organic compounds
6-(Adamantan-1-yl)-3-(3-fluorophenyl)-1,2,4-triazolo[3,4-b][1,3,4]thiadiazole
aDepartment of Chemistry, Quaid-i-Azam University, Islamabad 45320, Pakistan, and bInstitute of Physics, University of Neuchâtel, rue Emile-Argand 11, CH-2009 Neuchâtel, Switzerland
*Correspondence e-mail: shameed@qau.edu.pk
The title molecule, C19H19FN4S, displays Cs molecular symmetry, in which the crystallographic mirror plane bisects the adamantan-1-yl unit while the 3-fluorophenyl triazole ring is located on the mirror plane. The F atom of the 3-fluorophenyl ring is positionally disordered [occupancy ratio 0.9:0.1]. In the crystal, π–π interactions between the triazole and phenyl rings occur [centroid–centroid distance = 3.5849 (7) Å] and weak C—H⋯F interactions form a ribbon propagating in [010].
Related literature
For the biological significance of fused heterocycles, see: Khan et al. (2010a,b); Demirbas et al. (2005); Amir et al. (2007); Ashok et al. (2007); Palekar et al. (2009); Serwar et al. (2009); Akhtar et al. (2007, 2008a,b). For the activity of adamantyl derivatives, see: Kadi et al. (2007); Kouatly et al. (2009); Zahid et al. (2009). For a related structure, see: Khan et al. (2009). For standard bond lengths, see: Allen et al. (1987).
Experimental
Crystal data
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Data collection
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Refinement
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Data collection: X-AREA (Stoe & Cie, 2006); cell X-AREA; data reduction: X-RED32 (Stoe & Cie, 2006); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2009) and Mercury (Macrae et al., 2006); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008), PLATON and publCIF (Westrip, 2010).
Supporting information
https://doi.org/10.1107/S1600536810046428/kp2286sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536810046428/kp2286Isup2.hkl
A mixture of 4-amino-5-(3-fluorophenyl)-2H-1,2,4-triazole-3(4H)-thione (0.2 g, 0.56 mmol) and adamantane-1-carboxylic acid (0.10 g, 0.56 mmol) was refluxed in the presence of POCl3 (5.0 mL) for 4 h [Khan et al. 2010a]. The reaction mixture was cooled to RT, poured into crushed ice and neutralized using solid potassium carbonate until pH 8. The precipitated solid was filtered off, washed with excess water and recrystallised from chloroform to give colourless plate-like crystals, suitable for X-ray analysis.
A region of electron denstiy was located near atom C8 indicating a positional disorder of the 3-fluorophenyl moiety. In the final cycles of least-squares
atom F1 was split to give F1a (occupancy 0.45) bonded to atom C6 and atom F1b (occupancy 0.05) bonded to atom C8. Bond length C8—F1b was refined with a distance restraint of 1.36 (2) Å. H-atoms H6a, H8b and H7 were refined with distance restraints of 0.95 (2) A% with Uiso(H) = 1.2Ueq(C). The remaining H-atoms were included in calculated positions and treated as riding atoms: C—H = 0.95, 0.99, and 1.00 Å for CH-aromatic, CH2 and CH-methine H-atoms, respectively, with Uiso(H) = 1.2Ueq(parent C-atom).Fused heterocycles have received widespread attention in the recent years due to their outstanding biological applications [Khan et al. 2010a; Demirbas et al., 2005; Amir et al., 2007; Ashok et al., 2007; Palekar et al., 2009]. Moreover, compounds bearing an adamantyl moiety are gaining prominence due to their biological and pharmaceutical potential [Kadi et al., 2007; Kouatly et al., 2009; Zahid et al., 2009]. The title compound was synthesised in continuation of our previous studies on the synthesis and biological screening of five membered heterocycles [Akhtar et al., 2007, 2008a, 2008b; Serwar et al.,2009; Khan et al., 2009, 2010b].
Bond distances (Allen et al., 1987) and bond angles are normal and similar to those reported for the 2-fluorophenyl derivative (Khan et al., 2009). The 3-fluorophenyl moiety is positionally disordered, with atom F1 having occupancies of 0.45/0.05 (F1A/F1B), where F1A is bonded to atom C6, while atom F1B is bonded to atom C8 (Fig. 1).
The title molecule possesses crystallographic mirror symmetry; the mirror plane bisects the adamantane moiety while the rest of the molecule lies in the mirror plane. The 3-fluorophenyl moiety is positionally disordered. The 2-fluorophenyl derivative, however, crystallised in the orthorhombic
Pbca and the molecule possess no The 2-fluorophenyl ring is inclined to the triazole ring by 48.6 (1)°, to eliviate steric hindrance.In the crystal of the title compound there are weak C—H···F interactions [C11—H11A···F1Ai, H···F 2.67 Å, C—H···F 145 °, symmetry code (i) -x, y + 1/2, -z + 2)] leading to the formation of a one-dimensional ribbon-like structure running in [010] (Fig. 2). There are also π–π interactions with the centroid-to centroid distance between the mean planes of the triazole ring (N2,C2,N3,N4,C3) and symmetry related phenyl rings (C4—C9) being 3.5849 (7) Å [the perpendicular distance is 3.3278 (1) Å with a slippage of 1.333 Å].
For the biological significance of fused heterocycles, see: Khan et al. (2010a,b); Demirbas et al. (2005); Amir et al. (2007); Ashok et al. (2007); Palekar et al. (2009); Serwar et al. (2009); Akhtar et al. (2007, 2008a,b). For the activity of adamantyl derivatives, see: Kadi et al. (2007); Kouatly et al. (2009); Zahid et al. (2009). For a related structure, see: Khan et al. (2009). For standard bond lengths, see: Allen et al. (1987).
Data collection: X-AREA (Stoe & Cie, 2006); cell
X-AREA (Stoe & Cie, 2006); data reduction: X-RED32 (Stoe & Cie, 2006); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2009) and Mercury (Macrae et al., 2006); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008), PLATON (Spek, 2009) and publCIF (Westrip, 2010).C19H19FN4S | F(000) = 372 |
Mr = 354.44 | Dx = 1.467 Mg m−3 |
Monoclinic, P21/m | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2yb | Cell parameters from 4261 reflections |
a = 11.6385 (16) Å | θ = 3.1–26.0° |
b = 6.6555 (5) Å | µ = 0.22 mm−1 |
c = 11.6634 (16) Å | T = 173 K |
β = 117.379 (14)° | Plate, colourless |
V = 802.25 (17) Å3 | 0.34 × 0.30 × 0.11 mm |
Z = 2 |
Stoe IPDS-2 diffractometer | 1223 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.031 |
Graphite monochromator | θmax = 26.1°, θmin = 3.4° |
φ and ω scans | h = −14→14 |
6164 measured reflections | k = −7→8 |
1708 independent reflections | l = −14→14 |
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)] = 0.030 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.074 | H atoms treated by a mixture of independent and constrained refinement |
S = 0.95 | w = 1/[σ2(Fo2) + (0.0449P)2] where P = (Fo2 + 2Fc2)/3 |
1708 reflections | (Δ/σ)max = 0.001 |
154 parameters | Δρmax = 0.20 e Å−3 |
4 restraints | Δρmin = −0.26 e Å−3 |
C19H19FN4S | V = 802.25 (17) Å3 |
Mr = 354.44 | Z = 2 |
Monoclinic, P21/m | Mo Kα radiation |
a = 11.6385 (16) Å | µ = 0.22 mm−1 |
b = 6.6555 (5) Å | T = 173 K |
c = 11.6634 (16) Å | 0.34 × 0.30 × 0.11 mm |
β = 117.379 (14)° |
Stoe IPDS-2 diffractometer | 1223 reflections with I > 2σ(I) |
6164 measured reflections | Rint = 0.031 |
1708 independent reflections |
R[F2 > 2σ(F2)] = 0.030 | 4 restraints |
wR(F2) = 0.074 | H atoms treated by a mixture of independent and constrained refinement |
S = 0.95 | Δρmax = 0.20 e Å−3 |
1708 reflections | Δρmin = −0.26 e Å−3 |
154 parameters |
Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su's are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles |
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 | Occ. (<1) | |
S1 | 0.42509 (5) | 0.75000 | 0.98501 (5) | 0.0307 (2) | |
F1A | −0.2195 (2) | 0.75000 | 1.1429 (2) | 0.0500 (6) | 0.900 |
N1 | 0.17319 (15) | 0.75000 | 0.85412 (15) | 0.0251 (5) | |
N2 | 0.20898 (15) | 0.75000 | 0.98446 (16) | 0.0243 (5) | |
N3 | 0.35605 (17) | 0.75000 | 1.18934 (17) | 0.0325 (6) | |
N4 | 0.23242 (17) | 0.75000 | 1.18047 (16) | 0.0311 (6) | |
C1 | 0.27709 (18) | 0.75000 | 0.84027 (19) | 0.0249 (6) | |
C2 | 0.33636 (19) | 0.75000 | 1.06956 (19) | 0.0268 (6) | |
C3 | 0.14499 (19) | 0.75000 | 1.05806 (19) | 0.0257 (6) | |
C4 | 0.00535 (19) | 0.75000 | 1.0101 (2) | 0.0248 (6) | |
C5 | −0.0419 (2) | 0.75000 | 1.1000 (2) | 0.0318 (7) | |
C6 | −0.1732 (2) | 0.75000 | 1.0556 (2) | 0.0342 (7) | |
C7 | −0.2599 (2) | 0.75000 | 0.9272 (2) | 0.0378 (8) | |
C8 | −0.2117 (2) | 0.75000 | 0.8390 (2) | 0.0367 (8) | |
C9 | −0.08020 (19) | 0.75000 | 0.8790 (2) | 0.0299 (7) | |
C10 | 0.27522 (18) | 0.75000 | 0.71113 (18) | 0.0254 (6) | |
C11 | 0.34448 (16) | 0.9374 (3) | 0.69694 (15) | 0.0362 (5) | |
C12 | 0.34071 (17) | 0.9366 (3) | 0.56371 (15) | 0.0413 (6) | |
C13 | 0.20148 (17) | 0.9360 (3) | 0.45854 (15) | 0.0428 (6) | |
C14 | 0.1337 (2) | 0.75000 | 0.4720 (2) | 0.0382 (8) | |
C15 | 0.1355 (2) | 0.75000 | 0.6040 (2) | 0.0368 (7) | |
C16 | 0.4093 (2) | 0.75000 | 0.5501 (2) | 0.0441 (9) | |
F1B | −0.2859 (18) | 0.75000 | 0.7166 (11) | 0.052 (5) | 0.100 |
H7 | −0.3504 (11) | 0.75000 | 0.902 (2) | 0.0450* | |
H8A | −0.276 (4) | 0.75000 | 0.7516 (18) | 0.0440* | 0.900 |
H9 | −0.04830 | 0.75000 | 0.81730 | 0.0360* | |
H11A | 0.30140 | 1.05980 | 0.70660 | 0.0440* | |
H11B | 0.43540 | 0.93830 | 0.76530 | 0.0440* | |
H12 | 0.38550 | 1.05930 | 0.55460 | 0.0490* | |
H5 | 0.01550 | 0.75000 | 1.19000 | 0.0380* | |
H13B | 0.19930 | 0.93710 | 0.37270 | 0.0510* | |
H14 | 0.04200 | 0.75000 | 0.40260 | 0.0460* | |
H15A | 0.08990 | 0.87050 | 0.61220 | 0.0440* | 0.500 |
H15B | 0.08990 | 0.62950 | 0.61220 | 0.0440* | 0.500 |
H16A | 0.40810 | 0.75000 | 0.46460 | 0.0530* | |
H16B | 0.50060 | 0.75000 | 0.61760 | 0.0530* | |
H13A | 0.15650 | 1.05780 | 0.46590 | 0.0510* | |
H6B | −0.21 (3) | 0.75000 | 1.11 (2) | 0.0410* | 0.100 |
U11 | U22 | U33 | U12 | U13 | U23 | |
S1 | 0.0210 (3) | 0.0411 (4) | 0.0298 (3) | 0.0000 | 0.0116 (2) | 0.0000 |
F1A | 0.0514 (10) | 0.0583 (11) | 0.0639 (12) | 0.0000 | 0.0467 (9) | 0.0000 |
N1 | 0.0251 (8) | 0.0263 (10) | 0.0252 (8) | 0.0000 | 0.0128 (7) | 0.0000 |
N2 | 0.0218 (8) | 0.0275 (9) | 0.0245 (8) | 0.0000 | 0.0115 (6) | 0.0000 |
N3 | 0.0268 (9) | 0.0403 (12) | 0.0291 (9) | 0.0000 | 0.0118 (7) | 0.0000 |
N4 | 0.0285 (9) | 0.0371 (12) | 0.0285 (9) | 0.0000 | 0.0139 (7) | 0.0000 |
C1 | 0.0219 (9) | 0.0230 (11) | 0.0301 (10) | 0.0000 | 0.0123 (8) | 0.0000 |
C2 | 0.0207 (9) | 0.0285 (12) | 0.0289 (10) | 0.0000 | 0.0095 (8) | 0.0000 |
C3 | 0.0283 (10) | 0.0249 (12) | 0.0269 (10) | 0.0000 | 0.0153 (9) | 0.0000 |
C4 | 0.0260 (10) | 0.0206 (11) | 0.0320 (10) | 0.0000 | 0.0169 (9) | 0.0000 |
C5 | 0.0344 (12) | 0.0298 (13) | 0.0361 (11) | 0.0000 | 0.0205 (9) | 0.0000 |
C6 | 0.0368 (12) | 0.0282 (12) | 0.0520 (14) | 0.0000 | 0.0329 (11) | 0.0000 |
C7 | 0.0270 (11) | 0.0337 (14) | 0.0581 (15) | 0.0000 | 0.0243 (11) | 0.0000 |
C8 | 0.0254 (11) | 0.0401 (15) | 0.0414 (13) | 0.0000 | 0.0126 (10) | 0.0000 |
C9 | 0.0256 (10) | 0.0336 (13) | 0.0326 (11) | 0.0000 | 0.0153 (9) | 0.0000 |
C10 | 0.0217 (10) | 0.0288 (12) | 0.0276 (10) | 0.0000 | 0.0131 (8) | 0.0000 |
C11 | 0.0436 (9) | 0.0339 (10) | 0.0359 (8) | −0.0108 (7) | 0.0223 (7) | −0.0049 (7) |
C12 | 0.0535 (10) | 0.0393 (10) | 0.0405 (9) | −0.0168 (8) | 0.0298 (8) | −0.0033 (7) |
C13 | 0.0565 (11) | 0.0416 (11) | 0.0355 (8) | 0.0138 (8) | 0.0257 (8) | 0.0081 (7) |
C14 | 0.0291 (11) | 0.0576 (17) | 0.0279 (11) | 0.0000 | 0.0132 (9) | 0.0000 |
C15 | 0.0232 (10) | 0.0586 (17) | 0.0290 (10) | 0.0000 | 0.0123 (9) | 0.0000 |
C16 | 0.0313 (12) | 0.073 (2) | 0.0357 (12) | 0.0000 | 0.0220 (10) | 0.0000 |
F1B | 0.030 (7) | 0.084 (12) | 0.031 (7) | 0.0000 | 0.006 (7) | 0.0000 |
S1—C1 | 1.773 (2) | C10—C15 | 1.529 (3) |
S1—C2 | 1.725 (2) | C11—C12 | 1.534 (2) |
F1A—C6 | 1.353 (3) | C12—C13 | 1.517 (3) |
F1B—C8 | 1.285 (12) | C12—C16 | 1.524 (3) |
N1—N2 | 1.379 (2) | C13—C14 | 1.514 (3) |
N1—C1 | 1.292 (3) | C14—C15 | 1.530 (3) |
N2—C3 | 1.371 (3) | C5—H5 | 0.9500 |
N2—C2 | 1.353 (3) | C6—H6B | 0.9 (3) |
N3—N4 | 1.394 (3) | C7—H7 | 0.955 (17) |
N3—C2 | 1.308 (3) | C8—H8A | 0.95 (2) |
N4—C3 | 1.318 (3) | C9—H9 | 0.9500 |
C1—C10 | 1.496 (3) | C11—H11A | 0.9900 |
C3—C4 | 1.455 (3) | C11—H11B | 0.9900 |
C4—C9 | 1.389 (3) | C12—H12 | 1.0000 |
C4—C5 | 1.390 (3) | C13—H13A | 0.9900 |
C5—C6 | 1.370 (4) | C13—H13B | 0.9900 |
C6—C7 | 1.368 (3) | C14—H14 | 1.0000 |
C7—C8 | 1.380 (3) | C15—H15A | 0.9900 |
C8—C9 | 1.380 (4) | C15—H15B | 0.9900 |
C10—C11 | 1.535 (2) | C16—H16A | 0.9900 |
C10—C11i | 1.535 (2) | C16—H16B | 0.9900 |
C1—S1—C2 | 88.25 (11) | C13—C14—C13i | 109.66 (19) |
N2—N1—C1 | 108.20 (17) | C13i—C14—C15 | 109.73 (12) |
N1—N2—C2 | 118.84 (18) | C10—C15—C14 | 109.9 (2) |
N1—N2—C3 | 135.60 (19) | C12—C16—C12i | 109.20 (19) |
C2—N2—C3 | 105.56 (17) | C4—C5—H5 | 121.00 |
N4—N3—C2 | 104.65 (18) | C6—C5—H5 | 121.00 |
N3—N4—C3 | 109.67 (18) | C5—C6—H6B | 122.00 |
S1—C1—N1 | 115.88 (15) | C7—C6—H6B | 115.00 |
S1—C1—C10 | 121.10 (17) | C6—C7—H7 | 119.4 (13) |
N1—C1—C10 | 123.02 (19) | C8—C7—H7 | 122.7 (13) |
S1—C2—N2 | 108.83 (15) | C7—C8—H8A | 114 (3) |
S1—C2—N3 | 138.93 (19) | C9—C8—H8A | 125 (3) |
N2—C2—N3 | 112.2 (2) | C4—C9—H9 | 120.00 |
N2—C3—N4 | 107.9 (2) | C8—C9—H9 | 120.00 |
N2—C3—C4 | 126.26 (18) | C10—C11—H11A | 110.00 |
N4—C3—C4 | 125.9 (2) | C10—C11—H11B | 110.00 |
C3—C4—C5 | 117.99 (19) | C12—C11—H11A | 110.00 |
C3—C4—C9 | 122.1 (2) | C12—C11—H11B | 110.00 |
C5—C4—C9 | 119.9 (2) | H11A—C11—H11B | 108.00 |
C4—C5—C6 | 118.3 (2) | C11—C12—H12 | 109.00 |
F1A—C6—C5 | 118.5 (2) | C13—C12—H12 | 109.00 |
F1A—C6—C7 | 118.4 (2) | C16—C12—H12 | 109.00 |
C5—C6—C7 | 123.2 (2) | C12—C13—H13A | 110.00 |
C6—C7—C8 | 117.9 (2) | C12—C13—H13B | 110.00 |
C7—C8—C9 | 121.1 (2) | C14—C13—H13A | 110.00 |
F1B—C8—C7 | 122.2 (10) | C14—C13—H13B | 110.00 |
F1B—C8—C9 | 116.8 (10) | H13A—C13—H13B | 108.00 |
C4—C9—C8 | 119.6 (2) | C13—C14—H14 | 109.00 |
C1—C10—C11 | 110.08 (11) | C15—C14—H14 | 109.00 |
C1—C10—C15 | 109.90 (19) | C13i—C14—H14 | 109.00 |
C1—C10—C11i | 110.08 (11) | C10—C15—H15A | 110.00 |
C11—C10—C15 | 109.02 (11) | C10—C15—H15B | 110.00 |
C11—C10—C11i | 108.71 (18) | C14—C15—H15A | 110.00 |
C11i—C10—C15 | 109.02 (11) | C14—C15—H15B | 110.00 |
C10—C11—C12 | 109.55 (15) | H15A—C15—H15B | 108.00 |
C11—C12—C13 | 109.96 (17) | C12—C16—H16A | 110.00 |
C11—C12—C16 | 109.64 (15) | C12—C16—H16B | 110.00 |
C13—C12—C16 | 109.24 (16) | H16A—C16—H16B | 108.00 |
C12—C13—C14 | 109.39 (16) | C12i—C16—H16A | 110.00 |
C13—C14—C15 | 109.73 (12) | C12i—C16—H16B | 110.00 |
C2—S1—C1—N1 | 0.00 (1) | N4—C3—C4—C5 | 0.00 (1) |
C2—S1—C1—C10 | 180.00 (1) | N4—C3—C4—C9 | 180.00 (1) |
C1—S1—C2—N2 | 0.00 (1) | C3—C4—C5—C6 | 180.00 (1) |
C1—S1—C2—N3 | −180.00 (1) | C9—C4—C5—C6 | 0.00 (1) |
C1—N1—N2—C2 | 0.00 (1) | C3—C4—C9—C8 | 180.00 (1) |
C1—N1—N2—C3 | 180.00 (1) | C5—C4—C9—C8 | 0.00 (1) |
N2—N1—C1—S1 | 0.00 (1) | C4—C5—C6—F1A | 180.00 (1) |
N2—N1—C1—C10 | 180.00 (1) | C4—C5—C6—C7 | 0.00 (1) |
N1—N2—C3—C4 | 0.00 (1) | F1A—C6—C7—C8 | 180.00 (1) |
C3—N2—C2—N3 | 0.00 (1) | C5—C6—C7—C8 | 0.00 (1) |
N1—N2—C2—S1 | 0.00 (1) | C6—C7—C8—C9 | 0.00 (1) |
C3—N2—C2—S1 | 180.00 (1) | C7—C8—C9—C4 | 0.00 (1) |
N1—N2—C3—N4 | −180.00 (1) | C1—C10—C11—C12 | −179.45 (16) |
C2—N2—C3—C4 | 180.00 (1) | C15—C10—C11—C12 | −58.8 (2) |
C2—N2—C3—N4 | 0.00 (1) | C11i—C10—C11—C12 | 59.90 (19) |
N1—N2—C2—N3 | 180.00 (1) | C1—C10—C15—C14 | 180.00 (1) |
N4—N3—C2—S1 | 180.00 (1) | C11—C10—C15—C14 | 59.27 (12) |
N4—N3—C2—N2 | 0.00 (1) | C10—C11—C12—C13 | 59.6 (2) |
C2—N3—N4—C3 | 0.00 (1) | C10—C11—C12—C16 | −60.5 (2) |
N3—N4—C3—C4 | −180.00 (1) | C11—C12—C13—C14 | −60.1 (2) |
N3—N4—C3—N2 | 0.00 (1) | C16—C12—C13—C14 | 60.2 (2) |
N1—C1—C10—C11 | 120.09 (13) | C11—C12—C16—C12i | 60.3 (2) |
N1—C1—C10—C15 | 0.00 (1) | C13—C12—C16—C12i | −60.27 (19) |
S1—C1—C10—C15 | 180.00 (1) | C12—C13—C14—C15 | 60.2 (2) |
S1—C1—C10—C11 | −59.91 (13) | C12—C13—C14—C13i | −60.4 (2) |
N2—C3—C4—C5 | 180.00 (1) | C13—C14—C15—C10 | −60.28 (14) |
N2—C3—C4—C9 | 0.00 (1) |
Symmetry code: (i) x, −y+3/2, z. |
D—H···A | D—H | H···A | D···A | D—H···A |
C11—H11A···F1Aii | 0.99 | 2.67 | 3.526 (3) | 145 |
Symmetry code: (ii) −x, y+1/2, −z+2. |
Experimental details
Crystal data | |
Chemical formula | C19H19FN4S |
Mr | 354.44 |
Crystal system, space group | Monoclinic, P21/m |
Temperature (K) | 173 |
a, b, c (Å) | 11.6385 (16), 6.6555 (5), 11.6634 (16) |
β (°) | 117.379 (14) |
V (Å3) | 802.25 (17) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 0.22 |
Crystal size (mm) | 0.34 × 0.30 × 0.11 |
Data collection | |
Diffractometer | Stoe IPDS2 |
Absorption correction | – |
No. of measured, independent and observed [I > 2σ(I)] reflections | 6164, 1708, 1223 |
Rint | 0.031 |
(sin θ/λ)max (Å−1) | 0.620 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.030, 0.074, 0.95 |
No. of reflections | 1708 |
No. of parameters | 154 |
No. of restraints | 4 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.20, −0.26 |
Computer programs: X-AREA (Stoe & Cie, 2006), X-RED32 (Stoe & Cie, 2006), SHELXS97 (Sheldrick, 2008), PLATON (Spek, 2009) and Mercury (Macrae et al., 2006), SHELXL97 (Sheldrick, 2008), PLATON (Spek, 2009) and publCIF (Westrip, 2010).
D—H···A | D—H | H···A | D···A | D—H···A |
C11—H11A···F1Ai | 0.99 | 2.67 | 3.526 (3) | 145 |
Symmetry code: (i) −x, y+1/2, −z+2. |
Acknowledgements
HSE thanks the staff of the X-ray Application Lab of the CSEM, Neuchâtel, for access to the X-ray diffraction equipment.
References
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This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
Fused heterocycles have received widespread attention in the recent years due to their outstanding biological applications [Khan et al. 2010a; Demirbas et al., 2005; Amir et al., 2007; Ashok et al., 2007; Palekar et al., 2009]. Moreover, compounds bearing an adamantyl moiety are gaining prominence due to their biological and pharmaceutical potential [Kadi et al., 2007; Kouatly et al., 2009; Zahid et al., 2009]. The title compound was synthesised in continuation of our previous studies on the synthesis and biological screening of five membered heterocycles [Akhtar et al., 2007, 2008a, 2008b; Serwar et al.,2009; Khan et al., 2009, 2010b].
Bond distances (Allen et al., 1987) and bond angles are normal and similar to those reported for the 2-fluorophenyl derivative (Khan et al., 2009). The 3-fluorophenyl moiety is positionally disordered, with atom F1 having occupancies of 0.45/0.05 (F1A/F1B), where F1A is bonded to atom C6, while atom F1B is bonded to atom C8 (Fig. 1).
The title molecule possesses crystallographic mirror symmetry; the mirror plane bisects the adamantane moiety while the rest of the molecule lies in the mirror plane. The 3-fluorophenyl moiety is positionally disordered. The 2-fluorophenyl derivative, however, crystallised in the orthorhombic space group Pbca and the molecule possess no crystallographic symmetry. The 2-fluorophenyl ring is inclined to the triazole ring by 48.6 (1)°, to eliviate steric hindrance.
In the crystal of the title compound there are weak C—H···F interactions [C11—H11A···F1Ai, H···F 2.67 Å, C—H···F 145 °, symmetry code (i) -x, y + 1/2, -z + 2)] leading to the formation of a one-dimensional ribbon-like structure running in [010] (Fig. 2). There are also π–π interactions with the centroid-to centroid distance between the mean planes of the triazole ring (N2,C2,N3,N4,C3) and symmetry related phenyl rings (C4—C9) being 3.5849 (7) Å [the perpendicular distance is 3.3278 (1) Å with a slippage of 1.333 Å].