metal-organic compounds
Dibromido[methyl 2-(quinolin-8-yloxy-κ2N,O)acetic acid-κO]mercury(II)
aSchool of Chemistry and Bioengineering, Suzhou University of Science and Technology, Suzhou 215009, People's Republic of China
*Correspondence e-mail: wangyuhong@mail.usts.edu.cn
In the title complex, [HgBr2(C12H11NO3)], the HgII ion has a distorted core trigonal–planar geometry comprising two Br atoms and one quinoline N atom of the methyl 2-(quinolin-8-yloxy)acetic acid ligand. The angles around the Hg atom vary from 100.31 (15) to 152.65 (4)°. Two additional Hg⋯O interactions [2.739 (1) and 2.905 (1) Å] complete the coordination sphere about the HgII atom.
Related literature
For quinoline derivatives, see: Ghedini et al. (2002); Inomata et al. (1999); Jotterand et al. (2001). For transition metal coordination compounds with 8-quinolinyloxyacetic acid and its derivatives as ligands, see: Cheng et al. (2007); Song et al. (2004); Wang, Song et al. (2005); Wang, Fan et al. (2008).
Experimental
Crystal data
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Refinement
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Data collection: CrystalClear (Rigaku, 2001); cell CrystalClear; data reduction: CrystalStructure (Rigaku, 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.
Supporting information
https://doi.org/10.1107/S1600536812028085/gg2082sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536812028085/gg2082Isup2.hkl
Triethylamine (0.0101 g, 0.1 mmol) was added to 8-quinolinyloxyacetic acid (0.0203 g, 0.1 mmol) dissolved in methanol (3 ml). The mixture was stirred for 2 min, Then, the mixture and HgBr2 (0.0361 g, 0.1 mmol) were placed in a thick Pyrex tube and heated at 150°C for 3 days. After cooling at a rate of 5 °C per hour to ambient, colorless prism crystals were collected, washed with anhydrous ethanol, and dried at room temperature. The yield is 46% based on 8-quinolinyloxyacetic acid. Analysis found: C, 25.36; H, 1.97; N, 2.42%; calculated for C12H11Br2HgNO3: C, 24.95; H, 1.92; N, 2.42%.
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 methylene) = 1.2Ueq(C) and Uiso(methyl) = 1.5Ueq(C).
Derivatives of quinoline have received much attention in coordination chemistry (Ghedini et al., 2002; Inomata et al., 1999; Jotterand et al., 2001). 8-quinolinyloxyacetic acid and their derivatives exhibit rich structural variety, and reports of metal complexes with such ligands have increased in recent years (Cheng et al., 2007; Song et al., 2004; Wang, Song et al., 2005; Wang, Fan et al., 2008). In the light of this interest, we have prepared the title HgII complex with the 8-(methoxycarbonylmethoxy)quinoline ligand, (I).
The title HgBr2 adduct, (I), is a mononuclear compound. The HgII atom exists in a trigonal planar geometry formed by two Br atoms and one quinoline N atom of the 8-(methoxycarbonylmethoxy)quinoline ligand (Fig. 1). The Hg—Br bond lengths are 2.4569 (10) and 2.4667 (9) ° and Hg—N bond length is 2.451 (8) Å. The angles around the Hg atom vary from 100.31 (15) to 152.65 (4) ° (Table 1). There are weak Hg···O interactions with distances of 2.739 (1) Å and 2.905 (1) Å present (Fig. 1). Intermolecular face-to-face π-π interaction stacking is also observed between the parallel quinoline rings of neighbouring complex molecules, with a separation of approximately 3.521 (1) Å (Fig. 2).
For quinoline derivatives, see: Ghedini et al. (2002); Inomata et al. (1999); Jotterand et al.,(2001). For transition metal coordination compounds with 8-quinolinyloxyacetic acid and its derivatives as ligands, see: Cheng et al. (2007); Song et al. (2004); Wang, Song et al. (2005); Wang, Fan et al. (2008).
Data collection: CrystalClear (Rigaku, 2001); cell
CrystalClear (Rigaku, 2001); data reduction: CrystalStructure (Rigaku, 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 (Sheldrick, 2008).[HgBr2(C12H11NO3)] | Z = 2 |
Mr = 577.63 | F(000) = 528 |
Triclinic, P1 | Dx = 2.716 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71075 Å |
a = 7.3132 (8) Å | Cell parameters from 3544 reflections |
b = 9.9385 (10) Å | θ = 3.2–27.5° |
c = 10.9902 (10) Å | µ = 16.55 mm−1 |
α = 72.102 (11)° | T = 223 K |
β = 74.966 (12)° | Prism, colorless |
γ = 70.740 (11)° | 0.50 × 0.40 × 0.20 mm |
V = 706.40 (14) Å3 |
Rigaku Saturn diffractometer | 2599 independent reflections |
Radiation source: fine-focus sealed tube | 1949 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.068 |
Detector resolution: 14.63 pixels mm-1 | θmax = 25.5°, θmin = 3.2° |
ω scans | h = −8→8 |
Absorption correction: multi-scan (REQAB; Jacobson, 1998) | k = −11→12 |
Tmin = 0.044, Tmax = 0.137 | l = −12→13 |
6021 measured reflections |
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)] = 0.038 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.074 | H-atom parameters constrained |
S = 0.80 | w = 1/[σ2(Fo2) + (0.0232P)2] where P = (Fo2 + 2Fc2)/3 |
2599 reflections | (Δ/σ)max < 0.001 |
174 parameters | Δρmax = 2.41 e Å−3 |
0 restraints | Δρmin = −2.04 e Å−3 |
[HgBr2(C12H11NO3)] | γ = 70.740 (11)° |
Mr = 577.63 | V = 706.40 (14) Å3 |
Triclinic, P1 | Z = 2 |
a = 7.3132 (8) Å | Mo Kα radiation |
b = 9.9385 (10) Å | µ = 16.55 mm−1 |
c = 10.9902 (10) Å | T = 223 K |
α = 72.102 (11)° | 0.50 × 0.40 × 0.20 mm |
β = 74.966 (12)° |
Rigaku Saturn diffractometer | 2599 independent reflections |
Absorption correction: multi-scan (REQAB; Jacobson, 1998) | 1949 reflections with I > 2σ(I) |
Tmin = 0.044, Tmax = 0.137 | Rint = 0.068 |
6021 measured reflections |
R[F2 > 2σ(F2)] = 0.038 | 0 restraints |
wR(F2) = 0.074 | H-atom parameters constrained |
S = 0.80 | Δρmax = 2.41 e Å−3 |
2599 reflections | Δρmin = −2.04 e Å−3 |
174 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
Hg1 | 1.01854 (5) | 0.82765 (4) | 0.67755 (3) | 0.02656 (13) | |
Br1 | 1.28595 (13) | 0.77673 (12) | 0.79728 (8) | 0.0324 (3) | |
Br2 | 0.72668 (13) | 0.98864 (11) | 0.58446 (8) | 0.0316 (3) | |
O1 | 0.9081 (8) | 0.5789 (7) | 0.8222 (5) | 0.0260 (15) | |
O2 | 0.5235 (8) | 0.7032 (7) | 1.0669 (5) | 0.0303 (16) | |
O3 | 0.7280 (9) | 0.8198 (7) | 0.9145 (6) | 0.0311 (16) | |
N1 | 1.1332 (9) | 0.6134 (8) | 0.5841 (6) | 0.0211 (17) | |
C1 | 1.2348 (12) | 0.6300 (10) | 0.4657 (8) | 0.023 (2) | |
H1 | 1.2428 | 0.7252 | 0.4193 | 0.028* | |
C2 | 1.3332 (12) | 0.5136 (11) | 0.4032 (8) | 0.029 (2) | |
H2 | 1.4003 | 0.5321 | 0.3170 | 0.035* | |
C3 | 1.3281 (12) | 0.3746 (11) | 0.4709 (8) | 0.026 (2) | |
H3 | 1.3952 | 0.2947 | 0.4330 | 0.032* | |
C4 | 1.2191 (11) | 0.3517 (10) | 0.6005 (7) | 0.020 (2) | |
C5 | 1.2060 (12) | 0.2104 (10) | 0.6737 (9) | 0.029 (2) | |
H5 | 1.2722 | 0.1280 | 0.6392 | 0.035* | |
C6 | 1.0952 (13) | 0.1947 (11) | 0.7963 (9) | 0.033 (3) | |
H6 | 1.0871 | 0.1005 | 0.8461 | 0.040* | |
C7 | 0.9956 (12) | 0.3148 (11) | 0.8475 (8) | 0.026 (2) | |
H7 | 0.9182 | 0.3007 | 0.9309 | 0.031* | |
C8 | 1.0058 (11) | 0.4532 (10) | 0.7809 (8) | 0.021 (2) | |
C9 | 1.1234 (11) | 0.4738 (10) | 0.6524 (8) | 0.019 (2) | |
C10 | 0.7609 (12) | 0.5656 (11) | 0.9358 (8) | 0.027 (2) | |
H10A | 0.8196 | 0.4930 | 1.0083 | 0.033* | |
H10B | 0.6588 | 0.5320 | 0.9205 | 0.033* | |
C11 | 0.6734 (13) | 0.7084 (12) | 0.9681 (8) | 0.031 (3) | |
C12 | 0.4182 (13) | 0.8376 (12) | 1.1065 (9) | 0.041 (3) | |
H12A | 0.5058 | 0.8692 | 1.1378 | 0.062* | |
H12B | 0.3083 | 0.8212 | 1.1754 | 0.062* | |
H12C | 0.3696 | 0.9130 | 1.0331 | 0.062* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Hg1 | 0.0287 (2) | 0.0224 (2) | 0.02744 (19) | −0.00666 (15) | −0.00615 (14) | −0.00383 (15) |
Br1 | 0.0335 (5) | 0.0360 (7) | 0.0283 (5) | −0.0116 (5) | −0.0083 (4) | −0.0042 (4) |
Br2 | 0.0288 (5) | 0.0271 (6) | 0.0362 (5) | −0.0052 (4) | −0.0077 (4) | −0.0051 (4) |
O1 | 0.031 (3) | 0.021 (4) | 0.022 (3) | −0.012 (3) | 0.010 (3) | −0.008 (3) |
O2 | 0.036 (3) | 0.029 (4) | 0.023 (3) | −0.013 (3) | 0.014 (3) | −0.014 (3) |
O3 | 0.040 (4) | 0.017 (4) | 0.032 (3) | −0.009 (3) | 0.005 (3) | −0.008 (3) |
N1 | 0.020 (4) | 0.028 (5) | 0.018 (4) | −0.012 (3) | 0.003 (3) | −0.008 (3) |
C1 | 0.027 (5) | 0.019 (6) | 0.028 (5) | −0.010 (4) | −0.012 (4) | −0.001 (4) |
C2 | 0.025 (5) | 0.036 (7) | 0.028 (5) | −0.013 (5) | −0.002 (4) | −0.007 (5) |
C3 | 0.019 (4) | 0.031 (6) | 0.034 (5) | 0.000 (4) | −0.009 (4) | −0.018 (5) |
C4 | 0.014 (4) | 0.021 (6) | 0.022 (4) | −0.002 (4) | −0.001 (3) | −0.005 (4) |
C5 | 0.033 (5) | 0.014 (6) | 0.043 (5) | 0.000 (4) | −0.010 (4) | −0.014 (4) |
C6 | 0.040 (6) | 0.023 (6) | 0.033 (5) | −0.014 (5) | −0.005 (4) | 0.002 (5) |
C7 | 0.024 (5) | 0.025 (6) | 0.025 (5) | −0.002 (4) | −0.001 (4) | −0.010 (4) |
C8 | 0.018 (4) | 0.021 (6) | 0.026 (4) | −0.006 (4) | −0.003 (3) | −0.010 (4) |
C9 | 0.016 (4) | 0.019 (6) | 0.024 (4) | −0.003 (4) | −0.006 (3) | −0.007 (4) |
C10 | 0.025 (5) | 0.028 (6) | 0.027 (5) | −0.006 (4) | 0.000 (4) | −0.009 (4) |
C11 | 0.029 (5) | 0.046 (8) | 0.017 (4) | −0.013 (5) | −0.007 (4) | 0.000 (5) |
C12 | 0.034 (5) | 0.038 (8) | 0.047 (6) | −0.012 (5) | 0.009 (5) | −0.015 (5) |
Hg1—Br1 | 2.4667 (9) | C4—C9 | 1.396 (13) |
Hg1—Br2 | 2.4569 (10) | C4—C5 | 1.409 (12) |
Hg1—N1 | 2.451 (8) | C5—C6 | 1.372 (12) |
O1—C8 | 1.367 (11) | C5—H5 | 0.9400 |
O1—C10 | 1.425 (9) | C6—C7 | 1.378 (14) |
O2—C11 | 1.330 (10) | C6—H6 | 0.9400 |
O2—C12 | 1.440 (12) | C7—C8 | 1.362 (12) |
O3—C11 | 1.225 (11) | C7—H7 | 0.9400 |
N1—C1 | 1.312 (10) | C8—C9 | 1.444 (11) |
N1—C9 | 1.375 (11) | C10—C11 | 1.463 (14) |
C1—C2 | 1.418 (14) | C10—H10A | 0.9800 |
C1—H1 | 0.9400 | C10—H10B | 0.9800 |
C2—C3 | 1.361 (12) | C12—H12A | 0.9700 |
C2—H2 | 0.9400 | C12—H12B | 0.9700 |
C3—C4 | 1.431 (11) | C12—H12C | 0.9700 |
C3—H3 | 0.9400 | ||
N1—Hg1—Br2 | 106.34 (15) | C7—C6—H6 | 119.5 |
N1—Hg1—Br1 | 100.31 (15) | C8—C7—C6 | 122.0 (8) |
Br2—Hg1—Br1 | 152.65 (4) | C8—C7—H7 | 119.0 |
C8—O1—C10 | 116.2 (7) | C6—C7—H7 | 119.0 |
C11—O2—C12 | 117.3 (8) | C7—C8—O1 | 126.1 (8) |
C1—N1—C9 | 117.8 (8) | C7—C8—C9 | 118.6 (9) |
C1—N1—Hg1 | 116.8 (6) | O1—C8—C9 | 115.3 (7) |
C9—N1—Hg1 | 124.7 (5) | N1—C9—C4 | 122.2 (7) |
N1—C1—C2 | 124.2 (8) | N1—C9—C8 | 119.0 (8) |
N1—C1—H1 | 117.9 | C4—C9—C8 | 118.8 (8) |
C2—C1—H1 | 117.9 | O1—C10—C11 | 109.4 (7) |
C3—C2—C1 | 118.5 (9) | O1—C10—H10A | 109.8 |
C3—C2—H2 | 120.8 | C11—C10—H10A | 109.8 |
C1—C2—H2 | 120.8 | O1—C10—H10B | 109.8 |
C2—C3—C4 | 119.0 (10) | C11—C10—H10B | 109.8 |
C2—C3—H3 | 120.5 | H10A—C10—H10B | 108.2 |
C4—C3—H3 | 120.5 | O3—C11—O2 | 122.8 (10) |
C9—C4—C5 | 120.5 (8) | O3—C11—C10 | 126.2 (8) |
C9—C4—C3 | 118.2 (8) | O2—C11—C10 | 111.0 (8) |
C5—C4—C3 | 121.3 (9) | O2—C12—H12A | 109.5 |
C6—C5—C4 | 119.1 (9) | O2—C12—H12B | 109.5 |
C6—C5—H5 | 120.5 | H12A—C12—H12B | 109.5 |
C4—C5—H5 | 120.5 | O2—C12—H12C | 109.5 |
C5—C6—C7 | 121.0 (9) | H12A—C12—H12C | 109.5 |
C5—C6—H6 | 119.5 | H12B—C12—H12C | 109.5 |
Br2—Hg1—N1—C1 | 79.0 (6) | C1—N1—C9—C4 | 0.9 (11) |
Br1—Hg1—N1—C1 | −94.8 (6) | Hg1—N1—C9—C4 | −169.3 (6) |
Br2—Hg1—N1—C9 | −110.8 (6) | C1—N1—C9—C8 | −177.4 (7) |
Br1—Hg1—N1—C9 | 75.4 (6) | Hg1—N1—C9—C8 | 12.4 (10) |
C9—N1—C1—C2 | 0.7 (12) | C5—C4—C9—N1 | 179.8 (7) |
Hg1—N1—C1—C2 | 171.6 (6) | C3—C4—C9—N1 | −1.0 (11) |
N1—C1—C2—C3 | −2.1 (13) | C5—C4—C9—C8 | −1.9 (12) |
C1—C2—C3—C4 | 1.9 (12) | C3—C4—C9—C8 | 177.3 (7) |
C2—C3—C4—C9 | −0.5 (11) | C7—C8—C9—N1 | 179.5 (7) |
C2—C3—C4—C5 | 178.7 (7) | O1—C8—C9—N1 | 1.8 (11) |
C9—C4—C5—C6 | 1.0 (12) | C7—C8—C9—C4 | 1.1 (11) |
C3—C4—C5—C6 | −178.2 (8) | O1—C8—C9—C4 | −176.5 (7) |
C4—C5—C6—C7 | 0.8 (14) | C8—O1—C10—C11 | 179.0 (7) |
C5—C6—C7—C8 | −1.6 (14) | C12—O2—C11—O3 | 2.8 (12) |
C6—C7—C8—O1 | 178.0 (8) | C12—O2—C11—C10 | −177.8 (7) |
C6—C7—C8—C9 | 0.6 (13) | O1—C10—C11—O3 | −6.2 (12) |
C10—O1—C8—C7 | −9.9 (12) | O1—C10—C11—O2 | 174.5 (6) |
C10—O1—C8—C9 | 167.5 (7) |
Experimental details
Crystal data | |
Chemical formula | [HgBr2(C12H11NO3)] |
Mr | 577.63 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 223 |
a, b, c (Å) | 7.3132 (8), 9.9385 (10), 10.9902 (10) |
α, β, γ (°) | 72.102 (11), 74.966 (12), 70.740 (11) |
V (Å3) | 706.40 (14) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 16.55 |
Crystal size (mm) | 0.50 × 0.40 × 0.20 |
Data collection | |
Diffractometer | Rigaku Saturn |
Absorption correction | Multi-scan (REQAB; Jacobson, 1998) |
Tmin, Tmax | 0.044, 0.137 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 6021, 2599, 1949 |
Rint | 0.068 |
(sin θ/λ)max (Å−1) | 0.606 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.038, 0.074, 0.80 |
No. of reflections | 2599 |
No. of parameters | 174 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 2.41, −2.04 |
Computer programs: CrystalClear (Rigaku, 2001), CrystalStructure (Rigaku, 2004), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
Acknowledgements
This work was supported by the Science and Technology Foundation of the Ministry of Development of China (2010-K6–8).
References
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Derivatives of quinoline have received much attention in coordination chemistry (Ghedini et al., 2002; Inomata et al., 1999; Jotterand et al., 2001). 8-quinolinyloxyacetic acid and their derivatives exhibit rich structural variety, and reports of metal complexes with such ligands have increased in recent years (Cheng et al., 2007; Song et al., 2004; Wang, Song et al., 2005; Wang, Fan et al., 2008). In the light of this interest, we have prepared the title HgII complex with the 8-(methoxycarbonylmethoxy)quinoline ligand, (I).
The title HgBr2 adduct, (I), is a mononuclear compound. The HgII atom exists in a trigonal planar geometry formed by two Br atoms and one quinoline N atom of the 8-(methoxycarbonylmethoxy)quinoline ligand (Fig. 1). The Hg—Br bond lengths are 2.4569 (10) and 2.4667 (9) ° and Hg—N bond length is 2.451 (8) Å. The angles around the Hg atom vary from 100.31 (15) to 152.65 (4) ° (Table 1). There are weak Hg···O interactions with distances of 2.739 (1) Å and 2.905 (1) Å present (Fig. 1). Intermolecular face-to-face π-π interaction stacking is also observed between the parallel quinoline rings of neighbouring complex molecules, with a separation of approximately 3.521 (1) Å (Fig. 2).