Abstract
In the title compound, C15H14N2O, the molecule skeleton displays an approximately planar structure except for the ethyl group [maximum deviation = 0.042 (1) Å]. The methoxyphenyl ring and butanylidenemalononitrile groups are located on opposite sides of the C=C bond, showing an E configuration. Weak intermolecular C—H⋯N hydrogen bonding is present in the crystal structure.
Related literature
For the use of malononitrile-containing compounds as building blocks in synthesis, see: Liu et al. (2002 ▶); Sepiol & Milart (1985 ▶); Zhang et al. (2003 ▶). For a related structure, see: Kang & Chen (2009 ▶).
Experimental
Crystal data
C15H14N2O
M r = 238.28
Monoclinic,
a = 12.3371 (3) Å
b = 8.8832 (2) Å
c = 12.8554 (3) Å
β = 108.050 (2)°
V = 1339.53 (5) Å3
Z = 4
Cu Kα radiation
μ = 0.60 mm−1
T = 291 K
0.42 × 0.40 × 0.36 mm
Data collection
Oxford Diffraction Gemini S Ultra diffractometer
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009 ▶) T min = 0.787, T max = 0.813
9020 measured reflections
2456 independent reflections
2266 reflections with I > 2σ(I)
R int = 0.014
Refinement
R[F 2 > 2σ(F 2)] = 0.039
wR(F 2) = 0.112
S = 1.05
2456 reflections
165 parameters
3 restraints
H-atom parameters constrained
Δρmax = 0.11 e Å−3
Δρmin = −0.14 e Å−3
Data collection: CrysAlis CCD (Oxford Diffraction, 2008 ▶); cell refinement: CrysAlis RED (Oxford Diffraction, 2008 ▶); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810045381/xu5082sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810045381/xu5082Isup2.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 |
|---|---|---|---|---|
| C2—H2⋯N1i | 0.93 | 2.62 | 3.5285 (19) | 167 (1) |
Symmetry code: (i)
.
Acknowledgments
The authors thank the Testing Centre of Sichuan University for the diffraction measurements. We are grateful for financial support from China West Normal University (No. 412374).
supplementary crystallographic information
Comment
The chemistry of ylidene malononitrile have been studied extensively, from the ring closure reactions, the comounds containing newly formed five or six-membered rings, such as indans (Zhang et al.2003), naphthalenes (Liu, et al.2002), benzenes (Sepiol et al.1985) were obtained. Some crystal structures involving ylidene malononitrile groups have been published, including a recent report from our labratory (Kang et al., 2009). As a part of our interest in the synthsis of some complex ring systems, we investigated the title compound (I), which is a diene reagent in Diels-Alder reaction. We report herein the crystal structure of the title compound.
The molecular structure of (I) is shown in Fig. 1. Bond lengths and angles in (I) are normal. The phenyl ring with two double bond and triple bond is co-planar. The crystal packing is stabilized by C—H···N hydrogen bonding (Table 1).
Experimental
2-(Butan-2-ylidene)malononitrile (0.24 g 2 mmol) and 4-methoxy -benzaldehyde (0.272 g 2 mmol) were dissolved in 2-propanol (2 ml). To the solution was added piperidine (0.017 g, 0.2 mmol), the solution was stirred for 24 h at 343 K. Then the solution was cooled to room temperature, and was filtered to obtain a yellow solid. Recrystallization from hot ethanol afforded the pure compound. Single crystals of (I) suitable for X-ray analysis were obtained by slow evaporation ethanol solvent.
Refinement
The carbon-bound hydrogen atoms were placed in calculated positions, with C—H = 0.93–0.97 Å, and refined using a riding model, with Uiso(H) =1.5Ueq(C) for methyl H atoms and Uiso(H) =1.2Ueq(C) for the others.
Figures
Fig. 1.
The molecular structure of (I) with 30% probability displacement ellipsoids (arbitrary spheres for H atoms).
Crystal data
| C15H14N2O | F(000) = 504 |
| Mr = 238.28 | Dx = 1.182 Mg m−3 |
| Monoclinic, P21/n | Cu Kα radiation, λ = 1.54184 Å |
| Hall symbol: -P 2yn | Cell parameters from 6882 reflections |
| a = 12.3371 (3) Å | θ = 3.6–69.4° |
| b = 8.8832 (2) Å | µ = 0.60 mm−1 |
| c = 12.8554 (3) Å | T = 291 K |
| β = 108.050 (2)° | Block, yellow |
| V = 1339.53 (5) Å3 | 0.42 × 0.40 × 0.36 mm |
| Z = 4 |
Data collection
| Oxford Diffraction Gemini S Ultra diffractometer | 2456 independent reflections |
| Radiation source: Enhance Ultra (Cu) X-ray Source | 2266 reflections with I > 2σ(I) |
| mirror | Rint = 0.014 |
| Detector resolution: 15.9149 pixels mm-1 | θmax = 69.6°, θmin = 4.3° |
| ω scans | h = −14→14 |
| Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009) | k = −10→10 |
| Tmin = 0.787, Tmax = 0.813 | l = −15→8 |
| 9020 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)] = 0.039 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.112 | H-atom parameters constrained |
| S = 1.05 | w = 1/[σ2(Fo2) + (0.0607P)2 + 0.1456P] where P = (Fo2 + 2Fc2)/3 |
| 2456 reflections | (Δ/σ)max < 0.001 |
| 165 parameters | Δρmax = 0.11 e Å−3 |
| 3 restraints | Δρmin = −0.14 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 | ||
| O1 | 0.09486 (7) | −0.22305 (10) | 0.03379 (7) | 0.0668 (3) | |
| C14 | −0.13644 (11) | 0.27243 (16) | 0.51588 (10) | 0.0646 (3) | |
| C7 | 0.13090 (9) | 0.13033 (12) | 0.40443 (8) | 0.0486 (3) | |
| H7 | 0.2053 | 0.1581 | 0.4428 | 0.058* | |
| C2 | −0.00061 (9) | −0.10045 (13) | 0.15020 (9) | 0.0534 (3) | |
| H2 | −0.0720 | −0.1348 | 0.1083 | 0.064* | |
| C8 | 0.04916 (9) | 0.17842 (13) | 0.44506 (8) | 0.0505 (3) | |
| H8 | −0.0254 | 0.1492 | 0.4090 | 0.061* | |
| C4 | 0.11576 (9) | 0.03969 (11) | 0.30705 (8) | 0.0464 (3) | |
| C5 | 0.21124 (9) | 0.00232 (14) | 0.27569 (10) | 0.0559 (3) | |
| H5 | 0.2828 | 0.0364 | 0.3174 | 0.067* | |
| C1 | 0.09578 (9) | −0.13673 (12) | 0.12143 (9) | 0.0512 (3) | |
| C3 | 0.01045 (9) | −0.01297 (13) | 0.24151 (9) | 0.0525 (3) | |
| H3 | −0.0546 | 0.0117 | 0.2599 | 0.063* | |
| C6 | 0.20146 (9) | −0.08369 (14) | 0.18453 (10) | 0.0611 (3) | |
| H6 | 0.2661 | −0.1066 | 0.1649 | 0.073* | |
| C9 | 0.06860 (9) | 0.27216 (12) | 0.54059 (9) | 0.0507 (3) | |
| N1 | −0.22774 (11) | 0.23824 (19) | 0.46897 (11) | 0.0962 (5) | |
| C12 | −0.02183 (10) | 0.31596 (13) | 0.57378 (9) | 0.0552 (3) | |
| N2 | −0.00312 (13) | 0.48196 (17) | 0.74197 (12) | 0.0955 (4) | |
| C10 | 0.18745 (10) | 0.31909 (15) | 0.60535 (10) | 0.0640 (3) | |
| H10A | 0.1837 | 0.4087 | 0.6472 | 0.077* | |
| H10B | 0.2297 | 0.3441 | 0.5554 | 0.077* | |
| C15 | −0.01196 (12) | −0.28321 (15) | −0.03201 (11) | 0.0687 (4) | |
| H15A | −0.0445 | −0.3435 | 0.0128 | 0.103* | |
| H15B | −0.0002 | −0.3444 | −0.0891 | 0.103* | |
| H15C | −0.0629 | −0.2022 | −0.0638 | 0.103* | |
| C13 | −0.00959 (11) | 0.40823 (15) | 0.66777 (11) | 0.0670 (3) | |
| C11 | 0.25010 (13) | 0.1964 (2) | 0.68261 (12) | 0.0890 (5) | |
| H11A | 0.2143 | 0.1807 | 0.7382 | 0.133* | |
| H11B | 0.3280 | 0.2260 | 0.7161 | 0.133* | |
| H11C | 0.2477 | 0.1047 | 0.6424 | 0.133* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1 | 0.0564 (5) | 0.0802 (6) | 0.0658 (5) | 0.0005 (4) | 0.0219 (4) | −0.0264 (4) |
| C14 | 0.0545 (6) | 0.0853 (9) | 0.0560 (7) | 0.0201 (5) | 0.0199 (5) | 0.0060 (5) |
| C7 | 0.0477 (5) | 0.0515 (6) | 0.0483 (5) | −0.0039 (4) | 0.0173 (4) | −0.0007 (4) |
| C2 | 0.0417 (5) | 0.0614 (6) | 0.0569 (6) | −0.0034 (5) | 0.0150 (4) | −0.0094 (5) |
| C8 | 0.0483 (6) | 0.0564 (6) | 0.0481 (6) | 0.0002 (4) | 0.0167 (4) | −0.0022 (5) |
| C4 | 0.0451 (5) | 0.0490 (5) | 0.0476 (5) | −0.0006 (4) | 0.0179 (4) | 0.0000 (4) |
| C5 | 0.0405 (5) | 0.0666 (7) | 0.0609 (6) | −0.0030 (5) | 0.0163 (5) | −0.0113 (5) |
| C1 | 0.0505 (6) | 0.0527 (6) | 0.0526 (6) | 0.0020 (5) | 0.0194 (5) | −0.0070 (5) |
| C3 | 0.0426 (5) | 0.0620 (6) | 0.0576 (6) | −0.0014 (5) | 0.0225 (5) | −0.0076 (5) |
| C6 | 0.0444 (6) | 0.0742 (8) | 0.0697 (7) | 0.0008 (5) | 0.0250 (5) | −0.0176 (6) |
| C9 | 0.0556 (6) | 0.0511 (6) | 0.0487 (6) | 0.0024 (4) | 0.0209 (5) | 0.0016 (4) |
| N1 | 0.0536 (7) | 0.1471 (13) | 0.0840 (8) | 0.0179 (7) | 0.0154 (6) | 0.0044 (8) |
| C12 | 0.0588 (6) | 0.0598 (6) | 0.0503 (6) | 0.0116 (5) | 0.0215 (5) | 0.0034 (4) |
| N2 | 0.1005 (10) | 0.1055 (10) | 0.0906 (9) | 0.0068 (8) | 0.0443 (8) | −0.0336 (8) |
| C10 | 0.0619 (7) | 0.0708 (7) | 0.0652 (7) | −0.0132 (6) | 0.0284 (6) | −0.0197 (6) |
| C15 | 0.0699 (8) | 0.0710 (8) | 0.0633 (7) | −0.0060 (6) | 0.0179 (6) | −0.0210 (6) |
| C13 | 0.0705 (8) | 0.0706 (8) | 0.0664 (7) | 0.0122 (6) | 0.0308 (6) | −0.0064 (6) |
| C11 | 0.0617 (8) | 0.1201 (13) | 0.0720 (9) | −0.0096 (8) | 0.0015 (7) | −0.0004 (9) |
Geometric parameters (Å, °)
| O1—C1 | 1.3600 (13) | C1—C6 | 1.3873 (15) |
| O1—C15 | 1.4308 (15) | C3—H3 | 0.9300 |
| C14—N1 | 1.1417 (18) | C6—H6 | 0.9300 |
| C14—C12 | 1.4321 (18) | C9—C12 | 1.3686 (15) |
| C7—C8 | 1.3412 (15) | C9—C10 | 1.5035 (16) |
| C7—C4 | 1.4510 (14) | C12—C13 | 1.4289 (16) |
| C7—H7 | 0.9300 | N2—C13 | 1.1393 (17) |
| C2—C3 | 1.3788 (15) | C10—C11 | 1.516 (2) |
| C2—C1 | 1.3883 (14) | C10—H10A | 0.9700 |
| C2—H2 | 0.9300 | C10—H10B | 0.9700 |
| C8—C9 | 1.4410 (15) | C15—H15A | 0.9600 |
| C8—H8 | 0.9300 | C15—H15B | 0.9600 |
| C4—C3 | 1.3923 (15) | C15—H15C | 0.9600 |
| C4—C5 | 1.3980 (15) | C11—H11A | 0.9600 |
| C5—C6 | 1.3727 (16) | C11—H11B | 0.9600 |
| C5—H5 | 0.9300 | C11—H11C | 0.9600 |
| C1—O1—C15 | 118.04 (9) | C12—C9—C8 | 119.57 (10) |
| N1—C14—C12 | 179.45 (15) | C12—C9—C10 | 119.86 (10) |
| C8—C7—C4 | 126.97 (10) | C8—C9—C10 | 120.56 (9) |
| C8—C7—H7 | 116.5 | C9—C12—C13 | 122.96 (11) |
| C4—C7—H7 | 116.5 | C9—C12—C14 | 122.01 (11) |
| C3—C2—C1 | 119.38 (10) | C13—C12—C14 | 115.03 (10) |
| C3—C2—H2 | 120.3 | C9—C10—C11 | 112.04 (11) |
| C1—C2—H2 | 120.3 | C9—C10—H10A | 109.2 |
| C7—C8—C9 | 124.70 (10) | C11—C10—H10A | 109.2 |
| C7—C8—H8 | 117.7 | C9—C10—H10B | 109.2 |
| C9—C8—H8 | 117.7 | C11—C10—H10B | 109.2 |
| C3—C4—C5 | 117.22 (10) | H10A—C10—H10B | 107.9 |
| C3—C4—C7 | 123.72 (9) | O1—C15—H15A | 109.5 |
| C5—C4—C7 | 119.06 (10) | O1—C15—H15B | 109.5 |
| C6—C5—C4 | 121.29 (10) | H15A—C15—H15B | 109.5 |
| C6—C5—H5 | 119.4 | O1—C15—H15C | 109.5 |
| C4—C5—H5 | 119.4 | H15A—C15—H15C | 109.5 |
| O1—C1—C6 | 116.17 (9) | H15B—C15—H15C | 109.5 |
| O1—C1—C2 | 124.31 (10) | N2—C13—C12 | 178.06 (14) |
| C6—C1—C2 | 119.53 (10) | C10—C11—H11A | 109.5 |
| C2—C3—C4 | 122.15 (9) | C10—C11—H11B | 109.5 |
| C2—C3—H3 | 118.9 | H11A—C11—H11B | 109.5 |
| C4—C3—H3 | 118.9 | C10—C11—H11C | 109.5 |
| C5—C6—C1 | 120.42 (10) | H11A—C11—H11C | 109.5 |
| C5—C6—H6 | 119.8 | H11B—C11—H11C | 109.5 |
| C1—C6—H6 | 119.8 | ||
| C4—C7—C8—C9 | −178.09 (10) | C4—C5—C6—C1 | −0.5 (2) |
| C8—C7—C4—C3 | −1.00 (18) | O1—C1—C6—C5 | −178.94 (11) |
| C8—C7—C4—C5 | 178.78 (11) | C2—C1—C6—C5 | 0.91 (19) |
| C3—C4—C5—C6 | −0.49 (18) | C7—C8—C9—C12 | 179.18 (11) |
| C7—C4—C5—C6 | 179.72 (10) | C7—C8—C9—C10 | −2.24 (17) |
| C15—O1—C1—C6 | 178.49 (11) | C8—C9—C12—C13 | 179.74 (10) |
| C15—O1—C1—C2 | −1.35 (17) | C10—C9—C12—C13 | 1.14 (18) |
| C3—C2—C1—O1 | 179.44 (10) | C8—C9—C12—C14 | −0.48 (18) |
| C3—C2—C1—C6 | −0.40 (18) | C10—C9—C12—C14 | −179.08 (11) |
| C1—C2—C3—C4 | −0.58 (18) | C12—C9—C10—C11 | 98.07 (14) |
| C5—C4—C3—C2 | 1.01 (17) | C8—C9—C10—C11 | −80.51 (14) |
| C7—C4—C3—C2 | −179.20 (10) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C2—H2···N1i | 0.93 | 2.62 | 3.5285 (19) | 167 (1) |
Symmetry codes: (i) −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: XU5082).
References
- Farrugia, L. J. (1997). J. Appl. Cryst.30, 565.
- Kang, T.-R. & Chen, L.-M. (2009). Acta Cryst. E65, o3164. [DOI] [PMC free article] [PubMed]
- Liu, Y., Shen, B., Kotora, M., Nakajima, K. & Takahashi, T. (2002). J. Org. Chem.67, 7019–7028. [DOI] [PubMed]
- Oxford Diffraction (2008). CrysAlis CCD and CrysAlis RED Oxford Diffraction Ltd, Yarnton, England.
- Oxford Diffraction (2009). CrysAlis PRO Oxford Diffraction Ltd, Yarnton, England.
- Sepiol, J. & Milart, P. (1985). Tetrahedron, 41, 5261–5265.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Zhang, B., Zhu, X.-Q., Lu, J.-Y., He, J., Wang, P.-G. & Cheng, J.-P. (2003). J. Org. Chem.68, 3295–3298. [DOI] [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 global, I. DOI: 10.1107/S1600536810045381/xu5082sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810045381/xu5082Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

