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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2014 Jun 25;70(Pt 7):o806. doi: 10.1107/S1600536814014238

N 1-[(1H-Imidazol-2-yl)methyl­idene]-N 4-phenyl­benzene-1,4-di­amine

Md Serajul Haque Faizi a, Ashraf Mashrai b, M Shahid b,*, Musheer Ahmad a
PMCID: PMC4120595  PMID: 25161587

Abstract

The title compound, C16H14N4, is non-planar with dihedral angles between the planes of the imidazole and phenyl­enedi­amine rings of 30.66 (4)° and between the planes of the phenyl­enedi­amine and N-phenyl rings of 56.63 (7)°. In the crystal, mol­ecules are connected by N—H⋯N hydrogen bonds, generating a chain extending along the b-axis direction. The crystal structure is also stabilized by C—H⋯π inter­actions between N-phenyl and imidazole rings and slipped π–π stacking inter­actions between imidazole rings [centroid–centroid distance = 3.516 (4) Å] giving an overall two-dimensional layered structure lying parallel to (010).

Keywords: crystal structure

Related literature  

For applications of Schiff bases, see: Lozier et al. (1975); Dalapati et al. (2011); Sun et al. (2012). The present work is part of an ongoing structural study of Schiff base–metal complexes, see: Faizi & Hussain (2014); Faizi & Sen (2014). For related Schiff bases and their applications, see: Thompson et al. (2012); Shue et al. (1994); Garcia et al. (2006).graphic file with name e-70-0o806-scheme1.jpg

Experimental  

Crystal data  

  • C16H14N4

  • M r = 262.31

  • Monoclinic, Inline graphic

  • a = 15.663 (5) Å

  • b = 5.063 (3) Å

  • c = 16.800 (5) Å

  • β = 93.124 (5)°

  • V = 1330.3 (10) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 100 K

  • 0.15 × 0.13 × 0.10 mm

Data collection  

  • Bruker SMART APEX CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 2004) T min = 0.984, T max = 0.990

  • 11186 measured reflections

  • 3296 independent reflections

  • 2403 reflections with I > 2σ(I)

  • R int = 0.042

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.044

  • wR(F 2) = 0.110

  • S = 1.03

  • 3296 reflections

  • 189 parameters

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

  • Δρmax = 0.24 e Å−3

  • Δρmin = −0.18 e Å−3

Data collection: SMART (Bruker, 2003); cell refinement: SAINT (Bruker, 2003); data reduction: SAINT; program(s) used to solve structure: SIR97 (Altomare et al., 1999); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenberg & Putz, 2006); software used to prepare material for publication: DIAMOND.

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536814014238/gg2140sup1.cif

e-70-0o806-sup1.cif (17.5KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814014238/gg2140Isup2.hkl

e-70-0o806-Isup2.hkl (158.4KB, hkl)

Supporting information file. DOI: 10.1107/S1600536814014238/gg2140Isup3.cml

CCDC reference: 1008808

Additional supporting information: crystallographic information; 3D view; checkCIF report

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

Cg1 is the centroid of the N3/N4/C14–C16 ring.

D—H⋯A D—H H⋯A DA D—H⋯A
N4—H101⋯N3i 0.86 2.09 2.875 (3) 151
C2—H2⋯Cg1ii 0.93 2.83 3.691 (3) 155

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

Acknowledgments

The authors are grateful to the Department of Chemistry, Aligarh Muslim University, India, and SERB–DST, New Delhi, for financial assistance (Ref SR/FT/CS-76/2011).

supplementary crystallographic information

S1. Comment

Schiff bases often exhibit various biological activities and in many cases were shown to have antibacterial, anticancer, anti-inflammatory and antitoxic properties (Lozier et al., 1975). They are used as anion sensors (Dalapati et al., 2011) and as non-linear optics compounds (Sun et al., 2012). The present work is part of an ongoing structural study of Schiff base metal complexes (Faizi & Hussain, 2014; Faizi & Sen, 2014) and we report here the structure of N1-((1H-imidazol-2-yl)methylene)-N4-phenylbenzene-1,4-diamine (IMPD). There are very few examples similar to title compound and their metal complex have been reported in the literature (Thompson et al., 2012; Shue et al., 1994; Garcia et al., 2006). The synthesis of IMPD by condensation of 2-imidazolecarboxaldehyde and N-phenyl-p-phenylenediamine has not previously been reported. In the title compound (Fig. 1) IMPD has non planar structure, the dihedral angle between the imidazole and phenylenediamine rings is 30.66 (4) ° and the dihedral angle between the phenylenediamine and N-phenyl rings is 56.63 (7) °. The imine group displays a torsional angle (C10—N2—C13—C14) of 177.29 (2)°. In the crystal, molecules are connected by intermolecular N—H···N hydrogen bond interaction generate a one-dimensional chain structure extending along c axis (Table 1, Fig 2). The crystal structure is also stabilized by C—H···π interations between N-phenyl and imidazole and slipped π–π stacking interactions between imidazole rings [centroid–centroid distance = 3.516 (4) Å] give an overall two-dimensional layered structure lying parallel to (010) given in Fig 3.

S2. Experimental

100 mg (1 mmol) of N-phenyl-p-phenylenediamine were dissolved in 10 ml of absolute ethanol. To this solution, 52 mg (1 mmol) of 2-imidazolecarboxaldehyde in 5 ml of absolute ethanol was dropwisely added under stirring. Then, this mixture was stirred for 10 min, two drops of glacial acetic acid were then added and the mixture was further refluxed for 2h. The resulting light green precipitate was recovered by filtration, washed several times with a small portions of EtOH and then with diethyl ether to give 120 mg (86%) of N1-((1H-imidazol-2-yl)methylene)-N4-phenylbenzene-1,4-diamine (IMPD). The crystal of the title compound suitable for X-ray analysis was obtained within 3 days by slow evaporation of the MeOH solvent.

S3. Refinement

All H-atoms were positioned geometrically and refined using a riding model with C—H = 0.92–0.93 Å and Uiso(H) = 1.2Ueq(C).

Figures

Fig. 1.

Fig. 1.

The molecular conformation and atom-numbering scheme for the title compound with non-H atoms drawn as 40% probability displacement ellipsoids.

Fig. 2.

Fig. 2.

The one-dimensional hydrogen-bonded chain structure in the title compound extending along c, with hydrogen bonds shown as dashed lines.

Fig. 3.

Fig. 3.

The two-dimensional weak bond interaction present in the title compound extending along b, with weak bond interaction shown as dashed lines.

Crystal data

C16H14N4 F(000) = 552
Mr = 262.31 Dx = 1.310 Mg m3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn Cell parameters from 999 reflections
a = 15.663 (5) Å θ = 1.8–25.5°
b = 5.063 (3) Å µ = 0.08 mm1
c = 16.800 (5) Å T = 100 K
β = 93.124 (5)° Block, yellow
V = 1330.3 (10) Å3 0.15 × 0.13 × 0.10 mm
Z = 4

Data collection

Bruker SMART APEX CCD diffractometer 3296 independent reflections
Radiation source: fine-focus sealed tube 2403 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.042
ω scans θmax = 28.3°, θmin = 2.4°
Absorption correction: multi-scan (SADABS; Sheldrick, 2004) h = −13→20
Tmin = 0.984, Tmax = 0.990 k = −6→6
11186 measured reflections l = −22→22

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)] = 0.044 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.110 H atoms treated by a mixture of independent and constrained refinement
S = 1.03 w = 1/[σ2(Fo2) + (0.0458P)2 + 0.404P] where P = (Fo2 + 2Fc2)/3
3296 reflections (Δ/σ)max = 0.001
189 parameters Δρmax = 0.24 e Å3
0 restraints Δρmin = −0.18 e Å3

Special details

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 0.43125 (8) −0.1760 (3) 0.33278 (8) 0.0214 (3)
C2 0.38397 (9) −0.3415 (3) 0.28135 (9) 0.0282 (3)
H2 0.3891 −0.3274 0.2266 0.034*
C3 0.32914 (10) −0.5278 (3) 0.31101 (11) 0.0352 (4)
H3 0.2974 −0.6371 0.2761 0.042*
C4 0.32145 (10) −0.5514 (3) 0.39221 (11) 0.0337 (4)
H4 0.2861 −0.6802 0.4121 0.040*
C5 0.36660 (10) −0.3828 (3) 0.44371 (10) 0.0308 (4)
H5 0.3607 −0.3959 0.4984 0.037*
C6 0.42048 (9) −0.1945 (3) 0.41415 (9) 0.0275 (3)
H6 0.4498 −0.0793 0.4490 0.033*
C7 0.57160 (9) 0.0512 (3) 0.32757 (8) 0.0199 (3)
C8 0.61533 (9) −0.1149 (3) 0.38253 (8) 0.0202 (3)
H8 0.5862 −0.2506 0.4066 0.024*
C9 0.70154 (9) −0.0785 (3) 0.40118 (8) 0.0200 (3)
H9 0.7299 −0.1937 0.4367 0.024*
C10 0.74693 (8) 0.1273 (3) 0.36788 (8) 0.0174 (3)
C11 0.70272 (9) 0.2954 (3) 0.31390 (8) 0.0200 (3)
H11 0.7316 0.4341 0.2910 0.024*
C12 0.61719 (9) 0.2582 (3) 0.29428 (8) 0.0217 (3)
H12 0.5891 0.3725 0.2583 0.026*
C13 0.87684 (9) 0.3549 (3) 0.38064 (8) 0.0190 (3)
C14 0.96846 (8) 0.3614 (3) 0.39783 (8) 0.0173 (3)
C15 1.09852 (9) 0.2263 (3) 0.43150 (8) 0.0199 (3)
H15 1.1455 0.1208 0.4459 0.024*
C16 1.09789 (9) 0.4940 (3) 0.42150 (8) 0.0206 (3)
H16 1.1456 0.6027 0.4281 0.025*
N1 0.48649 (8) 0.0127 (3) 0.30203 (8) 0.0259 (3)
N2 0.83589 (7) 0.1392 (2) 0.38775 (6) 0.0185 (3)
N3 1.01646 (7) 0.5797 (2) 0.40025 (7) 0.0192 (3)
N4 1.01628 (7) 0.1451 (2) 0.41603 (6) 0.0181 (3)
H101 0.9981 −0.0150 0.4176 0.022*
H102 0.4709 (11) 0.072 (4) 0.2555 (11) 0.037 (5)*
H13 0.8508 (10) 0.525 (3) 0.3660 (9) 0.026 (4)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0150 (7) 0.0220 (7) 0.0272 (7) 0.0025 (5) 0.0010 (5) 0.0033 (6)
C2 0.0250 (8) 0.0332 (9) 0.0260 (8) −0.0003 (7) −0.0016 (6) 0.0003 (6)
C3 0.0268 (9) 0.0310 (9) 0.0470 (10) −0.0053 (7) −0.0044 (7) −0.0042 (8)
C4 0.0223 (8) 0.0287 (8) 0.0509 (11) −0.0015 (7) 0.0083 (7) 0.0113 (7)
C5 0.0254 (8) 0.0362 (9) 0.0316 (8) 0.0038 (7) 0.0071 (6) 0.0098 (7)
C6 0.0242 (8) 0.0320 (9) 0.0262 (8) −0.0016 (6) 0.0013 (6) −0.0003 (6)
C7 0.0200 (7) 0.0198 (7) 0.0202 (7) 0.0003 (5) 0.0021 (5) −0.0021 (5)
C8 0.0208 (7) 0.0172 (7) 0.0230 (7) −0.0029 (5) 0.0038 (5) 0.0020 (5)
C9 0.0234 (7) 0.0162 (6) 0.0204 (7) 0.0010 (5) 0.0017 (5) 0.0009 (5)
C10 0.0192 (7) 0.0153 (6) 0.0177 (6) 0.0002 (5) 0.0024 (5) −0.0037 (5)
C11 0.0246 (7) 0.0153 (6) 0.0204 (7) −0.0026 (5) 0.0040 (5) 0.0005 (5)
C12 0.0254 (8) 0.0183 (7) 0.0213 (7) 0.0011 (6) 0.0015 (5) 0.0028 (6)
C13 0.0228 (7) 0.0165 (7) 0.0178 (6) 0.0015 (6) 0.0027 (5) −0.0014 (5)
C14 0.0214 (7) 0.0141 (6) 0.0169 (6) −0.0004 (5) 0.0038 (5) −0.0007 (5)
C15 0.0180 (7) 0.0182 (7) 0.0234 (7) −0.0001 (5) 0.0002 (5) −0.0014 (5)
C16 0.0209 (7) 0.0176 (7) 0.0235 (7) −0.0028 (5) 0.0020 (5) −0.0018 (5)
N1 0.0198 (6) 0.0314 (7) 0.0260 (7) −0.0040 (5) −0.0027 (5) 0.0092 (6)
N2 0.0208 (6) 0.0169 (6) 0.0179 (6) −0.0023 (5) 0.0025 (4) −0.0010 (4)
N3 0.0200 (6) 0.0149 (6) 0.0226 (6) −0.0015 (4) 0.0018 (5) −0.0013 (4)
N4 0.0208 (6) 0.0117 (5) 0.0220 (6) −0.0024 (4) 0.0022 (4) −0.0001 (4)

Geometric parameters (Å, º)

C1—C2 1.388 (2) C9—H9 0.9300
C1—C6 1.390 (2) C10—C11 1.3990 (19)
C1—N1 1.4060 (19) C10—N2 1.4163 (18)
C2—C3 1.386 (2) C11—C12 1.375 (2)
C2—H2 0.9300 C11—H11 0.9300
C3—C4 1.381 (2) C12—H12 0.9300
C3—H3 0.9300 C13—N2 1.2757 (18)
C4—C5 1.383 (2) C13—C14 1.449 (2)
C4—H4 0.9300 C13—H13 0.976 (17)
C5—C6 1.383 (2) C14—N3 1.3358 (18)
C5—H5 0.9300 C14—N4 1.3526 (18)
C6—H6 0.9300 C15—N4 1.3636 (18)
C7—N1 1.3918 (18) C15—C16 1.366 (2)
C7—C8 1.400 (2) C15—H15 0.9300
C7—C12 1.402 (2) C16—N3 1.3757 (18)
C8—C9 1.382 (2) C16—H16 0.9300
C8—H8 0.9300 N1—H102 0.860 (19)
C9—C10 1.3957 (19) N4—H101 0.8600
C2—C1—C6 118.84 (13) C9—C10—N2 116.95 (12)
C2—C1—N1 119.97 (14) C11—C10—N2 124.95 (12)
C6—C1—N1 121.15 (13) C12—C11—C10 120.90 (13)
C3—C2—C1 120.45 (15) C12—C11—H11 119.6
C3—C2—H2 119.8 C10—C11—H11 119.5
C1—C2—H2 119.8 C11—C12—C7 121.16 (13)
C4—C3—C2 120.21 (16) C11—C12—H12 119.4
C4—C3—H3 119.9 C7—C12—H12 119.4
C2—C3—H3 119.9 N2—C13—C14 119.90 (13)
C3—C4—C5 119.69 (15) N2—C13—H13 124.9 (9)
C3—C4—H4 120.2 C14—C13—H13 115.2 (9)
C5—C4—H4 120.2 N3—C14—N4 111.05 (12)
C4—C5—C6 120.16 (15) N3—C14—C13 125.08 (12)
C4—C5—H5 119.9 N4—C14—C13 123.84 (12)
C6—C5—H5 119.9 N4—C15—C16 105.97 (13)
C5—C6—C1 120.58 (15) N4—C15—H15 127.0
C5—C6—H6 119.7 C16—C15—H15 127.0
C1—C6—H6 119.7 C15—C16—N3 110.19 (13)
N1—C7—C8 123.04 (13) C15—C16—H16 124.9
N1—C7—C12 118.81 (13) N3—C16—H16 124.9
C8—C7—C12 118.08 (13) C7—N1—C1 125.46 (13)
C9—C8—C7 120.43 (13) C7—N1—H102 116.8 (12)
C9—C8—H8 119.8 C1—N1—H102 114.9 (12)
C7—C8—H8 119.8 C13—N2—C10 120.49 (12)
C8—C9—C10 121.43 (13) C14—N3—C16 105.04 (12)
C8—C9—H9 119.3 C14—N4—C15 107.74 (11)
C10—C9—H9 119.3 C14—N4—H101 126.1
C9—C10—C11 117.97 (13) C15—N4—H101 126.1
C6—C1—C2—C3 −2.1 (2) C8—C7—C12—C11 1.0 (2)
N1—C1—C2—C3 −179.81 (14) N2—C13—C14—N3 −172.90 (12)
C1—C2—C3—C4 −0.4 (2) N2—C13—C14—N4 5.0 (2)
C2—C3—C4—C5 2.1 (2) N4—C15—C16—N3 0.14 (16)
C3—C4—C5—C6 −1.2 (2) C8—C7—N1—C1 6.8 (2)
C4—C5—C6—C1 −1.3 (2) C12—C7—N1—C1 −176.26 (14)
C2—C1—C6—C5 3.0 (2) C2—C1—N1—C7 −130.27 (16)
N1—C1—C6—C5 −179.36 (14) C6—C1—N1—C7 52.1 (2)
N1—C7—C8—C9 175.16 (13) C14—C13—N2—C10 −177.30 (11)
C12—C7—C8—C9 −1.8 (2) C9—C10—N2—C13 −158.92 (12)
C7—C8—C9—C10 1.8 (2) C11—C10—N2—C13 25.31 (19)
C8—C9—C10—C11 −0.8 (2) N4—C14—N3—C16 −0.39 (14)
C8—C9—C10—N2 −176.86 (12) C13—C14—N3—C16 177.74 (12)
C9—C10—C11—C12 −0.07 (19) C15—C16—N3—C14 0.15 (15)
N2—C10—C11—C12 175.65 (12) N3—C14—N4—C15 0.49 (15)
C10—C11—C12—C7 −0.1 (2) C13—C14—N4—C15 −177.67 (12)
N1—C7—C12—C11 −176.13 (13) C16—C15—N4—C14 −0.37 (15)

Hydrogen-bond geometry (Å, º)

Cg1 is the centroid of the N3/N4/C14–C16 ring.

D—H···A D—H H···A D···A D—H···A
N4—H101···N3i 0.86 2.09 2.875 (3) 151
C2—H2···Cg1ii 0.93 2.83 3.691 (3) 155

Symmetry codes: (i) x, y−1, z; (ii) −x+3/2, y−1/2, −z+1/2.

Footnotes

Supporting information for this paper is available from the IUCr electronic archives (Reference: GG2140).

References

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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/S1600536814014238/gg2140sup1.cif

e-70-0o806-sup1.cif (17.5KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814014238/gg2140Isup2.hkl

e-70-0o806-Isup2.hkl (158.4KB, hkl)

Supporting information file. DOI: 10.1107/S1600536814014238/gg2140Isup3.cml

CCDC reference: 1008808

Additional supporting information: crystallographic information; 3D view; checkCIF report


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