Abstract
In comprison with the previous structural study [Anulewicz et al. (1991 ▶). Pol. J. Chem. 65, 465–471], for which only the coordinates of all non-H atoms and of some H atoms were reported, the current redetermination of the title compound, C13H10Br2N2, additionally reports anisotropic displacement parameters for all non-H atoms and the coordinates of all H atoms, accompanied by higher accuracy of the geometric parameters. Two independent half-molecules are present in the asymmetric unit, which are completed by a twofold rotation axis as symmetry element. In the crystal, intermolecular N—H⋯N hydrogen bonds link the molecules into dimers. Linear chains parallel to [102] are formed by intermolecular Br⋯Br interactions of 3.4328 (7) Å between two Br atoms of adjacent molecules. The dihedral angles between the benzene rings are 50.05 (15) and 75.61 (11)° in the two independent molecules. Owing to the twofold symmetry of the molecules, H atoms attached to the N atoms are only half-occupied, leading to them being disordered over two positions of equal occupancy.
Related literature
For the previous structure determination, see: Anulewicz et al. (1991 ▶). For Br⋯Br interactions, see: Fujiwara et al. (2006 ▶); Reddy et al. (1996 ▶). For N—H⋯N hydrogen bonds, see: Del Bene & Elguero (2006 ▶); Grotjahn et al. (2000 ▶); Thar & Kirchner (2006 ▶).
Experimental
Crystal data
C13H10Br2N2
M r = 354.05
Monoclinic,
a = 11.563 (2) Å
b = 23.447 (5) Å
c = 9.881 (2) Å
β = 95.43 (3)°
V = 2666.9 (9) Å3
Z = 8
Mo Kα radiation
μ = 6.06 mm−1
T = 293 K
0.15 × 0.07 × 0.06 mm
Data collection
Bruker SMART CCD diffractometer
Absorption correction: multi-scan (SADABS; Sheldrick, 2004 ▶) T min = 0.403, T max = 0.695
5954 measured reflections
2611 independent reflections
1715 reflections with I > 2σ(I)
R int = 0.061
Refinement
R[F 2 > 2σ(F 2)] = 0.048
wR(F 2) = 0.114
S = 1.00
2611 reflections
155 parameters
H-atom parameters constrained
Δρmax = 0.48 e Å−3
Δρmin = −0.91 e Å−3
Data collection: APEX2 (Bruker, 2004 ▶); cell refinement: SAINT-Plus (Bruker, 2001 ▶); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: XP (Sheldrick, 2008 ▶) and DIAMOND (Brandenburg, 1999 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811013419/wm2476sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811013419/wm2476Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N1—H2A⋯N2i | 0.85 | 2.12 | 2.964 (4) | 180 |
| N2—H3A⋯N1ii | 0.88 | 2.12 | 2.964 (4) | 161 |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
This work was supported by the National Natural Scientific Foundation of China (No.20741004/B010303).
supplementary crystallographic information
Comment
With the determination of reliable intermolecular distances, Br···Br interactions (Fujiwara et al., 2006; Reddy et al., 1996) and N–H···N hydrogen bonding (Del Bene & Elguero, 2006; Grotjahn et al. 2000; Thar & Kirchner, 2006) became important criteria in the description of supramolecular chemistry and in applied crystal engineering. The title compound C13H10Br2N2, (I), has been determined previously by Anulewicz et al. (1991). However, in that study only coordinates of all non-H atoms and of some H atoms were given. The present re-determination additionally reports anisotropic displacement parameters for all non-H atoms and the coordinates of all H atoms, accompanied by higher accuracy of all geometric parameters.
In (I) two independent half-molecules are present in the asymmetric unit which are completed by a twofold rotation axis as symmetry element that runs to the central C—H groups (C1—H1 and C2—H2, respectively). One molecule is displayed in Fig. 1. The dihedral angles between the two benzene rings in the individual molecules are 50.05 (15) ° for the first and and 75.61 (11) ° for the second molecule.
In the crystal, intermolecular N—H···N hydrogen bonds link the individual molecules into dimers (Fig. 2). Linear chains parallel to [102] are formed by intermolecular Br···Br interactions of 3.4328 (7) Å between two bromine atoms of adjacent molecules (Fig. 3). This interaction is significantly less than the van der Waals contact of 3.90 Å (Reddy et al., 1996; Fujiwara et al., 2006), hence making this interaction important for consolidation of the crystal packing.
Experimental
The title compound was synthesized by the following reaction. 17.202 g (0.1 mol) of 4-bromobenzenamine and 8.33 ml (0.05 mol) of triethyl orthoformate were combined in a round-bottom flask equipped with a distillation tube and heated at 160 until the distillation of ethanol creased. The retained solid was washed with ether, and dried under a dynamic vacuum to yield 16.10 g of white solid, (91%). 0.04 g of the white solid was dissolved in THF (3 ml) and the solution was layered with hexane. Colourless needle-shaped crystals formed after several days. 1HNMR(CDCl3, p.p.m.): 8.08(s, 1H, –NCHN–), 7.43(d, 2H, aromatic), 7.40(d, 2H, aromatic), 6.93(d, 2H, aromatic), 6.91(d, 2H, aromatic). Anal. Calcd. C13H10Br2N2: C, 44.10; H, 2.85; N, 7.91; Found: C, 43.83; H, 2.69; N, 8.02.
Refinement
H atoms attached to C atoms were positioned geometrically with C—H = 0.93 (CH), and constrained to ride on their parent atoms, with Uiso(H) = 1.2Ueq(C). H atoms attached to N atoms were found from difference Fourier maps and were fixed. They were refined with Uiso(H) = 1.2Ueq(N). Owing to the 2 symmetry of the molecules, the H atoms attached to the N atoms are only half-occupied, leading to being disordered over two positions of equal occupancy.
Figures
Fig. 1.
Molecular structure of one of the two molecules of (I) drawn with displacement ellipsoids at the 30% probability level. [Symmetry code A) -x+1, y. -z+1/2.]
Fig. 2.
A dimer formed by intermolecular N–H···N hydrogen bonds.
Fig. 3.
Part of an one-dimensional linear chain of the title compound, viewed along [010]. Br···Br interactions are drawn with blue dashed lines.
Crystal data
| C13H10Br2N2 | F(000) = 1376 |
| Mr = 354.05 | Dx = 1.764 Mg m−3 |
| Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -C 2yc | Cell parameters from 4303 reflections |
| a = 11.563 (2) Å | θ = 2.5–26.7° |
| b = 23.447 (5) Å | µ = 6.06 mm−1 |
| c = 9.881 (2) Å | T = 293 K |
| β = 95.43 (3)° | Needle, colourless |
| V = 2666.9 (9) Å3 | 0.15 × 0.07 × 0.06 mm |
| Z = 8 |
Data collection
| Bruker SMART CCD diffractometer | 2611 independent reflections |
| Radiation source: fine-focus sealed tube | 1715 reflections with I > 2σ(I) |
| graphite | Rint = 0.061 |
| ω scans | θmax = 26.0°, θmin = 1.7° |
| Absorption correction: multi-scan (SADABS; Sheldrick, 2004) | h = −12→14 |
| Tmin = 0.403, Tmax = 0.695 | k = −26→28 |
| 5954 measured reflections | l = −12→11 |
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)] = 0.048 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.114 | H-atom parameters constrained |
| S = 1.00 | w = 1/[σ2(Fo2) + (0.0533P)2] where P = (Fo2 + 2Fc2)/3 |
| 2611 reflections | (Δ/σ)max = 0.001 |
| 155 parameters | Δρmax = 0.48 e Å−3 |
| 0 restraints | Δρmin = −0.91 e Å−3 |
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 | Occ. (<1) | |
| Br1 | 0.24399 (5) | 0.73912 (2) | 0.82770 (5) | 0.0708 (2) | |
| N1 | 0.4449 (3) | 0.63281 (13) | 0.3396 (3) | 0.0429 (8) | |
| H2A | 0.4352 | 0.5975 | 0.3271 | 0.052* | 0.50 |
| C1 | 0.5000 | 0.6600 (2) | 0.2500 | 0.0428 (13) | |
| H1 | 0.5000 | 0.6997 | 0.2500 | 0.051* | |
| C11 | 0.3994 (4) | 0.65996 (16) | 0.4505 (4) | 0.0404 (9) | |
| C12 | 0.4347 (4) | 0.71277 (17) | 0.4995 (4) | 0.0525 (11) | |
| H12A | 0.4903 | 0.7329 | 0.4570 | 0.063* | |
| C13 | 0.3885 (4) | 0.73617 (18) | 0.6108 (5) | 0.0569 (11) | |
| H13A | 0.4131 | 0.7719 | 0.6428 | 0.068* | |
| C14 | 0.3065 (4) | 0.70681 (17) | 0.6738 (4) | 0.0459 (10) | |
| C15 | 0.2716 (4) | 0.65412 (19) | 0.6293 (4) | 0.0560 (11) | |
| H15A | 0.2171 | 0.6340 | 0.6737 | 0.067* | |
| C16 | 0.3177 (4) | 0.63066 (17) | 0.5178 (4) | 0.0546 (11) | |
| H16A | 0.2935 | 0.5947 | 0.4873 | 0.066* | |
| Br2 | 0.02928 (6) | 0.61567 (3) | 1.05388 (8) | 0.1036 (3) | |
| N2 | 0.4121 (3) | 0.49146 (13) | 0.7963 (3) | 0.0507 (8) | |
| H3A | 0.4085 | 0.4541 | 0.7936 | 0.061* | 0.50 |
| C2 | 0.5000 | 0.5180 (2) | 0.7500 | 0.0520 (15) | |
| H2B | 0.5000 | 0.5577 | 0.7500 | 0.062* | |
| C21 | 0.3242 (4) | 0.52137 (16) | 0.8556 (4) | 0.0455 (10) | |
| C22 | 0.2110 (4) | 0.50352 (19) | 0.8320 (5) | 0.0588 (12) | |
| H32A | 0.1933 | 0.4723 | 0.7758 | 0.071* | |
| C23 | 0.1229 (4) | 0.53143 (19) | 0.8908 (5) | 0.0635 (12) | |
| H33A | 0.0466 | 0.5189 | 0.8746 | 0.076* | |
| C24 | 0.1488 (4) | 0.57764 (18) | 0.9729 (5) | 0.0561 (11) | |
| C25 | 0.2603 (4) | 0.59524 (19) | 0.9991 (4) | 0.0584 (12) | |
| H35A | 0.2774 | 0.6264 | 1.0557 | 0.070* | |
| C26 | 0.3483 (4) | 0.56719 (17) | 0.9422 (4) | 0.0561 (11) | |
| H36A | 0.4247 | 0.5791 | 0.9621 | 0.067* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Br1 | 0.0872 (4) | 0.0873 (4) | 0.0409 (3) | 0.0246 (3) | 0.0215 (2) | −0.0074 (2) |
| N1 | 0.046 (2) | 0.0446 (17) | 0.0413 (18) | 0.0019 (15) | 0.0199 (15) | −0.0018 (14) |
| C1 | 0.040 (3) | 0.042 (3) | 0.047 (3) | 0.000 | 0.006 (3) | 0.000 |
| C11 | 0.044 (2) | 0.046 (2) | 0.033 (2) | 0.0046 (18) | 0.0111 (17) | 0.0051 (17) |
| C12 | 0.059 (3) | 0.056 (2) | 0.045 (2) | −0.014 (2) | 0.017 (2) | −0.001 (2) |
| C13 | 0.070 (3) | 0.056 (2) | 0.046 (3) | −0.009 (2) | 0.012 (2) | −0.007 (2) |
| C14 | 0.056 (3) | 0.055 (2) | 0.028 (2) | 0.010 (2) | 0.0129 (18) | −0.0038 (18) |
| C15 | 0.053 (3) | 0.073 (3) | 0.047 (2) | −0.005 (2) | 0.029 (2) | 0.000 (2) |
| C16 | 0.064 (3) | 0.051 (2) | 0.053 (3) | −0.009 (2) | 0.025 (2) | −0.003 (2) |
| Br2 | 0.0764 (5) | 0.0940 (5) | 0.1485 (7) | 0.0149 (3) | 0.0538 (4) | −0.0264 (4) |
| N2 | 0.046 (2) | 0.0459 (18) | 0.063 (2) | 0.0002 (16) | 0.0217 (17) | −0.0012 (17) |
| C2 | 0.055 (4) | 0.043 (3) | 0.059 (4) | 0.000 | 0.011 (3) | 0.000 |
| C21 | 0.047 (3) | 0.044 (2) | 0.047 (2) | 0.0014 (18) | 0.0127 (19) | 0.0011 (18) |
| C22 | 0.049 (3) | 0.061 (3) | 0.067 (3) | −0.010 (2) | 0.014 (2) | −0.019 (2) |
| C23 | 0.035 (3) | 0.078 (3) | 0.079 (3) | −0.006 (2) | 0.014 (2) | −0.016 (3) |
| C24 | 0.052 (3) | 0.057 (3) | 0.062 (3) | 0.011 (2) | 0.019 (2) | 0.000 (2) |
| C25 | 0.057 (3) | 0.053 (3) | 0.067 (3) | 0.000 (2) | 0.017 (2) | −0.014 (2) |
| C26 | 0.047 (3) | 0.059 (3) | 0.061 (3) | −0.007 (2) | 0.005 (2) | −0.010 (2) |
Geometric parameters (Å, °)
| Br1—C14 | 1.901 (4) | Br2—C24 | 1.886 (4) |
| N1—C1 | 1.305 (4) | N2—C2 | 1.311 (4) |
| N1—C11 | 1.412 (5) | N2—C21 | 1.407 (5) |
| N1—H2A | 0.8422 | N2—H3A | 0.8763 |
| C1—N1i | 1.305 (4) | C2—N2ii | 1.311 (4) |
| C1—H1 | 0.9300 | C2—H2B | 0.9300 |
| C11—C12 | 1.377 (5) | C21—C22 | 1.373 (6) |
| C11—C16 | 1.388 (6) | C21—C26 | 1.385 (5) |
| C12—C13 | 1.381 (6) | C22—C23 | 1.383 (6) |
| C12—H12A | 0.9300 | C22—H32A | 0.9300 |
| C13—C14 | 1.369 (6) | C23—C24 | 1.369 (6) |
| C13—H13A | 0.9300 | C23—H33A | 0.9300 |
| C14—C15 | 1.360 (6) | C24—C25 | 1.355 (6) |
| C15—C16 | 1.383 (6) | C25—C26 | 1.375 (6) |
| C15—H15A | 0.9300 | C25—H35A | 0.9300 |
| C16—H16A | 0.9300 | C26—H36A | 0.9300 |
| C1—N1—C11 | 123.2 (3) | C2—N2—C21 | 121.5 (3) |
| C1—N1—H2A | 116.6 | C2—N2—H3A | 120.0 |
| C11—N1—H2A | 120.1 | C21—N2—H3A | 118.5 |
| N1i—C1—N1 | 121.4 (5) | N2ii—C2—N2 | 123.3 (5) |
| N1i—C1—H1 | 119.3 | N2ii—C2—H2B | 118.4 |
| N1—C1—H1 | 119.3 | N2—C2—H2B | 118.4 |
| C12—C11—C16 | 118.0 (4) | C22—C21—C26 | 118.3 (4) |
| C12—C11—N1 | 123.9 (4) | C22—C21—N2 | 119.4 (3) |
| C16—C11—N1 | 118.0 (3) | C26—C21—N2 | 122.2 (4) |
| C11—C12—C13 | 120.9 (4) | C21—C22—C23 | 120.8 (4) |
| C11—C12—H12A | 119.6 | C21—C22—H32A | 119.6 |
| C13—C12—H12A | 119.6 | C23—C22—H32A | 119.6 |
| C14—C13—C12 | 120.0 (4) | C24—C23—C22 | 119.6 (4) |
| C14—C13—H13A | 120.0 | C24—C23—H33A | 120.2 |
| C12—C13—H13A | 120.0 | C22—C23—H33A | 120.2 |
| C15—C14—C13 | 120.5 (4) | C25—C24—C23 | 120.3 (4) |
| C15—C14—Br1 | 119.8 (3) | C25—C24—Br2 | 119.8 (3) |
| C13—C14—Br1 | 119.7 (3) | C23—C24—Br2 | 119.8 (3) |
| C14—C15—C16 | 119.6 (4) | C24—C25—C26 | 120.2 (4) |
| C14—C15—H15A | 120.2 | C24—C25—H35A | 119.9 |
| C16—C15—H15A | 120.2 | C26—C25—H35A | 119.9 |
| C15—C16—C11 | 121.1 (4) | C25—C26—C21 | 120.7 (4) |
| C15—C16—H16A | 119.5 | C25—C26—H36A | 119.7 |
| C11—C16—H16A | 119.5 | C21—C26—H36A | 119.7 |
Symmetry codes: (i) −x+1, y, −z+1/2; (ii) −x+1, y, −z+3/2.
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H2A···N2iii | 0.85 | 2.12 | 2.964 (4) | 180 |
| N2—H3A···N1iv | 0.88 | 2.12 | 2.964 (4) | 161 |
Symmetry codes: (iii) x, −y+1, z−1/2; (iv) x, −y+1, z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: WM2476).
References
- Anulewicz, R., Krygowski, T. M., Jaroszewska-Manaj, J. & Pniewska, B. (1991). Pol. J. Chem. 65, 465–471.
- Brandenburg, K. (1999). DIAMOND Crystal Impact GbR. Bonn, Germany.
- Bruker. (2001). SAINT-Plus Bruker AXS Inc., Madison, Wisconsin, USA.
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- Del Bene, J. E. & Elguero, J. (2006). J. Phys. Chem. A, 110, 7496–7502. [DOI] [PubMed]
- Fujiwara, H., Hayashi, T., Sugimoto, T., Nakazumi, H., Noguchi, S., Li, L., Yokogawa, K., Yasuzuka, S., Murata, K. & Mori, T. (2006). Inorg. Chem. 45, 5712–5714. [DOI] [PubMed]
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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/S1600536811013419/wm2476sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811013419/wm2476Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report



