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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Jun 13;68(Pt 7):o2065. doi: 10.1107/S1600536812025913

1-Methyl-4-[(1E)-2-nitro­prop-1-en-1-yl]benzene

Zhao-Bo Li a,b,*, Li-Li Shen b, Jian-An Zheng c
PMCID: PMC3393329  PMID: 22807886

Abstract

The title compound, C10H11NO2, adopts an E conformation about the C=C bond. The C=C—C=C torsion angle is 32.5 (3)°. The crystal structure features weak inter­molecular C—H⋯O inter­actions.

Related literature  

For background to the chemistry of nitro­alkenes, see: Ballini & Petrini (2004); Berner et al. (2002); Ono (2001). For a related structure, see: Yang et al. (2010).graphic file with name e-68-o2065-scheme1.jpg

Experimental  

Crystal data  

  • C10H11NO2

  • M r = 177.20

  • Orthorhombic, Inline graphic

  • a = 11.0610 (5) Å

  • b = 7.5840 (4) Å

  • c = 22.6420 (11) Å

  • V = 1899.36 (16) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.09 mm−1

  • T = 296 K

  • 0.58 × 0.43 × 0.36 mm

Data collection  

  • Rigaku R-AXIS-RAPID/ZJUG diffractometer

  • Absorption correction: multi-scan (ABSCOR; Higashi, 1995) T min = 0.941, T max = 0.969

  • 16972 measured reflections

  • 2162 independent reflections

  • 1325 reflections with I > 2σ(I)

  • R int = 0.033

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.045

  • wR(F 2) = 0.134

  • S = 1.00

  • 2162 reflections

  • 121 parameters

  • H-atom parameters constrained

  • Δρmax = 0.15 e Å−3

  • Δρmin = −0.17 e Å−3

Data collection: PROCESS-AUTO (Rigaku, 2006); cell refinement: PROCESS-AUTO; data reduction: CrystalClear (Rigaku, 2007); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

Supplementary Material

Crystal structure: contains datablock(s) I. DOI: 10.1107/S1600536812025913/zq2167sup1.cif

e-68-o2065-sup1.cif (18.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812025913/zq2167Isup2.hkl

e-68-o2065-Isup2.hkl (104.2KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812025913/zq2167Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
C8—H8⋯O1i 0.93 2.55 3.369 (2) 147
C2—H2⋯O2ii 0.93 2.66 3.551 (3) 162

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Acknowledgments

The authors thank Mr Jianming Gu for the single-crystal X-ray analysis. They are also grateful for financial support from the State Key Laboratory Breeding Base of Green Chemistry–Synthesis Technology of Zhejiang University of Technology (GCTKF2012010).

supplementary crystallographic information

Comment

Nitroalkenes are important organic intermediates, since they can be converted to synthetically useful N- and O-containing organic molecules, such as amines, aldehydes, carboxylic acids, or denitrated compounds (Ono, 2001; Berner et al., 2002; Ballini & Petrini, 2004). As a contribution in this field, we have synthesized a series of nitroalkenes by employing benzaldehydes and nitroethane (Yang et al., 2010). We report here the crystal structure of the title compound (Fig. 1).

The molecule adopts an E configuration with respect to the C8=C9 double bond. The torsion angle C9—C8—C1—C6 is 32.5 (3)°. In the crystal structure, the molecules interact through weak intermolecular C8—H8···O1i and C2—H2···O2ii hydrogen bonds (symmetry codes: i = -x+1, -y, -z+1; ii = x+1/2, -y+1/2, -z+1; Fig. 2 and Table 1).

Experimental

To a solution of p-tolualdehyde (50 mmol) in AcOH (25 mL), nitroethane (75 mmol) was added, followed by butylamine (100 mmol, 7.4 mL). The mixture was sonicated at 60 °C, until GC showed full conversion of the aldehyde. The mixture was poured into ice water, the precipitate was filtered off, washed with water and recrystallized from EtOH/EtOAc to give the final product. Single crystals were obtained by slow evaporation of a n-hexane/EtOAc (10:1, v/v) solution.

Refinement

All H atoms were placed in calculated positions and refined using a riding model, with C—H = 0.93 Å and Uiso(H) = 1.2Ueq(C) for aromatic H atoms, and with C—H = 0.96 Å and Uiso(H) = 1.5Ueq(C) for methyl H atoms.

Figures

Fig. 1.

Fig. 1.

The asymmetric unit of the title compound with the atomic labeling scheme; displacement ellipsoids are drawn at the 50% probability level.

Fig. 2.

Fig. 2.

View of the intermolecular interactions illustrated as dashed lines.

Crystal data

C10H11NO2 F(000) = 752
Mr = 177.20 Dx = 1.239 Mg m3
Orthorhombic, Pbca Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2ab Cell parameters from 9467 reflections
a = 11.0610 (5) Å θ = 3.2–27.4°
b = 7.5840 (4) Å µ = 0.09 mm1
c = 22.6420 (11) Å T = 296 K
V = 1899.36 (16) Å3 Chunk, yellow
Z = 8 0.58 × 0.43 × 0.36 mm

Data collection

Rigaku R-AXIS-RAPID/ZJUG diffractometer 2162 independent reflections
Radiation source: rotating anode 1325 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.033
Detector resolution: 10.00 pixels mm-1 θmax = 27.4°, θmin = 3.4°
ω scans h = −14→14
Absorption correction: multi-scan (ABSCOR; Higashi, 1995) k = −9→9
Tmin = 0.941, Tmax = 0.969 l = −29→29
16972 measured reflections

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.045 H-atom parameters constrained
wR(F2) = 0.134 w = 1/[σ2(Fo2) + (0.0552P)2 + 0.4885P] where P = (Fo2 + 2Fc2)/3
S = 1.00 (Δ/σ)max = 0.001
2162 reflections Δρmax = 0.15 e Å3
121 parameters Δρmin = −0.17 e Å3
0 restraints Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.0051 (12)

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 0.35993 (13) 0.1487 (2) 0.63005 (7) 0.0487 (4)
C2 0.46387 (14) 0.2326 (2) 0.65095 (8) 0.0577 (4)
H2 0.5248 0.2634 0.6246 0.069*
C3 0.47750 (16) 0.2703 (2) 0.71015 (8) 0.0643 (5)
H3 0.5464 0.3300 0.7227 0.077*
C4 0.39139 (17) 0.2218 (2) 0.75151 (8) 0.0614 (5)
C5 0.29031 (16) 0.1324 (2) 0.73072 (8) 0.0615 (5)
H5 0.2318 0.0957 0.7575 0.074*
C6 0.27416 (14) 0.0963 (2) 0.67157 (7) 0.0547 (4)
H6 0.2053 0.0363 0.6592 0.066*
C7 0.4073 (2) 0.2610 (3) 0.81617 (9) 0.0938 (7)
H7A 0.4047 0.1529 0.8382 0.141*
H7B 0.3435 0.3374 0.8292 0.141*
H7C 0.4839 0.3177 0.8223 0.141*
C8 0.34896 (14) 0.1144 (2) 0.56645 (7) 0.0531 (4)
H8 0.4211 0.0963 0.5462 0.064*
C9 0.24878 (15) 0.1058 (2) 0.53415 (7) 0.0524 (4)
C10 0.12094 (14) 0.1404 (3) 0.55103 (8) 0.0676 (5)
H10A 0.0791 0.0304 0.5557 0.101*
H10B 0.0824 0.2087 0.5207 0.101*
H10C 0.1189 0.2043 0.5876 0.101*
N1 0.26510 (15) 0.0587 (2) 0.47133 (7) 0.0689 (4)
O1 0.36592 (15) 0.0320 (3) 0.45180 (6) 0.1156 (7)
O2 0.17592 (15) 0.0466 (3) 0.44070 (7) 0.1107 (6)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0436 (8) 0.0448 (8) 0.0577 (9) 0.0026 (6) −0.0012 (7) 0.0014 (7)
C2 0.0443 (8) 0.0582 (10) 0.0705 (11) −0.0013 (7) −0.0040 (8) 0.0051 (8)
C3 0.0588 (10) 0.0554 (10) 0.0788 (12) −0.0025 (8) −0.0221 (9) −0.0002 (8)
C4 0.0758 (11) 0.0482 (9) 0.0602 (10) 0.0081 (8) −0.0150 (9) −0.0001 (8)
C5 0.0675 (11) 0.0592 (10) 0.0576 (10) −0.0005 (8) 0.0030 (8) 0.0056 (8)
C6 0.0527 (9) 0.0527 (9) 0.0587 (9) −0.0081 (7) −0.0020 (7) 0.0009 (7)
C7 0.134 (2) 0.0821 (14) 0.0653 (12) 0.0051 (14) −0.0291 (13) −0.0057 (10)
C8 0.0474 (8) 0.0563 (9) 0.0555 (9) 0.0029 (7) 0.0031 (7) 0.0019 (7)
C9 0.0535 (8) 0.0525 (9) 0.0512 (8) 0.0023 (7) −0.0009 (7) 0.0009 (7)
C10 0.0500 (9) 0.0809 (12) 0.0718 (11) 0.0055 (9) −0.0033 (8) 0.0057 (9)
N1 0.0687 (10) 0.0811 (11) 0.0570 (9) 0.0123 (8) −0.0067 (8) −0.0012 (8)
O1 0.0869 (11) 0.197 (2) 0.0625 (9) 0.0435 (12) 0.0054 (8) −0.0159 (10)
O2 0.0889 (11) 0.1695 (18) 0.0737 (10) 0.0049 (11) −0.0255 (8) −0.0238 (10)

Geometric parameters (Å, º)

C1—C2 1.396 (2) C7—H7A 0.9600
C1—C6 1.394 (2) C7—H7B 0.9600
C1—C8 1.468 (2) C7—H7C 0.9600
C2—C3 1.379 (2) C8—C9 1.329 (2)
C2—H2 0.9300 C8—H8 0.9300
C3—C4 1.386 (3) C9—N1 1.478 (2)
C3—H3 0.9300 C9—C10 1.488 (2)
C4—C5 1.390 (2) C10—H10A 0.9600
C4—C7 1.504 (3) C10—H10B 0.9600
C5—C6 1.378 (2) C10—H10C 0.9600
C5—H5 0.9300 N1—O2 1.2094 (19)
C6—H6 0.9300 N1—O1 1.217 (2)
C2—C1—C6 117.50 (15) H7A—C7—H7B 109.5
C2—C1—C8 118.77 (14) C4—C7—H7C 109.5
C6—C1—C8 123.69 (14) H7A—C7—H7C 109.5
C3—C2—C1 120.94 (16) H7B—C7—H7C 109.5
C3—C2—H2 119.5 C9—C8—C1 128.09 (14)
C1—C2—H2 119.5 C9—C8—H8 116.0
C2—C3—C4 121.78 (16) C1—C8—H8 116.0
C2—C3—H3 119.1 C8—C9—N1 116.07 (14)
C4—C3—H3 119.1 C8—C9—C10 129.97 (15)
C3—C4—C5 116.99 (16) N1—C9—C10 113.95 (14)
C3—C4—C7 121.66 (18) C9—C10—H10A 109.5
C5—C4—C7 121.35 (19) C9—C10—H10B 109.5
C6—C5—C4 122.02 (16) H10A—C10—H10B 109.5
C6—C5—H5 119.0 C9—C10—H10C 109.5
C4—C5—H5 119.0 H10A—C10—H10C 109.5
C5—C6—C1 120.70 (15) H10B—C10—H10C 109.5
C5—C6—H6 119.7 O2—N1—O1 121.78 (17)
C1—C6—H6 119.7 O2—N1—C9 118.09 (16)
C4—C7—H7A 109.5 O1—N1—C9 120.13 (15)
C4—C7—H7B 109.5
C6—C1—C2—C3 −3.5 (2) C8—C1—C6—C5 179.77 (15)
C8—C1—C2—C3 178.93 (15) C2—C1—C8—C9 −150.12 (16)
C1—C2—C3—C4 2.3 (3) C6—C1—C8—C9 32.5 (3)
C2—C3—C4—C5 0.2 (2) C1—C8—C9—N1 −176.58 (15)
C2—C3—C4—C7 179.15 (17) C1—C8—C9—C10 4.9 (3)
C3—C4—C5—C6 −1.4 (2) C8—C9—N1—O2 178.77 (17)
C7—C4—C5—C6 179.65 (17) C10—C9—N1—O2 −2.5 (2)
C4—C5—C6—C1 0.1 (3) C8—C9—N1—O1 −0.8 (3)
C2—C1—C6—C5 2.3 (2) C10—C9—N1—O1 177.99 (18)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
C8—H8···O1 0.93 2.28 2.677 (2) 105
C8—H8···O1i 0.93 2.55 3.369 (2) 147
C2—H2···O2ii 0.93 2.66 3.551 (3) 162

Symmetry codes: (i) −x+1, −y, −z+1; (ii) x+1/2, −y+1/2, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: ZQ2167).

References

  1. Ballini, R. & Petrini, M. (2004). Tetrahedron, 60, 1017–1047.
  2. Berner, O. M., Tedeschi, L. & Enders, D. (2002). Eur. J. Org. Chem. 12, 1877–1894.
  3. Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
  4. Farrugia, L. J. (1999). J. Appl. Cryst. 32, 837–838.
  5. Higashi, T. (1995). ABSCOR Rigaku Corporation, Tokyo, Japan.
  6. Ono, N. (2001). The Nitro Group in Organic Synthesis New York: Wiley-VCH.
  7. Rigaku (2006). PROCESS-AUTO Rigaku Corporation, Tokyo, Japan.
  8. Rigaku (2007). CrystalClear. Rigaku Americas Corporation, Texas, USA.
  9. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  10. Yang, J.-K., Zheng, M., Luo, S.-P. & Li, Z.-B. (2010). Acta Cryst. E66, o1781. [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 datablock(s) I. DOI: 10.1107/S1600536812025913/zq2167sup1.cif

e-68-o2065-sup1.cif (18.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812025913/zq2167Isup2.hkl

e-68-o2065-Isup2.hkl (104.2KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812025913/zq2167Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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