Abstract
In the title compound, C16H10N2O, the dihedral angle formed by the benzene rings is 84.99 (7)°. The crystal structure is stabilized by intermolecular C—H⋯N and C—H⋯O hydrogen-bond interactions, forming chains running parallel to the b axis.
Related literature
For related literature, see: Arıcı et al. (2004 ▶); Radl et al. (2000 ▶); Bernstein et al. (1995 ▶); Zhao (2008 ▶).
Experimental
Crystal data
C16H10N2O
M r = 246.26
Triclinic,
a = 7.5217 (15) Å
b = 7.9759 (16) Å
c = 10.881 (2) Å
α = 96.78 (3)°
β = 93.34 (3)°
γ = 102.10 (3)°
V = 631.5 (2) Å3
Z = 2
Mo Kα radiation
μ = 0.08 mm−1
T = 293 (2) K
0.20 × 0.20 × 0.16 mm
Data collection
Rigaku Mercury2 diffractometer
Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2005 ▶) T min = 0.964, T max = 0.988
6576 measured reflections
2898 independent reflections
1943 reflections with I > 2σ(I)
R int = 0.028
Refinement
R[F 2 > 2σ(F 2)] = 0.059
wR(F 2) = 0.157
S = 1.04
2898 reflections
173 parameters
H-atom parameters constrained
Δρmax = 0.25 e Å−3
Δρmin = −0.21 e Å−3
Data collection: CrystalClear (Rigaku/MSC, 2005 ▶); cell refinement: CrystalClear; data reduction: CrystalClear; 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.
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808015079/rz2215sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536808015079/rz2215Isup2.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 |
|---|---|---|---|---|
| C3—H3⋯N1i | 0.93 | 2.62 | 3.486 (3) | 154 |
| C12—H12⋯O1ii | 0.93 | 2.42 | 3.268 (2) | 152 |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
This work was supported by a Start-up Grant from SEU to Professor Ren-Gen Xiong.
supplementary crystallographic information
Comment
Benzonitriles and their derivatives are important starting materials in the synthesis of some heterocyclic molecules (Radl et al., 2000; Arıcı et al., 2004). As part of our ongoing study on benzonitrile derivatives (Zhao, 2008), the crystal structure of one such derivatives is reported here.
The molecular structure of the title compound (Fig. 1) shows normal bond lengths and angles. The C≡N triple bond and C=O double bond lengths are 1.142 (2) and and 1.193 (2) Å, respectively. The benzene ring are oriented nearly perpendicular to each other, the dihedral angle they form being 84.99 (7)°. In the crystal structure, centrosymmetrically-related molecules are linked into dimeric units by intermolecular C—H···N hydrogen bonds (Table 1) forming ten-membered rings of graph-set R22(10) (Berstein et al., 1995). These dimers are further connected by intermolecular C—H···O hydrogen interactions to form chains running parallel to the b axis.
Experimental
To a solution of sodium cyanide (2 g) in water (18 ml) was added 4-formylbenzonitrile (2.62 g). The mixture was stirred for 15 min at room temperature, then a saturated sodium hydrosulfite solution (15 ml) was added dropwise. The resulting mixture was stirred at 293K until a yellow solid was obtained. The solid was filtered and recrystallized from a mixture of methanol (18 ml) and DMF (6 ml), to give crystals of the title compound suitable for X-ray diffraction analysis on slow evaporation of the solvents.
Refinement
All hydrogen atoms were placed at calculated positions and refined using the riding model approximation, with C—H = 0.93-0.97 Å and with Uiso(H) = 1.2 Ueq(C).
Figures
Fig. 1.
The molecular structure of the title compound with the atom-numbering scheme. Displacement ellipsoids were drawn at the 30% probability level
Crystal data
| C16H10N2O | Z = 2 |
| Mr = 246.26 | F000 = 256 |
| Triclinic, P1 | Dx = 1.295 Mg m−3 |
| Hall symbol: -P 1 | Mo Kα radiation λ = 0.71073 Å |
| a = 7.5217 (15) Å | Cell parameters from 2232 reflections |
| b = 7.9759 (16) Å | θ = 3.0–27.4º |
| c = 10.881 (2) Å | µ = 0.08 mm−1 |
| α = 96.78 (3)º | T = 293 (2) K |
| β = 93.34 (3)º | Block, yellow |
| γ = 102.10 (3)º | 0.20 × 0.20 × 0.16 mm |
| V = 631.5 (2) Å3 |
Data collection
| Rigaku Mercury2 diffractometer | 2898 independent reflections |
| Radiation source: fine-focus sealed tube | 1943 reflections with I > 2σ(I) |
| Monochromator: graphite | Rint = 0.028 |
| Detector resolution: 13.6612 pixels mm-1 | θmax = 27.5º |
| T = 293(2) K | θmin = 3.0º |
| CCD_Profile_fitting scans | h = −9→9 |
| Absorption correction: Multi-scan(CrystalClear; Rigaku/MSC, 2005) | k = −10→10 |
| Tmin = 0.964, Tmax = 0.988 | l = −14→14 |
| 6576 measured reflections |
Refinement
| Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
| Least-squares matrix: full | H-atom parameters constrained |
| R[F2 > 2σ(F2)] = 0.059 | w = 1/[σ2(Fo2) + (0.0717P)2 + 0.1009P] where P = (Fo2 + 2Fc2)/3 |
| wR(F2) = 0.157 | (Δ/σ)max = 0.002 |
| S = 1.04 | Δρmax = 0.25 e Å−3 |
| 2898 reflections | Δρmin = −0.21 e Å−3 |
| 173 parameters | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.168 (18) |
| Secondary atom site location: difference Fourier map |
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 | 0.1774 (2) | 0.4661 (2) | 0.18751 (15) | 0.0468 (4) | |
| C2 | 0.0347 (3) | 0.5506 (2) | 0.18255 (17) | 0.0546 (5) | |
| H2 | −0.0715 | 0.5081 | 0.2189 | 0.066* | |
| C3 | 0.0475 (3) | 0.6970 (2) | 0.12455 (17) | 0.0532 (5) | |
| H3 | −0.0493 | 0.7528 | 0.1218 | 0.064* | |
| C4 | 0.2055 (2) | 0.7599 (2) | 0.07065 (15) | 0.0468 (4) | |
| C5 | 0.3487 (3) | 0.6762 (2) | 0.07410 (17) | 0.0550 (5) | |
| H5 | 0.4545 | 0.7181 | 0.0371 | 0.066* | |
| C6 | 0.3339 (3) | 0.5301 (2) | 0.13273 (17) | 0.0550 (5) | |
| H6 | 0.4306 | 0.4742 | 0.1353 | 0.066* | |
| C7 | 0.2217 (3) | 0.9131 (2) | 0.00999 (17) | 0.0558 (5) | |
| C8 | 0.2389 (2) | 0.2017 (2) | 0.46012 (15) | 0.0457 (4) | |
| C9 | 0.2979 (3) | 0.2430 (2) | 0.58529 (16) | 0.0580 (5) | |
| H9 | 0.3178 | 0.3571 | 0.6226 | 0.070* | |
| C10 | 0.3274 (3) | 0.1162 (2) | 0.65476 (17) | 0.0599 (5) | |
| H10 | 0.3668 | 0.1447 | 0.7387 | 0.072* | |
| C11 | 0.2980 (2) | −0.0536 (2) | 0.59929 (16) | 0.0476 (4) | |
| C12 | 0.2369 (2) | −0.0974 (2) | 0.47534 (17) | 0.0521 (5) | |
| H12 | 0.2158 | −0.2118 | 0.4384 | 0.062* | |
| C13 | 0.2074 (3) | 0.0309 (2) | 0.40669 (16) | 0.0508 (5) | |
| H13 | 0.1656 | 0.0018 | 0.3232 | 0.061* | |
| C14 | 0.3367 (3) | −0.1839 (2) | 0.67244 (18) | 0.0560 (5) | |
| C15 | 0.2138 (3) | 0.3455 (2) | 0.38867 (17) | 0.0589 (5) | |
| N1 | 0.2355 (3) | 1.0349 (2) | −0.03745 (18) | 0.0757 (5) | |
| N2 | 0.3690 (3) | −0.2834 (2) | 0.73238 (17) | 0.0742 (6) | |
| O1 | 0.2335 (4) | 0.48933 (19) | 0.44054 (14) | 0.1312 (10) | |
| C16 | 0.1648 (3) | 0.3057 (2) | 0.25106 (16) | 0.0529 (5) | |
| H16A | 0.0413 | 0.2365 | 0.2358 | 0.063* | |
| H16B | 0.2458 | 0.2374 | 0.2147 | 0.063* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0585 (11) | 0.0387 (8) | 0.0433 (9) | 0.0106 (8) | −0.0022 (8) | 0.0092 (7) |
| C2 | 0.0563 (11) | 0.0512 (10) | 0.0595 (11) | 0.0119 (9) | 0.0080 (9) | 0.0189 (9) |
| C3 | 0.0581 (11) | 0.0491 (10) | 0.0585 (11) | 0.0204 (8) | 0.0042 (9) | 0.0166 (8) |
| C4 | 0.0600 (11) | 0.0400 (8) | 0.0405 (8) | 0.0105 (8) | −0.0016 (8) | 0.0090 (7) |
| C5 | 0.0575 (11) | 0.0531 (10) | 0.0572 (11) | 0.0126 (9) | 0.0064 (9) | 0.0171 (9) |
| C6 | 0.0573 (11) | 0.0531 (10) | 0.0592 (11) | 0.0196 (9) | 0.0014 (9) | 0.0142 (9) |
| C7 | 0.0694 (13) | 0.0504 (10) | 0.0516 (10) | 0.0168 (9) | 0.0060 (9) | 0.0153 (8) |
| C8 | 0.0579 (10) | 0.0367 (8) | 0.0456 (9) | 0.0140 (7) | 0.0060 (8) | 0.0104 (7) |
| C9 | 0.0864 (14) | 0.0370 (9) | 0.0500 (10) | 0.0134 (9) | 0.0019 (10) | 0.0055 (8) |
| C10 | 0.0798 (14) | 0.0507 (10) | 0.0478 (10) | 0.0099 (10) | −0.0036 (9) | 0.0133 (8) |
| C11 | 0.0474 (9) | 0.0431 (9) | 0.0569 (10) | 0.0109 (7) | 0.0092 (8) | 0.0212 (8) |
| C12 | 0.0656 (12) | 0.0330 (8) | 0.0596 (11) | 0.0121 (8) | 0.0076 (9) | 0.0106 (8) |
| C13 | 0.0668 (11) | 0.0378 (9) | 0.0486 (10) | 0.0132 (8) | 0.0022 (8) | 0.0073 (7) |
| C14 | 0.0566 (11) | 0.0512 (10) | 0.0661 (12) | 0.0144 (9) | 0.0103 (9) | 0.0243 (9) |
| C15 | 0.0930 (15) | 0.0367 (9) | 0.0514 (10) | 0.0225 (9) | 0.0028 (10) | 0.0108 (8) |
| N1 | 0.0880 (13) | 0.0672 (11) | 0.0853 (13) | 0.0269 (10) | 0.0212 (10) | 0.0399 (10) |
| N2 | 0.0837 (13) | 0.0672 (11) | 0.0843 (13) | 0.0263 (10) | 0.0116 (10) | 0.0410 (10) |
| O1 | 0.296 (3) | 0.0429 (8) | 0.0603 (10) | 0.0630 (13) | −0.0189 (13) | 0.0018 (7) |
| C16 | 0.0680 (12) | 0.0387 (9) | 0.0527 (10) | 0.0126 (8) | −0.0010 (9) | 0.0108 (8) |
Geometric parameters (Å, °)
| C1—C6 | 1.380 (3) | C8—C15 | 1.496 (2) |
| C1—C2 | 1.383 (2) | C9—C10 | 1.377 (2) |
| C1—C16 | 1.513 (2) | C9—H9 | 0.9300 |
| C2—C3 | 1.381 (2) | C10—C11 | 1.384 (3) |
| C2—H2 | 0.9300 | C10—H10 | 0.9300 |
| C3—C4 | 1.381 (3) | C11—C12 | 1.379 (2) |
| C3—H3 | 0.9300 | C11—C14 | 1.446 (2) |
| C4—C5 | 1.382 (3) | C12—C13 | 1.382 (2) |
| C4—C7 | 1.442 (2) | C12—H12 | 0.9300 |
| C5—C6 | 1.381 (2) | C13—H13 | 0.9300 |
| C5—H5 | 0.9300 | C14—N2 | 1.140 (2) |
| C6—H6 | 0.9300 | C15—O1 | 1.193 (2) |
| C7—N1 | 1.142 (2) | C15—C16 | 1.501 (3) |
| C8—C13 | 1.383 (2) | C16—H16A | 0.9700 |
| C8—C9 | 1.387 (2) | C16—H16B | 0.9700 |
| C6—C1—C2 | 118.89 (15) | C8—C9—H9 | 119.7 |
| C6—C1—C16 | 119.65 (16) | C9—C10—C11 | 119.80 (17) |
| C2—C1—C16 | 121.46 (16) | C9—C10—H10 | 120.1 |
| C3—C2—C1 | 121.07 (17) | C11—C10—H10 | 120.1 |
| C3—C2—H2 | 119.5 | C12—C11—C10 | 120.45 (15) |
| C1—C2—H2 | 119.5 | C12—C11—C14 | 120.50 (16) |
| C2—C3—C4 | 119.32 (17) | C10—C11—C14 | 119.03 (17) |
| C2—C3—H3 | 120.3 | C11—C12—C13 | 119.21 (16) |
| C4—C3—H3 | 120.3 | C11—C12—H12 | 120.4 |
| C3—C4—C5 | 120.28 (15) | C13—C12—H12 | 120.4 |
| C3—C4—C7 | 120.13 (16) | C12—C13—C8 | 121.10 (17) |
| C5—C4—C7 | 119.59 (16) | C12—C13—H13 | 119.5 |
| C6—C5—C4 | 119.70 (17) | C8—C13—H13 | 119.5 |
| C6—C5—H5 | 120.2 | N2—C14—C11 | 178.3 (2) |
| C4—C5—H5 | 120.2 | O1—C15—C8 | 120.30 (17) |
| C1—C6—C5 | 120.74 (17) | O1—C15—C16 | 120.78 (16) |
| C1—C6—H6 | 119.6 | C8—C15—C16 | 118.92 (15) |
| C5—C6—H6 | 119.6 | C15—C16—C1 | 113.15 (14) |
| N1—C7—C4 | 179.5 (2) | C15—C16—H16A | 108.9 |
| C13—C8—C9 | 118.91 (15) | C1—C16—H16A | 108.9 |
| C13—C8—C15 | 122.97 (16) | C15—C16—H16B | 108.9 |
| C9—C8—C15 | 118.12 (15) | C1—C16—H16B | 108.9 |
| C10—C9—C8 | 120.52 (16) | H16A—C16—H16B | 107.8 |
| C10—C9—H9 | 119.7 |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C3—H3···N1i | 0.93 | 2.62 | 3.486 (3) | 154 |
| C12—H12···O1ii | 0.93 | 2.42 | 3.268 (2) | 152 |
Symmetry codes: (i) −x, −y+2, −z; (ii) x, y−1, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: RZ2215).
References
- Arıcı, C., Ülkü, D., Kırılmış, C., Koca, M. & Ahmedzade, M. (2004). Acta Cryst. E60, o1211–o1212.
- Bernstein, J., Davis, R. E., Shimoni, L. & Chang, N.-L. (1995). Angew. Chem. Int. Ed. Engl 34, 1555–1573.
- Radl, S., Hezky, P., Konvicka, P. & Krejgi, J. (2000). Collect. Czech. Chem. Commun.65, 1093–1108.
- Rigaku/MSC (2005). CrystalClear and CrystalStructure Rigaku/MSC, The Woodlands, Texas, USA.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Zhao, Y.-Y. (2008). Acta Cryst. E64, o761. [DOI] [PMC free article] [PubMed]
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808015079/rz2215sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536808015079/rz2215Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

