supplementary materials


hk2319 scheme

Acta Cryst. (2007). E63, o3949    [ doi:10.1107/S1600536807041967 ]

3-(1H-Benzotriazol-1-yl)-1-(2-fluorobenzoyl)ethyl nicotinate

J. Wan, W.-L. Zeng, J. Li and S. Bi

Abstract top

In the molecule of the title compound, C21H15FN4O3, intramolecular C-H...O and C-H...F hydrogen bonds result in the formation of one six- and one five-membered ring. In the crystal structure, intermolecular C-H...O hydrogen bonds link the molecules into chains along the a axis. The packing is further stabilized by [pi]-[pi] interactions [centroid-centroid distance 3.632 (2) Å].

Comment top

We have recently reported the structure of 2-(1H-benzotriazol-1-yl)-1-(4 -chlorobenzoyl)ethyl isonicotinate (II) (Han et al., 2007). As part of our ongoing studies of triazole derivatives, the title compound, (I), was synthesized and its crystal structure is reported here.

In the molecule of the title compound, (I), the bond lengths and angles are generally within normal ranges (Allen et al., 1987), and are comparable to those in the related compound (II). In (I), the benzotriazole ring system is essentially planar with a dihedral angle of 0.45 (1)° between triazole A (N1—N3/C10/C11) and benzene B (C10—C15) rings. Rings C (N4/C17—C21) and D (C1—C6) are oriented with respect to the benzotriazole system at dihedral angles of 87.82 (1)° and 0.78 (1)°, respectively, while the dihedral angle between them is 87.62 (1)°. The intramolecular C—H···O and C—H···F hydrogen bonds (Table 1) cause to the formation of one six- and one five-membered rings (Fig. 1).

In the crystal structure, the intermolecular C—H···O hydrogen bonds (Table 1), link the molecules into chains along the a axis (Fig. 2). The packing is further stabilized by π-π interactions involving the C1—C6 benzene rings: Cg3···Cg3iv = 3.632 Å [symmetry code: (iv) 2 − x, −y, −1 − z, Cg3 is the centroid of th benzene ring].

Related literature top

For related literature, see: Han et al. (2007). For bond-length data, see: Allen et al. (1987).

Experimental top

The title compound was prepared according to the literature method (Han et al., 2007). Single crystals suitable for X-ray analysis were obtained by slow evaporation of an ethyl acetate solution at room temperature over a period of 6 d.

Refinement top

H atoms were positioned geometrically with C—H = 0.93, 0.98 and 0.97 Å for aromatic, methine and methylene H atoms, respectively, and constrained to ride on their parent atoms, with Uiso(H) = 1.2Ueq(C)

Computing details top

Data collection: SMART (Siemens, 1996); cell refinement: SAINT (Siemens, 1996); data reduction: SAINT (Siemens, 1996); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997a); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997a); molecular graphics: SHELXTL (Sheldrick, 1997b); software used to prepare material for publication: SHELXTL (Sheldrick, 1997b), PARST (Nardelli, 1995) and PLATON (Spek, 2003).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title molecule, with the atom-numbering scheme. Displacement ellipsoids are drawn at the 50% probability level.
[Figure 2] Fig. 2. A packing diagram for (I). Hydrogen bonds are shown as dashed lines.
3-(1H-Benzotriazol-1-yl)-1-(2-fluorobenzoyl)ethyl nicotinate top
Crystal data top
C21H15FN4O3Z = 2
Mr = 390.37F000 = 404
Triclinic, P1Dx = 1.398 Mg m3
Hall symbol: -P 1Mo Kα radiation
λ = 0.71073 Å
a = 9.8423 (9) ÅCell parameters from 2193 reflections
b = 9.9736 (10) Åθ = 2.3–24.9º
c = 11.4000 (11) ŵ = 0.10 mm1
α = 64.459 (1)ºT = 298 (2) K
β = 67.157 (1)ºBlock, yellow
γ = 76.313 (1)º0.36 × 0.30 × 0.26 mm
V = 927.28 (15) Å3
Data collection top
Siemens SMART 1000 CCD area-detector
diffractometer
3560 independent reflections
Radiation source: fine-focus sealed tube2877 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.013
Detector resolution: 8.33 pixels mm-1θmax = 26.0º
T = 293(2) Kθmin = 2.1º
ω scansh = 12→6
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
k = 12→12
Tmin = 0.964, Tmax = 0.974l = 14→14
5202 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.042  w = 1/[σ2(Fo2) + (0.0541P)2 + 0.1733P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.114(Δ/σ)max < 0.001
S = 1.05Δρmax = 0.14 e Å3
3560 reflectionsΔρmin = 0.18 e Å3
263 parametersExtinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.026 (3)
Secondary atom site location: difference Fourier map
Crystal data top
C21H15FN4O3γ = 76.313 (1)º
Mr = 390.37V = 927.28 (15) Å3
Triclinic, P1Z = 2
a = 9.8423 (9) ÅMo Kα
b = 9.9736 (10) ŵ = 0.10 mm1
c = 11.4000 (11) ÅT = 298 (2) K
α = 64.459 (1)º0.36 × 0.30 × 0.26 mm
β = 67.157 (1)º
Data collection top
Siemens SMART 1000 CCD area-detector
diffractometer
3560 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
2877 reflections with I > 2σ(I)
Tmin = 0.964, Tmax = 0.974Rint = 0.013
5202 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.042263 parameters
wR(F2) = 0.114H-atom parameters constrained
S = 1.05Δρmax = 0.14 e Å3
3560 reflectionsΔρmin = 0.18 e Å3
Special details top

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 > 2sigma(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) top
xyzUiso*/Ueq
F10.89959 (13)0.26256 (12)0.41995 (10)0.0754 (4)
O10.65340 (14)0.09185 (13)0.12652 (11)0.0621 (3)
O20.72673 (11)0.03294 (11)0.00182 (9)0.0444 (3)
O30.94370 (14)0.10059 (14)0.05293 (12)0.0660 (4)
N10.68866 (14)0.36422 (13)0.13452 (12)0.0433 (3)
N20.77269 (15)0.47243 (14)0.24241 (14)0.0539 (4)
N30.80732 (16)0.55330 (15)0.19591 (15)0.0592 (4)
N40.59613 (19)0.25912 (19)0.39906 (15)0.0761 (5)
C10.85535 (18)0.17262 (17)0.45709 (16)0.0487 (4)
C20.9011 (2)0.2013 (2)0.59553 (17)0.0607 (5)
H2B0.95980.27900.65960.073*
C30.8578 (2)0.1122 (2)0.63630 (19)0.0696 (5)
H3B0.88600.13050.72940.084*
C40.7734 (2)0.0035 (3)0.5410 (2)0.0749 (6)
H4B0.74470.06340.56970.090*
C50.73070 (19)0.0316 (2)0.40328 (18)0.0592 (5)
H5A0.67460.11150.33980.071*
C60.76984 (16)0.05731 (16)0.35668 (15)0.0420 (3)
C70.72116 (16)0.01687 (16)0.20536 (15)0.0416 (3)
C80.75139 (16)0.11471 (15)0.14647 (14)0.0406 (3)
H8A0.85330.14320.19370.049*
C90.64266 (17)0.25315 (16)0.15857 (15)0.0430 (3)
H9A0.63380.29630.24980.052*
H9B0.54600.22460.09240.052*
C100.66910 (16)0.37656 (15)0.01425 (15)0.0424 (3)
C110.74604 (18)0.49795 (17)0.05488 (18)0.0501 (4)
C120.7507 (2)0.5446 (2)0.0431 (2)0.0672 (5)
H12A0.80220.62530.01750.081*
C130.6769 (2)0.4668 (2)0.1771 (2)0.0705 (5)
H13A0.67820.49510.24440.085*
C140.5989 (2)0.3452 (2)0.21693 (19)0.0648 (5)
H14A0.54970.29540.30980.078*
C150.59284 (19)0.29725 (18)0.12321 (16)0.0532 (4)
H15A0.54090.21660.14970.064*
C160.82944 (17)0.07994 (16)0.03048 (15)0.0424 (3)
C170.78394 (16)0.17652 (15)0.17859 (15)0.0413 (3)
C180.64180 (19)0.16715 (19)0.26721 (16)0.0554 (4)
H18A0.57410.09260.23320.066*
C190.6977 (3)0.3626 (2)0.44441 (19)0.0743 (6)
H19A0.66870.42750.53600.089*
C200.8409 (2)0.37952 (19)0.36566 (19)0.0638 (5)
H20A0.90730.45270.40330.077*
C210.88514 (19)0.28663 (17)0.22992 (17)0.0528 (4)
H21A0.98150.29720.17310.063*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
F10.1104 (9)0.0647 (7)0.0472 (6)0.0452 (6)0.0100 (6)0.0125 (5)
O10.0804 (8)0.0543 (7)0.0468 (7)0.0304 (6)0.0125 (6)0.0097 (5)
O20.0525 (6)0.0432 (6)0.0325 (5)0.0024 (5)0.0155 (5)0.0117 (4)
O30.0592 (7)0.0693 (8)0.0489 (7)0.0123 (6)0.0107 (6)0.0192 (6)
N10.0509 (7)0.0341 (6)0.0392 (7)0.0053 (5)0.0133 (6)0.0090 (5)
N20.0618 (8)0.0377 (7)0.0470 (8)0.0077 (6)0.0109 (6)0.0067 (6)
N30.0655 (9)0.0405 (7)0.0637 (9)0.0134 (6)0.0132 (7)0.0150 (7)
N40.0797 (11)0.0737 (11)0.0437 (8)0.0012 (9)0.0101 (8)0.0072 (8)
C10.0556 (9)0.0452 (8)0.0424 (8)0.0058 (7)0.0139 (7)0.0152 (7)
C20.0640 (11)0.0623 (11)0.0390 (9)0.0032 (9)0.0076 (8)0.0133 (8)
C30.0701 (12)0.0952 (15)0.0451 (10)0.0061 (11)0.0163 (9)0.0368 (10)
C40.0765 (13)0.1037 (16)0.0658 (12)0.0143 (12)0.0180 (10)0.0523 (12)
C50.0573 (10)0.0714 (11)0.0567 (10)0.0162 (9)0.0099 (8)0.0334 (9)
C60.0418 (8)0.0440 (8)0.0396 (8)0.0017 (6)0.0125 (6)0.0169 (6)
C70.0432 (8)0.0391 (7)0.0398 (8)0.0059 (6)0.0135 (6)0.0112 (6)
C80.0461 (8)0.0405 (8)0.0317 (7)0.0070 (6)0.0117 (6)0.0098 (6)
C90.0489 (8)0.0402 (8)0.0398 (8)0.0040 (6)0.0180 (7)0.0116 (6)
C100.0435 (8)0.0372 (7)0.0462 (8)0.0025 (6)0.0169 (7)0.0166 (6)
C110.0509 (9)0.0380 (8)0.0607 (10)0.0013 (7)0.0186 (8)0.0189 (7)
C120.0780 (13)0.0521 (10)0.0888 (15)0.0037 (9)0.0355 (11)0.0356 (10)
C130.0881 (14)0.0685 (12)0.0761 (14)0.0069 (11)0.0382 (11)0.0431 (11)
C140.0776 (13)0.0669 (11)0.0501 (10)0.0029 (10)0.0199 (9)0.0275 (9)
C150.0581 (10)0.0512 (9)0.0469 (9)0.0086 (8)0.0127 (8)0.0176 (7)
C160.0473 (8)0.0415 (8)0.0420 (8)0.0001 (6)0.0176 (7)0.0185 (7)
C170.0503 (8)0.0387 (7)0.0411 (8)0.0015 (6)0.0210 (7)0.0163 (6)
C180.0585 (10)0.0539 (9)0.0438 (9)0.0045 (8)0.0190 (8)0.0124 (7)
C190.1031 (17)0.0611 (11)0.0426 (10)0.0030 (11)0.0272 (11)0.0043 (8)
C200.0812 (13)0.0489 (10)0.0616 (11)0.0050 (9)0.0412 (10)0.0109 (8)
C210.0559 (10)0.0469 (9)0.0571 (10)0.0020 (7)0.0272 (8)0.0165 (8)
Geometric parameters (Å, °) top
F1—C11.3525 (19)C8—H8A0.9800
O1—C71.2103 (17)C9—H9A0.9700
O2—C81.4376 (16)C9—H9B0.9700
O2—C161.3482 (17)C10—C111.390 (2)
O3—C161.2001 (18)C10—C151.394 (2)
N1—N21.3600 (17)C11—C121.401 (3)
N1—C91.4501 (19)C12—H12A0.9300
N1—C101.3643 (19)C13—C121.359 (3)
N3—N21.299 (2)C13—H13A0.9300
N3—C111.376 (2)C14—C151.370 (2)
N4—C191.336 (2)C14—C131.401 (3)
C1—C21.377 (2)C14—H14A0.9300
C2—C31.369 (3)C15—H15A0.9300
C2—H2B0.9300C16—C171.481 (2)
C3—C41.369 (3)C17—C181.382 (2)
C3—H3B0.9300C17—C211.386 (2)
C4—H4B0.9300C18—N41.336 (2)
C5—C41.372 (3)C18—H18A0.9300
C5—H5A0.9300C19—H19A0.9300
C6—C11.384 (2)C20—C191.363 (3)
C6—C51.394 (2)C20—H20A0.9300
C7—C61.489 (2)C21—C201.369 (2)
C7—C81.533 (2)C21—H21A0.9300
C8—C91.524 (2)
C16—O2—C8115.43 (11)C8—C9—H9B109.2
N2—N1—C10109.94 (12)H9A—C9—H9B107.9
N2—N1—C9119.71 (12)N1—C10—C11104.16 (13)
C10—N1—C9130.22 (12)N1—C10—C15133.48 (14)
N3—N2—N1108.89 (13)C11—C10—C15122.35 (15)
N2—N3—C11108.38 (13)N3—C11—C10108.63 (14)
C18—N4—C19116.17 (17)N3—C11—C12130.90 (16)
F1—C1—C2116.89 (15)C10—C11—C12120.47 (16)
F1—C1—C6119.52 (13)C13—C12—C11117.14 (17)
C2—C1—C6123.58 (16)C13—C12—H12A121.4
C3—C2—C1118.23 (17)C11—C12—H12A121.4
C3—C2—H2B120.9C12—C13—C14121.96 (18)
C1—C2—H2B120.9C12—C13—H13A119.0
C2—C3—C4120.45 (17)C14—C13—H13A119.0
C2—C3—H3B119.8C15—C14—C13122.02 (18)
C4—C3—H3B119.8C15—C14—H14A119.0
C3—C4—C5120.44 (18)C13—C14—H14A119.0
C3—C4—H4B119.8C14—C15—C10116.06 (16)
C5—C4—H4B119.8C14—C15—H15A122.0
C4—C5—C6121.31 (17)C10—C15—H15A122.0
C4—C5—H5A119.3O3—C16—O2123.21 (14)
C6—C5—H5A119.3O3—C16—C17124.15 (14)
C1—C6—C5115.97 (14)O2—C16—C17112.63 (12)
C1—C6—C7126.34 (14)C18—C17—C21118.07 (14)
C5—C6—C7117.65 (14)C18—C17—C16122.75 (13)
O1—C7—C6120.59 (13)C21—C17—C16119.08 (14)
O1—C7—C8118.64 (13)N4—C18—C17123.69 (15)
C6—C7—C8120.73 (12)N4—C18—H18A118.2
O2—C8—C9106.13 (11)C17—C18—H18A118.2
O2—C8—C7108.81 (11)N4—C19—C20124.51 (17)
C9—C8—C7110.90 (12)N4—C19—H19A117.7
O2—C8—H8A110.3C20—C19—H19A117.7
C9—C8—H8A110.3C19—C20—C21118.61 (16)
C7—C8—H8A110.3C19—C20—H20A120.7
N1—C9—C8112.17 (12)C21—C20—H20A120.7
N1—C9—H9A109.2C20—C21—C17118.91 (16)
C8—C9—H9A109.2C20—C21—H21A120.5
N1—C9—H9B109.2C17—C21—H21A120.5
C16—O2—C8—C9168.65 (11)C8—C7—C6—C5176.13 (14)
C16—O2—C8—C771.94 (15)O1—C7—C8—O215.96 (19)
C8—O2—C16—O39.4 (2)C6—C7—C8—O2165.99 (12)
C8—O2—C16—C17169.32 (11)O1—C7—C8—C9100.42 (16)
C10—N1—N2—N30.08 (17)C6—C7—C8—C977.63 (16)
C9—N1—N2—N3176.40 (12)O2—C8—C9—N175.59 (14)
N2—N1—C9—C891.87 (15)C7—C8—C9—N1166.39 (11)
C10—N1—C9—C883.59 (18)N1—C10—C11—N30.26 (16)
N2—N1—C10—C110.11 (15)C15—C10—C11—N3179.16 (14)
C9—N1—C10—C11175.70 (14)N1—C10—C11—C12179.94 (14)
N2—N1—C10—C15179.21 (16)C15—C10—C11—C120.6 (2)
C9—N1—C10—C155.0 (3)N1—C10—C15—C14179.72 (16)
C11—N3—N2—N10.24 (17)C11—C10—C15—C140.5 (2)
N2—N3—C11—C100.32 (18)N3—C11—C12—C13179.43 (17)
N2—N3—C11—C12179.91 (17)C10—C11—C12—C130.3 (3)
C18—N4—C19—C200.4 (3)C14—C13—C12—C110.1 (3)
F1—C1—C2—C3179.88 (15)C13—C14—C15—C100.1 (3)
C6—C1—C2—C31.0 (3)C15—C14—C13—C120.2 (3)
C1—C2—C3—C41.1 (3)C18—C17—C21—C200.8 (2)
C2—C3—C4—C50.1 (3)C16—C17—C21—C20177.42 (15)
C6—C5—C4—C30.9 (3)C21—C17—C18—N40.7 (3)
C5—C6—C1—F1179.08 (14)C16—C17—C18—N4175.74 (16)
C7—C6—C1—F11.4 (2)O3—C16—C17—C18167.62 (16)
C5—C6—C1—C20.0 (2)O2—C16—C17—C1811.0 (2)
C7—C6—C1—C2177.67 (15)O3—C16—C17—C218.8 (2)
C1—C6—C5—C41.0 (3)O2—C16—C17—C21172.55 (13)
C7—C6—C5—C4178.86 (17)C17—C18—N4—C191.3 (3)
O1—C7—C6—C1175.75 (15)C21—C20—C19—N41.1 (3)
C8—C7—C6—C16.2 (2)C17—C21—C20—C191.7 (3)
O1—C7—C6—C51.9 (2)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
C3—H3B···O3i0.932.503.355 (2)154
C8—H8A···F10.982.232.747 (2)112
C9—H9B···O1ii0.972.533.464 (2)161
C18—H18A···O20.932.432.758 (2)101
Symmetry codes: (i) −x+2, −y, −z−1; (ii) −x+1, −y, −z.
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
C3—H3B···O3i0.932.503.355 (2)154
C8—H8A···F10.982.232.747 (2)112
C9—H9B···O1ii0.972.533.464 (2)161
C18—H18A···O20.932.432.758 (2)101
Symmetry codes: (i) −x+2, −y, −z−1; (ii) −x+1, −y, −z.
Acknowledgements top

This project was supported by the Natural Science Foundation of Shandong Province (grant Nos. Z2006B01 and Y2006B07).

references
References top

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Sheldrick, G. M. (1996). SADABS. University of Göttingen, Germany.

Sheldrick, G. M. (1997a). SHELXS97 and SHELXL97. University of Göttingen, Germany.

Sheldrick, G. M. (1997b). SHELXTL. Bruker AXS Inc., Madison, Wisconsin, USA.

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Spek, A. L. (2003). J. Appl. Cryst. 36, 7–13.