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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Jun 30;68(Pt 7):o2297. doi: 10.1107/S1600536812029261

2-[4-(Azido­meth­yl)phen­yl]benzonitrile

Bo Peng a,*
PMCID: PMC3394073  PMID: 22798938

Abstract

The title compound, C14H10N4, was obtained by a reaction of 4′-(bromo­meth­yl)biphenyl-2-carbonitrile and sodium azide. The dihedral angle between the benzene rings is 46.41 (7)°. Weak inter­molecular C—H⋯π inter­actions occur in the crystal.

Related literature  

For background literature, see: Haertling (1999); Homes et al. (2001).graphic file with name e-68-o2297-scheme1.jpg

Experimental  

Crystal data  

  • C14H10N4

  • M r = 234.26

  • Triclinic, Inline graphic

  • a = 8.0763 (16) Å

  • b = 8.2183 (16) Å

  • c = 10.116 (2) Å

  • α = 76.22 (3)°

  • β = 69.36 (3)°

  • γ = 85.94 (3)°

  • V = 610.2 (2) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 293 K

  • 0.20 × 0.20 × 0.20 mm

Data collection  

  • Rigaku Mercury2 diffractometer

  • 6204 measured reflections

  • 2748 independent reflections

  • 1559 reflections with I > 2σ(I)

  • R int = 0.035

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.058

  • wR(F 2) = 0.146

  • S = 1.02

  • 2748 reflections

  • 163 parameters

  • H-atom parameters constrained

  • Δρmax = 0.14 e Å−3

  • Δρmin = −0.21 e Å−3

Data collection: CrystalClear (Rigaku, 2005); cell refinement: CrystalClear; data reduction: CrystalClear; 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 datablock(s) I, global. DOI: 10.1107/S1600536812029261/xu5575sup1.cif

e-68-o2297-sup1.cif (14.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812029261/xu5575Isup2.hkl

e-68-o2297-Isup2.hkl (134.9KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812029261/xu5575Isup3.cml

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

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

Cg is the centroid of the C7–C12 benzene ring.

D—H⋯A D—H H⋯A DA D—H⋯A
C14—H14BCg i 0.97 2.75 3.642 (3) 154

Symmetry code: (i) Inline graphic.

supplementary crystallographic information

Comment

At present, much attention in ferroelectric material field is focused on developing ferroelectric pure organic or inorganic compounds (Haertling et al. 1999; Homes et al. 2001). In order to find more dielectric ferroelectric materials, we investigate the physical properties of the title compound(Fig. 1). The dielectric constant of the title compound as a function of temperature indicates that the permittivity is basically temperature-independent (dielectric constant equaling to 3.5 to 4.8), suggesting that this compound should be not a real ferroelectrics or there may be no distinct phase transition occurred within the measured temperature range. Similarly, below the melting point (373 K) of the compound, the dielectric constant as a function of temperature also goes smoothly, and there is no dielectric anomaly observed (dielectric constant equaling to 3.5 to 4.8).Herein, we report the synthesis and crystal structure of the title compound, 2-[4-(azidomethyl)phenyl]benzonitrile.

Molecules of the title compound have normal geometric parameters. The bond lengths and angles are within their normal ranges. All benzene rings are planar and the azide group is linear.The dihedral angle between the benzene rings in the molecule is 46.41 (7). Dipole–dipole and van der Waals interactions are effective in the molecular packing.

Experimental

To a stirred solution of 4'-(bromomethyl)biphenyl-2-carbonitrile (5.42 g, 0.02 mol) in 30 mL of methanol, sodium azide (1.3 g, 0.02 mol) was added at the room temperature. The temperature was raised to 50°C in half an hour gradually and the mixture was stirred at this temperature for 12 h. The precipitate was filtered and washed with a small amount of water. The title compound was isolated using column chromatography (Petroleum ether: ethyl acetate-4:1). Single crystals suitable for X-ray diffraction analysis were obtained

Refinement

The H-atoms bonded to the C-atom were positioned geometrically and refined using a riding model, with C—H = 0.93 Å and Uiso(H) = 1.2Ueq(C).

Figures

Fig. 1.

Fig. 1.

Perspective structure of the title compound, showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level.

Crystal data

C14H10N4 Z = 2
Mr = 234.26 F(000) = 244
Triclinic, P1 Dx = 1.275 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 8.0763 (16) Å Cell parameters from 2748 reflections
b = 8.2183 (16) Å θ = 2.6–27.4°
c = 10.116 (2) Å µ = 0.08 mm1
α = 76.22 (3)° T = 293 K
β = 69.36 (3)° Prism, colorless
γ = 85.94 (3)° 0.20 × 0.20 × 0.20 mm
V = 610.2 (2) Å3

Data collection

Rigaku Mercury2 diffractometer 1559 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.035
Graphite monochromator θmax = 27.4°, θmin = 3.5°
Detector resolution: 13.6612 pixels mm-1 h = −10→10
CCD_Profile_fitting scans k = −10→10
6204 measured reflections l = −13→13
2748 independent 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)] = 0.058 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.146 H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0613P)2 + 0.0517P] where P = (Fo2 + 2Fc2)/3
2748 reflections (Δ/σ)max = 0.001
163 parameters Δρmax = 0.14 e Å3
0 restraints Δρmin = −0.21 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
C7 0.0733 (2) 0.6414 (2) 0.1795 (2) 0.0441 (5)
C1 −0.0353 (2) 0.7492 (2) 0.2778 (2) 0.0444 (5)
C9 0.2358 (3) 0.3876 (2) 0.1389 (2) 0.0519 (5)
H9A 0.2727 0.2827 0.1769 0.062*
C11 0.2308 (3) 0.6036 (3) −0.0645 (2) 0.0565 (5)
H11A 0.2629 0.6449 −0.1643 0.068*
C8 0.1297 (2) 0.4830 (2) 0.2324 (2) 0.0482 (5)
H8A 0.0957 0.4404 0.3321 0.058*
C3 −0.2866 (3) 0.7958 (2) 0.4875 (2) 0.0545 (5)
H3A −0.3858 0.7539 0.5675 0.065*
C12 0.1262 (3) 0.7001 (2) 0.0292 (2) 0.0538 (5)
H12A 0.0908 0.8055 −0.0091 0.065*
C6 0.0093 (3) 0.9192 (2) 0.2491 (2) 0.0579 (6)
H6A 0.1082 0.9631 0.1695 0.070*
C2 −0.1865 (2) 0.6899 (2) 0.3994 (2) 0.0446 (5)
C14 0.4070 (3) 0.3449 (3) −0.1131 (2) 0.0662 (6)
H14A 0.4233 0.4016 −0.2127 0.079*
H14B 0.5220 0.3337 −0.1020 0.079*
C10 0.2877 (2) 0.4470 (2) −0.0112 (2) 0.0499 (5)
C13 −0.2470 (3) 0.5166 (3) 0.4378 (2) 0.0555 (5)
C5 −0.0900 (3) 1.0228 (3) 0.3361 (2) 0.0655 (6)
H5A −0.0571 1.1349 0.3142 0.079*
C4 −0.2381 (3) 0.9620 (2) 0.4556 (2) 0.0612 (6)
H4A −0.3041 1.0327 0.5137 0.073*
N1 −0.2994 (3) 0.3814 (2) 0.4726 (2) 0.0849 (7)
N3 0.4183 (2) 0.0789 (2) −0.14723 (19) 0.0640 (5)
N2 0.3271 (3) 0.1777 (2) −0.0802 (2) 0.0799 (6)
N4 0.4870 (3) −0.0238 (3) −0.2027 (3) 0.1025 (8)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C7 0.0391 (10) 0.0458 (11) 0.0475 (11) 0.0000 (8) −0.0138 (9) −0.0123 (9)
C1 0.0476 (11) 0.0399 (10) 0.0465 (11) 0.0041 (9) −0.0176 (9) −0.0100 (9)
C9 0.0494 (11) 0.0464 (11) 0.0566 (13) 0.0062 (9) −0.0146 (10) −0.0128 (10)
C11 0.0573 (12) 0.0613 (13) 0.0447 (11) −0.0030 (11) −0.0098 (10) −0.0113 (10)
C8 0.0487 (11) 0.0478 (11) 0.0465 (11) 0.0024 (9) −0.0139 (10) −0.0123 (9)
C3 0.0575 (12) 0.0490 (12) 0.0486 (12) 0.0016 (10) −0.0079 (10) −0.0120 (10)
C12 0.0551 (12) 0.0487 (11) 0.0511 (12) 0.0022 (10) −0.0140 (10) −0.0062 (10)
C6 0.0596 (13) 0.0462 (11) 0.0567 (13) −0.0065 (10) −0.0073 (11) −0.0084 (10)
C2 0.0479 (11) 0.0382 (10) 0.0467 (11) 0.0005 (9) −0.0140 (9) −0.0114 (9)
C14 0.0547 (13) 0.0708 (15) 0.0653 (15) −0.0037 (12) −0.0034 (11) −0.0266 (12)
C10 0.0395 (10) 0.0560 (12) 0.0525 (12) −0.0037 (9) −0.0080 (9) −0.0202 (10)
C13 0.0507 (12) 0.0486 (12) 0.0593 (13) 0.0009 (10) −0.0055 (10) −0.0185 (11)
C5 0.0763 (16) 0.0402 (11) 0.0744 (16) −0.0047 (11) −0.0167 (13) −0.0153 (11)
C4 0.0704 (14) 0.0466 (12) 0.0632 (14) 0.0088 (11) −0.0148 (12) −0.0212 (11)
N1 0.0769 (14) 0.0530 (12) 0.1028 (17) −0.0111 (11) 0.0031 (12) −0.0261 (12)
N3 0.0634 (12) 0.0643 (12) 0.0597 (12) 0.0051 (10) −0.0131 (10) −0.0197 (10)
N2 0.0686 (12) 0.0743 (13) 0.0863 (14) −0.0054 (11) 0.0052 (11) −0.0461 (12)
N4 0.1053 (18) 0.0736 (15) 0.1081 (19) 0.0189 (14) −0.0048 (15) −0.0375 (14)

Geometric parameters (Å, º)

C7—C8 1.395 (2) C12—H12A 0.9300
C7—C12 1.397 (3) C6—C5 1.381 (3)
C7—C1 1.496 (2) C6—H6A 0.9300
C1—C6 1.403 (2) C2—C13 1.456 (3)
C1—C2 1.408 (3) C14—N2 1.474 (3)
C9—C8 1.389 (2) C14—C10 1.514 (3)
C9—C10 1.395 (3) C14—H14A 0.9700
C9—H9A 0.9300 C14—H14B 0.9700
C11—C10 1.386 (3) C13—N1 1.146 (2)
C11—C12 1.393 (3) C5—C4 1.385 (3)
C11—H11A 0.9300 C5—H5A 0.9300
C8—H8A 0.9300 C4—H4A 0.9300
C3—C4 1.378 (3) N3—N4 1.128 (2)
C3—C2 1.403 (2) N3—N2 1.220 (2)
C3—H3A 0.9300
C8—C7—C12 117.61 (17) C1—C6—H6A 119.2
C8—C7—C1 122.25 (17) C3—C2—C1 121.39 (17)
C12—C7—C1 120.11 (17) C3—C2—C13 117.21 (17)
C6—C1—C2 116.68 (17) C1—C2—C13 121.39 (16)
C6—C1—C7 120.17 (17) N2—C14—C10 109.67 (17)
C2—C1—C7 123.13 (16) N2—C14—H14A 109.7
C8—C9—C10 120.86 (18) C10—C14—H14A 109.7
C8—C9—H9A 119.6 N2—C14—H14B 109.7
C10—C9—H9A 119.6 C10—C14—H14B 109.7
C10—C11—C12 120.88 (19) H14A—C14—H14B 108.2
C10—C11—H11A 119.6 C11—C10—C9 118.27 (17)
C12—C11—H11A 119.6 C11—C10—C14 120.86 (19)
C9—C8—C7 121.18 (18) C9—C10—C14 120.84 (19)
C9—C8—H8A 119.4 N1—C13—C2 177.4 (2)
C7—C8—H8A 119.4 C6—C5—C4 120.90 (19)
C4—C3—C2 120.07 (19) C6—C5—H5A 119.6
C4—C3—H3A 120.0 C4—C5—H5A 119.6
C2—C3—H3A 120.0 C3—C4—C5 119.36 (19)
C11—C12—C7 121.20 (19) C3—C4—H4A 120.3
C11—C12—H12A 119.4 C5—C4—H4A 120.3
C7—C12—H12A 119.4 N4—N3—N2 172.5 (2)
C5—C6—C1 121.59 (19) N3—N2—C14 115.65 (18)
C5—C6—H6A 119.2

Hydrogen-bond geometry (Å, º)

Cg is the centroid of the C7–C12 benzene ring.

D—H···A D—H H···A D···A D—H···A
C14—H14B···Cgi 0.97 2.75 3.642 (3) 154

Symmetry code: (i) −x+1, −y+1, −z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: XU5575).

References

  1. Haertling, G. H. (1999). J. Am. Ceram. Soc. 82, 797–810.
  2. Homes, C. C., Vogt, T., Shapiro, S. M., Wakimoto, S. & Ramirez, A. P. (2001). Science, 293, 673–676. [DOI] [PubMed]
  3. Rigaku (2005). CrystalClear Rigaku Corporation, Tokyo, Japan.
  4. 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/S1600536812029261/xu5575sup1.cif

e-68-o2297-sup1.cif (14.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812029261/xu5575Isup2.hkl

e-68-o2297-Isup2.hkl (134.9KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812029261/xu5575Isup3.cml

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


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