supplementary materials


Acta Cryst. (2009). E65, o2598    [ doi:10.1107/S1600536809039178 ]

(E)-3-(9-Anthryl)-1-(4-fluorophenyl)-2-(1H-1,2,4-triazol-1-yl)prop-2-en-1-one

G.-Z. Wang, M. Su and C.-H. Zhou

Abstract top

The C=C double-bond in the title compound, C25H16FN3O, has an E configuration. The dihedral angle between the fluorophenyl and triazole rings is 80.57 (2)°.

Comment top

Chalcones have been investigated for a long time due to important biological activities. We have already synthesized and reported several related structures of chalcones (Lu et al., 2009; Wang et al., 2009; Yan et al., 2009). Azole compounds including imidazole and triazole derivatives are important types of antimicrobial drugs in clinical use, and are excellent ligands with several N-atoms which could coordinate with many kinds of metals (Luo et al., 2009; Zhou et al., 2009). The anthracene moiety is well known for its high absorption co-efficient as well as high fluorescence yields. These interesting properties lead us to develop the title anthryl-triazole chalcone derivatives containing the pharmacophore (triazole) and fluorophore (anthracene), and these compounds exhibit good antimicrobial, antitumor and fluorescent properties. Here we present the title compound (I) crystal structure.

The structure of title compound, C25H16FN3O, has orthorhombic (Pbca) symmetry. It is of interest with respect to biological activity. In the structure, the dihedral angle between the benzene and triazole ring is 80.57 (2)°. Weak intermolecular C—H···O and C—H···N interactions contribute to the crystal packing.

Related literature top

For the synthesis, see: Erhardt et al. (1985); Kranz et al. (1980). For the pharmacological activity of azoles including imidazole and triazole derivatives, see: Luo et al. (2009); Zhou et al. (2009). For related structures, see: Lu et al. (2009); Wang et al. (2009); Yan et al. (2009).

Experimental top

Compound (I) was synthesized according to the procedure of Erhardt et al. (1985) and Kranz et al. (1980). Single crystals used in X-ray diffraction studies were grown in dichlormethane by slow evaporation at room temperature.

Refinement top

All the hydrogen atoms were placed at their geometrical positions with C—H = 0.93Å and Uiso(H) = 1.2Ueq(C).

Computing details top

Data collection: SMART (Bruker, 2001); cell refinement: SAINT-Plus (Bruker, 2001); data reduction: SAINT-Plus (Bruker, 2001); 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 (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The molecular structure of (I), showing 50% probability displacement ellipsoids and the atom-numbering scheme.
[Figure 2] Fig. 2. A partial packing diagram. Hydrogen bonds are shown as dashed lines.
(E)-3-(9-Anthryl)-1-(4-fluorophenyl)-2-(1H-1,2,4-triazol-1- yl)prop-2-en-1-one top
Crystal data top
C25H16FN3OF(000) = 1632
Mr = 393.41Dx = 1.363 Mg m3
Orthorhombic, PbcaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2abCell parameters from 5206 reflections
a = 13.1115 (8) Åθ = 2.4–27.6°
b = 13.4737 (8) ŵ = 0.09 mm1
c = 21.7019 (14) ÅT = 298 K
V = 3833.9 (4) Å3Block, yellow
Z = 80.20 × 0.10 × 0.10 mm
Data collection top
Bruker SMART
diffractometer
4187 independent reflections
Radiation source: fine-focus sealed tube3550 reflections with I > 2σ(I)
graphiteRint = 0.041
φ and ω scansθmax = 27.0°, θmin = 2.4°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 166
Tmin = 0.982, Tmax = 0.991k = 1217
16309 measured reflectionsl = 2726
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.064Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.152H-atom parameters constrained
S = 1.14 w = 1/[σ2(Fo2) + (0.0581P)2 + 1.3538P]
where P = (Fo2 + 2Fc2)/3
4187 reflections(Δ/σ)max = 0.001
271 parametersΔρmax = 0.24 e Å3
0 restraintsΔρmin = 0.19 e Å3
Crystal data top
C25H16FN3OV = 3833.9 (4) Å3
Mr = 393.41Z = 8
Orthorhombic, PbcaMo Kα radiation
a = 13.1115 (8) ŵ = 0.09 mm1
b = 13.4737 (8) ÅT = 298 K
c = 21.7019 (14) Å0.20 × 0.10 × 0.10 mm
Data collection top
Bruker SMART
diffractometer
4187 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
3550 reflections with I > 2σ(I)
Tmin = 0.982, Tmax = 0.991Rint = 0.041
16309 measured reflectionsθmax = 27.0°
Refinement top
R[F2 > 2σ(F2)] = 0.064H-atom parameters constrained
wR(F2) = 0.152Δρmax = 0.24 e Å3
S = 1.14Δρmin = 0.19 e Å3
4187 reflectionsAbsolute structure: ?
271 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
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 > 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) top
xyzUiso*/Ueq
C10.33997 (13)0.03462 (14)0.19230 (8)0.0395 (4)
C20.28391 (14)0.00708 (17)0.14089 (9)0.0471 (5)
H20.25860.05720.13770.057*
C30.26557 (17)0.0751 (2)0.09435 (10)0.0613 (6)
H30.22960.05690.05920.074*
C40.30156 (18)0.1692 (2)0.10137 (12)0.0676 (7)
C50.35496 (19)0.19944 (19)0.15162 (13)0.0710 (7)
H50.37710.26480.15510.085*
C60.37565 (16)0.13104 (16)0.19739 (11)0.0544 (5)
H60.41360.14980.23170.065*
C70.35581 (14)0.03737 (14)0.24300 (8)0.0385 (4)
C80.45641 (13)0.03523 (13)0.27672 (8)0.0360 (4)
C90.37480 (17)0.02786 (19)0.38130 (9)0.0587 (6)
H90.31000.00690.36970.070*
C100.50043 (18)0.07070 (17)0.43119 (9)0.0542 (5)
H100.54150.08670.46470.065*
C110.54642 (14)0.03428 (14)0.24860 (8)0.0394 (4)
H110.60440.03100.27320.047*
C120.56121 (13)0.03800 (14)0.18104 (8)0.0376 (4)
C130.53007 (13)0.12230 (14)0.14735 (8)0.0392 (4)
C140.48685 (16)0.20863 (15)0.17516 (9)0.0475 (5)
H140.47830.21040.21770.057*
C150.45807 (18)0.28783 (18)0.14105 (11)0.0589 (6)
H150.43010.34300.16050.071*
C160.46980 (19)0.28793 (19)0.07665 (11)0.0634 (6)
H160.44850.34240.05370.076*
C170.51180 (17)0.20924 (18)0.04815 (10)0.0576 (6)
H170.51980.21050.00560.069*
C180.54443 (14)0.12368 (16)0.08176 (8)0.0437 (5)
C190.58943 (16)0.04302 (16)0.05307 (9)0.0488 (5)
H190.59680.04390.01050.059*
C200.62388 (14)0.03901 (15)0.08563 (9)0.0437 (5)
C210.67370 (18)0.12021 (18)0.05638 (10)0.0583 (6)
H210.68210.11950.01380.070*
C220.7087 (2)0.19767 (19)0.08895 (12)0.0696 (7)
H220.74120.24980.06890.083*
C230.6965 (2)0.20059 (18)0.15352 (12)0.0667 (7)
H230.72140.25450.17570.080*
C240.64870 (17)0.12541 (16)0.18361 (10)0.0532 (5)
H240.64080.12880.22610.064*
C250.61067 (14)0.04183 (14)0.15128 (8)0.0405 (4)
F10.28332 (14)0.23601 (15)0.05633 (9)0.1089 (7)
N10.45059 (11)0.04595 (11)0.34187 (7)0.0386 (4)
N20.40276 (16)0.04324 (16)0.43811 (8)0.0624 (5)
N30.53431 (13)0.07357 (14)0.37481 (7)0.0507 (4)
O10.29069 (10)0.09647 (12)0.25734 (7)0.0580 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0319 (9)0.0475 (11)0.0392 (9)0.0033 (8)0.0027 (7)0.0032 (8)
C20.0384 (10)0.0588 (12)0.0442 (11)0.0026 (9)0.0005 (8)0.0006 (9)
C30.0460 (11)0.0943 (19)0.0437 (11)0.0103 (12)0.0051 (9)0.0090 (12)
C40.0497 (12)0.0877 (19)0.0653 (15)0.0100 (13)0.0023 (11)0.0383 (14)
C50.0600 (14)0.0563 (14)0.097 (2)0.0019 (12)0.0040 (14)0.0270 (14)
C60.0499 (12)0.0502 (12)0.0632 (13)0.0028 (10)0.0088 (10)0.0064 (10)
C70.0342 (9)0.0441 (10)0.0372 (9)0.0024 (8)0.0023 (7)0.0008 (8)
C80.0386 (9)0.0398 (10)0.0297 (8)0.0014 (7)0.0009 (7)0.0012 (7)
C90.0463 (11)0.0879 (17)0.0418 (11)0.0146 (11)0.0088 (9)0.0002 (11)
C100.0641 (13)0.0643 (14)0.0343 (10)0.0054 (11)0.0020 (9)0.0053 (9)
C110.0350 (9)0.0499 (11)0.0334 (9)0.0006 (8)0.0030 (7)0.0003 (8)
C120.0307 (8)0.0506 (11)0.0315 (9)0.0065 (8)0.0011 (7)0.0026 (8)
C130.0324 (8)0.0494 (11)0.0358 (9)0.0089 (8)0.0008 (7)0.0002 (8)
C140.0499 (11)0.0516 (12)0.0411 (10)0.0046 (9)0.0025 (9)0.0013 (9)
C150.0624 (14)0.0503 (13)0.0641 (14)0.0032 (10)0.0060 (11)0.0028 (11)
C160.0622 (14)0.0642 (15)0.0637 (14)0.0088 (12)0.0056 (11)0.0229 (12)
C170.0559 (13)0.0763 (16)0.0405 (11)0.0025 (12)0.0027 (9)0.0155 (11)
C180.0378 (9)0.0573 (12)0.0360 (10)0.0068 (9)0.0002 (8)0.0032 (9)
C190.0485 (11)0.0691 (14)0.0288 (9)0.0086 (10)0.0025 (8)0.0007 (9)
C200.0389 (10)0.0542 (12)0.0381 (10)0.0091 (8)0.0022 (8)0.0093 (9)
C210.0662 (14)0.0628 (15)0.0460 (12)0.0052 (12)0.0095 (10)0.0147 (11)
C220.0804 (17)0.0574 (15)0.0710 (16)0.0056 (13)0.0183 (13)0.0151 (13)
C230.0755 (16)0.0506 (13)0.0741 (16)0.0068 (12)0.0109 (13)0.0064 (12)
C240.0554 (12)0.0562 (13)0.0481 (12)0.0005 (10)0.0085 (10)0.0039 (10)
C250.0355 (9)0.0472 (11)0.0389 (10)0.0084 (8)0.0027 (7)0.0014 (8)
F10.0917 (12)0.1308 (15)0.1043 (13)0.0117 (11)0.0058 (10)0.0780 (12)
N10.0392 (8)0.0445 (9)0.0321 (8)0.0036 (7)0.0021 (6)0.0009 (6)
N20.0652 (12)0.0856 (14)0.0365 (9)0.0080 (11)0.0098 (8)0.0014 (9)
N30.0491 (9)0.0681 (12)0.0350 (8)0.0111 (8)0.0023 (7)0.0072 (8)
O10.0419 (8)0.0665 (10)0.0657 (10)0.0116 (7)0.0041 (7)0.0224 (8)
Geometric parameters (Å, °) top
C1—C61.385 (3)C12—C251.412 (3)
C1—C21.387 (3)C13—C141.428 (3)
C1—C71.481 (3)C13—C181.436 (3)
C2—C31.385 (3)C14—C151.352 (3)
C2—H20.9300C14—H140.9300
C3—C41.362 (4)C15—C161.406 (3)
C3—H30.9300C15—H150.9300
C4—F11.350 (3)C16—C171.345 (3)
C4—C51.358 (4)C16—H160.9300
C5—C61.382 (3)C17—C181.430 (3)
C5—H50.9300C17—H170.9300
C6—H60.9300C18—C191.385 (3)
C7—O11.208 (2)C19—C201.387 (3)
C7—C81.509 (2)C19—H190.9300
C8—C111.329 (2)C20—C211.424 (3)
C8—N11.423 (2)C20—C251.436 (3)
C9—N21.303 (3)C21—C221.342 (3)
C9—N11.334 (2)C21—H210.9300
C9—H90.9300C22—C231.411 (4)
C10—N31.302 (3)C22—H220.9300
C10—N21.341 (3)C23—C241.358 (3)
C10—H100.9300C23—H230.9300
C11—C121.480 (2)C24—C251.417 (3)
C11—H110.9300C24—H240.9300
C12—C131.411 (3)N1—N31.362 (2)
C6—C1—C2119.61 (18)C15—C14—H14119.3
C6—C1—C7120.50 (17)C13—C14—H14119.3
C2—C1—C7119.78 (18)C14—C15—C16120.9 (2)
C3—C2—C1120.1 (2)C14—C15—H15119.5
C3—C2—H2119.9C16—C15—H15119.5
C1—C2—H2119.9C17—C16—C15120.1 (2)
C4—C3—C2118.3 (2)C17—C16—H16120.0
C4—C3—H3120.8C15—C16—H16120.0
C2—C3—H3120.8C16—C17—C18121.6 (2)
F1—C4—C5118.2 (3)C16—C17—H17119.2
F1—C4—C3118.6 (3)C18—C17—H17119.2
C5—C4—C3123.2 (2)C19—C18—C17122.07 (18)
C4—C5—C6118.6 (2)C19—C18—C13119.44 (18)
C4—C5—H5120.7C17—C18—C13118.49 (19)
C6—C5—H5120.7C18—C19—C20122.34 (17)
C5—C6—C1120.1 (2)C18—C19—H19118.8
C5—C6—H6119.9C20—C19—H19118.8
C1—C6—H6119.9C19—C20—C21122.31 (19)
O1—C7—C1121.59 (17)C19—C20—C25119.16 (18)
O1—C7—C8120.36 (17)C21—C20—C25118.53 (19)
C1—C7—C8118.06 (16)C22—C21—C20121.3 (2)
C11—C8—N1120.33 (16)C22—C21—H21119.3
C11—C8—C7123.64 (16)C20—C21—H21119.3
N1—C8—C7115.66 (15)C21—C22—C23120.4 (2)
N2—C9—N1111.61 (19)C21—C22—H22119.8
N2—C9—H9124.2C23—C22—H22119.8
N1—C9—H9124.2C24—C23—C22120.6 (2)
N3—C10—N2116.04 (19)C24—C23—H23119.7
N3—C10—H10122.0C22—C23—H23119.7
N2—C10—H10122.0C23—C24—C25121.1 (2)
C8—C11—C12124.83 (16)C23—C24—H24119.4
C8—C11—H11117.6C25—C24—H24119.4
C12—C11—H11117.6C12—C25—C24122.70 (17)
C13—C12—C25120.59 (16)C12—C25—C20119.28 (17)
C13—C12—C11120.18 (17)C24—C25—C20118.02 (18)
C25—C12—C11119.17 (17)C9—N1—N3108.28 (15)
C12—C13—C14123.48 (17)C9—N1—C8131.20 (16)
C12—C13—C18119.09 (17)N3—N1—C8120.40 (14)
C14—C13—C18117.41 (17)C9—N2—C10101.93 (17)
C15—C14—C13121.49 (19)C10—N3—N1102.13 (16)
C6—C1—C2—C31.3 (3)C14—C13—C18—C19177.72 (18)
C7—C1—C2—C3177.61 (18)C12—C13—C18—C17179.52 (17)
C1—C2—C3—C41.7 (3)C14—C13—C18—C172.0 (3)
C2—C3—C4—F1179.6 (2)C17—C18—C19—C20178.12 (19)
C2—C3—C4—C50.3 (4)C13—C18—C19—C201.6 (3)
F1—C4—C5—C6178.8 (2)C18—C19—C20—C21177.50 (19)
C3—C4—C5—C61.3 (4)C18—C19—C20—C251.4 (3)
C4—C5—C6—C11.6 (4)C19—C20—C21—C22178.3 (2)
C2—C1—C6—C50.4 (3)C25—C20—C21—C220.6 (3)
C7—C1—C6—C5175.9 (2)C20—C21—C22—C230.2 (4)
C6—C1—C7—O1141.0 (2)C21—C22—C23—C240.3 (4)
C2—C1—C7—O135.2 (3)C22—C23—C24—C250.5 (4)
C6—C1—C7—C839.1 (2)C13—C12—C25—C24176.20 (17)
C2—C1—C7—C8144.71 (18)C11—C12—C25—C241.1 (3)
O1—C7—C8—C11131.1 (2)C13—C12—C25—C203.5 (3)
C1—C7—C8—C1148.8 (3)C11—C12—C25—C20179.16 (16)
O1—C7—C8—N141.8 (3)C23—C24—C25—C12179.6 (2)
C1—C7—C8—N1138.21 (17)C23—C24—C25—C200.2 (3)
N1—C8—C11—C12170.82 (17)C19—C20—C25—C121.2 (3)
C7—C8—C11—C121.8 (3)C21—C20—C25—C12179.87 (18)
C8—C11—C12—C1363.7 (3)C19—C20—C25—C24178.53 (18)
C8—C11—C12—C25118.9 (2)C21—C20—C25—C240.4 (3)
C25—C12—C13—C14175.05 (17)N2—C9—N1—N31.0 (3)
C11—C12—C13—C142.2 (3)N2—C9—N1—C8176.88 (19)
C25—C12—C13—C183.3 (3)C11—C8—N1—C9163.3 (2)
C11—C12—C13—C18179.43 (16)C7—C8—N1—C923.5 (3)
C12—C13—C14—C15179.98 (19)C11—C8—N1—N312.2 (3)
C18—C13—C14—C151.6 (3)C7—C8—N1—N3160.99 (17)
C13—C14—C15—C160.0 (3)N1—C9—N2—C100.7 (3)
C14—C15—C16—C171.2 (4)N3—C10—N2—C90.2 (3)
C15—C16—C17—C180.7 (4)N2—C10—N3—N10.4 (3)
C16—C17—C18—C19178.8 (2)C9—N1—N3—C100.8 (2)
C16—C17—C18—C130.9 (3)C8—N1—N3—C10177.23 (17)
C12—C13—C18—C190.7 (3)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
C23—H23···O1i0.932.483.354 (3)156
C5—H5···N3i0.932.553.434 (3)158
Symmetry codes: (i) −x+1, y−1/2, −z+1/2.
Acknowledgements top

We thank Southwest University (SWUB2006018, XSGX0602 and SWUF2007023) and the Natural Science Foundation of Chongqing (2007BB5369) for financial support.

references
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