metal-organic compounds
catena-Poly[di-μ3-bromido-hexa-μ2-bromido-dibromidobis(O-methyl pyridine-2-carboximidate-κ2N,N′)pentamercury(II)]
aDepartment of Chemistry, Omidieh Branch, Islamic Azad University, Omidieh, Iran, and bDepartment of Chemistry, Faculty of Science, Azarbaijan Shahid Madani University, Tabriz, Iran
*Correspondence e-mail: sadifchemist@hotmail.com
The title compound, [Hg5Br10(C7H8N2O)2]n, contains two μ3-bridging Br atoms, six μ2-bridging Br atoms and two terminal Br atoms. One HgII atom, lying on an inversion center, adopts a distorted octahedral geometry defined by six Br atoms. Two HgII atoms adopt a distorted square-pyramidal geometry by five Br atoms and the other two HgII atoms have a distorted tetrahedral geometry by two N atoms from a chelating O-methyl pyridine-2-carboximidate ligand and two Br atoms. The Br atoms link the HgII atoms into a ribbon structure along [100].
Related literature
For metal complexes with O-alkyl pyridine-2-carboximidate, see: Barnard (1969); Du et al. (2005, 2006); Jamnicky et al. (1995); Seglá & Jamnicky (1988); Suzuki et al. (1974).
Experimental
Crystal data
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Refinement
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Data collection: APEX2 (Bruker, 2007); cell SAINT (Bruker, 2007); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 2012); software used to prepare material for publication: SHELXL97.
Supporting information
10.1107/S1600536812046545/hy2602sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536812046545/hy2602Isup2.hkl
For the preparation of the title compound, a solution of 2-cyanopyridine (0.47 g, 4.42 mmol) in methanol (10 ml) was added to a solution of HgBr2 (0.82 g, 2.21 mmol) in methanol (10 ml) and the resulting yellow solution was stirred for 20 min at room temperature. This solution was left to evaporate slowly at room temperature. After one week, yellow prismatic crystals of the title compound were isolated (yield: 0.75 g, 83.4%).
All H atoms were positioned geometrically and refined as riding atoms, with C—H = 0.93 (aromatic), 0.96 (CH3) and N—H = 0.86 Å and with Uiso(H) = 1.2Ueq(C, N). The highest residual electron density was found 1.09 Å from Hg3 the deepest hole 1.05 Å from Hg3.
Data collection: APEX2 (Bruker, 2007); cell
SAINT (Bruker, 2007); data reduction: SAINT (Bruker, 2007); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 2012); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).[Hg5Br10(C7H8N2O)2] | Z = 1 |
Mr = 2074.26 | F(000) = 894 |
Triclinic, P1 | Dx = 3.978 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 7.6768 (7) Å | Cell parameters from 7320 reflections |
b = 10.7223 (10) Å | θ = 1.9–26.0° |
c = 11.0663 (10) Å | µ = 33.65 mm−1 |
α = 92.067 (7)° | T = 298 K |
β = 102.850 (7)° | Prism, yellow |
γ = 101.879 (7)° | 0.30 × 0.19 × 0.18 mm |
V = 865.86 (14) Å3 |
Bruker APEXII CCD diffractometer | 3410 independent reflections |
Radiation source: fine-focus sealed tube | 2042 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.084 |
ϕ and ω scans | θmax = 26.0°, θmin = 1.9° |
Absorption correction: multi-scan (SADABS; Bruker, 2001) | h = −9→9 |
Tmin = 0.105, Tmax = 0.223 | k = −13→13 |
7320 measured reflections | l = −13→13 |
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)] = 0.062 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.148 | H-atom parameters constrained |
S = 0.93 | w = 1/[σ2(Fo2) + (0.0731P)2] where P = (Fo2 + 2Fc2)/3 |
3410 reflections | (Δ/σ)max = 0.003 |
160 parameters | Δρmax = 1.89 e Å−3 |
0 restraints | Δρmin = −1.90 e Å−3 |
[Hg5Br10(C7H8N2O)2] | γ = 101.879 (7)° |
Mr = 2074.26 | V = 865.86 (14) Å3 |
Triclinic, P1 | Z = 1 |
a = 7.6768 (7) Å | Mo Kα radiation |
b = 10.7223 (10) Å | µ = 33.65 mm−1 |
c = 11.0663 (10) Å | T = 298 K |
α = 92.067 (7)° | 0.30 × 0.19 × 0.18 mm |
β = 102.850 (7)° |
Bruker APEXII CCD diffractometer | 3410 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2001) | 2042 reflections with I > 2σ(I) |
Tmin = 0.105, Tmax = 0.223 | Rint = 0.084 |
7320 measured reflections |
R[F2 > 2σ(F2)] = 0.062 | 0 restraints |
wR(F2) = 0.148 | H-atom parameters constrained |
S = 0.93 | Δρmax = 1.89 e Å−3 |
3410 reflections | Δρmin = −1.90 e Å−3 |
160 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 | ||
C1 | −0.003 (4) | 0.838 (2) | −0.726 (2) | 0.076 (7) | |
H1A | −0.0886 | 0.7662 | −0.7095 | 0.091* | |
H1B | 0.0734 | 0.8091 | −0.7743 | 0.091* | |
H1C | −0.0680 | 0.8955 | −0.7723 | 0.091* | |
C2 | 0.211 (2) | 0.8446 (18) | −0.5315 (18) | 0.046 (4) | |
C3 | 0.327 (3) | 0.9261 (17) | −0.4289 (17) | 0.046 (4) | |
C4 | 0.329 (3) | 1.0579 (19) | −0.4102 (19) | 0.056 (5) | |
H4 | 0.2567 | 1.0962 | −0.4702 | 0.067* | |
C5 | 0.434 (3) | 1.128 (2) | −0.3060 (19) | 0.057 (5) | |
H5 | 0.4316 | 1.2142 | −0.2930 | 0.069* | |
C6 | 0.540 (3) | 1.075 (2) | −0.223 (2) | 0.063 (6) | |
H6 | 0.6140 | 1.1230 | −0.1517 | 0.076* | |
C7 | 0.539 (3) | 0.948 (2) | −0.244 (2) | 0.065 (6) | |
H7 | 0.6186 | 0.9131 | −0.1855 | 0.078* | |
N1 | 0.211 (2) | 0.7237 (14) | −0.5445 (16) | 0.054 (4) | |
H1D | 0.1406 | 0.6742 | −0.6067 | 0.065* | |
N2 | 0.435 (3) | 0.8714 (16) | −0.3409 (15) | 0.059 (5) | |
O1 | 0.110 (2) | 0.9040 (13) | −0.6109 (12) | 0.062 (4) | |
Hg1 | 0.41370 (13) | 0.64830 (8) | −0.39109 (9) | 0.0623 (3) | |
Hg2 | 0.5000 | 0.5000 | 0.0000 | 0.0588 (3) | |
Hg3 | 0.95464 (12) | 0.64042 (7) | −0.14661 (8) | 0.0591 (3) | |
Br1 | 0.7283 (3) | 0.6379 (2) | −0.4186 (2) | 0.0619 (6) | |
Br2 | 0.2253 (3) | 0.5162 (2) | −0.26046 (19) | 0.0549 (5) | |
Br3 | 0.6541 (3) | 0.72282 (19) | −0.0001 (2) | 0.0607 (5) | |
Br4 | 1.1178 (4) | 0.8617 (2) | −0.1174 (3) | 0.0788 (7) | |
Br5 | 0.7893 (3) | 0.41969 (18) | −0.1371 (2) | 0.0544 (5) |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.070 (15) | 0.080 (16) | 0.076 (17) | 0.026 (13) | 0.004 (13) | 0.002 (13) |
C2 | 0.027 (9) | 0.057 (11) | 0.051 (12) | 0.002 (8) | 0.008 (8) | 0.012 (9) |
C3 | 0.049 (10) | 0.043 (9) | 0.038 (10) | −0.010 (8) | 0.011 (9) | 0.005 (8) |
C4 | 0.057 (12) | 0.055 (12) | 0.051 (13) | 0.007 (10) | 0.007 (10) | −0.001 (10) |
C5 | 0.061 (13) | 0.053 (11) | 0.052 (12) | 0.001 (10) | 0.016 (11) | −0.018 (9) |
C6 | 0.058 (13) | 0.058 (13) | 0.072 (15) | −0.002 (11) | 0.028 (12) | −0.011 (11) |
C7 | 0.053 (13) | 0.065 (14) | 0.058 (14) | −0.023 (11) | 0.006 (11) | 0.007 (11) |
N1 | 0.059 (10) | 0.035 (8) | 0.068 (11) | 0.019 (8) | 0.008 (9) | 0.007 (7) |
N2 | 0.078 (12) | 0.051 (9) | 0.038 (9) | 0.015 (9) | −0.008 (9) | 0.003 (7) |
O1 | 0.078 (10) | 0.055 (8) | 0.047 (8) | 0.030 (8) | −0.010 (7) | −0.003 (6) |
Hg1 | 0.0624 (5) | 0.0600 (5) | 0.0714 (6) | 0.0192 (4) | 0.0229 (4) | 0.0187 (4) |
Hg2 | 0.0572 (7) | 0.0560 (6) | 0.0657 (8) | 0.0076 (5) | 0.0246 (6) | 0.0032 (5) |
Hg3 | 0.0575 (5) | 0.0477 (4) | 0.0686 (6) | 0.0021 (4) | 0.0159 (4) | 0.0045 (4) |
Br1 | 0.0548 (12) | 0.0756 (14) | 0.0564 (13) | 0.0195 (11) | 0.0106 (10) | 0.0052 (10) |
Br2 | 0.0528 (11) | 0.0612 (12) | 0.0505 (12) | 0.0070 (9) | 0.0162 (9) | 0.0068 (9) |
Br3 | 0.0698 (14) | 0.0512 (11) | 0.0631 (13) | 0.0113 (10) | 0.0208 (11) | 0.0071 (9) |
Br4 | 0.0762 (16) | 0.0521 (12) | 0.0983 (19) | −0.0031 (11) | 0.0148 (14) | 0.0127 (12) |
Br5 | 0.0573 (12) | 0.0446 (10) | 0.0632 (13) | 0.0040 (9) | 0.0263 (10) | −0.0037 (9) |
C1—O1 | 1.44 (3) | C7—N2 | 1.32 (3) |
C1—H1A | 0.9600 | C7—H7 | 0.9300 |
C1—H1B | 0.9600 | Hg1—N1 | 2.322 (14) |
C1—H1C | 0.9600 | N1—H1D | 0.8600 |
C2—N1 | 1.30 (2) | Hg1—N2 | 2.400 (16) |
C2—O1 | 1.313 (19) | Hg1—Br1 | 2.524 (2) |
C2—C3 | 1.42 (3) | Hg1—Br2 | 2.534 (2) |
C3—N2 | 1.36 (2) | Hg2—Br2 | 3.204 (2) |
C3—C4 | 1.42 (3) | Hg2—Br3 | 2.438 (2) |
C4—C5 | 1.35 (3) | Hg2—Br5 | 3.189 (2) |
C4—H4 | 0.9300 | Hg3—Br1 | 3.119 (2) |
C5—C6 | 1.31 (3) | Hg3—Br2i | 3.140 (2) |
C5—H5 | 0.9300 | Hg3—Br3 | 3.337 (2) |
C6—C7 | 1.38 (3) | Hg3—Br4 | 2.418 (2) |
C6—H6 | 0.9300 | Hg3—Br5 | 2.463 (2) |
O1—C1—H1A | 109.5 | N2—C7—C6 | 125 (2) |
O1—C1—H1B | 109.5 | N2—C7—H7 | 117.5 |
H1A—C1—H1B | 109.5 | C6—C7—H7 | 117.5 |
O1—C1—H1C | 109.5 | C2—N1—Hg1 | 116.5 (13) |
H1A—C1—H1C | 109.5 | C2—N1—H1D | 121.7 |
H1B—C1—H1C | 109.5 | Hg1—N1—H1D | 121.7 |
N1—C2—O1 | 124.8 (18) | C7—N2—C3 | 116.5 (17) |
N1—C2—C3 | 121.8 (16) | C7—N2—Hg1 | 129.5 (14) |
O1—C2—C3 | 113.4 (17) | C3—N2—Hg1 | 113.9 (12) |
N2—C3—C2 | 117.1 (16) | C2—O1—C1 | 120.6 (16) |
N2—C3—C4 | 119.2 (17) | N1—Hg1—N2 | 70.5 (5) |
C2—C3—C4 | 123.6 (17) | N1—Hg1—Br1 | 120.2 (4) |
C5—C4—C3 | 120.6 (18) | N2—Hg1—Br1 | 104.2 (5) |
C5—C4—H4 | 119.7 | N1—Hg1—Br2 | 107.2 (4) |
C3—C4—H4 | 119.7 | N2—Hg1—Br2 | 109.5 (5) |
C6—C5—C4 | 120 (2) | Br1—Hg1—Br2 | 128.56 (7) |
C6—C5—H5 | 120.2 | Br3ii—Hg2—Br3 | 180.0 |
C4—C5—H5 | 120.2 | Br4—Hg3—Br5 | 169.89 (9) |
C5—C6—C7 | 119 (2) | Br4—Hg3—Br1 | 98.67 (8) |
C5—C6—H6 | 120.5 | Br5—Hg3—Br1 | 89.75 (7) |
C7—C6—H6 | 120.5 | Hg1—Br1—Hg3 | 103.35 (8) |
N1—C2—C3—N2 | −3 (3) | N1—C2—O1—C1 | −4 (3) |
O1—C2—C3—N2 | 179.0 (17) | C3—C2—O1—C1 | 173.9 (19) |
N1—C2—C3—C4 | −179.0 (19) | C2—N1—Hg1—N2 | 1.7 (14) |
O1—C2—C3—C4 | 3 (3) | C2—N1—Hg1—Br1 | −93.8 (14) |
N2—C3—C4—C5 | −1 (3) | C2—N1—Hg1—Br2 | 106.8 (14) |
C2—C3—C4—C5 | 176 (2) | C7—N2—Hg1—N1 | 180 (2) |
C3—C4—C5—C6 | 2 (3) | C3—N2—Hg1—N1 | −3.0 (13) |
C4—C5—C6—C7 | −1 (3) | C7—N2—Hg1—Br1 | −63 (2) |
C5—C6—C7—N2 | −2 (4) | C3—N2—Hg1—Br1 | 114.5 (14) |
O1—C2—N1—Hg1 | 177.9 (14) | C7—N2—Hg1—Br2 | 78 (2) |
C3—C2—N1—Hg1 | 0 (2) | C3—N2—Hg1—Br2 | −104.9 (14) |
C6—C7—N2—C3 | 3 (3) | N1—Hg1—Br1—Hg3 | 157.3 (5) |
C6—C7—N2—Hg1 | −179.3 (17) | N2—Hg1—Br1—Hg3 | 81.8 (4) |
C2—C3—N2—C7 | −178.4 (19) | Br2—Hg1—Br1—Hg3 | −48.13 (13) |
C4—C3—N2—C7 | −2 (3) | Br4—Hg3—Br1—Hg1 | −102.16 (10) |
C2—C3—N2—Hg1 | 4 (2) | Br5—Hg3—Br1—Hg1 | 72.22 (8) |
C4—C3—N2—Hg1 | −179.6 (15) |
Symmetry codes: (i) x+1, y, z; (ii) −x+1, −y+1, −z. |
Experimental details
Crystal data | |
Chemical formula | [Hg5Br10(C7H8N2O)2] |
Mr | 2074.26 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 298 |
a, b, c (Å) | 7.6768 (7), 10.7223 (10), 11.0663 (10) |
α, β, γ (°) | 92.067 (7), 102.850 (7), 101.879 (7) |
V (Å3) | 865.86 (14) |
Z | 1 |
Radiation type | Mo Kα |
µ (mm−1) | 33.65 |
Crystal size (mm) | 0.30 × 0.19 × 0.18 |
Data collection | |
Diffractometer | Bruker APEXII CCD diffractometer |
Absorption correction | Multi-scan (SADABS; Bruker, 2001) |
Tmin, Tmax | 0.105, 0.223 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 7320, 3410, 2042 |
Rint | 0.084 |
(sin θ/λ)max (Å−1) | 0.617 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.062, 0.148, 0.93 |
No. of reflections | 3410 |
No. of parameters | 160 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 1.89, −1.90 |
Computer programs: APEX2 (Bruker, 2007), SAINT (Bruker, 2007), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), ORTEP-3 (Farrugia, 2012).
Hg1—N1 | 2.322 (14) | Hg2—Br5 | 3.189 (2) |
Hg1—N2 | 2.400 (16) | Hg3—Br1 | 3.119 (2) |
Hg1—Br1 | 2.524 (2) | Hg3—Br2i | 3.140 (2) |
Hg1—Br2 | 2.534 (2) | Hg3—Br3 | 3.337 (2) |
Hg2—Br2 | 3.204 (2) | Hg3—Br4 | 2.418 (2) |
Hg2—Br3 | 2.438 (2) | Hg3—Br5 | 2.463 (2) |
Symmetry code: (i) x+1, y, z. |
Acknowledgements
We are grateful to the Islamic Azad University, Omidieh Branch, for financial support.
References
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As has previously been observed, the reaction of 2-cyanopyridine (2-cnpy) with water or an alcohol in the presence of some metal(II) salts leads to the formation of complexes which contain O-alkylpyridine-2-carboximidate (Barnard, 1969; Seglá & Jamnicky, 1988; Suzuki et al., 1974). The reaction of 2-cnpy and CuII (Du et al., 2005), CdII (Du et al., 2006) and NiII (Jamnicky et al., 1995) in methanol leads to the formation of a chelate ligand, O-methylpyridine-2-carboximidate. Here, we report the synthesis and structure of the title compound.
The asymmetric unit of the title compound (Fig. 1) consists of 2.5 crystallographically independent HgII atoms, five bromide ions and one neutral O-methylpyridine-2-carboximidate ligand. The Br2 atom adopts a µ3-mode to bridge three HgII atoms, while Br1, Br3 and Br5 are coordinated to HgII atoms in a µ2-mode. The Br4 atom is coordinated to one HgII atom in a terminal fashion. The Hg1 atom adopts a distorted tetrahedral coordination geometry defined by two N atoms from one O-methylpyridine-2-carboximidate ligand and two Br atoms. The Hg2 atom, lying on an inversion center, adopts a distorted octahedral geometry by six Br atoms and Hg3 atom adopts a distorted square-pyramidal geometry by five Br atoms (Table 1). The HgII atoms are linked by the Br atoms into a ribbon structure along [100].