Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807054700/sj2399sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536807054700/sj2399Isup2.hkl |
CCDC reference: 672823
The title compound was prepared according to the literature method of Wan et al. (2006). Single crystals suitable for X-ray diffraction were obtained by slow evaporation of an ethyl acetate solution at room temperature over a period of six days.
All H-atoms were positioned geometrically and refined using a riding model with d(C—H) = 0.93 Å, Uiso=1.2Ueq (C) for aromatic and 0.97 Å, Uiso = 1.2Ueq (C) for CH2 atoms.
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).
Fig. 1. The structure of the compound (I) showing 50% probability displacement ellipsoids and the atom numbering scheme. | |
Fig. 2. A packing diagram of (I), viewed down the a axis |
C15H10Br2ClN3O | Z = 2 |
Mr = 443.53 | F(000) = 432 |
Triclinic, P1 | Dx = 1.837 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 7.7509 (18) Å | Cell parameters from 2538 reflections |
b = 9.182 (2) Å | θ = 2.4–25.6° |
c = 12.563 (3) Å | µ = 5.22 mm−1 |
α = 73.058 (3)° | T = 293 K |
β = 76.442 (3)° | Plate, colourless |
γ = 71.700 (3)° | 0.25 × 0.23 × 0.06 mm |
V = 801.9 (3) Å3 |
Siemens SMART 1000 CCD area detector diffractometer | 2964 independent reflections |
Radiation source: fine-focus sealed tube | 2528 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.012 |
Detector resolution: 8.33 pixels mm-1 | θmax = 25.7°, θmin = 1.7° |
ω scans | h = −6→9 |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | k = −11→11 |
Tmin = 0.361, Tmax = 0.738 | l = −15→14 |
4374 measured reflections |
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)] = 0.027 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.071 | H-atom parameters constrained |
S = 1.04 | w = 1/[σ2(Fo2) + (0.0397P)2 + 0.2687P] where P = (Fo2 + 2Fc2)/3 |
2964 reflections | (Δ/σ)max < 0.001 |
199 parameters | Δρmax = 0.69 e Å−3 |
0 restraints | Δρmin = −0.59 e Å−3 |
C15H10Br2ClN3O | γ = 71.700 (3)° |
Mr = 443.53 | V = 801.9 (3) Å3 |
Triclinic, P1 | Z = 2 |
a = 7.7509 (18) Å | Mo Kα radiation |
b = 9.182 (2) Å | µ = 5.22 mm−1 |
c = 12.563 (3) Å | T = 293 K |
α = 73.058 (3)° | 0.25 × 0.23 × 0.06 mm |
β = 76.442 (3)° |
Siemens SMART 1000 CCD area detector diffractometer | 2964 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | 2528 reflections with I > 2σ(I) |
Tmin = 0.361, Tmax = 0.738 | Rint = 0.012 |
4374 measured reflections |
R[F2 > 2σ(F2)] = 0.027 | 0 restraints |
wR(F2) = 0.071 | H-atom parameters constrained |
S = 1.04 | Δρmax = 0.69 e Å−3 |
2964 reflections | Δρmin = −0.59 e Å−3 |
199 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
Br1 | 0.10429 (4) | 0.39211 (3) | 0.34085 (2) | 0.04875 (11) | |
Br2 | 0.44143 (4) | 0.43973 (3) | 0.14942 (2) | 0.05179 (11) | |
Cl1 | 0.34216 (14) | 0.86655 (11) | 0.01049 (10) | 0.0815 (3) | |
N1 | 0.5040 (3) | 0.4005 (3) | 0.39885 (19) | 0.0444 (5) | |
N2 | 0.6829 (3) | 0.3765 (3) | 0.3484 (2) | 0.0556 (6) | |
N3 | 0.7793 (3) | 0.2462 (3) | 0.4054 (2) | 0.0594 (7) | |
O1 | 0.0957 (3) | 0.7883 (3) | 0.2727 (2) | 0.0677 (6) | |
C1 | 0.4867 (4) | 0.2817 (3) | 0.4925 (2) | 0.0414 (6) | |
C2 | 0.3399 (4) | 0.2528 (4) | 0.5773 (3) | 0.0541 (7) | |
H2 | 0.2212 | 0.3188 | 0.5761 | 0.065* | |
C3 | 0.3822 (5) | 0.1211 (4) | 0.6622 (3) | 0.0712 (10) | |
H3 | 0.2884 | 0.0968 | 0.7200 | 0.085* | |
C4 | 0.5594 (5) | 0.0216 (4) | 0.6660 (3) | 0.0731 (10) | |
H4 | 0.5804 | −0.0659 | 0.7263 | 0.088* | |
C5 | 0.7018 (5) | 0.0493 (4) | 0.5840 (3) | 0.0634 (9) | |
H5 | 0.8198 | −0.0176 | 0.5864 | 0.076* | |
C6 | 0.6638 (4) | 0.1829 (3) | 0.4955 (3) | 0.0474 (7) | |
C7 | 0.3712 (4) | 0.5435 (3) | 0.3528 (2) | 0.0443 (6) | |
H7A | 0.4347 | 0.6252 | 0.3163 | 0.053* | |
H7B | 0.2812 | 0.5782 | 0.4146 | 0.053* | |
C8 | 0.2698 (3) | 0.5274 (3) | 0.2683 (2) | 0.0396 (6) | |
C9 | 0.1419 (4) | 0.6891 (3) | 0.2196 (2) | 0.0443 (6) | |
C10 | 0.0762 (4) | 0.7164 (3) | 0.1099 (2) | 0.0465 (7) | |
C11 | 0.1573 (4) | 0.7987 (3) | 0.0101 (3) | 0.0574 (8) | |
C12 | 0.0944 (6) | 0.8256 (4) | −0.0910 (3) | 0.0786 (12) | |
H12 | 0.1506 | 0.8800 | −0.1578 | 0.094* | |
C13 | −0.0504 (7) | 0.7714 (5) | −0.0909 (4) | 0.0878 (13) | |
H13 | −0.0920 | 0.7881 | −0.1582 | 0.105* | |
C14 | −0.1343 (6) | 0.6934 (5) | 0.0063 (4) | 0.0781 (11) | |
H14 | −0.2346 | 0.6593 | 0.0050 | 0.094* | |
C15 | −0.0727 (4) | 0.6640 (4) | 0.1074 (3) | 0.0589 (8) | |
H15 | −0.1306 | 0.6095 | 0.1735 | 0.071* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Br1 | 0.04169 (17) | 0.04869 (18) | 0.05735 (19) | −0.01748 (12) | −0.00454 (13) | −0.01130 (13) |
Br2 | 0.04431 (17) | 0.05571 (19) | 0.04718 (18) | −0.00010 (13) | 0.00003 (12) | −0.01991 (13) |
Cl1 | 0.0693 (6) | 0.0616 (5) | 0.1009 (7) | −0.0246 (4) | 0.0143 (5) | −0.0143 (5) |
N1 | 0.0339 (12) | 0.0526 (14) | 0.0472 (13) | −0.0139 (10) | −0.0044 (10) | −0.0116 (11) |
N2 | 0.0350 (13) | 0.0698 (17) | 0.0593 (16) | −0.0190 (12) | −0.0050 (11) | −0.0073 (13) |
N3 | 0.0387 (13) | 0.0676 (17) | 0.0655 (17) | −0.0140 (12) | −0.0068 (12) | −0.0069 (14) |
O1 | 0.0695 (15) | 0.0545 (13) | 0.0823 (17) | 0.0054 (11) | −0.0242 (13) | −0.0349 (12) |
C1 | 0.0414 (15) | 0.0452 (15) | 0.0423 (14) | −0.0140 (12) | −0.0050 (12) | −0.0158 (12) |
C2 | 0.0463 (17) | 0.0572 (18) | 0.0503 (17) | −0.0078 (14) | 0.0013 (13) | −0.0132 (14) |
C3 | 0.065 (2) | 0.069 (2) | 0.062 (2) | −0.0191 (18) | 0.0106 (17) | −0.0047 (18) |
C4 | 0.073 (2) | 0.053 (2) | 0.072 (2) | −0.0104 (17) | −0.0037 (19) | 0.0046 (17) |
C5 | 0.0552 (19) | 0.0501 (18) | 0.077 (2) | −0.0038 (15) | −0.0121 (17) | −0.0122 (16) |
C6 | 0.0411 (15) | 0.0466 (16) | 0.0565 (17) | −0.0120 (12) | −0.0048 (13) | −0.0169 (13) |
C7 | 0.0434 (15) | 0.0438 (15) | 0.0499 (16) | −0.0140 (12) | −0.0075 (12) | −0.0145 (12) |
C8 | 0.0338 (13) | 0.0414 (14) | 0.0434 (14) | −0.0110 (11) | 0.0020 (11) | −0.0148 (11) |
C9 | 0.0343 (14) | 0.0457 (15) | 0.0518 (16) | −0.0098 (11) | −0.0011 (12) | −0.0152 (13) |
C10 | 0.0427 (15) | 0.0410 (15) | 0.0500 (16) | 0.0001 (12) | −0.0076 (13) | −0.0139 (12) |
C11 | 0.0537 (18) | 0.0425 (16) | 0.062 (2) | 0.0004 (13) | −0.0004 (15) | −0.0129 (14) |
C12 | 0.103 (3) | 0.057 (2) | 0.050 (2) | 0.009 (2) | −0.012 (2) | −0.0064 (16) |
C13 | 0.106 (4) | 0.080 (3) | 0.072 (3) | 0.010 (2) | −0.043 (3) | −0.024 (2) |
C14 | 0.070 (2) | 0.073 (2) | 0.098 (3) | 0.0038 (19) | −0.043 (2) | −0.031 (2) |
C15 | 0.0494 (18) | 0.0570 (19) | 0.070 (2) | −0.0050 (14) | −0.0172 (15) | −0.0174 (16) |
Br1—C8 | 1.952 (3) | C5—C6 | 1.400 (4) |
Br2—C8 | 1.935 (3) | C5—H5 | 0.9300 |
Cl1—C11 | 1.734 (4) | C7—C8 | 1.524 (4) |
N1—N2 | 1.360 (3) | C7—H7A | 0.9700 |
N1—C1 | 1.364 (4) | C7—H7B | 0.9700 |
N1—C7 | 1.451 (3) | C8—C9 | 1.547 (4) |
N2—N3 | 1.301 (4) | C9—C10 | 1.507 (4) |
N3—C6 | 1.374 (4) | C10—C11 | 1.384 (4) |
O1—C9 | 1.200 (3) | C10—C15 | 1.392 (4) |
C1—C6 | 1.390 (4) | C11—C12 | 1.394 (5) |
C1—C2 | 1.399 (4) | C12—C13 | 1.362 (6) |
C2—C3 | 1.368 (5) | C12—H12 | 0.9300 |
C2—H2 | 0.9300 | C13—C14 | 1.355 (6) |
C3—C4 | 1.393 (5) | C13—H13 | 0.9300 |
C3—H3 | 0.9300 | C14—C15 | 1.385 (5) |
C4—C5 | 1.355 (5) | C14—H14 | 0.9300 |
C4—H4 | 0.9300 | C15—H15 | 0.9300 |
N2—N1—C1 | 109.8 (2) | H7A—C7—H7B | 107.5 |
N2—N1—C7 | 118.7 (2) | C7—C8—C9 | 110.2 (2) |
C1—N1—C7 | 131.4 (2) | C7—C8—Br2 | 110.90 (17) |
N3—N2—N1 | 108.8 (2) | C9—C8—Br2 | 111.06 (19) |
N2—N3—C6 | 108.5 (2) | C7—C8—Br1 | 111.43 (18) |
N1—C1—C6 | 104.4 (2) | C9—C8—Br1 | 104.46 (17) |
N1—C1—C2 | 133.8 (3) | Br2—C8—Br1 | 108.57 (13) |
C6—C1—C2 | 121.8 (3) | O1—C9—C10 | 122.2 (3) |
C3—C2—C1 | 115.7 (3) | O1—C9—C8 | 118.0 (3) |
C3—C2—H2 | 122.2 | C10—C9—C8 | 119.8 (2) |
C1—C2—H2 | 122.2 | C11—C10—C15 | 118.4 (3) |
C2—C3—C4 | 123.0 (3) | C11—C10—C9 | 121.1 (3) |
C2—C3—H3 | 118.5 | C15—C10—C9 | 120.4 (3) |
C4—C3—H3 | 118.5 | C10—C11—C12 | 120.9 (4) |
C5—C4—C3 | 121.5 (3) | C10—C11—Cl1 | 119.5 (3) |
C5—C4—H4 | 119.3 | C12—C11—Cl1 | 119.6 (3) |
C3—C4—H4 | 119.3 | C13—C12—C11 | 119.3 (4) |
C4—C5—C6 | 117.2 (3) | C13—C12—H12 | 120.3 |
C4—C5—H5 | 121.4 | C11—C12—H12 | 120.3 |
C6—C5—H5 | 121.4 | C14—C13—C12 | 120.7 (4) |
N3—C6—C1 | 108.5 (3) | C14—C13—H13 | 119.6 |
N3—C6—C5 | 130.6 (3) | C12—C13—H13 | 119.6 |
C1—C6—C5 | 120.9 (3) | C13—C14—C15 | 120.9 (4) |
N1—C7—C8 | 115.0 (2) | C13—C14—H14 | 119.6 |
N1—C7—H7A | 108.5 | C15—C14—H14 | 119.6 |
C8—C7—H7A | 108.5 | C14—C15—C10 | 119.7 (4) |
N1—C7—H7B | 108.5 | C14—C15—H15 | 120.1 |
C8—C7—H7B | 108.5 | C10—C15—H15 | 120.1 |
D—H···A | D—H | H···A | D···A | D—H···A |
C7—H7A···Cg2i | 0.97 | 2.87 | 3.523 | 126 |
C7—H7B···Cg1i | 0.97 | 2.88 | 3.484 | 122 |
Symmetry code: (i) −x+1, −y+1, −z+1. |
Experimental details
Crystal data | |
Chemical formula | C15H10Br2ClN3O |
Mr | 443.53 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 293 |
a, b, c (Å) | 7.7509 (18), 9.182 (2), 12.563 (3) |
α, β, γ (°) | 73.058 (3), 76.442 (3), 71.700 (3) |
V (Å3) | 801.9 (3) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 5.22 |
Crystal size (mm) | 0.25 × 0.23 × 0.06 |
Data collection | |
Diffractometer | Siemens SMART 1000 CCD area detector diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 1996) |
Tmin, Tmax | 0.361, 0.738 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 4374, 2964, 2528 |
Rint | 0.012 |
(sin θ/λ)max (Å−1) | 0.611 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.027, 0.071, 1.04 |
No. of reflections | 2964 |
No. of parameters | 199 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.69, −0.59 |
Computer programs: SMART (Siemens, 1996), SAINT (Siemens, 1996), SHELXS97 (Sheldrick, 1997a), SHELXL97 (Sheldrick, 1997a), SHELXTL (Sheldrick, 1997b), PARST (Nardelli, 1995) and PLATON (Spek, 2003).
D—H···A | D—H | H···A | D···A | D—H···A |
C7—H7A···Cg2i | 0.97 | 2.867 | 3.523 | 125.74 |
C7—H7B···Cg1i | 0.97 | 2.878 | 3.484 | 121.49 |
Symmetry code: (i) −x+1, −y+1, −z+1. |
Recently we reported the structure of 2-(1H-1,2,3-benzotriazol-1-yl)-1-benzoylethyl 2-chlorobenzoate (II) (Wan et al., 2006). As part of our ongoing investigation of triazole derivatives with greater pharmacological activity, the title compound, (I), was synthesized and its structure is presented here, Fig. 1.
In the title compound (I), all bond lengths and angles are within normal ranges (Allen et al., 1987) and are comparable to those in the related compound, (II). The whole molecule is non-planar with a dihedral angle of 57.09 (1)° between the C10—C15 benzene ring and N1—N3/C1—C6 benzotriazole ring. The benzotriazole system is essentially planar with a dihedral angle of 3.27 (2)° between the N1—N3/C1/C6 triazole ring and C1—C6 benzene ring.
In the crystal structure, the packing is stabilized by C—H···π interactions (Table 1) and weak Br···N and Br···Br van der Waals forces with the distances Br1···N2, Br1···N3, Br2—N2 and Br2—Br2 of 3.292 (3), 3.054 (3), 3.279 (3) and 3.571 (1) Å, respectively.