Abstract
In the crystal structure of the title salt, (C5H9N2)2[CuCl4], the organic cations and the tetrahedral [CuCl4] anions are linked into a three-dimensional network by N—H⋯Cl hydrogen bonds. The two 2-ethyl imidazolium cations in the asymmetric unit differ in the orientation of the ethyl group, with N—C—C—C torsion angles of −170.0 (4) and −87.6 (5)°.
Related literature
For general background to ferroelectric metal-organic frameworks, see: Fu et al. (2009 ▶); Ye et al. (2006 ▶); Zhang et al. (2008 ▶, 2010 ▶).
Experimental
Crystal data
(C5H9N2)2[CuCl4]
M r = 399.63
Triclinic,
a = 7.992 (4) Å
b = 9.003 (4) Å
c = 12.216 (6) Å
α = 79.641 (14)°
β = 84.646 (14)°
γ = 72.154 (12)°
V = 822.4 (7) Å3
Z = 2
Mo Kα radiation
μ = 1.97 mm−1
T = 293 K
0.30 × 0.25 × 0.20 mm
Data collection
Rigaku SCXmini diffractometer
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005 ▶) T min = 0.559, T max = 0.674
9065 measured reflections
3775 independent reflections
3124 reflections with I > 2σ(I)
R int = 0.035
Refinement
R[F 2 > 2σ(F 2)] = 0.039
wR(F 2) = 0.123
S = 1.17
3775 reflections
174 parameters
H-atom parameters constrained
Δρmax = 0.59 e Å−3
Δρmin = −0.66 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: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S160053681005261X/vm2067sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S160053681005261X/vm2067Isup2.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—H1A⋯Cl1i | 0.86 | 2.39 | 3.217 (3) | 160 |
| N2—H2A⋯Cl2 | 0.86 | 2.39 | 3.195 (3) | 157 |
| N3—H3A⋯Cl3 | 0.86 | 2.46 | 3.178 (3) | 142 |
| N4—H4C⋯Cl4ii | 0.86 | 2.32 | 3.149 (3) | 164 |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
This work was supported by Southeast University.
supplementary crystallographic information
Comment
Dielectric constant measurements of compounds as a function of temperature is the basic method to find the materials which possess potential ferroelectric phase changes (Fu et al., 2009; Ye et al., 2006; Zhang et al., 2008; Zhang et al., 2010). The dielectric constant of the title compound has been measured, but showed no dielectric disuniformity in the range 93–365 K (m.p. 374–381 K).
X-ray crystallographic studies have been carried out for the complex 2[C5N2H9] +.CuCl42- at 123 K. An view of the complex is shown in Fig. 1. The structure is consolidated by extensive intermolecular and intramolecular hydrogen bonds between Cl and N. This hydrogen bonding (Table 1, Fig. 2) produces a three-dimensional network. Within the CuCl42- tetrahedra the Cu-Cl distances are: Cu1—Cl1 = 2.2287 (13) Å, Cu1—Cl2 = 2.2625 Å,Cu1—Cl3 = 2.2688 (12) Å, Cu1—Cl4 = 2.2501 (13) Å.
The two 2-ethyl imidazolium cations in the asymmetric unit differ in the orientation of the ethyl group. In one cation all atoms except H atoms are situated in the same plane(dihedral angle N1—C3—C4—C5 = -170.0 (4)°), while in the other cation the dihedral angle N3—C8—C9—C10 is -87.6 (5) °.
Experimental
A mixture of CuCl2 (4.26 g, 25 mmol), hydrochloric acid (50 mmol), and 2-ethyl imidazole (4.8 g, 50 mmol) in water was stirred for several days at room temperature, yellow block crystals were obtained.
Refinement
Hydrogen atom positions were calculated and allowed to ride on their respective C atoms and N atoms with C–H distances of 0.93–0.97Å and N–H = 0.86 Å, and with Uiso(H)=1.2Ueq(C or N).
Figures
Fig. 1.
The molecular structure of the title compound, with the displacement ellipsoids drawn at the 30% probability level. Intramolecular hydrogen bonds are shown as dashed lines.
Fig. 2.
Packing diagram of the title compound, showing the structure along the b axis. Hydrogen bonds are shown as dashed lines.
Crystal data
| (C5H9N2)2[CuCl4] | Z = 2 |
| Mr = 399.63 | F(000) = 406 |
| Triclinic, P1 | Dx = 1.614 Mg m−3 |
| Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
| a = 7.992 (4) Å | Cell parameters from 2088 reflections |
| b = 9.003 (4) Å | θ = 2.4–27.5° |
| c = 12.216 (6) Å | µ = 1.97 mm−1 |
| α = 79.641 (14)° | T = 293 K |
| β = 84.646 (14)° | Block, yellow |
| γ = 72.154 (12)° | 0.30 × 0.25 × 0.20 mm |
| V = 822.4 (7) Å3 |
Data collection
| Rigaku SCXmini diffractometer | 3775 independent reflections |
| Radiation source: fine-focus sealed tube | 3124 reflections with I > 2σ(I) |
| graphite | Rint = 0.035 |
| CCD_Profile_fitting scans | θmax = 27.5°, θmin = 1.7° |
| Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | h = −10→10 |
| Tmin = 0.559, Tmax = 0.674 | k = −11→11 |
| 9065 measured reflections | l = −15→15 |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.039 | H-atom parameters constrained |
| wR(F2) = 0.123 | w = 1/[σ2(Fo2) + (0.0636P)2] where P = (Fo2 + 2Fc2)/3 |
| S = 1.17 | (Δ/σ)max = 0.001 |
| 3775 reflections | Δρmax = 0.59 e Å−3 |
| 174 parameters | Δρmin = −0.66 e Å−3 |
| 0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008) |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.0014 (1) |
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 | ||
| Cu1 | 0.91120 (5) | 0.05748 (5) | 0.21071 (3) | 0.01639 (14) | |
| C1 | 0.8790 (5) | 0.4965 (4) | −0.1245 (3) | 0.0203 (7) | |
| H1 | 0.9490 | 0.4905 | −0.1897 | 0.024* | |
| C2 | 0.8332 (5) | 0.3759 (4) | −0.0584 (3) | 0.0192 (7) | |
| H2 | 0.8657 | 0.2709 | −0.0691 | 0.023* | |
| C3 | 0.7099 (4) | 0.5947 (4) | 0.0167 (3) | 0.0183 (7) | |
| C4 | 0.6042 (5) | 0.7072 (4) | 0.0911 (3) | 0.0250 (8) | |
| H4A | 0.5023 | 0.7782 | 0.0523 | 0.030* | |
| H4B | 0.6747 | 0.7704 | 0.1076 | 0.030* | |
| C5 | 0.5432 (5) | 0.6239 (5) | 0.1994 (3) | 0.0285 (9) | |
| H5A | 0.4760 | 0.5588 | 0.1835 | 0.043* | |
| H5B | 0.4713 | 0.7010 | 0.2426 | 0.043* | |
| H5C | 0.6436 | 0.5591 | 0.2406 | 0.043* | |
| C6 | 0.7322 (5) | 0.0989 (4) | 0.5488 (3) | 0.0223 (8) | |
| H6 | 0.8545 | 0.0669 | 0.5483 | 0.027* | |
| C7 | 0.6228 (5) | 0.0601 (4) | 0.6319 (3) | 0.0208 (7) | |
| H7 | 0.6544 | −0.0045 | 0.6998 | 0.025* | |
| C8 | 0.4588 (5) | 0.2168 (4) | 0.4944 (3) | 0.0177 (7) | |
| C9 | 0.3058 (5) | 0.3210 (4) | 0.4307 (3) | 0.0257 (8) | |
| H9A | 0.2071 | 0.2783 | 0.4487 | 0.031* | |
| H9B | 0.3347 | 0.3231 | 0.3517 | 0.031* | |
| C10 | 0.2529 (6) | 0.4888 (5) | 0.4567 (4) | 0.0397 (11) | |
| H10A | 0.2191 | 0.4877 | 0.5343 | 0.060* | |
| H10B | 0.1557 | 0.5535 | 0.4126 | 0.060* | |
| H10C | 0.3507 | 0.5311 | 0.4397 | 0.060* | |
| Cl1 | 1.16150 (11) | 0.01933 (9) | 0.10773 (7) | 0.01903 (19) | |
| Cl2 | 0.61789 (11) | 0.16204 (10) | 0.18983 (7) | 0.0194 (2) | |
| Cl3 | 0.94259 (11) | 0.24838 (10) | 0.29860 (7) | 0.0204 (2) | |
| Cl4 | 0.91629 (11) | −0.19331 (10) | 0.27848 (8) | 0.0233 (2) | |
| N1 | 0.8018 (4) | 0.6294 (3) | −0.0763 (2) | 0.0193 (6) | |
| H1A | 0.8113 | 0.7219 | −0.1024 | 0.023* | |
| N2 | 0.7279 (4) | 0.4409 (3) | 0.0285 (2) | 0.0187 (6) | |
| H2A | 0.6811 | 0.3891 | 0.0823 | 0.022* | |
| N3 | 0.6284 (4) | 0.1948 (3) | 0.4648 (2) | 0.0201 (6) | |
| H3A | 0.6673 | 0.2350 | 0.4020 | 0.024* | |
| N4 | 0.4552 (4) | 0.1350 (3) | 0.5963 (2) | 0.0186 (6) | |
| H4C | 0.3608 | 0.1298 | 0.6347 | 0.022* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cu1 | 0.0145 (2) | 0.0147 (2) | 0.0195 (2) | −0.00468 (17) | 0.00088 (16) | −0.00158 (16) |
| C1 | 0.0197 (18) | 0.0200 (17) | 0.0211 (18) | −0.0069 (14) | −0.0028 (14) | −0.0008 (14) |
| C2 | 0.0228 (18) | 0.0141 (16) | 0.0215 (18) | −0.0061 (14) | 0.0004 (14) | −0.0046 (13) |
| C3 | 0.0176 (17) | 0.0170 (16) | 0.0219 (18) | −0.0063 (14) | −0.0059 (14) | −0.0029 (13) |
| C4 | 0.029 (2) | 0.0196 (18) | 0.027 (2) | −0.0036 (16) | −0.0039 (16) | −0.0077 (15) |
| C5 | 0.029 (2) | 0.029 (2) | 0.025 (2) | 0.0003 (17) | −0.0018 (16) | −0.0111 (16) |
| C6 | 0.0176 (17) | 0.0208 (18) | 0.026 (2) | −0.0031 (14) | 0.0002 (15) | −0.0040 (15) |
| C7 | 0.0209 (18) | 0.0199 (17) | 0.0191 (18) | −0.0021 (14) | −0.0051 (14) | −0.0012 (14) |
| C8 | 0.0213 (18) | 0.0142 (16) | 0.0181 (17) | −0.0053 (14) | 0.0002 (14) | −0.0046 (13) |
| C9 | 0.0232 (19) | 0.0235 (19) | 0.028 (2) | 0.0009 (16) | −0.0101 (16) | −0.0062 (16) |
| C10 | 0.042 (3) | 0.023 (2) | 0.048 (3) | 0.0048 (19) | −0.020 (2) | −0.0072 (19) |
| Cl1 | 0.0178 (4) | 0.0166 (4) | 0.0227 (4) | −0.0061 (3) | 0.0043 (3) | −0.0042 (3) |
| Cl2 | 0.0147 (4) | 0.0207 (4) | 0.0209 (4) | −0.0052 (3) | −0.0015 (3) | 0.0019 (3) |
| Cl3 | 0.0213 (4) | 0.0221 (4) | 0.0206 (4) | −0.0103 (3) | 0.0030 (3) | −0.0061 (3) |
| Cl4 | 0.0208 (4) | 0.0152 (4) | 0.0293 (5) | −0.0035 (3) | 0.0054 (4) | 0.0017 (3) |
| N1 | 0.0217 (15) | 0.0157 (14) | 0.0206 (15) | −0.0080 (12) | −0.0038 (12) | 0.0027 (12) |
| N2 | 0.0195 (15) | 0.0158 (14) | 0.0195 (15) | −0.0052 (12) | −0.0007 (12) | 0.0006 (11) |
| N3 | 0.0221 (16) | 0.0188 (14) | 0.0177 (15) | −0.0058 (12) | 0.0012 (12) | 0.0000 (12) |
| N4 | 0.0161 (14) | 0.0221 (15) | 0.0181 (15) | −0.0067 (12) | 0.0034 (12) | −0.0048 (12) |
Geometric parameters (Å, °)
| Cu1—Cl1 | 2.2287 (13) | C6—C7 | 1.346 (5) |
| Cu1—Cl4 | 2.2501 (13) | C6—N3 | 1.374 (4) |
| Cu1—Cl2 | 2.2625 (14) | C6—H6 | 0.9300 |
| Cu1—Cl3 | 2.2688 (12) | C7—N4 | 1.374 (4) |
| C1—C2 | 1.355 (5) | C7—H7 | 0.9300 |
| C1—N1 | 1.375 (5) | C8—N4 | 1.330 (4) |
| C1—H1 | 0.9300 | C8—N3 | 1.333 (4) |
| C2—N2 | 1.391 (4) | C8—C9 | 1.481 (5) |
| C2—H2 | 0.9300 | C9—C10 | 1.523 (5) |
| C3—N2 | 1.330 (4) | C9—H9A | 0.9700 |
| C3—N1 | 1.335 (5) | C9—H9B | 0.9700 |
| C3—C4 | 1.493 (5) | C10—H10A | 0.9600 |
| C4—C5 | 1.516 (6) | C10—H10B | 0.9600 |
| C4—H4A | 0.9700 | C10—H10C | 0.9600 |
| C4—H4B | 0.9700 | N1—H1A | 0.8600 |
| C5—H5A | 0.9600 | N2—H2A | 0.8600 |
| C5—H5B | 0.9600 | N3—H3A | 0.8600 |
| C5—H5C | 0.9600 | N4—H4C | 0.8600 |
| Cl1—Cu1—Cl4 | 101.08 (4) | C6—C7—N4 | 106.2 (3) |
| Cl1—Cu1—Cl2 | 139.56 (4) | C6—C7—H7 | 126.9 |
| Cl4—Cu1—Cl2 | 98.32 (4) | N4—C7—H7 | 126.9 |
| Cl1—Cu1—Cl3 | 97.91 (4) | N4—C8—N3 | 105.9 (3) |
| Cl4—Cu1—Cl3 | 130.13 (5) | N4—C8—C9 | 126.9 (3) |
| Cl2—Cu1—Cl3 | 96.09 (4) | N3—C8—C9 | 127.0 (3) |
| C2—C1—N1 | 106.7 (3) | C8—C9—C10 | 111.8 (3) |
| C2—C1—H1 | 126.7 | C8—C9—H9A | 109.3 |
| N1—C1—H1 | 126.7 | C10—C9—H9A | 109.3 |
| C1—C2—N2 | 106.1 (3) | C8—C9—H9B | 109.3 |
| C1—C2—H2 | 127.0 | C10—C9—H9B | 109.3 |
| N2—C2—H2 | 127.0 | H9A—C9—H9B | 107.9 |
| N2—C3—N1 | 106.5 (3) | C9—C10—H10A | 109.5 |
| N2—C3—C4 | 126.7 (3) | C9—C10—H10B | 109.5 |
| N1—C3—C4 | 126.8 (3) | H10A—C10—H10B | 109.5 |
| C3—C4—C5 | 112.6 (3) | C9—C10—H10C | 109.5 |
| C3—C4—H4A | 109.1 | H10A—C10—H10C | 109.5 |
| C5—C4—H4A | 109.1 | H10B—C10—H10C | 109.5 |
| C3—C4—H4B | 109.1 | C3—N1—C1 | 110.5 (3) |
| C5—C4—H4B | 109.1 | C3—N1—H1A | 124.7 |
| H4A—C4—H4B | 107.8 | C1—N1—H1A | 124.7 |
| C4—C5—H5A | 109.5 | C3—N2—C2 | 110.3 (3) |
| C4—C5—H5B | 109.5 | C3—N2—H2A | 124.9 |
| H5A—C5—H5B | 109.5 | C2—N2—H2A | 124.9 |
| C4—C5—H5C | 109.5 | C8—N3—C6 | 110.3 (3) |
| H5A—C5—H5C | 109.5 | C8—N3—H3A | 124.8 |
| H5B—C5—H5C | 109.5 | C6—N3—H3A | 124.8 |
| C7—C6—N3 | 106.8 (3) | C8—N4—C7 | 110.8 (3) |
| C7—C6—H6 | 126.6 | C8—N4—H4C | 124.6 |
| N3—C6—H6 | 126.6 | C7—N4—H4C | 124.6 |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1A···Cl1i | 0.86 | 2.39 | 3.217 (3) | 160 |
| N2—H2A···Cl2 | 0.86 | 2.39 | 3.195 (3) | 157 |
| N3—H3A···Cl3 | 0.86 | 2.46 | 3.178 (3) | 142 |
| N4—H4C···Cl4ii | 0.86 | 2.32 | 3.149 (3) | 164 |
Symmetry codes: (i) −x+2, −y+1, −z; (ii) −x+1, −y, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: VM2067).
References
- Fu, D.-W., Ge, J.-Z., Dai, J., Ye, H.-Y. & Qu, Z.-R. (2009). Inorg. Chem. Commun. 12, 994–997.
- Rigaku (2005). CrystalClear Rigaku Corporation, Tokyo, Japan.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Ye, Q., Song, Y.-M., Wang, G.-X., Chen, K. & Fu, D.-W. (2006). J. Am. Chem. Soc. 128, 6554–6555. [DOI] [PubMed]
- Zhang, W., Xiong, R.-G. & Huang, S.-P. D. (2008). J. Am. Chem. Soc. 130, 10468–10469. [DOI] [PubMed]
- Zhang, W., Ye, H.-Y., Cai, H.-L., Ge, J.-Z. & Xiong, R.-G. (2010). J. Am. Chem. Soc. 132, 7300–7302. [DOI] [PubMed]
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/S160053681005261X/vm2067sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S160053681005261X/vm2067Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


