| Literature DB >> 21201846 |
Shouwen Jin, Daqi Wang, Yan-Lin Yu, Guan-Min Luo, Yan-Yan Ye.
Abstract
In the title compound, [Cu(C(4)H(4)O(4))(NH(3))(2)](n), the Cu atom is coordinated by the N atoms of two ammonia mol-ecules and four O atoms from three different succinate ligands in a highly distorted octa-hedral geometry. The Cu atom and the C and O atoms of the succinate ligands lie on a mirror plane. Two adjacent CuO(4)N(2) octa-hedra share one common O-O edge, forming a Cu(2)O(6)N(4) biocta-hedron with a Cu⋯Cu separation of 3.524 (2) Å. Neighboring biocta-hedra are connected by bis-unidentate succinate anions in the a-axis direction, while in the c-axis direction biocta-hedra are connected by bis-bidentate succinate anions, leading to an infinite two-dimensional network structure. These networks are further connected along the a-axis direction by hydrogen bonds between ammonia ligands and carboxyl-ate O atoms of neighboring network layers, forming a three-dimensional lamellar structure.Entities:
Year: 2008 PMID: 21201846 PMCID: PMC2960840 DOI: 10.1107/S1600536808002493
Source DB: PubMed Journal: Acta Crystallogr Sect E Struct Rep Online ISSN: 1600-5368
| [Cu(C4H4O4)(NH3)2] | |
| Monoclinic, | Mo |
| Hall symbol: -C 2y | Cell parameters from 1618 reflections |
| θ = 2.8–28.2º | |
| µ = 2.97 mm−1 | |
| β = 124.515 (4)º | Block, blue |
| 0.27 × 0.15 × 0.09 mm | |
| Bruker SMART APEX CCD diffractometer | 694 independent reflections |
| Radiation source: fine-focus sealed tube | 641 reflections with |
| Monochromator: graphite | |
| θmax = 25.0º | |
| φ and ω scans | θmin = 2.8º |
| Absorption correction: multi-scan(SADABS; Sheldrick, 1996) | |
| 1874 measured reflections |
| Refinement on | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| H-atom parameters constrained | |
| | |
| (Δ/σ)max = 0.001 | |
| 694 reflections | Δρmax = 0.37 e Å−3 |
| 64 parameters | Δρmin = −0.58 e Å−3 |
| Primary atom site location: structure-invariant direct methods | Extinction correction: none |
| 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 |
| Cu1 | 0.84469 (3) | 0.5000 | 0.85475 (5) | 0.0211 (2) | |
| O1 | 0.9788 (2) | 0.5000 | 0.8255 (3) | 0.0239 (6) | |
| O2 | 0.8291 (2) | 0.5000 | 0.5275 (4) | 0.0387 (8) | |
| O3 | 0.7184 (2) | 0.5000 | 0.8984 (4) | 0.0280 (6) | |
| O4 | 0.5330 (2) | 0.5000 | 0.8099 (4) | 0.0381 (7) | |
| N1 | 0.83799 (18) | 0.7693 (4) | 0.8316 (3) | 0.0280 (5) | |
| H1 | 0.8335 | 0.8263 | 0.9134 | 0.042* | |
| H2 | 0.7797 | 0.8073 | 0.7251 | 0.042* | |
| H3 | 0.8990 | 0.8131 | 0.8407 | 0.042* | |
| C1 | 0.9363 (3) | 0.5000 | 0.6510 (5) | 0.0223 (8) | |
| C2 | 1.0265 (3) | 0.5000 | 0.6041 (5) | 0.0275 (9) | |
| H2A | 1.0763 | 0.3939 | 0.6599 | 0.033* | |
| C3 | 0.6069 (3) | 0.5000 | 0.7718 (5) | 0.0241 (8) | |
| C4 | 0.5663 (3) | 0.5000 | 0.5694 (5) | 0.0261 (8) | |
| H4 | 0.5987 | 0.3939 | 0.5480 | 0.031* |
| Cu1 | 0.0203 (3) | 0.0245 (3) | 0.0180 (3) | 0.000 | 0.0106 (2) | 0.000 |
| O1 | 0.0217 (13) | 0.0359 (16) | 0.0144 (12) | 0.000 | 0.0104 (11) | 0.000 |
| O2 | 0.0267 (15) | 0.068 (2) | 0.0187 (13) | 0.000 | 0.0111 (12) | 0.000 |
| O3 | 0.0188 (13) | 0.0446 (17) | 0.0191 (12) | 0.000 | 0.0097 (11) | 0.000 |
| O4 | 0.0252 (15) | 0.066 (2) | 0.0255 (14) | 0.000 | 0.0159 (12) | 0.000 |
| N1 | 0.0283 (12) | 0.0266 (14) | 0.0233 (11) | 0.0018 (10) | 0.0111 (10) | −0.0004 (10) |
| C1 | 0.0249 (18) | 0.024 (2) | 0.0183 (16) | 0.000 | 0.0127 (15) | 0.000 |
| C2 | 0.0256 (19) | 0.039 (2) | 0.0200 (19) | 0.000 | 0.0139 (16) | 0.000 |
| C3 | 0.0256 (19) | 0.0239 (19) | 0.0215 (17) | 0.000 | 0.0126 (16) | 0.000 |
| C4 | 0.028 (2) | 0.031 (2) | 0.0179 (17) | 0.000 | 0.0118 (17) | 0.000 |
| Cu1—O3 | 1.978 (3) | N1—H2 | 0.8599 |
| Cu1—N1i | 1.993 (3) | N1—H3 | 0.8599 |
| Cu1—N1 | 1.993 (3) | C1—C2 | 1.510 (5) |
| Cu1—O1 | 2.001 (3) | C2—C2ii | 1.524 (7) |
| O1—C1 | 1.282 (4) | C2—H2A | 0.9698 |
| O2—C1 | 1.240 (5) | C3—C4 | 1.517 (5) |
| O3—C3 | 1.286 (5) | C4—C4iii | 1.514 (7) |
| O4—C3 | 1.236 (5) | C4—H4 | 0.9696 |
| N1—H1 | 0.8599 | ||
| O3—Cu1—N1i | 91.38 (6) | H2—N1—H3 | 104.0 |
| O3—Cu1—N1 | 91.38 (6) | O2—C1—O1 | 123.2 (3) |
| N1i—Cu1—N1 | 170.34 (12) | O2—C1—C2 | 121.5 (3) |
| O3—Cu1—O1 | 176.92 (9) | O1—C1—C2 | 115.3 (3) |
| N1i—Cu1—O1 | 88.87 (6) | C1—C2—C2ii | 114.1 (4) |
| N1—Cu1—O1 | 88.87 (6) | C1—C2—H2A | 108.7 |
| C1—O1—Cu1 | 108.5 (2) | C2ii—C2—H2A | 108.8 |
| C3—O3—Cu1 | 125.9 (2) | O4—C3—O3 | 122.2 (3) |
| Cu1—N1—H1 | 115.1 | O4—C3—C4 | 119.7 (3) |
| Cu1—N1—H2 | 113.3 | O3—C3—C4 | 118.1 (3) |
| H1—N1—H2 | 105.8 | C4iii—C4—C3 | 114.3 (4) |
| Cu1—N1—H3 | 112.2 | C4iii—C4—H4 | 108.9 |
| H1—N1—H3 | 105.4 | C3—C4—H4 | 108.5 |
| O3—Cu1—O1—C1 | 180.000 (10) | Cu1—O1—C1—C2 | 180.000 (1) |
| N1i—Cu1—O1—C1 | 85.31 (6) | O2—C1—C2—C2ii | 0.000 (1) |
| N1—Cu1—O1—C1 | −85.31 (6) | O1—C1—C2—C2ii | 180.000 (2) |
| N1i—Cu1—O3—C3 | −85.37 (6) | Cu1—O3—C3—O4 | 180.000 (1) |
| N1—Cu1—O3—C3 | 85.37 (6) | Cu1—O3—C3—C4 | 0.000 (2) |
| O1—Cu1—O3—C3 | 180.000 (12) | O4—C3—C4—C4iii | 0.0 |
| Cu1—O1—C1—O2 | 0.0 | O3—C3—C4—C4iii | 180.000 (2) |
| H··· | ||||
| N1—H3···O4iv | 0.86 | 2.44 | 3.272 (3) | 164 |
| N1—H2···O2v | 0.86 | 2.32 | 3.133 (3) | 159 |
| N1—H1···O3vi | 0.86 | 2.48 | 3.331 (3) | 169 |
| N1—H1···O4vi | 0.86 | 2.41 | 3.085 (3) | 136 |
Hydrogen-bond geometry (Å, °)
| H⋯ | ||||
|---|---|---|---|---|
| N1—H3⋯O4i | 0.86 | 2.44 | 3.272 (3) | 164 |
| N1—H2⋯O2ii | 0.86 | 2.32 | 3.133 (3) | 159 |
| N1—H1⋯O3iii | 0.86 | 2.48 | 3.331 (3) | 169 |
| N1—H1⋯O4iii | 0.86 | 2.41 | 3.085 (3) | 136 |
Symmetry codes: (i) ; (ii) ; (iii) .