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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Jun 7;64(Pt 7):o1221. doi: 10.1107/S1600536808016668

N-(4,5-Diaza­fluoren-9-yl­idene)aniline

Hui Cang a, Dong Jin b, Si-Qing Wang a, Shan Liu a, Jin-Tang Wang a,*
PMCID: PMC2961656  PMID: 21202858

Abstract

In the mol­ecule of the title compound, C17H11N3, the 4,5-diaza­fluorenyl­idene unit is nearly planar and is oriented with respect to the phenyl ring at a dihedral angle of 75.75 (3)°. In the crystal structure, the mol­ecules are aligned in the [100] direction in such a way that neighbouring 4,5-diaza­fluorenyl­idene planes face each other in an anti­parallel fashion.

Related literature

For related literature, see: Wang & Rillema (1997 ▶); Wang et al. (2006 ▶); Peters et al. (1998 ▶); Glagovich et al. (2004a ▶,b ▶). For bond-length data, see: Allen et al. (1987 ▶).graphic file with name e-64-o1221-scheme1.jpg

Experimental

Crystal data

  • C17H11N3

  • M r = 257.29

  • Triclinic, Inline graphic

  • a = 7.1950 (14) Å

  • b = 8.5860 (17) Å

  • c = 11.876 (2) Å

  • α = 80.63 (3)°

  • β = 74.78 (3)°

  • γ = 66.46 (3)°

  • V = 647.6 (2) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 298 (2) K

  • 0.20 × 0.10 × 0.05 mm

Data collection

  • Enraf–Nonius CAD-4 diffractometer

  • Absorption correction: ψ scan (North et al., 1968 ▶) T min = 0.984, T max = 0.996

  • 2529 measured reflections

  • 2326 independent reflections

  • 1642 reflections with I > 2σ(I)

  • R int = 0.057

  • 3 standard reflections frequency: 120 min intensity decay: none

Refinement

  • R[F 2 > 2σ(F 2)] = 0.056

  • wR(F 2) = 0.178

  • S = 1.02

  • 2326 reflections

  • 181 parameters

  • H-atom parameters constrained

  • Δρmax = 0.19 e Å−3

  • Δρmin = −0.25 e Å−3

Data collection: CAD-4 Software (Enraf–Nonius, 1989 ▶); cell refinement: CAD-4 Software; data reduction: XCAD4 (Harms & Wocadlo, 1995 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808016668/hk2468sup1.cif

e-64-o1221-sup1.cif (17.4KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808016668/hk2468Isup2.hkl

e-64-o1221-Isup2.hkl (114.3KB, hkl)

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

Acknowledgments

The authors thank the Center of Testing and Analysis, Nanjing University, for support.

supplementary crystallographic information

Comment

N-(4,5-diazafluorenylidene)benzenamine, is one of the important ligands, being utilized to synthesize complexes with interesting photochemical properties (Wang & Rillema, 1997). The crystal structure of 4-methyl-N-(4,5-diazafluorenylidene)benzenamine monohydrate, (II) (Wang et al., 2006) was reported, previously. We report herein the crystal structure of the title compound, (I).

In the molecule of (I) (Fig. 1), the bond lengths (Allen et al., 1987) and angles are within normal ranges, which are comparable with the corresponding values in other fluorenylidene compounds (II), N-fluorenylidene-aniline-benzene (4/1), (III) (Peters et al., 1998), N-(9H-fluoren-9-ylidene)-N-(4-methoxyphenyl)amine, (IV) (Glagovich et al., 2004a) and N-9H-fluoren-9-ylidene-3,4-dimethyl-aniline, (V) (Glagovich et al., 2004b). Rings A (C1–C6), B (N2/C8–C12), C (C7/C8/C12/C13/C17) and D (N3/C13–C17) are, of course, planar. In the 4,5-diazafluorenylidene unit, the dihedral angles between the rings are B/C = 0.29 (3)°, C/D = 2.30 (3)° and B/D = 2.15 (3)°. So, rings B, C and D are nearly coplanar. The coplanar ring system is oriented with respect to ring A at a dihedral angle of 75.75 (3)°, in which it is reported as 65.1 (1)° in (II).

In the crystal structure, the molecules are aligned in the [100] direction, in such a way that neighbouring 4,5-diazafluorenylidene planes face in anti-parallel fashion (Fig. 2), as in (II).

Experimental

The title compound, (I), was prepared according to the literature method (Wang & Rillema, 1997). Crystals suitable for X-ray analysis were obtained by dissolving (I) (2.0 g, 6.3 mmol) in acetate ester solution (50 ml, 1.0 mol/L) and evaporating the solvent slowly at room temperature for about 5 d.

Refinement

H atoms were positioned geometrically, with C—H = 0.93 Å for aromatic H, and constrained to ride on their parent atoms with Uiso(H) = 1.2Ueq(C).

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title molecule, with the atom-numbering scheme. Displacement ellipsoids are drawn at the 50% probability level.

Fig. 2.

Fig. 2.

A packing diagram of (I).

Crystal data

C17H11N3 Z = 2
Mr = 257.29 F000 = 268
Triclinic, P1 Dx = 1.319 Mg m−3
Hall symbol: -P 1 Mo Kα radiation λ = 0.71073 Å
a = 7.1950 (14) Å Cell parameters from 25 reflections
b = 8.5860 (17) Å θ = 9–13º
c = 11.876 (2) Å µ = 0.08 mm−1
α = 80.63 (3)º T = 298 (2) K
β = 74.78 (3)º Needle, colourless
γ = 66.46 (3)º 0.20 × 0.10 × 0.05 mm
V = 647.6 (2) Å3

Data collection

Enraf–Nonius CAD-4 diffractometer Rint = 0.057
Radiation source: fine-focus sealed tube θmax = 25.2º
Monochromator: graphite θmin = 1.8º
T = 298(2) K h = −8→8
ω/2θ scans k = −9→10
Absorption correction: ψ scan(North et al., 1968) l = 0→14
Tmin = 0.984, Tmax = 0.996 3 standard reflections
2529 measured reflections every 120 min
2326 independent reflections intensity decay: none
1642 reflections with I > 2σ(I)

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)] = 0.056 H-atom parameters constrained
wR(F2) = 0.178   w = 1/[σ2(Fo2) + (0.08P)2 + 0.4P] where P = (Fo2 + 2Fc2)/3
S = 1.02 (Δ/σ)max < 0.001
2326 reflections Δρmax = 0.19 e Å−3
181 parameters Δρmin = −0.25 e Å−3
Primary atom site location: structure-invariant direct methods Extinction correction: none

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 > 2sigma(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
N1 0.1000 (4) 1.2848 (3) 0.6315 (2) 0.0491 (6)
N2 0.3187 (4) 0.7234 (3) 0.4917 (2) 0.0492 (6)
N3 0.3994 (4) 0.9717 (3) 0.2888 (2) 0.0503 (6)
C1 0.0047 (6) 1.2899 (6) 0.9516 (3) 0.0808 (12)
H1B 0.0717 1.2935 1.0078 0.097*
C2 −0.1937 (6) 1.2891 (5) 0.9852 (3) 0.0778 (11)
H2B −0.2605 1.2921 1.0638 0.093*
C3 −0.2916 (6) 1.2841 (5) 0.9021 (3) 0.0675 (9)
H3B −0.4257 1.2845 0.9249 0.081*
C4 −0.1951 (5) 1.2783 (4) 0.7855 (3) 0.0561 (8)
H4A −0.2637 1.2753 0.7301 0.067*
C5 0.0048 (5) 1.2772 (3) 0.7513 (2) 0.0470 (7)
C6 0.1040 (5) 1.2853 (4) 0.8350 (3) 0.0616 (9)
H6A 0.2369 1.2877 0.8124 0.074*
C7 0.1686 (4) 1.1567 (3) 0.5708 (2) 0.0401 (6)
C8 0.1856 (4) 0.9756 (3) 0.6012 (2) 0.0385 (6)
C9 0.1347 (4) 0.8860 (4) 0.7046 (2) 0.0454 (7)
H9A 0.0739 0.9384 0.7750 0.055*
C10 0.1782 (5) 0.7148 (4) 0.6987 (3) 0.0501 (7)
H10A 0.1470 0.6498 0.7662 0.060*
C11 0.2673 (5) 0.6404 (4) 0.5935 (3) 0.0530 (8)
H11A 0.2936 0.5253 0.5929 0.064*
C12 0.2774 (4) 0.8874 (3) 0.4993 (2) 0.0409 (6)
C13 0.3186 (4) 1.0075 (3) 0.4004 (2) 0.0405 (6)
C14 0.4125 (5) 1.1058 (4) 0.2161 (3) 0.0574 (8)
H14A 0.4674 1.0878 0.1371 0.069*
C15 0.3502 (5) 1.2689 (4) 0.2504 (3) 0.0538 (8)
H15A 0.3631 1.3562 0.1951 0.065*
C16 0.2688 (4) 1.3018 (4) 0.3668 (3) 0.0502 (7)
H16A 0.2265 1.4099 0.3924 0.060*
C17 0.2534 (4) 1.1661 (3) 0.4432 (2) 0.0398 (6)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
N1 0.0548 (14) 0.0417 (13) 0.0454 (14) −0.0158 (11) −0.0029 (11) −0.0071 (11)
N2 0.0500 (14) 0.0445 (14) 0.0527 (15) −0.0180 (11) −0.0079 (11) −0.0066 (11)
N3 0.0466 (14) 0.0543 (15) 0.0451 (14) −0.0190 (11) 0.0006 (11) −0.0072 (11)
C1 0.079 (3) 0.109 (3) 0.048 (2) −0.027 (2) −0.0153 (19) −0.010 (2)
C2 0.080 (3) 0.102 (3) 0.046 (2) −0.032 (2) −0.0057 (18) −0.0088 (19)
C3 0.065 (2) 0.072 (2) 0.059 (2) −0.0299 (18) 0.0026 (17) −0.0032 (17)
C4 0.064 (2) 0.0534 (18) 0.0501 (18) −0.0241 (15) −0.0077 (15) −0.0049 (14)
C5 0.0553 (17) 0.0351 (15) 0.0422 (16) −0.0116 (12) −0.0043 (13) −0.0044 (12)
C6 0.0573 (19) 0.065 (2) 0.0533 (19) −0.0150 (16) −0.0067 (15) −0.0076 (15)
C7 0.0352 (13) 0.0419 (15) 0.0407 (15) −0.0114 (11) −0.0091 (11) −0.0023 (12)
C8 0.0351 (13) 0.0410 (14) 0.0432 (15) −0.0152 (11) −0.0133 (11) −0.0029 (11)
C9 0.0472 (16) 0.0462 (16) 0.0405 (15) −0.0140 (13) −0.0111 (12) −0.0034 (12)
C10 0.0534 (17) 0.0437 (16) 0.0510 (18) −0.0192 (13) −0.0116 (14) 0.0056 (13)
C11 0.0542 (18) 0.0402 (16) 0.061 (2) −0.0160 (13) −0.0102 (15) −0.0026 (14)
C12 0.0334 (13) 0.0409 (15) 0.0465 (16) −0.0125 (11) −0.0073 (12) −0.0038 (12)
C13 0.0311 (13) 0.0457 (16) 0.0429 (16) −0.0142 (11) −0.0040 (11) −0.0054 (12)
C14 0.0544 (18) 0.067 (2) 0.0446 (17) −0.0258 (16) 0.0040 (14) −0.0045 (15)
C15 0.0518 (17) 0.0566 (19) 0.0495 (18) −0.0250 (14) −0.0032 (14) 0.0057 (14)
C16 0.0450 (16) 0.0456 (17) 0.0511 (18) −0.0124 (13) −0.0039 (13) −0.0020 (13)
C17 0.0350 (13) 0.0431 (15) 0.0411 (15) −0.0152 (11) −0.0073 (11) −0.0021 (11)

Geometric parameters (Å, °)

N1—C7 1.269 (3) C7—C17 1.480 (4)
N1—C5 1.410 (3) C7—C8 1.500 (4)
N2—C12 1.331 (3) C8—C9 1.384 (4)
N2—C11 1.343 (4) C8—C12 1.398 (4)
N3—C13 1.333 (3) C9—C10 1.385 (4)
N3—C14 1.341 (4) C9—H9A 0.9300
C1—C2 1.380 (5) C10—C11 1.375 (4)
C1—C6 1.381 (5) C10—H10A 0.9300
C1—H1B 0.9300 C11—H11A 0.9300
C2—C3 1.369 (5) C12—C13 1.482 (4)
C2—H2B 0.9300 C13—C17 1.386 (4)
C3—C4 1.375 (4) C14—C15 1.385 (4)
C3—H3B 0.9300 C14—H14A 0.9300
C4—C5 1.385 (4) C15—C16 1.380 (4)
C4—H4A 0.9300 C15—H15A 0.9300
C5—C6 1.392 (4) C16—C17 1.379 (4)
C6—H6A 0.9300 C16—H16A 0.9300
C7—N1—C5 121.5 (2) C8—C9—C10 117.0 (3)
C12—N2—C11 114.6 (2) C8—C9—H9A 121.5
C13—N3—C14 114.1 (3) C10—C9—H9A 121.5
C2—C1—C6 120.2 (4) C11—C10—C9 120.4 (3)
C2—C1—H1B 119.9 C11—C10—H10A 119.8
C6—C1—H1B 119.9 C9—C10—H10A 119.8
C3—C2—C1 119.6 (3) N2—C11—C10 124.1 (3)
C3—C2—H2B 120.2 N2—C11—H11A 117.9
C1—C2—H2B 120.2 C10—C11—H11A 117.9
C2—C3—C4 121.2 (3) N2—C12—C8 125.8 (3)
C2—C3—H3B 119.4 N2—C12—C13 125.6 (2)
C4—C3—H3B 119.4 C8—C12—C13 108.6 (2)
C3—C4—C5 119.6 (3) N3—C13—C17 125.4 (3)
C3—C4—H4A 120.2 N3—C13—C12 126.3 (2)
C5—C4—H4A 120.2 C17—C13—C12 108.3 (2)
C4—C5—C6 119.6 (3) N3—C14—C15 124.7 (3)
C4—C5—N1 120.3 (3) N3—C14—H14A 117.6
C6—C5—N1 119.8 (3) C15—C14—H14A 117.6
C1—C6—C5 119.9 (3) C16—C15—C14 119.8 (3)
C1—C6—H6A 120.1 C16—C15—H15A 120.1
C5—C6—H6A 120.1 C14—C15—H15A 120.1
N1—C7—C17 122.3 (2) C17—C16—C15 116.6 (3)
N1—C7—C8 132.7 (2) C17—C16—H16A 121.7
C17—C7—C8 105.0 (2) C15—C16—H16A 121.7
C9—C8—C12 118.0 (2) C16—C17—C13 119.3 (3)
C9—C8—C7 133.7 (2) C16—C17—C7 130.9 (3)
C12—C8—C7 108.3 (2) C13—C17—C7 109.7 (2)
C6—C1—C2—C3 −0.1 (6) C9—C8—C12—N2 0.9 (4)
C1—C2—C3—C4 0.5 (6) C7—C8—C12—N2 179.7 (2)
C2—C3—C4—C5 0.2 (5) C9—C8—C12—C13 −179.9 (2)
C3—C4—C5—C6 −1.3 (5) C7—C8—C12—C13 −1.1 (3)
C3—C4—C5—N1 −175.0 (3) C14—N3—C13—C17 −0.7 (4)
C7—N1—C5—C4 −75.0 (4) C14—N3—C13—C12 177.4 (3)
C7—N1—C5—C6 111.3 (3) N2—C12—C13—N3 1.2 (4)
C2—C1—C6—C5 −1.0 (6) C8—C12—C13—N3 −177.9 (2)
C4—C5—C6—C1 1.7 (5) N2—C12—C13—C17 179.7 (2)
N1—C5—C6—C1 175.5 (3) C8—C12—C13—C17 0.5 (3)
C5—N1—C7—C17 174.9 (2) C13—N3—C14—C15 0.2 (4)
C5—N1—C7—C8 −4.7 (5) N3—C14—C15—C16 0.4 (5)
N1—C7—C8—C9 −0.6 (5) C14—C15—C16—C17 −0.4 (4)
C17—C7—C8—C9 179.8 (3) C15—C16—C17—C13 0.0 (4)
N1—C7—C8—C12 −179.1 (3) C15—C16—C17—C7 −177.7 (3)
C17—C7—C8—C12 1.2 (3) N3—C13—C17—C16 0.7 (4)
C12—C8—C9—C10 −0.3 (4) C12—C13—C17—C16 −177.8 (2)
C7—C8—C9—C10 −178.7 (3) N3—C13—C17—C7 178.8 (2)
C8—C9—C10—C11 −0.3 (4) C12—C13—C17—C7 0.3 (3)
C12—N2—C11—C10 0.3 (4) N1—C7—C17—C16 −2.9 (4)
C9—C10—C11—N2 0.3 (5) C8—C7—C17—C16 176.9 (3)
C11—N2—C12—C8 −0.9 (4) N1—C7—C17—C13 179.3 (2)
C11—N2—C12—C13 −180.0 (2) C8—C7—C17—C13 −1.0 (3)

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HK2468).

References

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  4. Glagovich, N. M., Reed, E. M., Crundwell, G., Updegraff, J. B. III, Zeller, M. & Hunter, A. D. (2004b). Acta Cryst. E60, o1269–o1270.
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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 datablocks I, global. DOI: 10.1107/S1600536808016668/hk2468sup1.cif

e-64-o1221-sup1.cif (17.4KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808016668/hk2468Isup2.hkl

e-64-o1221-Isup2.hkl (114.3KB, hkl)

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


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