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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Apr 16;67(Pt 5):m595. doi: 10.1107/S1600536811013274

Dibromidobis(pyridine-3-carbonitrile-κN 1)mercury(II)

Reza Ghiasi a,*
PMCID: PMC3089369  PMID: 21754315

Abstract

In the crystal structure of the title compound, [HgBr2(C6H4N2)2], the Hg atom is four coordinated by two pyridine N atoms and two Br anions in a considerably distorted tetrahedral environment. π–π inter­actions between adjacent pyridine rings [centroid–centroid distance of 3.648 (3) Å] stabilize the crystal structure.

Related literature

For related structures, see: Ghiasi (2011); Steffen & Palenik (1977); Li et al. (2004).graphic file with name e-67-0m595-scheme1.jpg

Experimental

Crystal data

  • [HgBr2(C6H4N2)2]

  • M r = 568.61

  • Triclinic, Inline graphic

  • a = 8.5823 (6) Å

  • b = 9.4069 (6) Å

  • c = 9.8562 (7) Å

  • α = 81.935 (5)°

  • β = 71.435 (6)°

  • γ = 80.508 (6)°

  • V = 740.70 (9) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 15.78 mm−1

  • T = 120 K

  • 0.45 × 0.22 × 0.20 mm

Data collection

  • Bruker SMART CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 1998) T min = 0.033, T max = 0.052

  • 8486 measured reflections

  • 3967 independent reflections

  • 3751 reflections with I > 2σ(I)

  • R int = 0.043

Refinement

  • R[F 2 > 2σ(F 2)] = 0.030

  • wR(F 2) = 0.084

  • S = 1.18

  • 3967 reflections

  • 172 parameters

  • H-atom parameters constrained

  • Δρmax = 1.13 e Å−3

  • Δρmin = −2.48 e Å−3

Data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 1998); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811013274/bt5511sup1.cif

e-67-0m595-sup1.cif (15.4KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811013274/bt5511Isup2.hkl

e-67-0m595-Isup2.hkl (194.4KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

supplementary crystallographic information

Comment

Recently, the crystal satructure of dibromozinc(II)-di-3-pyridine-carbonitrile have been reported, (Ghiasi, 2011). On the other hand there are several complexes, with formula, [MX2L2], such as [ZnCl2(4-cypy)2], (Steffen & Palenik, 1977), [CuBr2(3-Cypy)2], (Li et al. 2004), [where py is pyridine, 4-cypy is 4-cyanopyridine and 3-cypy is 3-cyanopyridine] have been synthesized and characterized by single-crystal X-ray diffraction methods. The molecular structure of the title compound is shown in Fig. 1. The HgII atom is four-coordinated in a slightly distorted tetrahedral configuration by two N atoms from two pyridine rings and two Br- anions. The Hg—Br and Hg—N bond distances and angles (Table 1) are within normal ranges. π-π interactions between adjacent pyridine rings [centroid···centroid distance of 3.648 (3) Å, symmetry code: –x,1-y,1-z] stabilize the packing of the crystal structure.

Experimental

Mercury(II) bromide (0.72 gr, 2 mmol) was disolved in methanol (12 ml) and the solution was mixed with a methanolic solution (10 ml) of 3-pyridinecarbonitrile (0.42 g, 4 mmol). This solution was left to evaporate slowly at room temperature. After one week, colorless prismatic crystals of the title compound were isolated (yield 0.64 g, 56.0%, m.p. < 570 K).

Refinement

All H atoms were positioned geometrically, with C—H=0.96Å aromatics hydrogen atoms and constrained to ride on their parent atoms, with Uiso(H)=1.2Ueq.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title molecule, with the atom-numbering scheme. Displacement ellipsoids are drawn at the 50% probability level.

Fig. 2.

Fig. 2.

Unit-cell packing diagram for (I).

Crystal data

[HgBr2(C6H4N2)2] Z = 2
Mr = 568.61 F(000) = 516
Triclinic, P1 Dx = 2.549 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 8.5823 (6) Å Cell parameters from 8405 reflections
b = 9.4069 (6) Å θ = 2.2–29.2°
c = 9.8562 (7) Å µ = 15.78 mm1
α = 81.935 (5)° T = 120 K
β = 71.435 (6)° Prism, colorless
γ = 80.508 (6)° 0.45 × 0.22 × 0.2 mm
V = 740.70 (9) Å3

Data collection

Bruker SMART CCD diffractometer 3751 reflections with I > 2σ(I)
graphite Rint = 0.043
phi and ω scans θmax = 29.2°, θmin = 2.2°
Absorption correction: multi-scan (SADABS; Bruker, 1998) h = −11→11
Tmin = 0.033, Tmax = 0.052 k = −12→12
8486 measured reflections l = −13→13
3967 independent 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)] = 0.030 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.084 H-atom parameters constrained
S = 1.18 w = 1/[σ2(Fo2) + (0.0481P)2 + 0.8751P] where P = (Fo2 + 2Fc2)/3
3967 reflections (Δ/σ)max = 0.013
172 parameters Δρmax = 1.13 e Å3
0 restraints Δρmin = −2.48 e Å3

Special details

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq
C1 0.0093 (6) 0.7134 (5) 0.4103 (5) 0.0225 (9)
H1 0.0187 0.784 0.4635 0.027*
C2 −0.1379 (6) 0.6544 (5) 0.4499 (6) 0.0239 (9)
H2 −0.2248 0.6851 0.5286 0.029*
C3 −0.1559 (7) 0.5491 (5) 0.3719 (5) 0.0241 (9)
H3 −0.2534 0.5073 0.3971 0.029*
C4 −0.0218 (6) 0.5089 (5) 0.2548 (5) 0.0224 (9)
C5 −0.0290 (6) 0.4010 (5) 0.1668 (6) 0.0241 (9)
C6 0.1248 (7) 0.5712 (5) 0.2222 (5) 0.0227 (9)
H6 0.2146 0.5409 0.1454 0.027*
C7 0.2284 (7) 1.0208 (6) −0.0244 (6) 0.0277 (10)
H7 0.1906 1.0754 0.0541 0.033*
C8 0.1848 (9) 1.0747 (6) −0.1468 (6) 0.0355 (13)
H8 0.1204 1.1641 −0.1508 0.043*
C9 0.2387 (8) 0.9933 (6) −0.2636 (6) 0.0308 (11)
H9 0.2099 1.0259 −0.347 0.037*
C10 0.3368 (6) 0.8616 (5) −0.2530 (5) 0.0221 (9)
C11 0.3959 (7) 0.7725 (6) −0.3706 (6) 0.0265 (10)
C12 0.3758 (7) 0.8154 (5) −0.1251 (5) 0.0237 (9)
H12 0.4413 0.7271 −0.118 0.028*
Br1 0.59621 (7) 0.60216 (6) 0.12550 (6) 0.02802 (12)
Br2 0.25093 (7) 1.02533 (5) 0.34027 (6) 0.02714 (12)
Hg1 0.38539 (2) 0.805335 (18) 0.216864 (18) 0.02106 (7)
N1 0.1397 (5) 0.6727 (5) 0.2979 (4) 0.0223 (8)
N2 −0.0327 (6) 0.3162 (5) 0.0956 (6) 0.0311 (10)
N3 0.3219 (6) 0.8943 (5) −0.0129 (5) 0.0238 (8)
N4 0.4417 (7) 0.7012 (5) −0.4646 (6) 0.0351 (11)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.027 (2) 0.019 (2) 0.022 (2) 0.0020 (17) −0.0076 (19) −0.0081 (17)
C2 0.020 (2) 0.025 (2) 0.024 (2) 0.0023 (17) −0.0048 (18) −0.0038 (18)
C3 0.027 (2) 0.022 (2) 0.021 (2) −0.0032 (18) −0.0052 (19) 0.0010 (18)
C4 0.025 (2) 0.022 (2) 0.021 (2) −0.0013 (18) −0.0076 (18) −0.0055 (17)
C5 0.024 (2) 0.024 (2) 0.025 (2) −0.0017 (18) −0.0073 (19) −0.0041 (18)
C6 0.025 (2) 0.022 (2) 0.020 (2) −0.0005 (17) −0.0043 (18) −0.0075 (17)
C7 0.035 (3) 0.024 (2) 0.025 (2) 0.002 (2) −0.010 (2) −0.0065 (19)
C8 0.055 (4) 0.025 (2) 0.026 (3) 0.010 (2) −0.017 (3) −0.007 (2)
C9 0.043 (3) 0.025 (2) 0.026 (2) 0.004 (2) −0.016 (2) −0.005 (2)
C10 0.025 (2) 0.021 (2) 0.020 (2) −0.0017 (17) −0.0062 (18) −0.0037 (17)
C11 0.031 (3) 0.025 (2) 0.024 (2) 0.0001 (19) −0.011 (2) −0.0036 (19)
C12 0.027 (2) 0.021 (2) 0.024 (2) −0.0018 (18) −0.010 (2) −0.0032 (18)
Br1 0.0268 (2) 0.0291 (2) 0.0289 (3) 0.00759 (19) −0.0111 (2) −0.01227 (19)
Br2 0.0334 (3) 0.0236 (2) 0.0239 (2) 0.00029 (19) −0.0065 (2) −0.01056 (18)
Hg1 0.02188 (10) 0.02100 (10) 0.02036 (10) 0.00031 (7) −0.00584 (7) −0.00698 (7)
N1 0.024 (2) 0.0245 (19) 0.0182 (18) −0.0005 (15) −0.0058 (16) −0.0068 (15)
N2 0.030 (2) 0.029 (2) 0.034 (2) −0.0031 (18) −0.007 (2) −0.0104 (19)
N3 0.023 (2) 0.0250 (19) 0.022 (2) 0.0014 (16) −0.0068 (16) −0.0052 (16)
N4 0.044 (3) 0.031 (2) 0.031 (2) −0.001 (2) −0.010 (2) −0.009 (2)

Geometric parameters (Å, °)

C1—N1 1.347 (6) C7—H7 0.93
C1—C2 1.384 (7) C8—C9 1.385 (8)
C1—H1 0.93 C8—H8 0.93
C2—C3 1.391 (7) C9—C10 1.389 (7)
C2—H2 0.93 C9—H9 0.93
C3—C4 1.390 (7) C10—C12 1.399 (7)
C3—H3 0.93 C10—C11 1.436 (7)
C4—C6 1.401 (7) C11—N4 1.148 (7)
C4—C5 1.446 (7) C12—N3 1.334 (7)
C5—N2 1.144 (7) C12—H12 0.93
C6—N1 1.337 (6) Br1—Hg1 2.4581 (5)
C6—H6 0.93 Br2—Hg1 2.4736 (5)
C7—N3 1.333 (7) Hg1—N1 2.481 (4)
C7—C8 1.381 (8) Hg1—N3 2.496 (4)
N1—C1—C2 122.7 (5) C8—C9—C10 118.4 (5)
N1—C1—H1 118.7 C8—C9—H9 120.8
C2—C1—H1 118.7 C10—C9—H9 120.8
C1—C2—C3 120.0 (5) C9—C10—C12 119.1 (5)
C1—C2—H2 120 C9—C10—C11 120.7 (5)
C3—C2—H2 120 C12—C10—C11 120.1 (4)
C4—C3—C2 117.1 (5) N4—C11—C10 179.3 (6)
C4—C3—H3 121.4 N3—C12—C10 121.9 (5)
C2—C3—H3 121.4 N3—C12—H12 119
C3—C4—C6 120.0 (5) C10—C12—H12 119
C3—C4—C5 121.2 (5) Br1—Hg1—Br2 159.99 (2)
C6—C4—C5 118.8 (5) Br1—Hg1—N1 98.01 (10)
N2—C5—C4 179.0 (6) Br2—Hg1—N1 97.02 (10)
N1—C6—C4 122.1 (5) Br1—Hg1—N3 97.22 (10)
N1—C6—H6 119 Br2—Hg1—N3 95.88 (10)
C4—C6—H6 119 N1—Hg1—N3 90.10 (14)
N3—C7—C8 123.4 (5) C6—N1—C1 118.1 (4)
N3—C7—H7 118.3 C6—N1—Hg1 121.2 (3)
C8—C7—H7 118.3 C1—N1—Hg1 120.3 (3)
C7—C8—C9 118.7 (5) C7—N3—C12 118.5 (5)
C7—C8—H8 120.6 C7—N3—Hg1 120.3 (3)
C9—C8—H8 120.6 C12—N3—Hg1 121.2 (3)
N1—C1—C2—C3 −0.3 (8) C2—C1—N1—C6 0.0 (7)
C1—C2—C3—C4 −0.5 (7) C2—C1—N1—Hg1 172.5 (4)
C2—C3—C4—C6 1.7 (7) Br1—Hg1—N1—C6 −38.3 (4)
C2—C3—C4—C5 −179.7 (5) Br2—Hg1—N1—C6 155.0 (4)
C3—C4—C5—N2 16E1(4) N3—Hg1—N1—C6 59.0 (4)
C6—C4—C5—N2 −2E1(4) Br1—Hg1—N1—C1 149.5 (4)
C3—C4—C6—N1 −2.1 (8) Br2—Hg1—N1—C1 −17.2 (4)
C5—C4—C6—N1 179.3 (5) N3—Hg1—N1—C1 −113.2 (4)
N3—C7—C8—C9 0.8 (10) C8—C7—N3—C12 −0.2 (9)
C7—C8—C9—C10 −1.0 (10) C8—C7—N3—Hg1 −178.2 (5)
C8—C9—C10—C12 0.7 (9) C10—C12—N3—C7 −0.1 (8)
C8—C9—C10—C11 179.9 (6) C10—C12—N3—Hg1 177.9 (4)
C9—C10—C11—N4 −6E1(5) Br1—Hg1—N3—C7 −169.9 (4)
C12—C10—C11—N4 12E1(5) Br2—Hg1—N3—C7 −5.0 (4)
C9—C10—C12—N3 −0.2 (8) N1—Hg1—N3—C7 92.1 (4)
C11—C10—C12—N3 −179.3 (5) Br1—Hg1—N3—C12 12.2 (4)
C4—C6—N1—C1 1.2 (7) Br2—Hg1—N3—C12 177.1 (4)
C4—C6—N1—Hg1 −171.2 (4) N1—Hg1—N3—C12 −85.9 (4)

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BT5511).

References

  1. Bruker (1998). SMART, SAINT and SADABS Bruker AXS Inc., Madison, Wisconsin, USA.
  2. Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
  3. Farrugia, L. J. (1999). J. Appl. Cryst. 32, 837–838.
  4. Ghiasi, R. (2011). Acta Cryst. E67, m101. [DOI] [PMC free article] [PubMed]
  5. Li, X.-H., Wu, H.-Y. & Hu, J.-G. (2004). Acta Cryst. E60, m1533–m1535.
  6. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  7. Steffen, W. L. & Palenik, G. J. (1977). Inorg. Chem. 16, 1119–1127.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811013274/bt5511sup1.cif

e-67-0m595-sup1.cif (15.4KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811013274/bt5511Isup2.hkl

e-67-0m595-Isup2.hkl (194.4KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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