z; (iv) −x, −y+1, −z; (v) x−1/2, y+1/2, z; (vi) −x+3/2, y+1/2, −z+1/2; (vii) x+1/2, y−1/2, z; (viii) x−1/2, y−1/2, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: KP2409).
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) I, global. DOI: 10.1107/S1600536812021666/kp2409sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812021666/kp2409Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


