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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Mar 28;68(Pt 4):o1210. doi: 10.1107/S1600536812012299

4-(Anthracen-9-yl)-2-phenyl-6-(pyridin-2-yl)pyridine

Hao-Wei Wang a, Jun Ren a, Wen-Bo Ye a, Jia-Xiang Yang a,*
PMCID: PMC3344146  PMID: 22606149

Abstract

In the title compound, C30H20N2, the anthracene ring system is approximately planar [maximum deviation = 0.035 (2) Å] and is nearly perpendicular to the central pyridine ring, making a dihedral angle of 75.73 (7)°. The terminal pyridine ring and the phenyl ring are oriented at dihedral angles of 8.11 (10) and 13.22 (10)°, respectively, to the central pyridine ring.

Related literature  

For applications of aromatic conjugated organic compounds, see: Nishihara et al. (1989); Mi et al. (2003); Roberto et al. (2000).graphic file with name e-68-o1210-scheme1.jpg

Experimental  

Crystal data  

  • C30H20N2

  • M r = 408.48

  • Monoclinic, Inline graphic

  • a = 12.6420 (3) Å

  • b = 14.8499 (4) Å

  • c = 11.8707 (3) Å

  • β = 104.006 (2)°

  • V = 2162.26 (9) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.07 mm−1

  • T = 298 K

  • 0.2 × 0.2 × 0.2 mm

Data collection  

  • Bruker SMART 1000 CCD area-detector diffractometer

  • 35644 measured reflections

  • 4951 independent reflections

  • 3128 reflections with I > 2σ(I)

  • R int = 0.038

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.063

  • wR(F 2) = 0.215

  • S = 1.33

  • 4951 reflections

  • 289 parameters

  • H-atom parameters constrained

  • Δρmax = 0.20 e Å−3

  • Δρmin = −0.20 e Å−3

Data collection: SMART (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812012299/xu5476sup1.cif

e-68-o1210-sup1.cif (19KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812012299/xu5476Isup2.hkl

e-68-o1210-Isup2.hkl (242.5KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812012299/xu5476Isup3.cml

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

Acknowledgments

The work was supported by the National Natural Science Foundation of China (50873001, 21071001) and the Education Committee of Anhui Province, China (KJ2011Z338).

supplementary crystallographic information

Comment

The aromatic conjugated organic compounds are investigated with great interest due to their potential applications in optical image processing, all-optical switching, organic light emitting diodes (OLEDs) and integrated optical devices (Nishihara et al., 1989; Mi et al., 2003; Roberto et al., 2000). As a part of our continuing studies of the synthesis and characterization of optical materials, we have prepared a new anthracene derivative containing two pyridine rings and investigated its crystal structure.

The molecule structure of (I) is shown in Fig. 1. Two pyridine rings makes the dihedral angle of 8.11 (10)°. The anthracen moiety is almost planar, and make the dihedral angles of 75.73 (7)° and 67.84 (2)° with two pyridine rings, respectively.

Experimental

3-(Anthracen-9-yl)-1-phenylprop-2-en-1-one (1.54 g, 5.0 mmol), 2-acetylpyridine (1.82 g, 15 mmol) and NaOH (0.20 g, 5.0 mmol) were crashed together with a pestle and mortar for 3 h. The light yellow powder was added to a stirred solution of ammonium acetate (15.4 g, 200.0 mmol) in ethanol (200 ml). The reaction mixture was heated at reflux. Thin layer chromatography analysis tracking reaction, evaporated solvent, extracted with dichloromethane, and dried to afford the product. It was purified by flash column chromatography on silica. Elution with petroleum/ethyl acetate (10:1) gave a white solid (yield; 1.3 g, 65%). Single crystals of (I) were grown by slow evaporation of a dichloromethane/ethyl acetate (1:1) solution.

Refinement

H atoms were positioned geometrically with C—H = 0.93 Å 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

C30H20N2 F(000) = 856
Mr = 408.48 Dx = 1.255 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 5640 reflections
a = 12.6420 (3) Å θ = 2.2–22.7°
b = 14.8499 (4) Å µ = 0.07 mm1
c = 11.8707 (3) Å T = 298 K
β = 104.006 (2)° Block, pale yellow
V = 2162.26 (9) Å3 0.2 × 0.2 × 0.2 mm
Z = 4

Data collection

Bruker SMART 1000 CCD area-detector diffractometer 3128 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.038
Graphite monochromator θmax = 27.5°, θmin = 2.2°
φ and ω scans h = −16→16
35644 measured reflections k = −19→17
4951 independent reflections l = −15→15

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)] = 0.063 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.215 H-atom parameters constrained
S = 1.33 w = 1/[σ2(Fo2) + (0.1P)2] where P = (Fo2 + 2Fc2)/3
4951 reflections (Δ/σ)max < 0.001
289 parameters Δρmax = 0.20 e Å3
0 restraints Δρmin = −0.20 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 0.56725 (12) 0.37331 (10) 0.11808 (12) 0.0487 (4)
C18 0.64872 (14) 0.37932 (12) 0.21431 (15) 0.0488 (5)
C20 0.47454 (15) 0.29870 (13) −0.05928 (15) 0.0509 (5)
C10 0.82717 (15) 0.18045 (13) 0.18202 (16) 0.0529 (5)
N2 0.71173 (15) 0.45087 (13) 0.40278 (15) 0.0651 (5)
C16 0.65564 (15) 0.24508 (14) 0.05996 (16) 0.0533 (5)
H16 0.6560 0.2001 0.0056 0.064*
C17 0.57066 (15) 0.30714 (13) 0.04214 (15) 0.0481 (5)
C6 0.82357 (16) 0.11106 (13) 0.26209 (17) 0.0551 (5)
C9 0.90771 (15) 0.18139 (13) 0.11945 (17) 0.0547 (5)
C15 0.73990 (14) 0.25080 (13) 0.15945 (17) 0.0522 (5)
C5 0.90315 (17) 0.04023 (14) 0.27789 (19) 0.0619 (6)
C30 0.47702 (17) 0.24029 (15) −0.14691 (16) 0.0588 (5)
H30 0.5407 0.2087 −0.1464 0.071*
C25 0.63672 (15) 0.44908 (12) 0.29968 (16) 0.0479 (4)
C8 0.98524 (16) 0.10877 (15) 0.13417 (18) 0.0612 (6)
C19 0.73694 (15) 0.31995 (13) 0.23649 (17) 0.0547 (5)
H19 0.7933 0.3269 0.3027 0.066*
C1 0.74384 (18) 0.10684 (15) 0.32911 (19) 0.0646 (6)
H1 0.6908 0.1515 0.3199 0.078*
C29 0.69808 (19) 0.51083 (16) 0.48382 (18) 0.0668 (6)
H29 0.7490 0.5117 0.5550 0.080*
C7 0.98102 (17) 0.04122 (15) 0.2135 (2) 0.0675 (6)
H7 1.0322 −0.0050 0.2239 0.081*
C13 0.99391 (19) 0.24831 (18) −0.0222 (2) 0.0722 (6)
H13 0.9983 0.2948 −0.0733 0.087*
C14 0.91720 (17) 0.25100 (16) 0.03936 (18) 0.0634 (6)
H14 0.8692 0.2994 0.0294 0.076*
C26 0.54987 (18) 0.50785 (16) 0.2783 (2) 0.0708 (6)
H26 0.4988 0.5066 0.2072 0.085*
C24 0.38033 (18) 0.34689 (19) −0.06388 (19) 0.0791 (7)
H24 0.3781 0.3885 −0.0060 0.095*
C4 0.8981 (2) −0.02999 (16) 0.3592 (2) 0.0798 (7)
H4 0.9490 −0.0764 0.3699 0.096*
C28 0.6140 (2) 0.56951 (17) 0.4665 (2) 0.0732 (7)
H28 0.6075 0.6099 0.5243 0.088*
C2 0.7437 (2) 0.03950 (17) 0.4056 (2) 0.0762 (7)
H2 0.6917 0.0391 0.4491 0.091*
C12 1.0679 (2) 0.1750 (2) −0.0096 (2) 0.0813 (7)
H12 1.1196 0.1728 −0.0536 0.098*
C11 1.06313 (19) 0.10878 (18) 0.0663 (2) 0.0780 (7)
H11 1.1126 0.0615 0.0744 0.094*
C3 0.8214 (2) −0.03005 (19) 0.4202 (2) 0.0858 (8)
H3 0.8197 −0.0764 0.4724 0.103*
C27 0.5389 (2) 0.56830 (18) 0.3625 (2) 0.0873 (8)
H27 0.4805 0.6082 0.3485 0.105*
C22 0.2928 (2) 0.2736 (2) −0.2388 (2) 0.0911 (9)
H22 0.2314 0.2637 −0.2989 0.109*
C21 0.3868 (2) 0.22766 (18) −0.23564 (19) 0.0789 (7)
H21 0.3896 0.1872 −0.2947 0.095*
C23 0.2893 (2) 0.3338 (2) −0.1538 (2) 0.1001 (10)
H23 0.2258 0.3662 −0.1561 0.120*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
N1 0.0500 (9) 0.0484 (10) 0.0466 (8) 0.0047 (7) 0.0096 (7) 0.0033 (7)
C18 0.0479 (10) 0.0460 (11) 0.0515 (10) 0.0006 (8) 0.0099 (8) 0.0042 (8)
C20 0.0507 (11) 0.0549 (12) 0.0459 (9) 0.0089 (8) 0.0092 (8) 0.0081 (9)
C10 0.0471 (10) 0.0473 (11) 0.0576 (10) 0.0069 (8) −0.0006 (8) −0.0051 (9)
N2 0.0652 (11) 0.0657 (12) 0.0604 (10) 0.0019 (9) 0.0072 (8) −0.0023 (9)
C16 0.0526 (11) 0.0504 (12) 0.0537 (10) 0.0086 (8) 0.0069 (8) −0.0021 (9)
C17 0.0492 (10) 0.0491 (11) 0.0455 (9) 0.0037 (8) 0.0105 (8) 0.0064 (8)
C6 0.0487 (10) 0.0481 (12) 0.0603 (11) 0.0038 (8) −0.0028 (8) −0.0032 (9)
C9 0.0477 (10) 0.0511 (12) 0.0578 (11) 0.0050 (8) −0.0021 (8) −0.0067 (9)
C15 0.0483 (10) 0.0449 (11) 0.0603 (11) 0.0059 (8) 0.0069 (8) 0.0028 (9)
C5 0.0532 (12) 0.0502 (12) 0.0728 (13) 0.0069 (9) −0.0032 (10) −0.0010 (10)
C30 0.0584 (12) 0.0651 (13) 0.0499 (10) 0.0119 (10) 0.0073 (9) −0.0045 (10)
C25 0.0503 (10) 0.0412 (10) 0.0519 (10) −0.0012 (8) 0.0116 (8) 0.0042 (8)
C8 0.0476 (11) 0.0617 (14) 0.0687 (13) 0.0084 (9) 0.0031 (9) −0.0096 (11)
C19 0.0495 (10) 0.0497 (12) 0.0583 (11) 0.0041 (8) 0.0001 (8) 0.0009 (9)
C1 0.0580 (12) 0.0584 (14) 0.0726 (13) 0.0030 (10) 0.0064 (10) 0.0001 (11)
C29 0.0793 (15) 0.0669 (15) 0.0522 (11) −0.0039 (11) 0.0117 (10) −0.0084 (10)
C7 0.0564 (12) 0.0540 (13) 0.0845 (15) 0.0153 (10) 0.0024 (11) 0.0009 (11)
C13 0.0628 (13) 0.0835 (17) 0.0662 (13) −0.0037 (12) 0.0080 (11) 0.0032 (12)
C14 0.0548 (12) 0.0640 (14) 0.0648 (12) 0.0050 (10) 0.0017 (10) −0.0022 (11)
C26 0.0701 (14) 0.0677 (15) 0.0673 (13) 0.0178 (11) 0.0026 (10) −0.0121 (11)
C24 0.0676 (15) 0.1003 (19) 0.0601 (12) 0.0295 (13) −0.0026 (10) −0.0151 (13)
C4 0.0747 (16) 0.0581 (15) 0.0971 (17) 0.0133 (12) 0.0022 (14) 0.0174 (13)
C28 0.0850 (16) 0.0680 (15) 0.0690 (14) 0.0044 (12) 0.0233 (12) −0.0180 (12)
C2 0.0725 (15) 0.0716 (16) 0.0825 (15) −0.0037 (12) 0.0151 (12) 0.0121 (13)
C12 0.0626 (14) 0.099 (2) 0.0828 (16) 0.0047 (14) 0.0188 (12) −0.0051 (15)
C11 0.0585 (13) 0.0804 (17) 0.0913 (17) 0.0164 (12) 0.0109 (12) −0.0061 (15)
C3 0.0856 (18) 0.0694 (17) 0.0977 (18) −0.0010 (13) 0.0133 (15) 0.0244 (14)
C27 0.0881 (18) 0.0794 (18) 0.0926 (18) 0.0285 (14) 0.0182 (14) −0.0137 (15)
C22 0.0741 (17) 0.128 (2) 0.0582 (13) 0.0138 (16) −0.0095 (12) −0.0087 (15)
C21 0.0836 (17) 0.0906 (18) 0.0563 (12) 0.0096 (14) 0.0047 (11) −0.0143 (12)
C23 0.0695 (16) 0.150 (3) 0.0691 (15) 0.0432 (17) −0.0065 (12) −0.0183 (17)

Geometric parameters (Å, º)

N1—C17 1.341 (2) C1—H1 0.9300
N1—C18 1.343 (2) C29—C28 1.351 (3)
C18—C19 1.396 (3) C29—H29 0.9300
C18—C25 1.482 (3) C7—H7 0.9300
C20—C30 1.361 (3) C13—C14 1.349 (3)
C20—C24 1.379 (3) C13—C12 1.420 (4)
C20—C17 1.494 (2) C13—H13 0.9300
C10—C9 1.398 (3) C14—H14 0.9300
C10—C6 1.410 (3) C26—C27 1.375 (3)
C10—C15 1.496 (3) C26—H26 0.9300
N2—C29 1.352 (3) C24—C23 1.381 (3)
N2—C25 1.355 (2) C24—H24 0.9300
C16—C15 1.388 (2) C4—C3 1.344 (4)
C16—C17 1.392 (3) C4—H4 0.9300
C16—H16 0.9300 C28—C27 1.363 (3)
C6—C1 1.429 (3) C28—H28 0.9300
C6—C5 1.436 (3) C2—C3 1.407 (4)
C9—C14 1.429 (3) C2—H2 0.9300
C9—C8 1.439 (3) C12—C11 1.345 (4)
C15—C19 1.382 (3) C12—H12 0.9300
C5—C7 1.385 (3) C11—H11 0.9300
C5—C4 1.433 (3) C3—H3 0.9300
C30—C21 1.365 (3) C27—H27 0.9300
C30—H30 0.9300 C22—C23 1.357 (4)
C25—C26 1.377 (3) C22—C21 1.363 (4)
C8—C7 1.386 (3) C22—H22 0.9300
C8—C11 1.415 (3) C21—H21 0.9300
C19—H19 0.9300 C23—H23 0.9300
C1—C2 1.351 (3)
C17—N1—C18 118.52 (15) N2—C29—H29 118.4
N1—C18—C19 122.12 (17) C5—C7—C8 122.16 (19)
N1—C18—C25 116.33 (16) C5—C7—H7 118.9
C19—C18—C25 121.45 (16) C8—C7—H7 118.9
C30—C20—C24 118.68 (18) C14—C13—C12 120.5 (2)
C30—C20—C17 120.31 (17) C14—C13—H13 119.8
C24—C20—C17 120.95 (18) C12—C13—H13 119.8
C9—C10—C6 120.79 (17) C13—C14—C9 121.8 (2)
C9—C10—C15 119.89 (18) C13—C14—H14 119.1
C6—C10—C15 119.23 (19) C9—C14—H14 119.1
C29—N2—C25 118.27 (18) C27—C26—C25 119.7 (2)
C15—C16—C17 119.58 (18) C27—C26—H26 120.1
C15—C16—H16 120.2 C25—C26—H26 120.1
C17—C16—H16 120.2 C20—C24—C23 120.5 (2)
N1—C17—C16 122.14 (16) C20—C24—H24 119.7
N1—C17—C20 116.79 (16) C23—C24—H24 119.7
C16—C17—C20 120.93 (17) C3—C4—C5 121.3 (2)
C10—C6—C1 123.35 (18) C3—C4—H4 119.4
C10—C6—C5 119.2 (2) C5—C4—H4 119.4
C1—C6—C5 117.49 (19) C29—C28—C27 118.6 (2)
C10—C9—C14 123.36 (18) C29—C28—H28 120.7
C10—C9—C8 119.35 (19) C27—C28—H28 120.7
C14—C9—C8 117.3 (2) C1—C2—C3 120.8 (3)
C19—C15—C16 118.06 (16) C1—C2—H2 119.6
C19—C15—C10 122.51 (16) C3—C2—H2 119.6
C16—C15—C10 119.37 (17) C11—C12—C13 119.7 (2)
C7—C5—C4 122.2 (2) C11—C12—H12 120.1
C7—C5—C6 119.3 (2) C13—C12—H12 120.1
C4—C5—C6 118.5 (2) C12—C11—C8 122.1 (2)
C20—C30—C21 120.5 (2) C12—C11—H11 118.9
C20—C30—H30 119.7 C8—C11—H11 118.9
C21—C30—H30 119.7 C4—C3—C2 120.4 (2)
N2—C25—C26 120.42 (18) C4—C3—H3 119.8
N2—C25—C18 117.79 (16) C2—C3—H3 119.8
C26—C25—C18 121.73 (17) C28—C27—C26 119.7 (2)
C7—C8—C11 122.3 (2) C28—C27—H27 120.1
C7—C8—C9 119.2 (2) C26—C27—H27 120.1
C11—C8—C9 118.6 (2) C23—C22—C21 119.6 (2)
C15—C19—C18 119.54 (16) C23—C22—H22 120.2
C15—C19—H19 120.2 C21—C22—H22 120.2
C18—C19—H19 120.2 C22—C21—C30 120.8 (2)
C2—C1—C6 121.5 (2) C22—C21—H21 119.6
C2—C1—H1 119.3 C30—C21—H21 119.6
C6—C1—H1 119.3 C22—C23—C24 119.8 (2)
C28—C29—N2 123.2 (2) C22—C23—H23 120.1
C28—C29—H29 118.4 C24—C23—H23 120.1

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: XU5476).

References

  1. Bruker (2007). SMART and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  2. Mi, B.-X., Wang, P.-F., Liu, M.-W., Kwong, H.-L., Wong, N.-B., Lee, C.-S. & Lee, S.-T. (2003). Chem. Mater. 15, 3148–3151.
  3. Nishihara, H., Haruna, M. & Suhara, T. (1989). In Optical Intergrated Circuits New York: McGraw–Hill.
  4. Roberto, D., Ugo, R., Bruni, S., Cariati, E., Cariati, F., Fantucci, P., Invernizzi, I., Quici, S., Ledoux, I. & Zyss, J. (2000). Organometallics, 19, 1775–1788.
  5. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]

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) I, global. DOI: 10.1107/S1600536812012299/xu5476sup1.cif

e-68-o1210-sup1.cif (19KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812012299/xu5476Isup2.hkl

e-68-o1210-Isup2.hkl (242.5KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812012299/xu5476Isup3.cml

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


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