Skip to main content
Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 May 31;68(Pt 6):o1967. doi: 10.1107/S1600536812024348

N-(4-Methyl­benz­yl)-3-nitro­aniline

Marijana Đaković a,*, Tomislav Portada b, Tin Klačić c
PMCID: PMC3379515  PMID: 22719713

Abstract

In the title compound, C14H14N2O2, the angle between the mean plane of the N-methyl-3-nitro­aniline system (r.m.s. deviation = 0.0185 Å) and the p-tolyl unit is 89.79 (4)°. In the crystal, hydrogen-bonded chains running along [10-1] are generated by the linking of neighbouring mol­ecules via N—H⋯O and C—H⋯O hydrogen bonds involving the 3-nitro­aniline systems and forming R 2 2(8) motifs.

Related literature  

For related structures, see: Betz et al. (2011); Stilinović & Portada (2011); Xing et al. (2006). For the synthesis, see: Magyarfalvi (2008). For graph-set theory, see: Etter (1990); Bernstein et al. (1995).graphic file with name e-68-o1967-scheme1.jpg

Experimental  

Crystal data  

  • C14H14N2O2

  • M r = 242.27

  • Monoclinic, Inline graphic

  • a = 5.1851 (4) Å

  • b = 21.408 (2) Å

  • c = 5.6833 (4) Å

  • β = 98.010 (7)°

  • V = 624.71 (8) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.09 mm−1

  • T = 296 K

  • 0.57 × 0.50 × 0.19 mm

Data collection  

  • Oxford Diffraction Xcalibur diffractometer with a Sapphire-3 CCD area detector

  • Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009) T min = 0.953, T max = 0.958

  • 11868 measured reflections

  • 1856 independent reflections

  • 1373 reflections with I > 2σ(I)

  • R int = 0.042

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.046

  • wR(F 2) = 0.117

  • S = 1.03

  • 1856 reflections

  • 167 parameters

  • 1 restraint

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.16 e Å−3

  • Δρmin = −0.11 e Å−3

Data collection: CrysAlis PRO (Oxford Diffraction, 2009); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997) and Mercury (Macrae et al., 2006); software used to prepare material for publication: SHELXL97 and PLATON (Spek, 2009).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812024348/fj2555sup1.cif

e-68-o1967-sup1.cif (23.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812024348/fj2555Isup2.hkl

e-68-o1967-Isup2.hkl (89.5KB, hkl)

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
N1—H1N⋯O2i 0.78 (3) 2.52 (3) 3.277 (3) 168 (3)
C6—H6⋯O1i 0.93 2.44 3.364 (3) 171
C7—H7A⋯O2ii 0.97 2.64 3.352 (3) 130
C13—H13⋯O2iii 0.93 2.69 3.282 (4) 122

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

Acknowledgments

This research was supported by the Ministry of Science, Education and Sports of the Republic of Croatia, Zagreb (grant Nos. 119–1193079–1332 and 098–0982904–2912) and the 5th High School, Zagreb, Croatia.

supplementary crystallographic information

Comment

The title compound, N-(4-methylbenzyl)-3-nitroaniline, is prepared as a part of the laboratory work with high school students, and the synthesis followed the Preparatory problems for the 40th International Chemistry Olympiad (Magyarfalvi, 2008) involving slight modifications.

Recently, N-benzyl-3-nitroaniline was reported (Stilinović & Portada, 2011). The difference between the title compound and the previously reported one is only in methyl substituent on the N-benzyl moiety, since it was of interest to study the influence of the benzyl moiety substituents on the molecular conformation, and consequently the hydrogen bonding formation.

The addition of methyl substituent on the benzyl moiety in the title compound did not cause any significant conformational difference. The molecule retained a bent conformation with the torsion angle about the central C—N bond of 73.9 (2)° being very similar to analogous one in the recently reported compound (Stilinović & Portada, 2011). Furthermore, the N-methyl-3-nitroaniline system in the title compound is nearly ideally planar (r.m.s. deviation of the atoms C1–C7/N1/N2/O1/O2 from their mean plane is 0.0185 Å, with oxygen atom O2 being the one that deviates most from that plane, 0.031 (2) Å). The p-tolyl substituent is tilted at an angle of 89.79 (4)° to the rest of the molecule.

Two neighbouring molecules are connected through the set of N—H···O and C—H···O hydrogen bonds in the head to tail manner forming R22(8) motifs (Etter, 1990; Bernstein et al., 1995) that generate one-dimensional chains running in the [101] direction. The same hydrogen bonding pattern is also found in N-benzyl-3-nitroaniline (Stilinović & Portada, 2011) what leads to the conclusion that the methyl substituent in p-position to the central C—N bond do not influence neither hydrogen bonding geometry nor general hydrogen bonding framework formation.

Experimental

The title compound was prepared using a slightly modified procedure (Magyarfalvi, 2008) and isolated in a form of yellow crystalline product. Used: 3-nitroaniline (1.10 g; 7.96 mmol), p-tolualdehyde (1.74 ml; 1.77 g; 14.7 mmol), sodium tetrahydridoborate (0.50 g; 13.2 mmol). Yield: 1.12 g (58%). Upon re-crystallization in ethanol, yellow block-like crystalls suitable for the X-ray experiment were obtained in 3–4 days.

Refinement

In the final cycles of refinement, in the absence of significant anomalous scattering effect, 1856 Friedel pairs were merged and Δf'' set to zero. The amine H atom was located in the difference Fourier map and freely refined, giving N—H distance of 0.78 (3) Å. All other H atoms were placed in geometrically idealized positions and constrained to ride on their parent C atom at distances of 0.93, 0.96 and 0.97 Å for aromatic, methyl and CH2 H atoms, respectively, and with Uiso(H) = 1.2Ueq(C) (for aromatic and CH2 H atoms), and Uiso(H) = 1.5Ueq(C) (for methyl group).

Figures

Fig. 1.

Fig. 1.

Molecular structure of the title compound with the atom labelling scheme. Displacement ellipsoids for non-H atoms are drawn at the 30% probability level. Hydrogen atoms are shown as a spheres of arbitrary radius.

Fig. 2.

Fig. 2.

Infinite one-dimensional chains running in the [101] direction constructed via N—H···O and C—H···O hydrogen bonds between neighbouring molecules forming R22(8) motifs.

Crystal data

C14H14N2O2 F(000) = 256
Mr = 242.27 Dx = 1.288 Mg m3
Monoclinic, P21 Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2 yb Cell parameters from 4334 reflections
a = 5.1851 (4) Å θ = 4.4–32.7°
b = 21.408 (2) Å µ = 0.09 mm1
c = 5.6833 (4) Å T = 296 K
β = 98.010 (7)° Plate, yellow
V = 624.71 (8) Å3 0.57 × 0.50 × 0.19 mm
Z = 2

Data collection

Oxford Diffraction Xcalibur diffractometer with a Sapphire-3 CCD area detector 1856 independent reflections
Radiation source: Enhance (Mo) X-ray Source 1373 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.042
Detector resolution: 16.3426 pixels mm-1 θmax = 30.0°, θmin = 4.4°
CCD scans h = −7→7
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009) k = −30→30
Tmin = 0.953, Tmax = 0.958 l = −7→7
11868 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)] = 0.046 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.117 H atoms treated by a mixture of independent and constrained refinement
S = 1.03 w = 1/[σ2(Fo2) + (0.0688P)2] where P = (Fo2 + 2Fc2)/3
1856 reflections (Δ/σ)max < 0.001
167 parameters Δρmax = 0.16 e Å3
1 restraint Δρmin = −0.11 e Å3

Special details

Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su's are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles
Refinement. Refinement on F2 for ALL reflections except those flagged by the user for potential systematic errors. Weighted R-factors wR and all goodnesses of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The observed criterion of F2 > σ(F2) is used only for calculating -R-factor-obs 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 0.0400 (4) 0.59135 (11) 0.2460 (4) 0.0814 (8)
O2 0.1836 (4) 0.49767 (11) 0.2911 (3) 0.0688 (7)
N1 0.8389 (4) 0.47827 (11) −0.2730 (5) 0.0645 (8)
N2 0.1802 (4) 0.54885 (10) 0.1976 (3) 0.0525 (7)
C1 0.6686 (4) 0.52300 (11) −0.2149 (4) 0.0455 (6)
C2 0.5065 (4) 0.51224 (10) −0.0402 (4) 0.0417 (6)
C3 0.3489 (4) 0.56021 (10) 0.0150 (4) 0.0434 (6)
C4 0.3374 (5) 0.61797 (11) −0.0925 (5) 0.0564 (8)
C5 0.4936 (5) 0.62762 (13) −0.2656 (5) 0.0627 (9)
C6 0.6563 (5) 0.58119 (12) −0.3245 (4) 0.0558 (8)
C7 0.8676 (5) 0.41780 (13) −0.1683 (5) 0.0619 (8)
C8 0.6482 (4) 0.37253 (11) −0.2473 (4) 0.0511 (7)
C9 0.5891 (6) 0.32463 (15) −0.1024 (5) 0.0703 (10)
C10 0.3929 (7) 0.28214 (14) −0.1763 (6) 0.0747 (11)
C11 0.2506 (6) 0.28531 (12) −0.3980 (5) 0.0628 (9)
C12 0.3078 (6) 0.33344 (14) −0.5412 (5) 0.0669 (9)
C13 0.5021 (6) 0.37587 (13) −0.4681 (5) 0.0608 (8)
C14 0.0335 (7) 0.23991 (16) −0.4795 (9) 0.0912 (13)
H1N 0.913 (6) 0.4885 (14) −0.376 (5) 0.061 (8)*
H2 0.50580 0.47380 0.03580 0.0500*
H4 0.22830 0.64920 −0.04980 0.0680*
H5 0.48930 0.66590 −0.34350 0.0750*
H6 0.76130 0.58890 −0.44120 0.0670*
H7A 0.88320 0.42240 0.00290 0.0740*
H7B 1.02900 0.39970 −0.20470 0.0740*
H9 0.68320 0.32070 0.04860 0.0840*
H10 0.35690 0.25070 −0.07280 0.0890*
H12 0.21290 0.33750 −0.69180 0.0800*
H13 0.53540 0.40770 −0.57100 0.0730*
H14A −0.04300 0.25020 −0.63840 0.1370*
H14B −0.09690 0.24240 −0.37530 0.1370*
H14C 0.10230 0.19820 −0.47650 0.1370*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1 0.0779 (13) 0.0904 (15) 0.0858 (13) 0.0136 (12) 0.0468 (11) −0.0109 (11)
O2 0.0736 (12) 0.0795 (13) 0.0590 (10) −0.0050 (10) 0.0297 (9) 0.0073 (10)
N1 0.0566 (13) 0.0626 (13) 0.0834 (15) −0.0065 (10) 0.0420 (12) −0.0110 (11)
N2 0.0432 (10) 0.0693 (14) 0.0474 (10) −0.0029 (9) 0.0144 (8) −0.0086 (10)
C1 0.0394 (10) 0.0524 (12) 0.0462 (11) −0.0081 (9) 0.0108 (8) −0.0108 (9)
C2 0.0376 (9) 0.0446 (11) 0.0443 (10) −0.0026 (8) 0.0111 (8) −0.0001 (8)
C3 0.0394 (10) 0.0537 (12) 0.0387 (9) −0.0031 (9) 0.0116 (8) −0.0042 (8)
C4 0.0525 (13) 0.0498 (13) 0.0695 (14) 0.0056 (11) 0.0173 (11) −0.0005 (12)
C5 0.0689 (16) 0.0546 (14) 0.0668 (15) 0.0009 (12) 0.0177 (13) 0.0136 (12)
C6 0.0534 (13) 0.0654 (15) 0.0530 (13) −0.0136 (11) 0.0226 (10) 0.0013 (11)
C7 0.0446 (12) 0.0669 (15) 0.0753 (16) 0.0093 (12) 0.0120 (11) −0.0171 (13)
C8 0.0521 (12) 0.0502 (12) 0.0528 (12) 0.0131 (10) 0.0142 (10) −0.0040 (10)
C9 0.0801 (19) 0.0749 (17) 0.0551 (14) 0.0082 (16) 0.0069 (13) 0.0144 (14)
C10 0.085 (2) 0.0564 (15) 0.088 (2) 0.0077 (14) 0.0303 (17) 0.0262 (15)
C11 0.0629 (16) 0.0478 (13) 0.0820 (19) 0.0067 (11) 0.0252 (15) −0.0065 (13)
C12 0.0719 (17) 0.0706 (17) 0.0572 (14) −0.0026 (14) 0.0057 (12) −0.0049 (13)
C13 0.0720 (15) 0.0569 (13) 0.0547 (13) −0.0022 (13) 0.0135 (11) 0.0080 (12)
C14 0.078 (2) 0.0619 (18) 0.137 (3) −0.0059 (15) 0.027 (2) −0.021 (2)

Geometric parameters (Å, º)

O1—N2 1.220 (3) C11—C14 1.510 (5)
O2—N2 1.217 (3) C11—C12 1.371 (4)
N1—C1 1.374 (3) C12—C13 1.377 (4)
N1—C7 1.424 (4) C2—H2 0.9300
N2—C3 1.468 (3) C4—H4 0.9300
N1—H1N 0.78 (3) C5—H5 0.9300
C1—C6 1.390 (3) C6—H6 0.9300
C1—C2 1.406 (3) C7—H7A 0.9700
C2—C3 1.376 (3) C7—H7B 0.9700
C3—C4 1.377 (3) C9—H9 0.9300
C4—C5 1.374 (4) C10—H10 0.9300
C5—C6 1.375 (4) C12—H12 0.9300
C7—C8 1.514 (4) C13—H13 0.9300
C8—C13 1.374 (4) C14—H14A 0.9600
C8—C9 1.376 (4) C14—H14B 0.9600
C9—C10 1.386 (5) C14—H14C 0.9600
C10—C11 1.370 (4)
O1···C1i 3.362 (3) C13···H7Bi 3.0900
O1···C6ii 3.364 (3) H1N···O2vi 2.52 (3)
O2···C7i 3.352 (3) H1N···H6 2.3000
O2···C13iii 3.282 (4) H2···O2 2.4200
O1···H14Civ 2.7900 H2···C7 2.6300
O1···H4 2.4000 H2···C8 2.8600
O1···H6ii 2.4400 H2···H7A 2.2800
O2···H1Nii 2.52 (3) H4···O1 2.4000
O2···H2 2.4200 H5···H14Cviii 2.5700
O2···H7Ai 2.6400 H6···O1vi 2.4400
O2···H13iii 2.6900 H6···H1N 2.3000
N1···C3v 3.398 (3) H6···H14Cviii 2.5100
N2···C1i 3.333 (3) H7A···O2v 2.6400
N1···H13 2.6200 H7A···C2 2.7300
C1···O1v 3.362 (3) H7A···H2 2.2800
C1···N2v 3.333 (3) H7A···H9 2.4400
C1···C13 3.520 (4) H7B···C11v 2.9800
C2···C8 3.333 (3) H7B···C12v 2.9200
C3···N1i 3.398 (3) H7B···C13v 3.0900
C6···O1vi 3.364 (3) H9···H7A 2.4400
C7···O2v 3.352 (3) H9···H14Aix 2.6000
C8···C2 3.333 (3) H12···H14A 2.3400
C13···C1 3.520 (4) H13···O2vii 2.6900
C13···O2vii 3.282 (4) H13···N1 2.6200
C2···H7A 2.7300 H14A···H9x 2.6000
C6···H14Cviii 3.0800 H14A···H12 2.3400
C7···H2 2.6300 H14B···C9i 2.9800
C8···H2 2.8600 H14C···O1xi 2.7900
C9···H14Bv 2.9800 H14C···C6xii 3.0800
C11···H7Bi 2.9800 H14C···H5xii 2.5700
C12···H7Bi 2.9200 H14C···H6xii 2.5100
C1—N1—C7 124.5 (2) C1—C2—H2 121.00
O1—N2—O2 123.1 (2) C3—C2—H2 121.00
O1—N2—C3 117.9 (2) C3—C4—H4 121.00
O2—N2—C3 119.0 (2) C5—C4—H4 121.00
C7—N1—H1N 123 (2) C4—C5—H5 120.00
C1—N1—H1N 113 (2) C6—C5—H5 120.00
N1—C1—C6 120.5 (2) C1—C6—H6 119.00
C2—C1—C6 117.9 (2) C5—C6—H6 119.00
N1—C1—C2 121.5 (2) N1—C7—H7A 108.00
C1—C2—C3 118.1 (2) N1—C7—H7B 108.00
N2—C3—C4 118.0 (2) C8—C7—H7A 108.00
N2—C3—C2 117.97 (19) C8—C7—H7B 108.00
C2—C3—C4 124.0 (2) H7A—C7—H7B 107.00
C3—C4—C5 117.3 (2) C8—C9—H9 119.00
C4—C5—C6 120.6 (2) C10—C9—H9 119.00
C1—C6—C5 122.0 (2) C9—C10—H10 119.00
N1—C7—C8 115.3 (2) C11—C10—H10 119.00
C9—C8—C13 116.4 (2) C11—C12—H12 119.00
C7—C8—C9 121.4 (2) C13—C12—H12 119.00
C7—C8—C13 122.2 (2) C8—C13—H13 119.00
C8—C9—C10 121.5 (3) C12—C13—H13 119.00
C9—C10—C11 121.7 (3) C11—C14—H14A 109.00
C10—C11—C14 122.2 (3) C11—C14—H14B 110.00
C10—C11—C12 116.7 (3) C11—C14—H14C 109.00
C12—C11—C14 121.0 (3) H14A—C14—H14B 109.00
C11—C12—C13 121.8 (3) H14A—C14—H14C 109.00
C8—C13—C12 121.9 (3) H14B—C14—H14C 109.00
C7—N1—C1—C2 0.7 (4) C3—C4—C5—C6 −0.9 (4)
C7—N1—C1—C6 179.2 (2) C4—C5—C6—C1 0.6 (4)
C1—N1—C7—C8 73.9 (3) N1—C7—C8—C9 −152.7 (3)
O1—N2—C3—C2 −179.8 (2) N1—C7—C8—C13 29.0 (4)
O1—N2—C3—C4 −0.6 (3) C7—C8—C13—C12 178.1 (3)
O2—N2—C3—C2 −0.8 (3) C7—C8—C9—C10 −178.3 (3)
O2—N2—C3—C4 178.5 (2) C13—C8—C9—C10 0.1 (4)
N1—C1—C2—C3 177.4 (2) C9—C8—C13—C12 −0.3 (4)
C6—C1—C2—C3 −1.1 (3) C8—C9—C10—C11 0.8 (5)
N1—C1—C6—C5 −178.1 (2) C9—C10—C11—C12 −1.5 (5)
C2—C1—C6—C5 0.5 (4) C9—C10—C11—C14 −179.0 (3)
C1—C2—C3—N2 −179.93 (19) C10—C11—C12—C13 1.3 (5)
C1—C2—C3—C4 0.9 (3) C14—C11—C12—C13 178.9 (3)
N2—C3—C4—C5 −179.1 (2) C11—C12—C13—C8 −0.4 (5)
C2—C3—C4—C5 0.1 (4)

Symmetry codes: (i) x−1, y, z; (ii) x−1, y, z+1; (iii) x, y, z+1; (iv) −x, y+1/2, −z; (v) x+1, y, z; (vi) x+1, y, z−1; (vii) x, y, z−1; (viii) −x+1, y+1/2, −z−1; (ix) x+1, y, z+1; (x) x−1, y, z−1; (xi) −x, y−1/2, −z; (xii) −x+1, y−1/2, −z−1.

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
N1—H1N···O2vi 0.78 (3) 2.52 (3) 3.277 (3) 168 (3)
C6—H6···O1vi 0.93 2.44 3.364 (3) 171
C7—H7A···O2v 0.97 2.64 3.352 (3) 130
C13—H13···O2vii 0.93 2.69 3.282 (4) 122

Symmetry codes: (v) x+1, y, z; (vi) x+1, y, z−1; (vii) x, y, z−1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: FJ2555).

References

  1. Bernstein, J., Davis, R. E., Shimoni, L. & Chang, N.-L. (1995). Angew. Chem. Int. Ed. Engl. 34, 1555–1573.
  2. Betz, R., McCleland, C. & Marchand, H. (2011). Acta Cryst. E67, o1195. [DOI] [PMC free article] [PubMed]
  3. Etter, M. C. (1990). Acc. Chem. Res. 23, 120–126.
  4. Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
  5. Macrae, C. F., Edgington, P. R., McCabe, P., Pidcock, E., Shields, G. P., Taylor, R., Towler, M. & van de Streek, J. (2006). J. Appl. Cryst. 39, 453–457.
  6. Magyarfalvi, G. (2008). Preparatory problems for the 40th International Chemistry Olympiad, edited by G. Magyarfalvi, p. 48. Chemistry Olympiad, Budapest.
  7. Oxford Diffraction (2009). CrysAlis PRO Oxford Diffraction Ltd, Yarnton, England.
  8. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  9. Spek, A. L. (2009). Acta Cryst. D65, 148–155. [DOI] [PMC free article] [PubMed]
  10. Stilinović, V. & Portada, T. (2011). Acta Cryst. E67, o3013. [DOI] [PMC free article] [PubMed]
  11. Xing, J.-D., Bai, G.-Y., Zeng, T. & Li, J.-S. (2006). Acta Cryst. E62, o79–o80.

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) global, I. DOI: 10.1107/S1600536812024348/fj2555sup1.cif

e-68-o1967-sup1.cif (23.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812024348/fj2555Isup2.hkl

e-68-o1967-Isup2.hkl (89.5KB, hkl)

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


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

RESOURCES