metal-organic compounds
(2-Aminoethan-1-aminium-κN2)trichloridozinc(II)
aInorganic and Analytical Chemistry Laboratory, Department of Chemistry, Faculty of Science and Technology, Cheikh Anta Diop University, Dakar, Senegal, bInstitute for Molecules & Materials (IMM), Solid State Chemistry, Faculty of Science, Radboud University, Nijmegen, The Netherlands, cDepartement of Chemical and Pharmaceutical Sciences, University of Trieste, Trieste, Italy, and dInorganic and Analytical Chemistry Laboratory, Departement of Chemistry, Faculty of Science and Technology, Cheikh Anta Diop University, Dakar, Senegal
*Correspondence e-mail: [email protected]
The mononuclear zwitterionic ZnII complex, [ZnCl3(C2H9N2)], contains a monodentate 2-ammonioethylamine moiety and three chloride anions coordinating to the central zinc atom in form of a distorted tetrahedron. The molecular packing shows amine and ammonium groups interacting through hydrogen-bonding interactions with chlorine atoms of symmetry-related complexes to form a supramolecular framework structure.
Keywords: crystal structure; zinc(II); zwitterionic complex; ethylenediamine.
CCDC reference: 2483701
Structure description
Zwitterionic trichloridozinc(II) complexes with the metal additionally ligated in a monodentate manner by a protonated organic molecule are known (Clemente et al., 2002
; Maixner & Zachová, 1993
; Purnell & Hodgson, 1976
; Sheldrick, 1982
; Steffen & Palenik, 1978
; Zhu et al., 2002
), including a protonated quinine ligand (Kang et al., 2013
). The commonly used ethylenediamine (en) ligand acts primarily as a chelating ligand, and monodentate (Fanshawe et al., 2000
) or bridging forms (Çolak et al., 2008
) of en are rather rare. An example of a protonated and monodentate en ligand has been reported within a germanotungstate polyanion composed of two [GeW9O34]10– moieties sandwiching a rhomboid-like Zn4 cluster, in which two central ZnII atoms are coordinated by the N atom of the non-protonated amino group (Wang et al. 2010
). In this context, we synthesized the title complex [ZnCl3(C2H9N2)] using en, hydrochloric acid and zinc chloride as starting materials.
The molecular structure of [ZnCl3(C2H9N2)] is characterized by a protonated en ligand, monodentately binding through the amine N atom (N1) to the central ZnII atom. The tetrahedral coordination environment is completed by three Cl− ligands (Fig. 1
). The Zn—N bond length is 2.0345 (10) Å, much shorter than the values found in the ZnII complexes with chelating ethylendiamine (en) ligands, for example [Zn(en)(acetate)2] (Kim et al., 2007
) where the Zn—N distance is 2.0784 (16) Å, or in the complex octahedral cation [Zn(en)3]2+ (Cheng et al., 2008
) with distances between 2.159 (2) and 2.220 (2). The present Zn—N bond length is also considerably shorter than in the germanotungstate cluster comprising a ZnII atom bound to a monodentate en ligand [2.121 (16) Å; Wang et al., 2010
]. The three Zn—Cl bond lengths in the title complex range from 2.2600 (3) to 2.2686 (3) Å, which is comparable to those previously reported in the complexes having a ZnCl3 moiety mentioned above. The present Cl—Zn—Cl and N—Zn—Cl bond angles vary from 104.52 (3) to 115.969 (12)°, indicating a considerable distortion from an ideal tetrahedron. The protonated en ligand has an anti-conformation with an N1—C1—C2—N2 torsion angle of 178.18 (10)°.
| Figure 1 Molecular structure of the title complex with displacement ellipsoids drawn at the 50% probability level. |
The molecular packing is stabilized by an intricate framework of intermolecular N—H⋯Cl hydrogen bonds involving both the amine (N1) and ammonium (N2) groups as donors and all three Cl ligands as acceptor atoms (Table 1
). Part of the crystal packing is illustrated in Fig. 2
.
|
| Figure 2 Partial view of the molecular packing in the crystal of the title complex with N—H⋯Cl hydrogen bonds indicated as dashed lines |
Synthesis and crystallization
The title complex was obtained by addition of a methanolic solution (10 ml) of ZnCl2 (0.136 g, 1 mmol) to a flask containing 10 ml of a methanolic solution of ethylenediamine, C2H8N2 (0.06 g, 1 mmol) and 5 ml of hydrochloric acid HCl (1 N). The resulting mixture was stirred for 2 h at room temperature. A clear solution was obtained and left to evaporate slowly at room temperature, leading to colorless single crystals suitable for single-crystal X-ray diffraction after 24 h.
Refinement
Crystal data, data collection and structure details are summarized in Table 2
.
|
Structural data
CCDC reference: 2483701
contains datablock I. DOI: https://doi.org/10.1107/S2414314625007710/wm4235sup1.cif
Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2414314625007710/wm4235Isup3.hkl
| [ZnCl3(C2H9N2)] | Dx = 1.936 Mg m−3 |
| Mr = 232.83 | Mo Kα radiation, λ = 0.71073 Å |
| Orthorhombic, P212121 | Cell parameters from 7854 reflections |
| a = 6.6669 (4) Å | θ = 1.9–25.0° |
| b = 8.1192 (4) Å | µ = 3.99 mm−1 |
| c = 14.7559 (7) Å | T = 150 K |
| V = 798.74 (7) Å3 | Block, colorless |
| Z = 4 | 0.24 × 0.13 × 0.11 mm |
| F(000) = 464 |
| Bruker APEX CCD area-detector diffractometer | 3036 independent reflections |
| Radiation source: fine-focus sealed tube | 3017 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.020 |
| ω scans | θmax = 33.2°, θmin = 2.8° |
| Absorption correction: multi-scan (SADABS; Krause et al., 2015) | h = −9→10 |
| Tmin = 0.407, Tmax = 0.520 | k = −12→12 |
| 11232 measured reflections | l = −22→22 |
| Refinement on F2 | Hydrogen site location: difference Fourier map |
| Least-squares matrix: full | Only H-atom coordinates refined |
| R[F2 > 2σ(F2)] = 0.012 | w = 1/[σ2(Fo2) + (0.0075P)2 + 0.0649P] where P = (Fo2 + 2Fc2)/3 |
| wR(F2) = 0.026 | (Δ/σ)max = 0.002 |
| S = 1.12 | Δρmax = 0.28 e Å−3 |
| 3036 reflections | Δρmin = −0.33 e Å−3 |
| 101 parameters | Absolute structure: Refined as an inversion twin Parsons et al., 2013] |
| 0 restraints | Absolute structure parameter: 0.374 (5) |
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes. |
Refinement. Refined as a 2-component inversion twin. H atoms were freely refined with Uiso(H) 1.2× or 1.5×Ueq of the parent atom. The was refined as a two-component [Flack parameter = 0.374 (5); Parsons et al., 2013]. |
| x | y | z | Uiso*/Ueq | ||
| Zn1 | 0.45714 (2) | 0.91365 (2) | 0.38549 (2) | 0.01331 (3) | |
| Cl1 | 0.29829 (4) | 0.98873 (3) | 0.25628 (2) | 0.01659 (5) | |
| Cl2 | 0.79364 (4) | 0.95070 (4) | 0.37517 (2) | 0.01909 (5) | |
| Cl3 | 0.30307 (5) | 1.04462 (3) | 0.50133 (2) | 0.01698 (5) | |
| N1 | 0.42319 (16) | 0.66776 (12) | 0.40719 (7) | 0.01523 (18) | |
| H1A | 0.535 (3) | 0.620 (2) | 0.3886 (11) | 0.018* | |
| H1B | 0.427 (3) | 0.642 (2) | 0.4615 (12) | 0.018* | |
| N2 | 0.08625 (17) | 0.31486 (12) | 0.33981 (8) | 0.0185 (2) | |
| H2A | −0.023 (3) | 0.342 (2) | 0.3659 (12) | 0.028* | |
| H2B | 0.105 (3) | 0.209 (2) | 0.3455 (12) | 0.028* | |
| H2C | 0.074 (3) | 0.338 (2) | 0.2865 (14) | 0.028* | |
| C1 | 0.25042 (17) | 0.58592 (14) | 0.36385 (7) | 0.01499 (19) | |
| H1C | 0.260 (3) | 0.612 (2) | 0.2975 (11) | 0.018* | |
| H1D | 0.129 (3) | 0.631 (2) | 0.3899 (11) | 0.018* | |
| C2 | 0.26187 (17) | 0.40102 (13) | 0.38011 (8) | 0.01628 (19) | |
| H2E | 0.374 (3) | 0.356 (2) | 0.3522 (11) | 0.020* | |
| H2D | 0.265 (3) | 0.3787 (19) | 0.4438 (12) | 0.020* |
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Zn1 | 0.01369 (6) | 0.01376 (5) | 0.01250 (5) | −0.00133 (4) | −0.00035 (5) | 0.00047 (4) |
| Cl1 | 0.01636 (12) | 0.02048 (10) | 0.01292 (10) | 0.00025 (10) | −0.00161 (9) | 0.00117 (8) |
| Cl2 | 0.01381 (11) | 0.02772 (12) | 0.01575 (11) | −0.00389 (10) | −0.00020 (9) | 0.00146 (9) |
| Cl3 | 0.01857 (12) | 0.01778 (10) | 0.01460 (10) | −0.00088 (9) | 0.00209 (9) | −0.00156 (8) |
| N1 | 0.0162 (5) | 0.0142 (4) | 0.0153 (4) | −0.0002 (3) | −0.0010 (3) | 0.0007 (3) |
| N2 | 0.0190 (5) | 0.0143 (4) | 0.0222 (5) | −0.0001 (3) | −0.0010 (4) | −0.0024 (4) |
| C1 | 0.0161 (5) | 0.0123 (4) | 0.0165 (4) | 0.0001 (4) | −0.0016 (3) | 0.0011 (4) |
| C2 | 0.0162 (5) | 0.0128 (4) | 0.0198 (5) | −0.0001 (3) | −0.0024 (4) | 0.0012 (4) |
| Zn1—N1 | 2.0345 (10) | N2—H2A | 0.85 (2) |
| Zn1—Cl3 | 2.2600 (3) | N2—H2B | 0.87 (2) |
| Zn1—Cl1 | 2.2646 (3) | N2—H2C | 0.81 (2) |
| Zn1—Cl2 | 2.2686 (3) | C1—C2 | 1.5222 (15) |
| N1—C1 | 1.4755 (15) | C1—H1C | 1.003 (16) |
| N1—H1A | 0.883 (18) | C1—H1D | 0.967 (18) |
| N1—H1B | 0.828 (17) | C2—H2E | 0.930 (18) |
| N2—C2 | 1.4879 (16) | C2—H2D | 0.958 (17) |
| N1—Zn1—Cl3 | 106.99 (3) | C2—N2—H2C | 110.9 (14) |
| N1—Zn1—Cl1 | 110.15 (3) | H2A—N2—H2C | 107.2 (19) |
| Cl3—Zn1—Cl1 | 107.313 (12) | H2B—N2—H2C | 109.4 (18) |
| N1—Zn1—Cl2 | 104.52 (3) | N1—C1—C2 | 109.68 (9) |
| Cl3—Zn1—Cl2 | 115.969 (12) | N1—C1—H1C | 106.1 (10) |
| Cl1—Zn1—Cl2 | 111.728 (11) | C2—C1—H1C | 110.9 (9) |
| C1—N1—Zn1 | 117.43 (7) | N1—C1—H1D | 108.1 (10) |
| C1—N1—H1A | 109.2 (11) | C2—C1—H1D | 110.6 (10) |
| Zn1—N1—H1A | 106.5 (11) | H1C—C1—H1D | 111.2 (14) |
| C1—N1—H1B | 109.4 (13) | N2—C2—C1 | 111.18 (9) |
| Zn1—N1—H1B | 113.2 (11) | N2—C2—H2E | 105.8 (11) |
| H1A—N1—H1B | 99.6 (16) | C1—C2—H2E | 111.0 (11) |
| C2—N2—H2A | 112.0 (13) | N2—C2—H2D | 108.7 (11) |
| C2—N2—H2B | 108.0 (14) | C1—C2—H2D | 110.0 (10) |
| H2A—N2—H2B | 109.3 (19) | H2E—C2—H2D | 110.1 (16) |
| Zn1—N1—C1—C2 | 174.46 (7) | N1—C1—C2—N2 | 178.18 (10) |
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1A···Cl1i | 0.883 (18) | 2.636 (17) | 3.3733 (11) | 141.7 (14) |
| N1—H1B···Cl2ii | 0.828 (17) | 2.678 (18) | 3.4620 (11) | 158.6 (17) |
| N2—H2A···Cl3ii | 0.85 (2) | 2.46 (2) | 3.2188 (12) | 149.2 (17) |
| N2—H2B···Cl1iii | 0.87 (2) | 2.566 (19) | 3.2449 (11) | 135.2 (16) |
| N2—H2C···Cl2i | 0.81 (2) | 2.70 (2) | 3.4526 (12) | 154.2 (19) |
| Symmetry codes: (i) −x+1, y−1/2, −z+1/2; (ii) x−1/2, −y+3/2, −z+1; (iii) x, y−1, z. |
Acknowledgements
The authors thank the Solid State Chemistry Department of the Institute for Molecules and Materials (IMM), Radboud University, The Netherlands.
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