Skip to main content
Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2009 Feb 11;65(Pt 3):o507. doi: 10.1107/S1600536809004127

3-(1H-Benzotriazol-1-yl)-1-(3-methoxy­phen­yl)propan-1-one

Guang-Jiu Li a, Kong-Cheng Hu a,*
PMCID: PMC2968644  PMID: 21582170

Abstract

In the title mol­ecule, C16H15N3O2, the benzotriazole fragment and the benzene ring form a dihedral angle of 75.02 (1)°. In the crystal structure, mol­ecules related by translation along the a axis are linked into chains via weak C—H⋯π inter­actions.

Related literature

For the pharmacological activity of 1H-benzotriazole derivatives, see: Chen & Wu (2005). Some details of the synthesis have been described by Zhu et al. (2007). For reference values of geometric parameters in organic mol­ecules, see: Allen et al. (1987).graphic file with name e-65-0o507-scheme1.jpg

Experimental

Crystal data

  • C16H15N3O2

  • M r = 281.31

  • Monoclinic, Inline graphic

  • a = 5.3583 (14) Å

  • b = 12.976 (4) Å

  • c = 19.688 (5) Å

  • β = 91.146 (4)°

  • V = 1368.6 (6) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.09 mm−1

  • T = 293 (2) K

  • 0.21 × 0.15 × 0.07 mm

Data collection

  • Siemens SMART 1000 CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996) T min = 0.981, T max = 0.994

  • 7461 measured reflections

  • 2693 independent reflections

  • 2279 reflections with I > 2σ(I)

  • R int = 0.018

Refinement

  • R[F 2 > 2σ(F 2)] = 0.041

  • wR(F 2) = 0.112

  • S = 1.04

  • 2693 reflections

  • 190 parameters

  • H-atom parameters constrained

  • Δρmax = 0.14 e Å−3

  • Δρmin = −0.23 e Å−3

Data collection: SMART (Siemens, 1996); cell refinement: SAINT (Siemens, 1996); data reduction: SAINT; 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, PARST (Nardelli, 1995) and PLATON (Spek, 2003).

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809004127/cv2510sup1.cif

e-65-0o507-sup1.cif (18.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809004127/cv2510Isup2.hkl

e-65-0o507-Isup2.hkl (132.2KB, hkl)

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

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

D—H⋯A D—H H⋯A DA D—H⋯A
C9—H9ACg1i 0.97 2.74 3.504 136

Symmetry code: (i) Inline graphic. Cg1 is the centroid of atoms C10–C15.

Acknowledgments

This project was supported by the Natural Science Foundation of Shandong Province (grant Nos. Y2008B02 and Y2008B32).

supplementary crystallographic information

Comment

1H-Benzotriazole and its derivatives exhibit a broad spectrum of pharmacological activities, such as antifungal, antitumor and antineoplastic (Chen & Wu, 2005). In order to search for new benzotriazole derivatives with higher bioactivity, the title compound, (I), was synthesized and its structure is shown here.

In the title molecule (Fig. 1), all bond lengths and angles are within normal ranges (Allen et al., 1987). The benzotriazole system is almost planar with a dihedral angle of 1.45 (1)° between the triazole (N1–N3/C10/C11) and benzene (C10—C15) rings. The whole molecular is non-planar with a dihedral angle of 75.02 (1)° between the benzotriazole fragment and benzene C1–C6 ring. In the crystal, the molecules related by translation along axis a are linked into chains via the weak C—H···π interactions (Table 1).

Experimental

The title compound was prepared according to the literature method of Zhu et al.(2007). Single crystals suitable for X-ray diffraction were obtained by slow evaporation of an ethyl acetate solution at room temperature over a period of one week.

Refinement

All H atoms were located in difference Fourier maps and constrained to ride on their parent atoms, with C—H distances in the range 0.93–0.97 Å, and with Uiso(H) = 1.2 Ueq(C) and 1.5 Ueq(methyl C).

Figures

Fig. 1.

Fig. 1.

The molecular structure of (I) showing 50% probability displacement ellipsoids and the atom numbering scheme.

Crystal data

C16H15N3O2 F(000) = 592
Mr = 281.31 Dx = 1.365 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
a = 5.3583 (14) Å Cell parameters from 3062 reflections
b = 12.976 (4) Å θ = 2.6–25.9°
c = 19.688 (5) Å µ = 0.09 mm1
β = 91.146 (4)° T = 293 K
V = 1368.6 (6) Å3 Block, colourless
Z = 4 0.21 × 0.15 × 0.07 mm

Data collection

Siemens SMART 1000 CCD area-detector diffractometer 2693 independent reflections
Radiation source: fine-focus sealed tube 2279 reflections with I > 2σ(I)
graphite Rint = 0.018
Detector resolution: 8.33 pixels mm-1 θmax = 26.0°, θmin = 1.9°
ω scans h = −6→6
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) k = −16→16
Tmin = 0.981, Tmax = 0.994 l = −24→17
7461 measured 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)] = 0.041 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.112 H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0577P)2 + 0.249P] where P = (Fo2 + 2Fc2)/3
2693 reflections (Δ/σ)max < 0.001
190 parameters Δρmax = 0.14 e Å3
0 restraints Δρmin = −0.23 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
O1 0.2340 (2) 0.48618 (9) 0.09618 (6) 0.0607 (3)
O2 −0.2250 (2) 0.87656 (8) −0.00231 (6) 0.0570 (3)
N1 0.0340 (2) 0.44726 (9) 0.23515 (6) 0.0427 (3)
C6 0.1036 (2) 0.64278 (10) 0.04534 (6) 0.0396 (3)
C2 −0.0452 (3) 0.80221 (11) −0.00439 (7) 0.0444 (3)
C1 −0.0680 (3) 0.72307 (11) 0.04300 (7) 0.0428 (3)
H1A −0.1990 0.7240 0.0733 0.051*
C10 0.2033 (2) 0.37083 (10) 0.24527 (7) 0.0390 (3)
C7 0.0797 (2) 0.55465 (11) 0.09372 (7) 0.0415 (3)
C5 0.3012 (3) 0.64292 (12) 0.00019 (7) 0.0462 (3)
H5A 0.4176 0.5898 0.0012 0.055*
C8 −0.1429 (3) 0.55249 (11) 0.13963 (7) 0.0458 (3)
H8A −0.2938 0.5586 0.1119 0.055*
H8B −0.1348 0.6120 0.1694 0.055*
N2 0.0569 (3) 0.51863 (10) 0.28486 (7) 0.0573 (4)
C12 0.5305 (3) 0.33871 (12) 0.32934 (8) 0.0541 (4)
H12A 0.6189 0.3565 0.3687 0.065*
C13 0.5867 (3) 0.25211 (13) 0.29353 (8) 0.0579 (4)
H13A 0.7178 0.2106 0.3087 0.070*
N3 0.2374 (3) 0.49148 (10) 0.32671 (7) 0.0589 (4)
C3 0.1519 (3) 0.80179 (12) −0.04920 (7) 0.0498 (4)
H3B 0.1684 0.8543 −0.0810 0.060*
C11 0.3340 (3) 0.39961 (11) 0.30415 (7) 0.0440 (3)
C15 0.2589 (3) 0.28109 (11) 0.20939 (8) 0.0505 (4)
H15A 0.1686 0.2617 0.1706 0.061*
C4 0.3230 (3) 0.72214 (13) −0.04583 (7) 0.0518 (4)
H4A 0.4562 0.7221 −0.0754 0.062*
C9 −0.1613 (3) 0.45603 (12) 0.18278 (8) 0.0516 (4)
H9A −0.3224 0.4553 0.2044 0.062*
H9B −0.1536 0.3962 0.1533 0.062*
C14 0.4524 (3) 0.22363 (12) 0.23434 (9) 0.0590 (4)
H14A 0.4972 0.1638 0.2116 0.071*
C16 −0.2412 (4) 0.94720 (13) −0.05808 (9) 0.0621 (4)
H16A −0.3743 0.9952 −0.0507 0.093*
H16B −0.2738 0.9098 −0.0994 0.093*
H16C −0.0865 0.9839 −0.0616 0.093*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1 0.0544 (6) 0.0619 (7) 0.0661 (7) 0.0170 (5) 0.0131 (5) 0.0130 (5)
O2 0.0617 (7) 0.0522 (6) 0.0572 (7) 0.0079 (5) 0.0049 (5) 0.0124 (5)
N1 0.0441 (6) 0.0438 (6) 0.0404 (6) −0.0021 (5) 0.0016 (5) 0.0031 (5)
C6 0.0367 (7) 0.0471 (7) 0.0348 (7) −0.0026 (6) −0.0028 (5) −0.0029 (5)
C2 0.0446 (8) 0.0454 (8) 0.0430 (8) −0.0040 (6) −0.0049 (6) 0.0004 (6)
C1 0.0406 (7) 0.0493 (8) 0.0386 (7) −0.0021 (6) 0.0024 (6) 0.0005 (6)
C10 0.0389 (7) 0.0402 (7) 0.0381 (7) −0.0062 (5) 0.0051 (5) 0.0047 (5)
C7 0.0368 (7) 0.0471 (8) 0.0405 (7) 0.0005 (6) −0.0024 (5) −0.0024 (6)
C5 0.0394 (7) 0.0570 (8) 0.0423 (8) 0.0010 (6) 0.0016 (6) −0.0028 (6)
C8 0.0358 (7) 0.0545 (8) 0.0471 (8) 0.0020 (6) 0.0005 (6) 0.0077 (6)
N2 0.0683 (9) 0.0498 (7) 0.0537 (8) 0.0062 (6) 0.0001 (7) −0.0052 (6)
C12 0.0559 (9) 0.0585 (9) 0.0476 (9) −0.0050 (7) −0.0089 (7) 0.0084 (7)
C13 0.0536 (9) 0.0557 (9) 0.0644 (10) 0.0074 (7) −0.0007 (8) 0.0161 (8)
N3 0.0747 (9) 0.0522 (8) 0.0493 (8) 0.0034 (7) −0.0080 (7) −0.0087 (6)
C3 0.0522 (9) 0.0562 (9) 0.0409 (8) −0.0107 (7) −0.0002 (6) 0.0070 (6)
C11 0.0497 (8) 0.0437 (7) 0.0387 (7) −0.0074 (6) 0.0006 (6) 0.0021 (6)
C15 0.0588 (9) 0.0473 (8) 0.0453 (8) −0.0034 (7) −0.0015 (7) −0.0053 (6)
C4 0.0453 (8) 0.0683 (10) 0.0420 (8) −0.0070 (7) 0.0079 (6) 0.0004 (7)
C9 0.0385 (8) 0.0610 (9) 0.0552 (9) −0.0070 (7) −0.0021 (6) 0.0119 (7)
C14 0.0703 (11) 0.0457 (8) 0.0613 (10) 0.0074 (8) 0.0072 (8) −0.0018 (7)
C16 0.0732 (11) 0.0537 (9) 0.0591 (10) 0.0047 (8) −0.0062 (8) 0.0119 (8)

Geometric parameters (Å, °)

O1—C7 1.2137 (17) C8—H8B 0.9700
O2—C2 1.3649 (18) N2—N3 1.3063 (19)
O2—C16 1.4316 (18) C12—C13 1.363 (2)
N1—N2 1.3511 (17) C12—C11 1.399 (2)
N1—C10 1.3563 (17) C12—H12A 0.9300
N1—C9 1.4586 (18) C13—C14 1.407 (2)
C6—C1 1.3896 (19) C13—H13A 0.9300
C6—C5 1.3961 (19) N3—C11 1.3769 (19)
C6—C7 1.4954 (19) C3—C4 1.382 (2)
C2—C3 1.389 (2) C3—H3B 0.9300
C2—C1 1.394 (2) C15—C14 1.361 (2)
C1—H1A 0.9300 C15—H15A 0.9300
C10—C11 1.3933 (19) C4—H4A 0.9300
C10—C15 1.397 (2) C9—H9A 0.9700
C7—C8 1.511 (2) C9—H9B 0.9700
C5—C4 1.377 (2) C14—H14A 0.9300
C5—H5A 0.9300 C16—H16A 0.9600
C8—C9 1.517 (2) C16—H16B 0.9600
C8—H8A 0.9700 C16—H16C 0.9600
C2—O2—C16 117.48 (12) C12—C13—C14 122.05 (15)
N2—N1—C10 110.12 (12) C12—C13—H13A 119.0
N2—N1—C9 120.80 (12) C14—C13—H13A 119.0
C10—N1—C9 128.99 (12) N2—N3—C11 107.97 (12)
C1—C6—C5 119.18 (13) C4—C3—C2 118.97 (13)
C1—C6—C7 121.97 (12) C4—C3—H3B 120.5
C5—C6—C7 118.83 (12) C2—C3—H3B 120.5
O2—C2—C3 124.61 (13) N3—C11—C10 108.32 (13)
O2—C2—C1 115.41 (13) N3—C11—C12 131.29 (14)
C3—C2—C1 119.98 (14) C10—C11—C12 120.37 (14)
C6—C1—C2 120.50 (13) C14—C15—C10 116.26 (14)
C6—C1—H1A 119.7 C14—C15—H15A 121.9
C2—C1—H1A 119.7 C10—C15—H15A 121.9
N1—C10—C11 104.48 (12) C5—C4—C3 121.66 (14)
N1—C10—C15 133.14 (13) C5—C4—H4A 119.2
C11—C10—C15 122.38 (13) C3—C4—H4A 119.2
O1—C7—C6 121.22 (12) N1—C9—C8 113.99 (12)
O1—C7—C8 120.51 (13) N1—C9—H9A 108.8
C6—C7—C8 118.28 (12) C8—C9—H9A 108.8
C4—C5—C6 119.69 (14) N1—C9—H9B 108.8
C4—C5—H5A 120.2 C8—C9—H9B 108.8
C6—C5—H5A 120.2 H9A—C9—H9B 107.7
C7—C8—C9 114.27 (12) C15—C14—C13 121.90 (15)
C7—C8—H8A 108.7 C15—C14—H14A 119.0
C9—C8—H8A 108.7 C13—C14—H14A 119.0
C7—C8—H8B 108.7 O2—C16—H16A 109.5
C9—C8—H8B 108.7 O2—C16—H16B 109.5
H8A—C8—H8B 107.6 H16A—C16—H16B 109.5
N3—N2—N1 109.11 (12) O2—C16—H16C 109.5
C13—C12—C11 117.02 (15) H16A—C16—H16C 109.5
C13—C12—H12A 121.5 H16B—C16—H16C 109.5
C11—C12—H12A 121.5
C16—O2—C2—C3 13.0 (2) N1—N2—N3—C11 −0.44 (17)
C16—O2—C2—C1 −167.35 (13) O2—C2—C3—C4 179.60 (13)
C5—C6—C1—C2 0.8 (2) C1—C2—C3—C4 0.0 (2)
C7—C6—C1—C2 −177.70 (12) N2—N3—C11—C10 0.20 (17)
O2—C2—C1—C6 179.60 (12) N2—N3—C11—C12 178.69 (15)
C3—C2—C1—C6 −0.8 (2) N1—C10—C11—N3 0.12 (15)
N2—N1—C10—C11 −0.40 (14) C15—C10—C11—N3 179.28 (13)
C9—N1—C10—C11 −176.92 (12) N1—C10—C11—C12 −178.56 (12)
N2—N1—C10—C15 −179.42 (15) C15—C10—C11—C12 0.6 (2)
C9—N1—C10—C15 4.1 (2) C13—C12—C11—N3 −177.86 (15)
C1—C6—C7—O1 −178.41 (13) C13—C12—C11—C10 0.5 (2)
C5—C6—C7—O1 3.1 (2) N1—C10—C15—C14 177.59 (14)
C1—C6—C7—C8 1.83 (19) C11—C10—C15—C14 −1.3 (2)
C5—C6—C7—C8 −176.67 (12) C6—C5—C4—C3 −0.7 (2)
C1—C6—C5—C4 −0.1 (2) C2—C3—C4—C5 0.7 (2)
C7—C6—C5—C4 178.46 (13) N2—N1—C9—C8 61.53 (17)
O1—C7—C8—C9 −4.4 (2) C10—N1—C9—C8 −122.27 (15)
C6—C7—C8—C9 175.40 (12) C7—C8—C9—N1 68.40 (17)
C10—N1—N2—N3 0.54 (16) C10—C15—C14—C13 1.0 (2)
C9—N1—N2—N3 177.39 (12) C12—C13—C14—C15 0.1 (3)
C11—C12—C13—C14 −0.8 (2)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C9—H9A···Cg1i 0.97 2.74 3.504 136

Symmetry codes: (i) x−1, y, z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: CV2510).

References

  1. Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1–19.
  2. Chen, Z.-Y. & Wu, M.-T. (2005). Org. Lett.7, 475–477. [DOI] [PubMed]
  3. Nardelli, M. (1995). J. Appl. Cryst.28, 659.
  4. Sheldrick, G. M. (1996). SADABS University of Göttingen, Germany.
  5. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  6. Siemens (1996). SMART and SAINT Siemens Analytical X-ray Instruments Inc., Madison, Wisconsin, USA.
  7. Spek, A. L. (2003). J. Appl. Cryst.36, 7–13.
  8. Zhu, Y.-J., Wang, M., Bi, J.-L. & Li, F. (2007). Acta Cryst. E63, o4548.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809004127/cv2510sup1.cif

e-65-0o507-sup1.cif (18.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809004127/cv2510Isup2.hkl

e-65-0o507-Isup2.hkl (132.2KB, hkl)

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


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

RESOURCES