Acta Cryst. (2009). E65, o2373 [ doi:10.1107/S1600536809032863 ]
In the title compound, C7H7N2+·BF4-, the non-H atoms of the cation are almost coplanar (r.m.s. deviation = 0.035 Å). The cations and anions are connected by intermolecular N-H
F and N-HN hydrogen bonds, forming a two-dimensional network parallel to (10
).
The commercial 2-aminobenzonitrile (3 mmol, 0.55 g) and HBF4 (0.5 ml) were dissolved in ethanol (20 ml). Colourless block-shaped crystals of the title compound suitable for X-ray analysis were obtained by slow evaporation at room temperature.
All H atoms attached to C and N atoms were positioned geometrically and treated as riding, with C-H = 0.93 Å, N-H = 0.89 Å and Uiso(H) = 1.2Ueq(C) and Uiso(H) = 1.5Ueq(N). A rotating-group model was used for the -NH3 group.
Data collection: CrystalClear (Rigaku, 2005); cell refinement: CrystalClear (Rigaku, 2005); data reduction: CrystalClear (Rigaku, 2005); 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).
![[Figure 1]](./ci2881fig1thm.gif)
| Fig. 1. A view of the title compound with the atomic numbering scheme. Displacement ellipsoids are drawn at the 30% probability level. |
![[Figure 2]](./ci2881fig2thm.gif)
| Fig. 2. The crystal packing of the title compound, viewed along the c axis. Hydrogen bonds are shown as dashed lines. C-bound H atoms have been omitted for clarity |
| C7H7N2+·BF4− | F(000) = 416 |
| Mr = 205.96 | Dx = 1.579 Mg m−3 |
| Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2yn | Cell parameters from 1417 reflections |
| a = 10.971 (2) Å | θ = 3.4–27.5° |
| b = 7.3565 (15) Å | µ = 0.16 mm−1 |
| c = 11.022 (2) Å | T = 298 K |
| β = 103.11 (3)° | Block, colourless |
| V = 866.4 (3) Å3 | 0.30 × 0.25 × 0.20 mm |
| Z = 4 |
| Rigaku Mercury2 diffractometer | 1978 independent reflections |
| Radiation source: fine-focus sealed tube | 1417 reflections with I > 2σ(I) |
| graphite | Rint = 0.041 |
| Detector resolution: 13.6612 pixels mm-1 | θmax = 27.5°, θmin = 3.4° |
| CCD profile fitting scans | h = −14→14 |
| Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | k = −9→9 |
| Tmin = 0.96, Tmax = 1.00 | l = −14→14 |
| 8625 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)] = 0.056 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.141 | H-atom parameters constrained |
| S = 1.08 | w = 1/[σ2(Fo2) + (0.0571P)2 + 0.4139P] where P = (Fo2 + 2Fc2)/3 |
| 1978 reflections | (Δ/σ)max = 0.001 |
| 128 parameters | Δρmax = 0.32 e Å−3 |
| 0 restraints | Δρmin = −0.32 e Å−3 |
| C7H7N2+·BF4− | V = 866.4 (3) Å3 |
| Mr = 205.96 | Z = 4 |
| Monoclinic, P21/n | Mo Kα radiation |
| a = 10.971 (2) Å | µ = 0.16 mm−1 |
| b = 7.3565 (15) Å | T = 298 K |
| c = 11.022 (2) Å | 0.30 × 0.25 × 0.20 mm |
| β = 103.11 (3)° |
| Rigaku Mercury2 diffractometer | 1978 independent reflections |
| Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | 1417 reflections with I > 2σ(I) |
| Tmin = 0.96, Tmax = 1.00 | Rint = 0.041 |
| 8625 measured reflections | θmax = 27.5° |
| R[F2 > 2σ(F2)] = 0.056 | H-atom parameters constrained |
| wR(F2) = 0.141 | Δρmax = 0.32 e Å−3 |
| S = 1.08 | Δρmin = −0.32 e Å−3 |
| 1978 reflections | Absolute structure: ? |
| 128 parameters | Flack parameter: ? |
| 0 restraints | Rogers parameter: ? |
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 | ||
| F4 | 0.36113 (13) | 0.72246 (19) | 0.25229 (13) | 0.0500 (4) | |
| F3 | 0.48625 (14) | 0.7353 (2) | 0.44366 (13) | 0.0575 (4) | |
| N1 | 0.59296 (16) | 0.6600 (3) | 0.69414 (15) | 0.0337 (4) | |
| H1A | 0.6182 | 0.5482 | 0.6812 | 0.051* | |
| H1B | 0.6589 | 0.7275 | 0.7293 | 0.051* | |
| H1C | 0.5548 | 0.7094 | 0.6218 | 0.051* | |
| F2 | 0.34337 (15) | 0.9602 (2) | 0.37300 (16) | 0.0625 (5) | |
| C1 | 0.50557 (18) | 0.6518 (3) | 0.77689 (18) | 0.0302 (5) | |
| F1 | 0.51445 (14) | 0.9330 (3) | 0.29556 (18) | 0.0737 (6) | |
| C2 | 0.5337 (2) | 0.7425 (3) | 0.89064 (19) | 0.0348 (5) | |
| C6 | 0.3969 (2) | 0.5547 (3) | 0.7402 (2) | 0.0437 (6) | |
| H6 | 0.3792 | 0.4939 | 0.6643 | 0.052* | |
| N2 | 0.7317 (2) | 0.9429 (3) | 0.9488 (2) | 0.0586 (6) | |
| C7 | 0.6444 (2) | 0.8517 (3) | 0.9248 (2) | 0.0428 (6) | |
| B1 | 0.4282 (2) | 0.8402 (3) | 0.3425 (2) | 0.0359 (6) | |
| C4 | 0.3405 (3) | 0.6365 (4) | 0.9311 (3) | 0.0580 (8) | |
| H4 | 0.2840 | 0.6313 | 0.9824 | 0.070* | |
| C3 | 0.4507 (2) | 0.7323 (3) | 0.9687 (2) | 0.0483 (6) | |
| H3 | 0.4693 | 0.7897 | 1.0458 | 0.058* | |
| C5 | 0.3138 (2) | 0.5485 (4) | 0.8180 (3) | 0.0570 (7) | |
| H5 | 0.2393 | 0.4842 | 0.7934 | 0.068* |
| U11 | U22 | U33 | U12 | U13 | U23 | |
| F4 | 0.0566 (9) | 0.0453 (8) | 0.0442 (8) | −0.0023 (6) | 0.0037 (7) | −0.0056 (6) |
| F3 | 0.0587 (9) | 0.0613 (10) | 0.0455 (8) | 0.0069 (7) | −0.0029 (7) | 0.0162 (7) |
| N1 | 0.0376 (10) | 0.0351 (9) | 0.0291 (9) | 0.0028 (8) | 0.0092 (7) | −0.0004 (7) |
| F2 | 0.0658 (9) | 0.0467 (9) | 0.0762 (11) | 0.0167 (7) | 0.0186 (8) | −0.0097 (8) |
| C1 | 0.0324 (10) | 0.0288 (10) | 0.0303 (10) | 0.0072 (8) | 0.0091 (8) | 0.0036 (8) |
| F1 | 0.0435 (8) | 0.0830 (12) | 0.0922 (13) | −0.0162 (8) | 0.0107 (8) | 0.0342 (10) |
| C2 | 0.0420 (11) | 0.0316 (11) | 0.0311 (11) | 0.0065 (9) | 0.0091 (9) | 0.0001 (9) |
| C6 | 0.0356 (12) | 0.0447 (14) | 0.0491 (14) | 0.0034 (10) | 0.0058 (10) | −0.0046 (11) |
| N2 | 0.0597 (14) | 0.0587 (14) | 0.0558 (14) | −0.0010 (12) | 0.0095 (11) | −0.0178 (11) |
| C7 | 0.0542 (15) | 0.0392 (13) | 0.0347 (12) | 0.0088 (12) | 0.0094 (11) | −0.0075 (10) |
| B1 | 0.0324 (12) | 0.0315 (12) | 0.0412 (13) | 0.0004 (10) | 0.0030 (10) | 0.0053 (11) |
| C4 | 0.0609 (17) | 0.0541 (17) | 0.0729 (19) | 0.0135 (14) | 0.0445 (15) | 0.0118 (14) |
| C3 | 0.0670 (16) | 0.0430 (13) | 0.0422 (13) | 0.0147 (12) | 0.0277 (12) | 0.0018 (10) |
| C5 | 0.0375 (13) | 0.0529 (16) | 0.085 (2) | 0.0011 (12) | 0.0223 (13) | 0.0022 (14) |
| F4—B1 | 1.396 (3) | C2—C3 | 1.389 (3) |
| F3—B1 | 1.387 (3) | C2—C7 | 1.434 (3) |
| N1—C1 | 1.467 (2) | C6—C5 | 1.387 (4) |
| N1—H1A | 0.89 | C6—H6 | 0.93 |
| N1—H1B | 0.89 | N2—C7 | 1.150 (3) |
| N1—H1C | 0.89 | C4—C5 | 1.376 (4) |
| F2—B1 | 1.379 (3) | C4—C3 | 1.379 (4) |
| C1—C6 | 1.370 (3) | C4—H4 | 0.93 |
| C1—C2 | 1.392 (3) | C3—H3 | 0.93 |
| F1—B1 | 1.361 (3) | C5—H5 | 0.93 |
| C1—N1—H1A | 109.5 | F1—B1—F2 | 109.7 (2) |
| C1—N1—H1B | 109.5 | F1—B1—F3 | 110.68 (19) |
| H1A—N1—H1B | 109.5 | F2—B1—F3 | 111.9 (2) |
| C1—N1—H1C | 109.5 | F1—B1—F4 | 109.9 (2) |
| H1A—N1—H1C | 109.5 | F2—B1—F4 | 107.16 (18) |
| H1B—N1—H1C | 109.5 | F3—B1—F4 | 107.42 (19) |
| C6—C1—C2 | 121.1 (2) | C5—C4—C3 | 120.3 (2) |
| C6—C1—N1 | 119.06 (19) | C5—C4—H4 | 119.9 |
| C2—C1—N1 | 119.87 (19) | C3—C4—H4 | 119.9 |
| C3—C2—C1 | 119.3 (2) | C4—C3—C2 | 119.7 (2) |
| C3—C2—C7 | 120.2 (2) | C4—C3—H3 | 120.2 |
| C1—C2—C7 | 120.42 (19) | C2—C3—H3 | 120.2 |
| C1—C6—C5 | 119.0 (2) | C4—C5—C6 | 120.6 (2) |
| C1—C6—H6 | 120.5 | C4—C5—H5 | 119.7 |
| C5—C6—H6 | 120.5 | C6—C5—H5 | 119.7 |
| N2—C7—C2 | 177.7 (3) | ||
| C6—C1—C2—C3 | 0.8 (3) | C5—C4—C3—C2 | 1.2 (4) |
| N1—C1—C2—C3 | −179.40 (19) | C1—C2—C3—C4 | −1.6 (3) |
| C6—C1—C2—C7 | −176.6 (2) | C7—C2—C3—C4 | 175.8 (2) |
| N1—C1—C2—C7 | 3.2 (3) | C3—C4—C5—C6 | 0.0 (4) |
| C2—C1—C6—C5 | 0.4 (3) | C1—C6—C5—C4 | −0.8 (4) |
| N1—C1—C6—C5 | −179.4 (2) |
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1A···N2i | 0.89 | 2.54 | 3.179 (3) | 130 |
| N1—H1A···F4ii | 0.89 | 2.12 | 2.896 (2) | 146 |
| N1—H1B···F4iii | 0.89 | 2.21 | 2.993 (2) | 147 |
| N1—H1C···F3 | 0.89 | 1.95 | 2.799 (2) | 160 |
| Symmetry codes: (i) −x+3/2, y−1/2, −z+3/2; (ii) −x+1, −y+1, −z+1; (iii) x+1/2, −y+3/2, z+1/2. |
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1A···N2i | 0.89 | 2.54 | 3.179 (3) | 130 |
| N1—H1A···F4ii | 0.89 | 2.12 | 2.896 (2) | 146 |
| N1—H1B···F4iii | 0.89 | 2.21 | 2.993 (2) | 147 |
| N1—H1C···F3 | 0.89 | 1.95 | 2.799 (2) | 160 |
| Symmetry codes: (i) −x+3/2, y−1/2, −z+3/2; (ii) −x+1, −y+1, −z+1; (iii) x+1/2, −y+3/2, z+1/2. |
This work was supported by the Outstanding Doctoral Dissertation Fund of Southeast University.
Chen, Z.-F., Xiong, R.-G., Zhang, J., Zuo, J.-L., You, X.-Z., Che, C.-M. & Fun, H.-K. (2000). J. Chem. Soc. Dalton Trans. pp. 4010–4012.
Fu, D.-W., Song, Y.-M., Wang, G.-X., Ye, Q., Xiong, R.-G., Akutagawa, T., Nakamura, T., Chan, P. W. H. & Huang, S.-P. (2007). J. Am. Chem. Soc. 129, 5346–5347.
Fu, D.-W. & Xiong, R.-G. (2008). Dalton Trans. pp. 3946–3948.
Fu, D.-W., Zhang, W. & Xiong, R.-G. (2008). Cryst. Growth Des. 8, 3461–3464.
Rigaku (2005). CrystalClear. Rigaku Corporation, Tokyo, Japan.
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.
Wang, L.-Z., Wang, X.-S., Li, Y.-H., Bai, Z.-P., Xiong, R.-G., Xiong, M. & Li, G.-W. (2002). Chin. J. Inorg. Chem. 18, 1191–1194.
Xie, Y.-R., Zhao, H., Wang, X.-S., Qu, Z.-R., Xiong, R.-G., Xue, X.-A., Xue, Z.-L. & You, X.-Z. (2003). Eur. J. Inorg. Chem. 20, 3712-3715.
Xiong, R.-G., Zuo, J.-L., You, X.-Z., Fun, H.-K. & Raj, S. S. S. (1999). New J. Chem. 23, 1051–1052.
Zhang, J., Xiong, R.-G., Chen, X.-T., Che, C.-M., Xue, Z.-L. & You, X.-Z. (2001). Organometallics, 20, 4118–4121.
The construction of metal-organic coordination compounds has attracted much attention owing to potential functions, such as permittivity, fluorescence, magnetism and optical properties (Fu et al., 2007; Chen et al., 2000; Fu & Xiong (2008); Xie et al., 2003; Zhang et al.,2001; Xiong et al., 1999). Nitrile derivatives are a class of excellent ligands for the construction of novel metal-organic frameworks. (Wang et al. 2002; Fu et al., 2008). We report here the crystal structure of the title compound, 2-cyanobenzenaminium tetrafluoroborate.
In the 2-cyanobenzenaminium cation (Fig.1), the nitrile group and the benzene ring are almost coplanar. The nitrile group C7≡N2 bond length of 1.150 (3) Å is within the normal range.
In the crystal structure, all the amine group H atoms are involved in N—H···F hydrogen bonds (Table 1) with F atoms of the BF4- anion. These hydrogen bonds along with N—H···N hydrogen bonds link the ionic units into a two-dimensional network (Fig. 2) parallel to the (101).