Abstract
In the title compound, NCCH2C6H4CH2CN, the bond lengths and angles are within normal ranges. The benzene ring makes dihedral angles of 4.94 (8) and 77.04 (8)° with the C—C—C—N mean planes. Weak non-conventional C—H⋯N hydrogen bonds are effective in the stabilization of the crystal structure. The weak C—H⋯N contacts form antiparallel chains running in the a + c direction, and ring systems with two N-atom acceptors and four H-atom donors.
Related literature
For reactions of Woollins’ Reagent see: Gray et al. (2005 ▶); Hua et al. (2006 ▶, 2009 ▶); Hua & Woollins (2009 ▶). For bond-length data, see: Allen et al. (1987 ▶).
Experimental
Crystal data
C10H8N2
M r = 156.18
Monoclinic,
a = 8.3882 (18) Å
b = 8.1605 (15) Å
c = 11.993 (2) Å
β = 101.890 (6)°
V = 803.4 (3) Å3
Z = 4
Mo Kα radiation
μ = 0.08 mm−1
T = 93 K
0.30 × 0.25 × 0.15 mm
Data collection
Rigaku Mercury CCD diffractometer
Absorption correction: multi-scan (CrystalClear; Rigaku, 2004 ▶) T min = 0.977, T max = 0.988
5271 measured reflections
1660 independent reflections
1330 reflections with I > 2σ(I)
R int = 0.031
Refinement
R[F 2 > 2σ(F 2)] = 0.051
wR(F 2) = 0.133
S = 1.09
1660 reflections
109 parameters
H-atom parameters constrained
Δρmax = 0.28 e Å−3
Δρmin = −0.21 e Å−3
Data collection: CrystalClear (Rigaku, 2004 ▶); 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: PLATON (Spek, 2009 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809041506/si2203sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809041506/si2203Isup2.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 |
|---|---|---|---|---|
| C9—H9A⋯N1i | 0.99 | 2.57 | 3.5605 (18) | 176 |
| C9—H9B⋯N1ii | 0.99 | 2.56 | 3.5210 (17) | 165 |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
The authors are grateful to the University of St Andrews and the Engineering and Physical Science Research Council (EPRSC, UK) for financial support.
supplementary crystallographic information
Comment
Recently, we have continued our studies exploring the reactivity of Woollins reagent towards different organic substituents (Gray et al. 2005, Hua et al. 2006 and 2009; Hua & Woollins 2009). Thereby 2,2'-(1,2-phenylene)diacetonitrile represents one of the starting materials. Single crystals of 2,5-dihydroxybenzaldehyde for X-ray crystallographic analysis were obtained by recrystallization from dichloromethane-hexane solution.
The bond lengths (Allen et al., 1987) and angles are within normal ranges.The benzene ring makes the dihedral angles of 4.94 (8) and 77.04 (8)° with the mean planes of C1—C7—C8—N1 and C2—C9—C10—N2 respectively. The antiparallel chains running in a+cdirection are generated through the weak C—H···N contacts, glide plane and inversinon symmetry operations[see Fig. 2 and Table 1]. Inversion symmetry forms also C—H···N ring systems consisting of two N acceptors and four H atom donors,where the centroid-centroid distance between the inversion-related benzene ring planes is 3.6809 (10) Å, the perpendicular plane to plane distance is 3.364 Å, and the slippage between the planes is 1.495 Å.
Experimental
Commercially available 2,2'-(1,2-phenylene)diacetonitrile was recrystallized from dichloromethane-hexane.
Refinement
H atoms were positioned geometrically (C—H = 0.93–0.97 Å) and were treated as riding on their parent C atoms with Uiso(H)= 1.2–1.5Ueq(C).
Figures
Fig. 1.
The molecular structure of the title compound with displacement ellipsoids drawn at the 50% probability level.
Fig. 2.
View along the b direction of the crystal packing of the title compound with non-conventional hydrogen bonding shown as dashed lines.
Crystal data
| C10H8N2 | F(000) = 328 |
| Mr = 156.18 | Dx = 1.291 Mg m−3 |
| Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
| a = 8.3882 (18) Å | Cell parameters from 2633 reflections |
| b = 8.1605 (15) Å | θ = 2.7–28.3° |
| c = 11.993 (2) Å | µ = 0.08 mm−1 |
| β = 101.890 (6)° | T = 93 K |
| V = 803.4 (3) Å3 | Block, colorless |
| Z = 4 | 0.30 × 0.25 × 0.15 mm |
Data collection
| Rigaku Mercury CCD diffractometer | 1660 independent reflections |
| Radiation source: rotating anode | 1330 reflections with I > 2σ(I) |
| confocal | Rint = 0.031 |
| Detector resolution: 0.83 pixels mm-1 | θmax = 28.7°, θmin = 2.7° |
| ω scans | h = −11→10 |
| Absorption correction: multi-scan (CrystalClear; Rigaku, 2004) | k = −9→10 |
| Tmin = 0.977, Tmax = 0.988 | l = −13→15 |
| 5271 measured 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)] = 0.051 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.133 | H-atom parameters constrained |
| S = 1.09 | w = 1/[σ2(Fo2) + (0.0698P)2 + 0.0077P] where P = (Fo2 + 2Fc2)/3 |
| 1660 reflections | (Δ/σ)max = 0.001 |
| 109 parameters | Δρmax = 0.28 e Å−3 |
| 0 restraints | Δρmin = −0.21 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 | ||
| C1 | 0.77845 (13) | 0.05887 (16) | 0.95174 (10) | 0.0215 (3) | |
| C2 | 0.72184 (13) | 0.13136 (16) | 1.04228 (10) | 0.0218 (3) | |
| C7 | 0.83384 (14) | 0.16768 (16) | 0.86390 (10) | 0.0257 (3) | |
| H7A | 0.7404 | 0.2350 | 0.8253 | 0.031* | |
| H7B | 0.9191 | 0.2433 | 0.9038 | 0.031* | |
| C3 | 0.66532 (15) | 0.03264 (16) | 1.12009 (11) | 0.0250 (3) | |
| H3 | 0.6273 | 0.0817 | 1.1816 | 0.030* | |
| C8 | 0.89813 (14) | 0.07728 (16) | 0.77779 (10) | 0.0252 (3) | |
| N1 | 0.94789 (13) | 0.00673 (14) | 0.70957 (10) | 0.0313 (3) | |
| C10 | 0.88145 (15) | 0.38338 (15) | 1.10361 (10) | 0.0248 (4) | |
| C9 | 0.71906 (14) | 0.31597 (16) | 1.05579 (11) | 0.0249 (3) | |
| H9A | 0.6768 | 0.3666 | 0.9805 | 0.030* | |
| H9B | 0.6438 | 0.3448 | 1.1064 | 0.030* | |
| C5 | 0.71958 (14) | −0.20835 (16) | 1.02028 (11) | 0.0278 (4) | |
| H5 | 0.7192 | −0.3242 | 1.0126 | 0.033* | |
| C6 | 0.77646 (14) | −0.11076 (16) | 0.94203 (11) | 0.0248 (4) | |
| H6 | 0.8146 | −0.1607 | 0.8809 | 0.030* | |
| N2 | 1.00792 (13) | 0.43446 (14) | 1.14226 (9) | 0.0318 (3) | |
| C4 | 0.66348 (14) | −0.13701 (17) | 1.10929 (11) | 0.0271 (3) | |
| H4 | 0.6239 | −0.2034 | 1.1628 | 0.033* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0169 (6) | 0.0226 (7) | 0.0238 (7) | 0.0002 (4) | 0.0009 (5) | 0.0007 (5) |
| C2 | 0.0176 (6) | 0.0247 (7) | 0.0221 (7) | 0.0023 (5) | 0.0013 (5) | −0.0002 (5) |
| C7 | 0.0267 (7) | 0.0232 (7) | 0.0274 (7) | 0.0013 (5) | 0.0062 (5) | 0.0001 (6) |
| C3 | 0.0207 (7) | 0.0311 (8) | 0.0220 (7) | −0.0002 (5) | 0.0019 (5) | −0.0002 (6) |
| C8 | 0.0217 (7) | 0.0285 (7) | 0.0252 (7) | −0.0031 (5) | 0.0043 (5) | 0.0008 (6) |
| N1 | 0.0292 (7) | 0.0337 (8) | 0.0319 (7) | −0.0012 (5) | 0.0085 (5) | −0.0019 (5) |
| C10 | 0.0321 (7) | 0.0198 (7) | 0.0243 (7) | 0.0044 (5) | 0.0097 (6) | −0.0012 (5) |
| C9 | 0.0256 (7) | 0.0240 (8) | 0.0250 (7) | 0.0021 (5) | 0.0049 (5) | −0.0018 (6) |
| C5 | 0.0257 (7) | 0.0210 (7) | 0.0342 (8) | −0.0006 (5) | 0.0007 (6) | 0.0018 (6) |
| C6 | 0.0241 (7) | 0.0235 (8) | 0.0263 (7) | 0.0027 (5) | 0.0040 (5) | −0.0023 (6) |
| N2 | 0.0325 (7) | 0.0272 (7) | 0.0359 (7) | −0.0019 (5) | 0.0071 (5) | −0.0044 (5) |
| C4 | 0.0234 (7) | 0.0314 (8) | 0.0253 (7) | −0.0034 (5) | 0.0022 (5) | 0.0054 (6) |
Geometric parameters (Å, °)
| C1—C6 | 1.3890 (19) | C8—N1 | 1.1471 (15) |
| C1—C2 | 1.4025 (16) | C10—N2 | 1.1452 (15) |
| C1—C7 | 1.5218 (18) | C10—C9 | 1.4714 (17) |
| C2—C3 | 1.3882 (18) | C9—H9A | 0.9900 |
| C2—C9 | 1.5159 (18) | C9—H9B | 0.9900 |
| C7—C8 | 1.4599 (17) | C5—C4 | 1.3809 (18) |
| C7—H7A | 0.9900 | C5—C6 | 1.3882 (17) |
| C7—H7B | 0.9900 | C5—H5 | 0.9500 |
| C3—C4 | 1.390 (2) | C6—H6 | 0.9500 |
| C3—H3 | 0.9500 | C4—H4 | 0.9500 |
| C6—C1—C2 | 119.02 (11) | N2—C10—C9 | 178.97 (14) |
| C6—C1—C7 | 121.58 (11) | C10—C9—C2 | 112.32 (10) |
| C2—C1—C7 | 119.36 (12) | C10—C9—H9A | 109.1 |
| C3—C2—C1 | 119.52 (13) | C2—C9—H9A | 109.1 |
| C3—C2—C9 | 119.34 (11) | C10—C9—H9B | 109.1 |
| C1—C2—C9 | 121.14 (11) | C2—C9—H9B | 109.1 |
| C8—C7—C1 | 113.88 (11) | H9A—C9—H9B | 107.9 |
| C8—C7—H7A | 108.8 | C4—C5—C6 | 120.00 (12) |
| C1—C7—H7A | 108.8 | C4—C5—H5 | 120.0 |
| C8—C7—H7B | 108.8 | C6—C5—H5 | 120.0 |
| C1—C7—H7B | 108.8 | C1—C6—C5 | 121.00 (11) |
| H7A—C7—H7B | 107.7 | C1—C6—H6 | 119.5 |
| C2—C3—C4 | 120.94 (12) | C5—C6—H6 | 119.5 |
| C2—C3—H3 | 119.5 | C5—C4—C3 | 119.53 (12) |
| C4—C3—H3 | 119.5 | C5—C4—H4 | 120.2 |
| N1—C8—C7 | 179.54 (14) | C3—C4—H4 | 120.2 |
| C6—C1—C2—C3 | 0.04 (16) | C3—C2—C9—C10 | 103.33 (13) |
| C7—C1—C2—C3 | 177.52 (11) | C1—C2—C9—C10 | −77.54 (13) |
| C6—C1—C2—C9 | −179.09 (11) | C2—C1—C6—C5 | 0.00 (17) |
| C7—C1—C2—C9 | −1.61 (15) | C7—C1—C6—C5 | −177.43 (10) |
| C6—C1—C7—C8 | −5.75 (16) | C4—C5—C6—C1 | 0.15 (18) |
| C2—C1—C7—C8 | 176.84 (10) | C6—C5—C4—C3 | −0.34 (18) |
| C1—C2—C3—C4 | −0.23 (17) | C2—C3—C4—C5 | 0.38 (18) |
| C9—C2—C3—C4 | 178.91 (11) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C9—H9A···N1i | 0.99 | 2.57 | 3.5605 (18) | 176 |
| C9—H9B···N1ii | 0.99 | 2.56 | 3.5210 (17) | 165 |
Symmetry codes: (i) −x+3/2, y+1/2, −z+3/2; (ii) x−1/2, −y+1/2, z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SI2203).
References
- Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1–19.
- Gray, I. P., Bhattachcharyya, P., Slawin, A. M. Z. & Woollins, J. D. (2005). Chem. Eur. J 11, 6221–6227. [DOI] [PubMed]
- Hua, G., Li, Y., Fuller, A., Slawin, A. M. Z. & Woollins, J. D. (2009). Eur. J. Org. Chem pp. 1612–1618.
- Hua, G., Li, Y., Slawin, A. M. Z. & Woollins, J. D. (2006). Org. Lett 8, 5251–5254. [DOI] [PubMed]
- Hua, G. & Woollins, J. D. (2009). Angew. Chem., Int. Ed 48, 1368–1377. [DOI] [PubMed]
- Rigaku (2004). CrystalClear Rigaku Corporation, Tokyo, Japan.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Spek, A. L. (2009). Acta Cryst. D65, 148–155. [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/S1600536809041506/si2203sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809041506/si2203Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


