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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Nov 12;67(Pt 12):o3298. doi: 10.1107/S1600536811047556

5-Chloro-2-(phenyl­diazen­yl)pyridine

Steffen Thies a, Christian Näther b,*, Rainer Herges a,*
PMCID: PMC3238951  PMID: 22199800

Abstract

In the title compound, C11H8ClN3, the azo group adopts a trans conformation and the dihedral angle between the six-membered rings is 15.47 (8)°.

Related literature

For background to this work, see: Thies et al. (2010, 2011); Venkataramani et al. (2011). For the structure of a bis­(5-chloro-2-(phenyl­azo)pyridine)­dichloro–ruthenium(II) complex, see: Hansongnern et al. (2008).graphic file with name e-67-o3298-scheme1.jpg

Experimental

Crystal data

  • C11H8ClN3

  • M r = 217.65

  • Monoclinic, Inline graphic

  • a = 6.1136 (2) Å

  • b = 9.0940 (4) Å

  • c = 18.6839 (8) Å

  • β = 91.459 (3)°

  • V = 1038.43 (7) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.33 mm−1

  • T = 293 K

  • 0.3 × 0.2 × 0.2 mm

Data collection

  • Stoe IPDS-2 diffractometer

  • 19329 measured reflections

  • 2818 independent reflections

  • 2456 reflections with I > 2σ(I)

  • R int = 0.028

Refinement

  • R[F 2 > 2σ(F 2)] = 0.044

  • wR(F 2) = 0.117

  • S = 1.15

  • 2818 reflections

  • 137 parameters

  • H-atom parameters constrained

  • Δρmax = 0.22 e Å−3

  • Δρmin = −0.17 e Å−3

Data collection: X-AREA (Stoe & Cie, 2008); cell refinement: X-AREA; data reduction: X-AREA; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: XP in SHELXTL (Sheldrick, 2008) and DIAMOND (Brandenburg, 2011); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811047556/bt5703sup1.cif

e-67-o3298-sup1.cif (13.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811047556/bt5703Isup2.hkl

e-67-o3298-Isup2.hkl (138.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811047556/bt5703Isup3.cml

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

Acknowledgments

We gratefully acknowledge financial support by the Deutsche Forschungsgemeinschaft via SFB 677.

supplementary crystallographic information

Comment

We recently reported about a change of the spin state by association/dissociation of photodissociable ligands (PDL's) at square planar Ni(II) porphyrine complexes (Thies et al. 2010, Thies et al. 2011, Venkataramani et al., 2011). Within this project the title compound, was obtained as an intermediate in the synthesis of 5-methoxy-2-phenylazopyridine which can be used as PDL. For the identification of this intermediate a structure determination was performed.

In the structure of the title compound, the 5-chloro-2-phenylazopyridine molecules, are not coplanar. Both 6-membered rings are twisted by 15.47 (8) °. The azo group is in a trans configuration and the torsion angle C1—N2—N3—C6 amounts to 178.5 (2) °). In the crystal structure the molecules exhibit a sandwich herringbone arrangement with neighbouring molecules stacked onto each other. The molecules are also linked by weak C—H···N interactions.

Experimental

Synthesis of 5-Chloro-2-phenylazopyridine

A mixture of sodium hydroxide (12.0 ml of 25%), pyridine (8.00 ml) and 2-amino-5-chlorpyridine (15.6 mmol, 2.00 g) (Merck) was stirred at 80 °C. Nitrosobenzene (16.0 mmol, 1.71 g) dissolved in pyridine (60.0 ml) was added dropwise during a period of 45 min. The mixture was stirred for additional 30 min at 80 °C and stirred at RT for 72 h. The reaction mixture was extracted with toluene. The combined organic layer was dried over magnesium sulfate. After removal of the solvent, recrystallization with diethylether afforded red crystalls in 36% yield.

mp.: 84.5–87 °C

1H-NMR (600 MHz, 300 K, CDCl3, TMS): δ = 8.69 (d, 4J=2.4 Hz, 1H, 6-H), 8.04- 8.03 (m, 2H, 2`-H), 7.87 (dd, 4J=2.5 Hz, 3J=8.5 Hz, 1H, 4-H), 7.81 (d, 3J=8.5 Hz, 1H, 3-H), 7.53–7.56 (m, 3H, 3`-H, 4`-H) p.p.m.. 13C-NMR (150 MHz, 300 K, CDCl3, TMS): δ = 161.0 (C2), 152.3 (C10), 148.4 (C6), 138.1 (C4), 133.6 (C5), 132.5 (C40), 129.2 (C30), 123.7 (C20), 115.9 (C3) p.p.m.. MS (EI, 70 eV): m/z(%)= 217 (1) [M]+, 105 (89) [M—C5H3NCl]+. MS (CI, Isobutan): m/z(%)= 218 (100) [M+H]+. UV/Vis (Toluol): λ(max)(lg ε)= 315 nm (4.058), 448 nm (2.494).

Refinement

The H atoms were located in difference map but were positioned with idealized geometry with C—H = 0.93Å and refined with isotropic displacement parameters (Uiso(H) = 1.2Ueq(C)) using a riding model.

Figures

Fig. 1.

Fig. 1.

: Crystal structure of the title compound with labeling and displacement ellipsoids drawn at the 50% probability level.

Fig. 2.

Fig. 2.

: Crystal structure of the title compound with view in the direction of the crystallographic c axis.

Crystal data

C11H8ClN3 F(000) = 448
Mr = 217.65 Dx = 1.392 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
a = 6.1136 (2) Å Cell parameters from 23258 reflections
b = 9.0940 (4) Å θ = 2.2–29.2°
c = 18.6839 (8) Å µ = 0.33 mm1
β = 91.459 (3)° T = 293 K
V = 1038.43 (7) Å3 Block, colourless
Z = 4 0.3 × 0.2 × 0.2 mm

Data collection

Stoe IPDS-2 diffractometer 2456 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.028
graphite θmax = 29.2°, θmin = 2.2°
ω scans h = −7→8
19329 measured reflections k = −12→12
2818 independent reflections l = −25→25

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)] = 0.044 H-atom parameters constrained
wR(F2) = 0.117 w = 1/[σ2(Fo2) + (0.0494P)2 + 0.1607P] where P = (Fo2 + 2Fc2)/3
S = 1.15 (Δ/σ)max < 0.001
2818 reflections Δρmax = 0.22 e Å3
137 parameters Δρmin = −0.17 e Å3
0 restraints Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.013 (2)

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
Cl1 0.82419 (7) −0.02057 (5) 0.37109 (2) 0.07091 (17)
C1 0.4709 (2) 0.27818 (16) 0.51393 (7) 0.0521 (3)
C2 0.4706 (3) 0.12003 (19) 0.42028 (8) 0.0610 (4)
H2 0.3950 0.0699 0.3840 0.073*
N1 0.3601 (2) 0.20937 (16) 0.46186 (7) 0.0620 (3)
C3 0.6925 (2) 0.09777 (16) 0.42821 (7) 0.0529 (3)
C4 0.8081 (2) 0.17112 (19) 0.48142 (9) 0.0605 (4)
H4 0.9585 0.1591 0.4872 0.073*
C5 0.6949 (2) 0.26232 (18) 0.52564 (8) 0.0586 (4)
H5 0.7666 0.3125 0.5627 0.070*
N2 0.3334 (2) 0.37225 (14) 0.55510 (7) 0.0588 (3)
N3 0.4247 (2) 0.41302 (15) 0.61134 (7) 0.0593 (3)
C6 0.2969 (3) 0.51050 (16) 0.65384 (8) 0.0559 (3)
C7 0.3993 (3) 0.5565 (2) 0.71665 (9) 0.0685 (4)
H7 0.5377 0.5211 0.7292 0.082*
C8 0.2973 (4) 0.6544 (2) 0.76071 (9) 0.0773 (5)
H8 0.3672 0.6861 0.8027 0.093*
C9 0.0916 (4) 0.7056 (2) 0.74256 (10) 0.0778 (5)
H9 0.0224 0.7721 0.7723 0.093*
C10 −0.0123 (3) 0.6581 (2) 0.68026 (11) 0.0750 (5)
H10 −0.1523 0.6919 0.6686 0.090*
C11 0.0890 (3) 0.56153 (19) 0.63543 (9) 0.0626 (4)
H11 0.0192 0.5307 0.5932 0.075*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cl1 0.0752 (3) 0.0732 (3) 0.0646 (3) 0.0099 (2) 0.00810 (19) −0.00282 (19)
C1 0.0511 (7) 0.0541 (7) 0.0511 (7) −0.0032 (6) −0.0005 (6) 0.0062 (6)
C2 0.0545 (8) 0.0704 (9) 0.0577 (8) −0.0019 (7) −0.0079 (6) −0.0056 (7)
N1 0.0487 (6) 0.0749 (8) 0.0619 (7) 0.0003 (6) −0.0077 (5) −0.0061 (6)
C3 0.0534 (7) 0.0551 (7) 0.0502 (7) −0.0004 (6) 0.0027 (6) 0.0077 (6)
C4 0.0429 (7) 0.0727 (9) 0.0658 (9) −0.0039 (6) −0.0015 (6) 0.0023 (7)
C5 0.0510 (7) 0.0670 (9) 0.0575 (8) −0.0113 (6) −0.0050 (6) −0.0028 (7)
N2 0.0553 (7) 0.0622 (7) 0.0587 (7) −0.0034 (6) −0.0047 (5) 0.0004 (6)
N3 0.0580 (7) 0.0654 (7) 0.0540 (7) −0.0035 (6) −0.0044 (5) 0.0024 (6)
C6 0.0605 (8) 0.0544 (8) 0.0529 (7) −0.0063 (6) 0.0053 (6) 0.0058 (6)
C7 0.0691 (10) 0.0797 (11) 0.0565 (8) 0.0001 (8) −0.0019 (7) −0.0023 (8)
C8 0.0968 (14) 0.0797 (12) 0.0554 (9) −0.0021 (10) 0.0015 (9) −0.0046 (8)
C9 0.1020 (14) 0.0649 (10) 0.0675 (10) 0.0085 (10) 0.0238 (10) 0.0046 (8)
C10 0.0705 (10) 0.0715 (11) 0.0835 (12) 0.0104 (8) 0.0104 (9) 0.0137 (9)
C11 0.0639 (9) 0.0614 (9) 0.0623 (9) −0.0049 (7) −0.0011 (7) 0.0069 (7)

Geometric parameters (Å, °)

Cl1—C3 1.7288 (15) N3—C6 1.435 (2)
C1—N1 1.3278 (19) C6—C7 1.381 (2)
C1—C5 1.389 (2) C6—C11 1.388 (2)
C1—N2 1.436 (2) C7—C8 1.373 (3)
C2—N1 1.322 (2) C7—H7 0.9300
C2—C3 1.376 (2) C8—C9 1.375 (3)
C2—H2 0.9300 C8—H8 0.9300
C3—C4 1.377 (2) C9—C10 1.381 (3)
C4—C5 1.370 (2) C9—H9 0.9300
C4—H4 0.9300 C10—C11 1.372 (3)
C5—H5 0.9300 C10—H10 0.9300
N2—N3 1.2341 (17) C11—H11 0.9300
N1—C1—C5 123.29 (15) C7—C6—C11 120.09 (15)
N1—C1—N2 112.26 (13) C7—C6—N3 114.62 (14)
C5—C1—N2 124.44 (13) C11—C6—N3 125.27 (14)
N1—C2—C3 123.00 (14) C8—C7—C6 120.23 (17)
N1—C2—H2 118.5 C8—C7—H7 119.9
C3—C2—H2 118.5 C6—C7—H7 119.9
C2—N1—C1 117.49 (13) C7—C8—C9 119.86 (18)
C2—C3—C4 119.51 (14) C7—C8—H8 120.1
C2—C3—Cl1 119.90 (12) C9—C8—H8 120.1
C4—C3—Cl1 120.59 (12) C8—C9—C10 120.02 (18)
C5—C4—C3 118.09 (14) C8—C9—H9 120.0
C5—C4—H4 121.0 C10—C9—H9 120.0
C3—C4—H4 121.0 C11—C10—C9 120.62 (18)
C4—C5—C1 118.60 (14) C11—C10—H10 119.7
C4—C5—H5 120.7 C9—C10—H10 119.7
C1—C5—H5 120.7 C10—C11—C6 119.17 (16)
N3—N2—C1 112.15 (13) C10—C11—H11 120.4
N2—N3—C6 114.60 (13) C6—C11—H11 120.4

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BT5703).

References

  1. Brandenburg, K. (2011). DIAMOND Crystal Impact GbR, Bonn, Germany.
  2. Hansongnern, K., Sahavisit, L. & Pakawatchai, C. (2008). Anal. Sci. X-Ray Struct. Anal. Online. 24, x57–x58.
  3. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  4. Stoe & Cie (2008). X-AREA Stoe & Cie, Darmstadt, Germany.
  5. Thies, S., Bornholdt, C., Koehler, F., Sönnichsen, F. D., Naether, C., Tuczek, F. & Herges, R. (2010). Chem. Eur. J. 16, 10074–10083. [DOI] [PubMed]
  6. Thies, S., Sell, H., Schütt, C., Bornholdt, C., Näther, C., Tuczek, F. & Herges, R. (2011). J. Am. Chem. Soc. 133, 16243–16250. [DOI] [PubMed]
  7. Venkataramani, S., Jana, U., Dommaschk, M., Sönnichsen, F. D., Tuczek, F. & Herges, H. (2011). Science, 331, 445–448. [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/S1600536811047556/bt5703sup1.cif

e-67-o3298-sup1.cif (13.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811047556/bt5703Isup2.hkl

e-67-o3298-Isup2.hkl (138.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811047556/bt5703Isup3.cml

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


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