Abstract
In the neutral title complex, [HgCl2(C12H11NO3)], the HgII ion is pentacoordinated by two Cl atoms, one N atom and two weakly coordinating O atoms from the methyl 2-(quinolin-8-yloxy)acetate ligand. The coordination around the HgII ion may be described as highly distorted trigonal–bipyramidal. Centrosymmetric dimers are formed by an additional weak Hg⋯Cl interaction, leading to a distorted octahedral coordination geometry around the HgII ion.
Related literature
For the use of quinolin-8-yloxy acetic acid and its derivatives as ligands in transition metal complexes, see: Cheng et al. (2007 ▶); Song et al. (2004 ▶); Wang et al. (2005 ▶, 2008 ▶).
Experimental
Crystal data
[HgCl2(C12H11NO3)]
M r = 488.71
Triclinic,
a = 7.2644 (4) Å
b = 9.7607 (2) Å
c = 10.8411 (6) Å
α = 71.317 (7)°
β = 75.453 (7)°
γ = 69.816 (8)°
V = 674.87 (5) Å3
Z = 2
Mo Kα radiation
μ = 11.80 mm−1
T = 223 K
0.50 × 0.25 × 0.10 mm
Data collection
Rigaku Saturn diffractometer
Absorption correction: multi-scan (REQAB; Jacobson, 1998 ▶) T min = 0.067, T max = 0.385
5090 measured reflections
2432 independent reflections
2330 reflections with I > 2σ(I)
R int = 0.050
Refinement
R[F 2 > 2σ(F 2)] = 0.052
wR(F 2) = 0.142
S = 1.07
2432 reflections
174 parameters
H-atom parameters constrained
Δρmax = 3.58 e Å−3
Δρmin = −2.39 e Å−3
Data collection: CrystalClear (Rigaku/MSC, 2001 ▶); cell refinement: CrystalClear; data reduction: CrystalStructure (Rigaku/MSC, 2004 ▶); 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: SHELXTL.
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812026591/im2385sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812026591/im2385Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Selected bond lengths (Å).
| Hg1—Cl1 | 2.340 (2) |
| Hg1—Cl2 | 2.350 (2) |
| Hg1—N1 | 2.463 (6) |
| Hg1—O1 | 2.746 (6) |
| Hg1—O3 | 2.876 (6) |
| Hg1—Cl1i | 3.204 (2) |
Symmetry code: (i)
.
Acknowledgments
The work was supported by the Science and Technology Foundation of the Ministry of Development of China (2010-K6–8).
supplementary crystallographic information
Comment
Quinolin-8-yloxy acetic acid and it's derivatives are well known ligands in transition metal coordination compounds (Cheng et al., 2007; Song et al., 2004; Wang et al., 2005; Wang et al., 2008). Some metal complexes with such ligands are being prepared because of their intriguing structural diversity and potential uses as functional materials (Cheng et al., 2007; Song et al., 2004; Wang et al., 2005; Wang et al., 2008). So, we prepared the title HgII complex with methyl-2-(quinoline-8-yloxy)-acetate ligand, (I).
In the title compound, the HgII atom is five-coordinated by two Cl atoms, one N atom and two O atoms from methyl-2-(quinoline-8-yloxy)-acetate ligand, forming a highly distorted trigonal bipyramidal geometry (Fig. 1). Hg—Cl bond lengths are 2.340 (2) and 2.350 (2) Å, and Hg—N bond lengths are 2.463 (6) Å. The weak coordinative Hg—O bond lengths are 2.746 (6) Å and 2.876 (6) Å. Angles around Hg are in a range of 56.55 (16)–153.41 (8)° (Table 1). If these are considered to be chemically signifcant interactions, two monoclear Hg complexes are formed into the centrosymmetric dimers by weak Hg—Cl interactions (Fig. 1). So, the coordination around Hg atom can act as a distrorted octahedral geometry.
The molecular packing is controlled by these dimers and intermolecular π-π interactions; the quinoline rings are separated by 3.527 (1) and 3.813 (1) Å (Fig. 2).
Experimental
Quinolin-8-yloxy acetic acid (0.0203 g, 0.1 mmol), HgCl2 (0.0272 g, 0.1 mmol), methanol (3 ml) and triethylamine (0.0101 g, 0.1 mmol) were placed in a thick Pyrex tube and heated to 130 C° for 5 days. After cooling at a rate of 5 C°/h to ambient temperature, yellow prismatic crystals were collected, washed with anhydrous ethanol, and dried at room temperature. The yield is 51% based on quinolin-8-yloxy acetic acid. Analysis found: C, 29.91; H, 2.30; N, 2.87%; calculated for C12H11Cl2HgNO3: C, 29.49; H, 2.27; N, 2.87%.
Refinement
H atoms were included in calculated positions and refined as riding, with C—H distances of 0.94 (aromatic), 0.98 (methylene) and 0.97 Å (methyl), and with Uiso(aromatic and ethyl) = 1.2Ueq(C) and Uiso(methylene) = 1.5Ueq(C).
Figures
Fig. 1.
The molecular structure of (I), with 30% probability displacement ellipsoids [symmetry codes: (i) 1 - x, -y, 2 - z]. The dashed line indicates the weak Hg···Cl interaction.
Fig. 2.
A view of intermolecular π-π interactions, interactions between the parallel quinoline rings of neighbouring complexes [symmetry codes: (i) 1 - x, 1 - y, 2 - z; (ii) -x, 1 - y, 2 - z].
Crystal data
| [HgCl2(C12H11NO3)] | Z = 2 |
| Mr = 488.71 | F(000) = 456 |
| Triclinic, P1 | Dx = 2.405 Mg m−3 |
| Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71075 Å |
| a = 7.2644 (4) Å | Cell parameters from 3438 reflections |
| b = 9.7607 (2) Å | θ = 3.0–27.5° |
| c = 10.8411 (6) Å | µ = 11.80 mm−1 |
| α = 71.317 (7)° | T = 223 K |
| β = 75.453 (7)° | Prism, yellow |
| γ = 69.816 (8)° | 0.50 × 0.25 × 0.10 mm |
| V = 674.87 (5) Å3 |
Data collection
| Rigaku Saturn diffractometer | 2432 independent reflections |
| Radiation source: fine-focus sealed tube | 2330 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.050 |
| Detector resolution: 14.63 pixels mm-1 | θmax = 25.5°, θmin = 3.0° |
| ω scans | h = −8→8 |
| Absorption correction: multi-scan (REQAB; Jacobson, 1998) | k = −11→9 |
| Tmin = 0.067, Tmax = 0.385 | l = −13→10 |
| 5090 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)] = 0.052 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.142 | H-atom parameters constrained |
| S = 1.07 | w = 1/[σ2(Fo2) + (0.114P)2] where P = (Fo2 + 2Fc2)/3 |
| 2432 reflections | (Δ/σ)max = 0.001 |
| 174 parameters | Δρmax = 3.58 e Å−3 |
| 0 restraints | Δρmin = −2.39 e Å−3 |
Special details
| 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. 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 > 2sigma(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 | ||
| Hg1 | 0.48080 (4) | 0.17195 (3) | 0.82524 (2) | 0.0283 (2) | |
| Cl1 | 0.7584 (4) | 0.0079 (3) | 0.9214 (2) | 0.0343 (5) | |
| Cl2 | 0.2251 (4) | 0.2330 (3) | 0.7032 (2) | 0.0328 (5) | |
| O1 | 0.5887 (9) | 0.4276 (6) | 0.6794 (5) | 0.0267 (12) | |
| O2 | 0.9795 (10) | 0.3004 (7) | 0.4386 (6) | 0.0293 (13) | |
| O3 | 0.7782 (11) | 0.1803 (7) | 0.5930 (6) | 0.0350 (15) | |
| N1 | 0.3624 (11) | 0.3914 (8) | 0.9197 (6) | 0.0229 (14) | |
| C1 | 0.2572 (13) | 0.3719 (9) | 1.0411 (8) | 0.0250 (17) | |
| H1 | 0.2485 | 0.2744 | 1.0883 | 0.030* | |
| C2 | 0.1591 (14) | 0.4918 (11) | 1.1008 (8) | 0.0291 (19) | |
| H2 | 0.0929 | 0.4727 | 1.1882 | 0.035* | |
| C3 | 0.1596 (13) | 0.6348 (10) | 1.0327 (8) | 0.0280 (18) | |
| H3 | 0.0892 | 0.7160 | 1.0707 | 0.034* | |
| C4 | 0.2680 (12) | 0.6597 (9) | 0.9034 (7) | 0.0229 (16) | |
| C5 | 0.2793 (15) | 0.8066 (10) | 0.8262 (9) | 0.032 (2) | |
| H5 | 0.2102 | 0.8915 | 0.8595 | 0.038* | |
| C6 | 0.3906 (15) | 0.8224 (9) | 0.7043 (9) | 0.0306 (19) | |
| H6 | 0.3995 | 0.9189 | 0.6541 | 0.037* | |
| C7 | 0.4920 (14) | 0.6985 (10) | 0.6522 (8) | 0.0288 (19) | |
| H7 | 0.5649 | 0.7133 | 0.5665 | 0.035* | |
| C8 | 0.4873 (13) | 0.5564 (9) | 0.7230 (8) | 0.0232 (16) | |
| C9 | 0.3727 (12) | 0.5317 (9) | 0.8506 (7) | 0.0226 (16) | |
| C10 | 0.7341 (16) | 0.4428 (10) | 0.5679 (8) | 0.030 (2) | |
| H10A | 0.8339 | 0.4787 | 0.5842 | 0.037* | |
| H10B | 0.6737 | 0.5164 | 0.4927 | 0.037* | |
| C11 | 0.8301 (13) | 0.2914 (9) | 0.5380 (7) | 0.0221 (16) | |
| C12 | 1.0873 (14) | 0.1595 (10) | 0.3990 (9) | 0.0313 (19) | |
| H12A | 1.1489 | 0.0841 | 0.4717 | 0.047* | |
| H12B | 1.1890 | 0.1780 | 0.3236 | 0.047* | |
| H12C | 0.9953 | 0.1234 | 0.3756 | 0.047* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Hg1 | 0.0304 (3) | 0.0247 (3) | 0.0247 (3) | −0.00519 (19) | −0.00101 (17) | −0.00514 (17) |
| Cl1 | 0.0304 (12) | 0.0320 (12) | 0.0350 (11) | −0.0028 (10) | −0.0050 (9) | −0.0083 (9) |
| Cl2 | 0.0360 (13) | 0.0344 (11) | 0.0255 (10) | −0.0096 (10) | −0.0038 (9) | −0.0057 (8) |
| O1 | 0.027 (3) | 0.025 (3) | 0.022 (3) | −0.011 (3) | 0.017 (2) | −0.009 (2) |
| O2 | 0.030 (3) | 0.025 (3) | 0.028 (3) | −0.006 (3) | 0.010 (3) | −0.012 (2) |
| O3 | 0.041 (4) | 0.025 (3) | 0.034 (3) | −0.013 (3) | 0.014 (3) | −0.012 (2) |
| N1 | 0.027 (4) | 0.023 (3) | 0.019 (3) | −0.008 (3) | 0.002 (3) | −0.009 (3) |
| C1 | 0.024 (4) | 0.030 (4) | 0.021 (4) | −0.007 (4) | 0.000 (3) | −0.009 (3) |
| C2 | 0.029 (5) | 0.039 (5) | 0.019 (4) | −0.012 (4) | 0.005 (4) | −0.012 (3) |
| C3 | 0.018 (4) | 0.038 (5) | 0.030 (4) | −0.005 (4) | 0.003 (3) | −0.019 (4) |
| C4 | 0.020 (4) | 0.024 (4) | 0.022 (4) | −0.001 (3) | 0.002 (3) | −0.011 (3) |
| C5 | 0.041 (6) | 0.025 (4) | 0.034 (4) | −0.012 (4) | 0.000 (4) | −0.014 (4) |
| C6 | 0.034 (5) | 0.017 (4) | 0.034 (5) | −0.004 (4) | −0.003 (4) | −0.003 (3) |
| C7 | 0.035 (5) | 0.028 (4) | 0.022 (4) | −0.009 (4) | −0.002 (4) | −0.005 (3) |
| C8 | 0.021 (4) | 0.020 (4) | 0.024 (4) | −0.003 (3) | 0.003 (3) | −0.009 (3) |
| C9 | 0.018 (4) | 0.030 (4) | 0.020 (3) | −0.006 (3) | −0.001 (3) | −0.009 (3) |
| C10 | 0.041 (6) | 0.032 (5) | 0.018 (4) | −0.015 (4) | 0.010 (4) | −0.012 (3) |
| C11 | 0.023 (4) | 0.024 (4) | 0.019 (4) | −0.009 (3) | 0.005 (3) | −0.008 (3) |
| C12 | 0.023 (5) | 0.029 (5) | 0.035 (5) | −0.002 (4) | 0.011 (4) | −0.018 (4) |
Geometric parameters (Å, º)
| Hg1—Cl1 | 2.340 (2) | C3—C4 | 1.416 (12) |
| Hg1—Cl2 | 2.350 (2) | C3—H3 | 0.9400 |
| Hg1—N1 | 2.463 (6) | C4—C9 | 1.432 (11) |
| Hg1—O1 | 2.746 (6) | C4—C5 | 1.428 (12) |
| Hg1—O3 | 2.876 (6) | C5—C6 | 1.357 (13) |
| Hg1—Cl1i | 3.204 (2) | C5—H5 | 0.9400 |
| O1—C8 | 1.383 (10) | C6—C7 | 1.392 (13) |
| O1—C10 | 1.396 (10) | C6—H6 | 0.9400 |
| O2—C11 | 1.329 (10) | C7—C8 | 1.361 (12) |
| O2—C12 | 1.468 (10) | C7—H7 | 0.9400 |
| O3—C11 | 1.195 (10) | C8—C9 | 1.418 (11) |
| N1—C1 | 1.337 (11) | C10—C11 | 1.502 (12) |
| N1—C9 | 1.352 (11) | C10—H10A | 0.9800 |
| C1—C2 | 1.405 (12) | C10—H10B | 0.9800 |
| C1—H1 | 0.9400 | C12—H12A | 0.9700 |
| C2—C3 | 1.355 (14) | C12—H12B | 0.9700 |
| C2—H2 | 0.9400 | C12—H12C | 0.9700 |
| Cl1—Hg1—Cl2 | 153.41 (8) | C3—C4—C5 | 122.3 (7) |
| Cl1—Hg1—N1 | 106.61 (17) | C9—C4—C5 | 119.5 (7) |
| Cl2—Hg1—N1 | 99.30 (17) | C6—C5—C4 | 119.5 (8) |
| Cl1—Hg1—O1 | 105.43 (15) | C6—C5—H5 | 120.3 |
| Cl2—Hg1—O1 | 91.75 (15) | C4—C5—H5 | 120.3 |
| N1—Hg1—O1 | 62.08 (19) | C5—C6—C7 | 121.3 (8) |
| Cl1—Hg1—O3 | 80.81 (15) | C5—C6—H6 | 119.4 |
| Cl2—Hg1—O3 | 92.53 (16) | C7—C6—H6 | 119.4 |
| N1—Hg1—O3 | 117.7 (2) | C8—C7—C6 | 121.2 (8) |
| O1—Hg1—O3 | 56.55 (16) | C8—C7—H7 | 119.4 |
| Cl1—Hg1—Cl1i | 83.50 (8) | C6—C7—H7 | 119.4 |
| Cl2—Hg1—Cl1i | 90.92 (7) | C7—C8—O1 | 124.5 (7) |
| N1—Hg1—Cl1i | 89.63 (16) | C7—C8—C9 | 120.5 (7) |
| O1—Hg1—Cl1i | 151.64 (12) | O1—C8—C9 | 115.1 (7) |
| O3—Hg1—Cl1i | 151.45 (13) | N1—C9—C8 | 120.7 (7) |
| C8—O1—C10 | 116.4 (6) | N1—C9—C4 | 121.2 (7) |
| C8—O1—Hg1 | 115.6 (4) | C8—C9—C4 | 118.0 (7) |
| C10—O1—Hg1 | 128.0 (5) | O1—C10—C11 | 108.5 (7) |
| C11—O2—C12 | 115.3 (7) | O1—C10—H10A | 110.0 |
| C11—O3—Hg1 | 121.0 (5) | C11—C10—H10A | 110.0 |
| C1—N1—C9 | 119.1 (7) | O1—C10—H10B | 110.0 |
| C1—N1—Hg1 | 116.1 (5) | C11—C10—H10B | 110.0 |
| C9—N1—Hg1 | 124.1 (5) | H10A—C10—H10B | 108.4 |
| N1—C1—C2 | 122.4 (8) | O3—C11—O2 | 124.9 (8) |
| N1—C1—H1 | 118.8 | O3—C11—C10 | 125.5 (8) |
| C2—C1—H1 | 118.8 | O2—C11—C10 | 109.6 (7) |
| C3—C2—C1 | 120.2 (8) | O2—C12—H12A | 109.5 |
| C3—C2—H2 | 119.9 | O2—C12—H12B | 109.5 |
| C1—C2—H2 | 119.9 | H12A—C12—H12B | 109.5 |
| C2—C3—C4 | 118.8 (8) | O2—C12—H12C | 109.5 |
| C2—C3—H3 | 120.6 | H12A—C12—H12C | 109.5 |
| C4—C3—H3 | 120.6 | H12B—C12—H12C | 109.5 |
| C3—C4—C9 | 118.2 (7) | ||
| Cl1—Hg1—O1—C8 | −113.6 (5) | C3—C4—C5—C6 | 178.0 (9) |
| Cl2—Hg1—O1—C8 | 86.9 (5) | C9—C4—C5—C6 | −0.6 (13) |
| N1—Hg1—O1—C8 | −12.7 (5) | C4—C5—C6—C7 | 0.9 (15) |
| O3—Hg1—O1—C8 | 178.8 (6) | C5—C6—C7—C8 | −1.8 (15) |
| Cl1i—Hg1—O1—C8 | −8.3 (7) | C6—C7—C8—O1 | −178.0 (8) |
| Cl1—Hg1—O1—C10 | 65.7 (7) | C6—C7—C8—C9 | 2.2 (14) |
| Cl2—Hg1—O1—C10 | −93.8 (7) | C10—O1—C8—C7 | 13.2 (13) |
| N1—Hg1—O1—C10 | 166.6 (8) | Hg1—O1—C8—C7 | −167.4 (7) |
| O3—Hg1—O1—C10 | −1.9 (7) | C10—O1—C8—C9 | −167.0 (8) |
| Cl1i—Hg1—O1—C10 | 171.0 (6) | Hg1—O1—C8—C9 | 12.4 (9) |
| Cl1—Hg1—O3—C11 | −110.2 (7) | C1—N1—C9—C8 | 178.2 (8) |
| Cl2—Hg1—O3—C11 | 95.7 (7) | Hg1—N1—C9—C8 | −11.9 (11) |
| N1—Hg1—O3—C11 | −6.1 (8) | C1—N1—C9—C4 | −2.1 (11) |
| O1—Hg1—O3—C11 | 5.3 (6) | Hg1—N1—C9—C4 | 167.8 (6) |
| Cl1i—Hg1—O3—C11 | −167.7 (5) | C7—C8—C9—N1 | 177.9 (8) |
| Cl1—Hg1—N1—C1 | −78.3 (6) | O1—C8—C9—N1 | −1.9 (11) |
| Cl2—Hg1—N1—C1 | 95.7 (6) | C7—C8—C9—C4 | −1.8 (12) |
| O1—Hg1—N1—C1 | −177.3 (7) | O1—C8—C9—C4 | 178.4 (7) |
| O3—Hg1—N1—C1 | −166.5 (5) | C3—C4—C9—N1 | 2.7 (12) |
| Cl1i—Hg1—N1—C1 | 4.8 (6) | C5—C4—C9—N1 | −178.7 (8) |
| Cl1—Hg1—N1—C9 | 111.5 (6) | C3—C4—C9—C8 | −177.6 (8) |
| Cl2—Hg1—N1—C9 | −74.5 (6) | C5—C4—C9—C8 | 1.0 (11) |
| O1—Hg1—N1—C9 | 12.5 (6) | C8—O1—C10—C11 | 178.6 (7) |
| O3—Hg1—N1—C9 | 23.4 (7) | Hg1—O1—C10—C11 | −0.7 (11) |
| Cl1i—Hg1—N1—C9 | −165.4 (6) | Hg1—O3—C11—O2 | 173.0 (6) |
| C9—N1—C1—C2 | −1.0 (12) | Hg1—O3—C11—C10 | −8.8 (12) |
| Hg1—N1—C1—C2 | −171.7 (7) | C12—O2—C11—O3 | −1.6 (12) |
| N1—C1—C2—C3 | 3.6 (14) | C12—O2—C11—C10 | 179.9 (7) |
| C1—C2—C3—C4 | −2.9 (13) | O1—C10—C11—O3 | 6.4 (13) |
| C2—C3—C4—C9 | −0.1 (12) | O1—C10—C11—O2 | −175.1 (7) |
| C2—C3—C4—C5 | −178.7 (9) |
Symmetry code: (i) −x+1, −y, −z+2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: IM2385).
References
- Cheng, X. N., Zhang, W. X. & Chen, X. M. (2007). J. Am. Chem. Soc. 129, 15738–15739. [DOI] [PubMed]
- Jacobson, R. (1998). Private communication to the Rigaku Corporation, Tokyo, Japan.
- Rigaku/MSC (2001). CrystalClear Rigaku/MSC, Tokyo, Japan.
- Rigaku/MSC (2004). CrystalStructure Rigaku/MSC, The Woodlands, Texas, USA.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Song, R.-F., Wang, Y.-H. & Jiang, F. (2004). Acta Cryst. E60, m1695–m1696.
- Wang, Z., Fan, J., Zhang, W. & Wang, J. (2008). Acta Cryst. E64, m1446. [DOI] [PMC free article] [PubMed]
- Wang, Y. H., Song, R. F. & Zhang, F. Y. (2005). J. Mol. Struct. 752, 104–109.
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/S1600536812026591/im2385sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812026591/im2385Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


