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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Dec 3;65(Pt 1):o6. doi: 10.1107/S1600536808039627

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

Hui Cang a, Dong Jin b, Si-Qing Wang a, Bin Xu a, Jin-Tang Wang a,*
PMCID: PMC2967858  PMID: 21581701

Abstract

In the mol­ecule of the title compound, C18H13N3, the 4,5-diaza­fluorenyl­idene unit is nearly planar and is oriented at a dihedral angle of 66.31 (1)° with respect to the benzene ring. In the crystal structure, mol­ecules are stacked regularly along the c axis.

Related literature

For the photochemical properties of 4-methyl-N-(4,5-diaza­fluorenyl­idene)benzenamine, see: Wang & Rillema (1997). For related structures, see: Glagovich et al. (2004a ,b ); Peters et al. (1998); Wang et al. (2006).graphic file with name e-65-000o6-scheme1.jpg

Experimental

Crystal data

  • C18H13N3

  • M r = 271.31

  • Triclinic, Inline graphic

  • a = 7.5970 (15) Å

  • b = 8.6100 (17) Å

  • c = 10.998 (2) Å

  • α = 77.11 (3)°

  • β = 87.48 (3)°

  • γ = 85.79 (3)°

  • V = 699.1 (2) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 293 (2) K

  • 0.30 × 0.20 × 0.20 mm

Data collection

  • Enraf–Nonius CAD-4 diffractometer

  • Absorption correction: ψ scan (North et al., 1968) T min = 0.977, T max = 0.985

  • 2742 measured reflections

  • 2534 independent reflections

  • 1829 reflections with I > 2σ(I)

  • R int = 0.025

  • 3 standard reflections every 200 reflections intensity decay: none

Refinement

  • R[F 2 > 2σ(F 2)] = 0.058

  • wR(F 2) = 0.167

  • S = 1.00

  • 2534 reflections

  • 190 parameters

  • H-atom parameters constrained

  • Δρmax = 0.50 e Å−3

  • Δρmin = −0.28 e Å−3

Data collection: CAD-4 Software (Enraf–Nonius, 1985); 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/S1600536808039627/bx2187sup1.cif

e-65-000o6-sup1.cif (18KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808039627/bx2187Isup2.hkl

e-65-000o6-Isup2.hkl (124.4KB, 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

4-Methyl-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), Fig. 1.The bond lengths and angles are comparable with the solvated form (II), and with other fluorenylidene compounds : 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). The coplanar ring system is oriented with respect to benzene ring at a dihedral angle of 66.31 (1)°.In the crystal of the title compound, no obvious hydrogen bond is observed, and molecules are stacked regularly along c axis, Fig. 2.

Experimental

The title compound was synthesized by a method reported in literature (Wang & Rillema, 1997). The crystals were obtained by dissolving compound (I) (2.0 g, 6.3 mmol) into solution of acetic ether (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 O—H = 0.82 and C—H = 0.93Å for aromatic H, and constrained to ride on their parent atoms, with Uiso(H) = xUeq(C/O), where x = 1.2 for aromatic H and x = 1.5 for other H.

Figures

Fig. 1.

Fig. 1.

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

Fig. 2.

Fig. 2.

A packing diagram for (I).

Crystal data

C18H13N3 Z = 2
Mr = 271.31 F(000) = 284
Triclinic, P1 Dx = 1.289 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 7.5970 (15) Å Cell parameters from 25 reflections
b = 8.6100 (17) Å θ = 10–13°
c = 10.998 (2) Å µ = 0.08 mm1
α = 77.11 (3)° T = 293 K
β = 87.48 (3)° Plate, yellow
γ = 85.79 (3)° 0.30 × 0.20 × 0.20 mm
V = 699.1 (2) Å3

Data collection

Enraf–Nonius CAD-4 diffractometer 1829 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.026
graphite θmax = 25.3°, θmin = 1.9°
ω/2θ scans h = −9→9
Absorption correction: ψ scan (North et al., 1968) k = −9→10
Tmin = 0.977, Tmax = 0.985 l = 0→13
2742 measured reflections 3 standard reflections every 200 reflections
2534 independent reflections intensity decay: none

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)] = 0.058 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.167 H-atom parameters constrained
S = 1.00 w = 1/[σ2(Fo2) + (0.05P)2 + 0.85P] where P = (Fo2 + 2Fc2)/3
2534 reflections (Δ/σ)max < 0.001
190 parameters Δρmax = 0.50 e Å3
0 restraints Δρmin = −0.28 e Å3

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
N1 0.2577 (3) 1.3579 (3) 0.5598 (2) 0.0539 (7)
C1 0.0220 (6) 1.2134 (6) 1.0717 (3) 0.0953 (14)
H1B −0.0898 1.2705 1.0794 0.143*
H1C 0.1063 1.2457 1.1223 0.143*
H1D 0.0091 1.1008 1.0992 0.143*
N2 0.2970 (3) 0.8734 (3) 0.3984 (2) 0.0507 (6)
C2 0.0855 (5) 1.2499 (5) 0.9378 (3) 0.0658 (9)
N3 0.4535 (3) 1.1454 (3) 0.2071 (2) 0.0526 (6)
C3 0.2450 (4) 1.1836 (4) 0.8993 (3) 0.0584 (8)
H3B 0.3152 1.1156 0.9583 0.070*
C4 0.3018 (4) 1.2158 (4) 0.7759 (3) 0.0551 (8)
H4A 0.4094 1.1703 0.7528 0.066*
C5 0.1987 (4) 1.3158 (3) 0.6866 (3) 0.0501 (7)
C6 0.0411 (4) 1.3877 (4) 0.7236 (3) 0.0602 (8)
H6A −0.0268 1.4590 0.6650 0.072*
C7 −0.0137 (5) 1.3531 (5) 0.8469 (3) 0.0723 (10)
H7A −0.1203 1.4002 0.8701 0.087*
C8 0.2867 (4) 1.2521 (3) 0.4951 (2) 0.0432 (6)
C9 0.2518 (3) 1.0803 (3) 0.5183 (2) 0.0398 (6)
C10 0.1712 (4) 0.9757 (3) 0.6156 (3) 0.0463 (7)
H10A 0.1279 1.0086 0.6868 0.056*
C11 0.1576 (4) 0.8219 (4) 0.6030 (3) 0.0490 (7)
H11A 0.1044 0.7485 0.6663 0.059*
C12 0.2236 (4) 0.7763 (4) 0.4952 (3) 0.0537 (8)
H12A 0.2157 0.6705 0.4907 0.064*
C13 0.3085 (3) 1.0227 (3) 0.4114 (2) 0.0421 (6)
C14 0.3829 (3) 1.1547 (3) 0.3185 (2) 0.0429 (6)
C15 0.5163 (4) 1.2817 (4) 0.1427 (3) 0.0586 (8)
H15A 0.5670 1.2820 0.0641 0.070*
C16 0.5114 (4) 1.4213 (4) 0.1839 (3) 0.0617 (9)
H16A 0.5590 1.5111 0.1338 0.074*
C17 0.4364 (4) 1.4296 (4) 0.2994 (3) 0.0545 (8)
H17A 0.4317 1.5228 0.3292 0.065*
C18 0.3691 (4) 1.2917 (3) 0.3673 (2) 0.0457 (7)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
N1 0.0653 (17) 0.0495 (14) 0.0480 (14) 0.0060 (12) 0.0035 (12) −0.0170 (11)
C1 0.086 (3) 0.149 (4) 0.054 (2) −0.014 (3) 0.016 (2) −0.029 (2)
N2 0.0502 (15) 0.0541 (15) 0.0501 (14) 0.0092 (11) −0.0023 (11) −0.0200 (12)
C2 0.058 (2) 0.097 (3) 0.0483 (18) −0.0093 (18) 0.0060 (16) −0.0284 (18)
N3 0.0500 (15) 0.0690 (17) 0.0361 (13) 0.0112 (12) −0.0010 (11) −0.0111 (12)
C3 0.059 (2) 0.072 (2) 0.0459 (17) 0.0002 (16) −0.0022 (14) −0.0174 (15)
C4 0.0563 (19) 0.0615 (19) 0.0507 (18) 0.0054 (15) 0.0036 (14) −0.0233 (15)
C5 0.0569 (18) 0.0489 (16) 0.0487 (17) 0.0000 (13) 0.0049 (14) −0.0220 (13)
C6 0.0562 (19) 0.068 (2) 0.057 (2) 0.0105 (15) 0.0007 (15) −0.0220 (16)
C7 0.055 (2) 0.106 (3) 0.060 (2) 0.0086 (19) 0.0085 (17) −0.036 (2)
C8 0.0416 (15) 0.0473 (15) 0.0401 (15) 0.0086 (12) −0.0030 (12) −0.0117 (12)
C9 0.0340 (14) 0.0480 (15) 0.0382 (14) 0.0065 (11) −0.0050 (11) −0.0135 (12)
C10 0.0424 (15) 0.0585 (18) 0.0401 (15) 0.0051 (13) −0.0046 (12) −0.0171 (13)
C11 0.0469 (17) 0.0540 (18) 0.0452 (16) 0.0011 (13) −0.0054 (13) −0.0096 (13)
C12 0.0573 (19) 0.0476 (17) 0.0589 (19) 0.0029 (14) −0.0046 (15) −0.0186 (15)
C13 0.0368 (15) 0.0523 (16) 0.0375 (14) 0.0120 (12) −0.0069 (11) −0.0142 (12)
C14 0.0348 (14) 0.0567 (17) 0.0363 (14) 0.0108 (12) −0.0068 (11) −0.0116 (12)
C15 0.0571 (19) 0.081 (2) 0.0335 (15) 0.0107 (17) 0.0004 (13) −0.0087 (15)
C16 0.062 (2) 0.074 (2) 0.0424 (17) 0.0018 (16) −0.0010 (15) −0.0003 (15)
C17 0.0590 (19) 0.0542 (18) 0.0468 (17) 0.0046 (14) −0.0015 (14) −0.0062 (14)
C18 0.0436 (16) 0.0542 (17) 0.0366 (14) 0.0103 (12) −0.0056 (12) −0.0078 (12)

Geometric parameters (Å, °)

N1—C8 1.277 (3) C7—H7A 0.9300
N1—C5 1.422 (4) C8—C9 1.486 (4)
C1—C2 1.501 (5) C8—C18 1.491 (4)
C1—H1B 0.9600 C9—C10 1.387 (4)
C1—H1C 0.9600 C9—C13 1.414 (4)
C1—H1D 0.9600 C10—C11 1.373 (4)
N2—C12 1.327 (4) C10—H10A 0.9300
N2—C13 1.334 (4) C11—C12 1.392 (4)
C2—C7 1.388 (5) C11—H11A 0.9300
C2—C3 1.391 (5) C12—H12A 0.9300
N3—C14 1.332 (3) C13—C14 1.477 (4)
N3—C15 1.337 (4) C14—C18 1.397 (4)
C3—C4 1.380 (4) C15—C16 1.374 (5)
C3—H3B 0.9300 C15—H15A 0.9300
C4—C5 1.382 (4) C16—C17 1.383 (4)
C4—H4A 0.9300 C16—H16A 0.9300
C5—C6 1.394 (4) C17—C18 1.375 (4)
C6—C7 1.374 (4) C17—H17A 0.9300
C6—H6A 0.9300
C8—N1—C5 121.0 (3) C10—C9—C13 117.7 (3)
C2—C1—H1B 109.5 C10—C9—C8 133.8 (2)
C2—C1—H1C 109.5 C13—C9—C8 108.3 (2)
H1B—C1—H1C 109.5 C11—C10—C9 117.7 (3)
C2—C1—H1D 109.5 C11—C10—H10A 121.2
H1B—C1—H1D 109.5 C9—C10—H10A 121.2
H1C—C1—H1D 109.5 C10—C11—C12 119.8 (3)
C12—N2—C13 115.1 (2) C10—C11—H11A 120.1
C7—C2—C3 117.2 (3) C12—C11—H11A 120.1
C7—C2—C1 120.8 (3) N2—C12—C11 124.6 (3)
C3—C2—C1 122.0 (4) N2—C12—H12A 117.7
C14—N3—C15 114.0 (3) C11—C12—H12A 117.7
C4—C3—C2 121.8 (3) N2—C13—C9 125.1 (3)
C4—C3—H3B 119.1 N2—C13—C14 126.4 (2)
C2—C3—H3B 119.1 C9—C13—C14 108.5 (2)
C3—C4—C5 119.9 (3) N3—C14—C18 125.3 (3)
C3—C4—H4A 120.0 N3—C14—C13 126.1 (3)
C5—C4—H4A 120.0 C18—C14—C13 108.6 (2)
C4—C5—C6 119.2 (3) N3—C15—C16 124.8 (3)
C4—C5—N1 121.3 (3) N3—C15—H15A 117.6
C6—C5—N1 119.3 (3) C16—C15—H15A 117.6
C7—C6—C5 119.9 (3) C15—C16—C17 120.6 (3)
C7—C6—H6A 120.1 C15—C16—H16A 119.7
C5—C6—H6A 120.1 C17—C16—H16A 119.7
C6—C7—C2 121.9 (3) C18—C17—C16 115.9 (3)
C6—C7—H7A 119.1 C18—C17—H17A 122.0
C2—C7—H7A 119.1 C16—C17—H17A 122.0
N1—C8—C9 133.1 (3) C17—C18—C14 119.4 (3)
N1—C8—C18 121.3 (3) C17—C18—C8 131.6 (3)
C9—C8—C18 105.6 (2) C14—C18—C8 108.9 (2)
C7—C2—C3—C4 −1.2 (5) C12—N2—C13—C14 −179.6 (3)
C1—C2—C3—C4 179.2 (3) C10—C9—C13—N2 −2.8 (4)
C2—C3—C4—C5 −0.4 (5) C8—C9—C13—N2 −179.6 (2)
C3—C4—C5—C6 2.5 (5) C10—C9—C13—C14 177.7 (2)
C3—C4—C5—N1 176.7 (3) C8—C9—C13—C14 0.8 (3)
C8—N1—C5—C4 63.1 (4) C15—N3—C14—C18 1.2 (4)
C8—N1—C5—C6 −122.7 (3) C15—N3—C14—C13 −178.0 (3)
C4—C5—C6—C7 −2.9 (5) N2—C13—C14—N3 −1.2 (4)
N1—C5—C6—C7 −177.3 (3) C9—C13—C14—N3 178.4 (2)
C5—C6—C7—C2 1.3 (6) N2—C13—C14—C18 179.5 (3)
C3—C2—C7—C6 0.7 (6) C9—C13—C14—C18 −1.0 (3)
C1—C2—C7—C6 −179.7 (4) C14—N3—C15—C16 0.0 (4)
C5—N1—C8—C9 8.7 (5) N3—C15—C16—C17 −0.6 (5)
C5—N1—C8—C18 −172.5 (3) C15—C16—C17—C18 −0.1 (4)
N1—C8—C9—C10 2.4 (5) C16—C17—C18—C14 1.2 (4)
C18—C8—C9—C10 −176.5 (3) C16—C17—C18—C8 177.0 (3)
N1—C8—C9—C13 178.6 (3) N3—C14—C18—C17 −1.9 (4)
C18—C8—C9—C13 −0.3 (3) C13—C14—C18—C17 177.4 (2)
C13—C9—C10—C11 2.2 (4) N3—C14—C18—C8 −178.6 (2)
C8—C9—C10—C11 178.1 (3) C13—C14—C18—C8 0.7 (3)
C9—C10—C11—C12 0.0 (4) N1—C8—C18—C17 4.5 (5)
C13—N2—C12—C11 1.5 (4) C9—C8—C18—C17 −176.4 (3)
C10—C11—C12—N2 −2.0 (5) N1—C8—C18—C14 −179.3 (3)
C12—N2—C13—C9 0.9 (4) C9—C8—C18—C14 −0.3 (3)

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BX2187).

References

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  3. Glagovich, N. M., Reed, E. M., Crundwell, G., Updegraff, J. B. III, Zeller, M. & Hunter, A. D. (2004b). Acta Cryst. E60, o1269–o1270.
  4. Harms, K. & Wocadlo, S. (1995). XCAD4 University of Marburg, Germany.
  5. North, A. C. T., Phillips, D. C. & Mathews, F. S. (1968). Acta Cryst. A24, 351–359.
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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/S1600536808039627/bx2187sup1.cif

e-65-000o6-sup1.cif (18KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808039627/bx2187Isup2.hkl

e-65-000o6-Isup2.hkl (124.4KB, hkl)

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


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