Literature DB >> 21581353

N-(3-Nitro-benzyl-idene)aniline.

Muhammad Zaheer, Zareen Akhter, Michael Bolte, Humaira M Siddiqi.   

Abstract

In the title compound, C(13)H(10)N(2)O(2), a Schiff base derivative, the dihedral angle between the two aromatic rings is 31.58 (3)°. The C=N double bond is essentially coplanar with the nitro-phenyl ring. The torsion angle of the imine double bond is 175.97 (13)°, indicating that the C=N double bond is in a trans configuration. The crystal structure is stabilized by C-H⋯O contacts and π-π inter-actions (centroid-centroid distances of 3.807 and 3.808Å).

Entities:  

Year:  2008        PMID: 21581353      PMCID: PMC2960009          DOI: 10.1107/S1600536808036970

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

Choi et al. (2000 ▶) and Nakamura et al. (1999 ▶) discuss the use of Schiff bases in the reduction of thionyl chloride, while Maruyama et al. (1995 ▶) and Burrows et al. (1996 ▶) describe their use in degradation processes. Hodnett & Mooney (1970 ▶), Rajavel et al. (2008 ▶) and Yu et al. (2007 ▶) discuss anti­neoplastic, anti­bacterial and anti­fungal activities, respectively. Hartley et al. (2002 ▶), Torregrosa et al. (2005 ▶) and Naeimi et al. (2008 ▶) describe different synthetic routes towards Schiff bases. Landy (1989 ▶) describes their role in biological redox systems. Yoon et al. (1990 ▶) and Park et al. (1998 ▶) discuss properties of Schiff base complexes such as alkene epoxidation and oxygen absorption by cobalt(II) complexes. Flack (1983 ▶) discusses the Rogers’s parameter for the characterization of enanti­o­morphic-polar compounds.

Experimental

Crystal data

C13H10N2O2 M = 226.23 Orthorhombic, a = 7.3177 (6) Å b = 12.1022 (11) Å c = 12.4672 (12) Å V = 1104.10 (17) Å3 Z = 4 Mo Kα radiation μ = 0.09 mm−1 T = 173 (2) K 0.48 × 0.48 × 0.46 mm

Data collection

Stoe IPDSII two-circle diffractometer Absorption correction: none 9868 measured reflections 1585 independent reflections 1421 reflections with I > 2σ(I) R int = 0.053

Refinement

R[F 2 > 2σ(F 2)] = 0.034 wR(F 2) = 0.093 S = 1.04 1585 reflections 154 parameters H-atom parameters constrained Δρmax = 0.26 e Å−3 Δρmin = −0.14 e Å−3 Data collection: X-AREA (Stoe & Cie, 2001 ▶); cell refinement: X-AREA; data reduction: X-AREA; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: XP in SHELXTL-Plus (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXL97. Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808036970/zl2143sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536808036970/zl2143Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C13H10N2O2F000 = 472
Mr = 226.23Dx = 1.361 Mg m3
Orthorhombic, P212121Mo Kα radiation λ = 0.71073 Å
Hall symbol: P 2ac 2abCell parameters from 7899 reflections
a = 7.3177 (6) Åθ = 3.7–25.8º
b = 12.1022 (11) ŵ = 0.09 mm1
c = 12.4672 (12) ÅT = 173 (2) K
V = 1104.10 (17) Å3Block, colourless
Z = 40.48 × 0.48 × 0.46 mm
Stoe IPDSII two-circle diffractometer1421 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.054
Monochromator: graphiteθmax = 29.5º
T = 173(2) Kθmin = 3.6º
ω scansh = −9→8
Absorption correction: nonek = −16→14
9868 measured reflectionsl = −15→17
1585 independent reflections
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.034H-atom parameters constrained
wR(F2) = 0.093  w = 1/[σ2(Fo2) + (0.0638P)2 + 0.081P] where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max < 0.001
1585 reflectionsΔρmax = 0.26 e Å3
154 parametersΔρmin = −0.14 e Å3
Primary atom site location: structure-invariant direct methodsExtinction correction: none
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.
xyzUiso*/Ueq
N10.85150 (17)0.74236 (10)0.59232 (10)0.0265 (3)
N20.9518 (2)0.83182 (11)0.11436 (10)0.0339 (3)
O10.9459 (2)0.90457 (11)0.04548 (10)0.0507 (4)
O20.9936 (2)0.73588 (10)0.09536 (9)0.0525 (4)
C10.9027 (2)0.72475 (11)0.49536 (12)0.0255 (3)
H10.95300.65490.47710.031*
C20.8855 (2)0.81012 (11)0.41137 (12)0.0239 (3)
C30.9276 (2)0.78262 (11)0.30530 (11)0.0243 (3)
H30.96850.71040.28760.029*
C40.9088 (2)0.86252 (12)0.22632 (11)0.0262 (3)
C50.8499 (2)0.96943 (12)0.24807 (12)0.0296 (3)
H50.83831.02250.19240.036*
C60.8086 (2)0.99625 (12)0.35358 (13)0.0314 (4)
H60.76781.06870.37050.038*
C70.8262 (2)0.91791 (12)0.43499 (12)0.0277 (3)
H70.79790.93750.50690.033*
C110.86161 (19)0.65339 (11)0.66706 (11)0.0239 (3)
C120.9017 (2)0.67860 (12)0.77429 (12)0.0291 (3)
H120.92290.75310.79470.035*
C130.9105 (2)0.59535 (14)0.85102 (12)0.0337 (4)
H130.93990.61300.92320.040*
C140.8763 (2)0.48619 (13)0.82226 (13)0.0332 (4)
H140.88320.42920.87450.040*
C150.8317 (2)0.46086 (12)0.71627 (13)0.0308 (3)
H150.80620.38660.69680.037*
C160.8244 (2)0.54339 (12)0.63890 (12)0.0261 (3)
H160.79420.52530.56690.031*
U11U22U33U12U13U23
N10.0264 (6)0.0264 (6)0.0267 (6)−0.0005 (5)0.0001 (5)0.0030 (5)
N20.0391 (8)0.0365 (7)0.0262 (6)−0.0015 (6)−0.0042 (6)0.0052 (5)
O10.0677 (9)0.0548 (7)0.0297 (6)0.0073 (8)0.0022 (7)0.0184 (5)
O20.0883 (12)0.0392 (7)0.0301 (6)0.0053 (7)0.0001 (7)−0.0027 (5)
C10.0230 (7)0.0265 (7)0.0271 (7)0.0011 (6)−0.0012 (6)0.0032 (6)
C20.0210 (6)0.0249 (6)0.0259 (7)−0.0010 (5)−0.0021 (6)0.0033 (5)
C30.0227 (7)0.0242 (6)0.0261 (6)−0.0004 (5)−0.0030 (6)0.0026 (5)
C40.0255 (7)0.0278 (7)0.0255 (7)−0.0031 (6)−0.0027 (6)0.0043 (6)
C50.0279 (8)0.0267 (7)0.0342 (7)−0.0009 (6)−0.0048 (6)0.0093 (6)
C60.0304 (8)0.0239 (7)0.0399 (8)0.0012 (6)−0.0006 (7)0.0031 (6)
C70.0257 (7)0.0270 (7)0.0305 (7)0.0009 (6)0.0022 (6)0.0023 (6)
C110.0204 (6)0.0264 (6)0.0248 (7)0.0013 (5)0.0026 (6)0.0024 (6)
C120.0297 (8)0.0313 (7)0.0264 (7)0.0001 (6)0.0013 (6)−0.0029 (6)
C130.0351 (8)0.0439 (8)0.0222 (6)0.0014 (7)−0.0008 (7)0.0021 (6)
C140.0306 (8)0.0376 (8)0.0314 (7)0.0023 (6)0.0023 (6)0.0127 (7)
C150.0297 (8)0.0269 (7)0.0359 (8)−0.0003 (6)0.0037 (7)0.0032 (6)
C160.0252 (7)0.0283 (7)0.0247 (6)−0.0001 (6)0.0015 (6)−0.0001 (6)
N1—C11.283 (2)C6—C71.395 (2)
N1—C111.4258 (18)C6—H60.9500
N2—O21.2237 (18)C7—H70.9500
N2—O11.2306 (17)C11—C121.402 (2)
N2—C41.4783 (19)C11—C161.4034 (19)
C1—C21.476 (2)C12—C131.391 (2)
C1—H10.9500C12—H120.9500
C2—C31.398 (2)C13—C141.391 (2)
C2—C71.4060 (19)C13—H130.9500
C3—C41.3869 (19)C14—C151.395 (2)
C3—H30.9500C14—H140.9500
C4—C51.390 (2)C15—C161.390 (2)
C5—C61.388 (2)C15—H150.9500
C5—H50.9500C16—H160.9500
C1—N1—C11118.36 (12)C6—C7—C2120.45 (14)
O2—N2—O1123.54 (14)C6—C7—H7119.8
O2—N2—C4118.32 (12)C2—C7—H7119.8
O1—N2—C4118.14 (13)C12—C11—C16119.04 (13)
N1—C1—C2121.80 (13)C12—C11—N1118.00 (12)
N1—C1—H1119.1C16—C11—N1122.88 (13)
C2—C1—H1119.1C13—C12—C11120.52 (14)
C3—C2—C7119.15 (12)C13—C12—H12119.7
C3—C2—C1119.04 (12)C11—C12—H12119.7
C7—C2—C1121.81 (13)C12—C13—C14120.15 (14)
C4—C3—C2118.92 (13)C12—C13—H13119.9
C4—C3—H3120.5C14—C13—H13119.9
C2—C3—H3120.5C13—C14—C15119.65 (14)
C3—C4—C5122.76 (14)C13—C14—H14120.2
C3—C4—N2118.30 (13)C15—C14—H14120.2
C5—C4—N2118.94 (12)C16—C15—C14120.57 (14)
C6—C5—C4118.03 (13)C16—C15—H15119.7
C6—C5—H5121.0C14—C15—H15119.7
C4—C5—H5121.0C15—C16—C11120.04 (13)
C5—C6—C7120.69 (14)C15—C16—H16120.0
C5—C6—H6119.7C11—C16—H16120.0
C7—C6—H6119.7
C11—N1—C1—C2175.97 (13)C5—C6—C7—C2−0.3 (2)
N1—C1—C2—C3−174.08 (15)C3—C2—C7—C60.4 (2)
N1—C1—C2—C75.3 (2)C1—C2—C7—C6−179.00 (14)
C7—C2—C3—C4−0.3 (2)C1—N1—C11—C12146.81 (14)
C1—C2—C3—C4179.08 (12)C1—N1—C11—C16−36.5 (2)
C2—C3—C4—C50.1 (2)C16—C11—C12—C132.1 (2)
C2—C3—C4—N2−179.28 (15)N1—C11—C12—C13179.00 (13)
O2—N2—C4—C33.5 (2)C11—C12—C13—C14−1.1 (2)
O1—N2—C4—C3−175.59 (15)C12—C13—C14—C15−0.5 (2)
O2—N2—C4—C5−175.94 (16)C13—C14—C15—C161.1 (2)
O1—N2—C4—C55.0 (2)C14—C15—C16—C11−0.1 (2)
C3—C4—C5—C60.0 (2)C12—C11—C16—C15−1.5 (2)
N2—C4—C5—C6179.38 (14)N1—C11—C16—C15−178.20 (13)
C4—C5—C6—C70.1 (2)
D—H···AD—HH···AD···AD—H···A
C6—H6···O1i0.952.703.261 (2)118
C6—H6···O2ii0.952.713.303 (2)122
C7—H7···O1i0.952.663.237 (2)120
C13—H13···O2iii0.952.643.541 (2)159
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
C6—H6⋯O1i0.952.703.261 (2)118
C6—H6⋯O2ii0.952.713.303 (2)122
C7—H7⋯O1i0.952.663.237 (2)120
C13—H13⋯O2iii0.952.643.541 (2)159

Symmetry codes: (i) ; (ii) ; (iii) .

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