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A study of three isomeric com­pounds containing a phenolic moiety attached to the nitro­gen-rich triazolo–triazole bicycle is presented. In the three isomers, the phenolic OH group is in the ortho, meta and para positions. The crystal structure analysis of the meta isomer (C10H9N5O) shows that the 2H-tautomer is present in the crystal and that the mol­ecule adopts a substanti­ally planar geometry. However, the conformation found in the crystal is different com­pared to the monoprotonated cation of the same com­pound previously investigated in several salts. The packing of the meta isomer is driven by the formation of strong hydrogen bonds and shows the formation of infinite planar ribbons, parallel to a, formed around 21 crystallographic axes. The three isomers were tested against some cancer cell lines and also against normal cell lines. The ortho isomer shows a weak anti­proliferative activity, the meta isomer shows significant anti­proliferative activity against some cancer lines and no activity against healthy cell lines, and the para isomer is active against all the tested cell lines.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229619012403/yp3193sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229619012403/yp3193Isup2.hkl
Contains datablock I

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S2053229619012403/yp3193Isup3.cml
Supplementary material

CCDC reference: 1951747

Computing details top

Data collection: COLLECT (Nonius, 1999); cell refinement: DIRAX/LSQ (Duisenberg et al., 2000); data reduction: EVALCCD (Duisenberg et al., 2003); program(s) used to solve structure: SIR97 (Altomare et al., 1999); program(s) used to refine structure: SHELXL2016 (Sheldrick, 2015); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012) and Mercury (Macrae et al., 2008); software used to prepare material for publication: WinGX (Farrugia, 2012).

3-(3-Hydroxyphenyl)-6-methyl-1H-[1,2,4]triazolo[3,2-c][1,2,4]triazole top
Crystal data top
C10H9N5ODx = 1.500 Mg m3
Mr = 215.22Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PbcaCell parameters from 138 reflections
a = 12.251 (5) Åθ = 3.6–23.8°
b = 7.457 (3) ŵ = 0.11 mm1
c = 20.863 (6) ÅT = 173 K
V = 1906.0 (12) Å3Prism, colourless
Z = 80.40 × 0.40 × 0.10 mm
F(000) = 896
Data collection top
Bruker–Nonius KappaCCD
diffractometer
2171 independent reflections
Radiation source: normal-focus sealed tube1351 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.071
Detector resolution: 9 pixels mm-1θmax = 27.6°, θmin = 3.3°
CCD rotation images, thick slices scansh = 1514
Absorption correction: multi-scan
(SADABS; Bruker, 2001)
k = 89
Tmin = 0.950, Tmax = 0.981l = 2626
14282 measured reflections
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)] = 0.056Hydrogen site location: mixed
wR(F2) = 0.118H atoms treated by a mixture of independent and constrained refinement
S = 1.07 w = 1/[σ2(Fo2) + (0.0463P)2 + 0.6519P]
where P = (Fo2 + 2Fc2)/3
2171 reflections(Δ/σ)max < 0.001
152 parametersΔρmax = 0.22 e Å3
0 restraintsΔρmin = 0.22 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.64043 (16)0.4373 (3)0.12741 (9)0.0257 (5)
C20.68973 (18)0.5154 (3)0.18050 (10)0.0314 (5)
H20.7668900.5131310.1849630.038*
C30.62617 (17)0.5961 (3)0.22650 (10)0.0342 (6)
H30.6598750.6517630.2623610.041*
C40.51393 (17)0.5970 (3)0.22113 (10)0.0315 (5)
H40.4708610.6532200.2532250.038*
C50.46382 (16)0.5162 (3)0.16903 (9)0.0270 (5)
C60.52748 (16)0.4378 (3)0.12145 (9)0.0258 (5)
H60.4938560.3848220.0850500.031*
C70.71111 (15)0.3614 (3)0.07796 (9)0.0241 (5)
C80.77250 (15)0.2236 (3)0.00878 (10)0.0248 (5)
C90.64025 (15)0.1345 (3)0.06245 (10)0.0259 (5)
C100.57846 (17)0.0455 (3)0.11475 (10)0.0358 (6)
H10A0.5002490.0490970.1049750.054*
H10B0.5921170.1082400.1552430.054*
H10C0.6022260.0795170.1185690.054*
N10.81769 (13)0.3690 (2)0.07994 (8)0.0285 (4)
N20.85626 (14)0.2823 (2)0.02622 (8)0.0279 (4)
H2N0.9308 (18)0.281 (3)0.0182 (10)0.034*
N30.75169 (13)0.1352 (2)0.06233 (8)0.0269 (4)
N40.59113 (12)0.2149 (2)0.01296 (8)0.0253 (4)
N50.68080 (12)0.2726 (2)0.02216 (8)0.0231 (4)
O10.35366 (12)0.5210 (2)0.16658 (8)0.0408 (4)
H1O0.330 (2)0.461 (3)0.1305 (12)0.049*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0267 (11)0.0256 (11)0.0246 (11)0.0013 (8)0.0017 (8)0.0068 (10)
C20.0278 (12)0.0397 (12)0.0268 (11)0.0038 (9)0.0043 (9)0.0052 (10)
C30.0376 (14)0.0420 (13)0.0229 (11)0.0068 (10)0.0040 (9)0.0004 (11)
C40.0351 (13)0.0365 (12)0.0229 (11)0.0002 (10)0.0017 (9)0.0024 (10)
C50.0230 (12)0.0305 (11)0.0277 (12)0.0002 (8)0.0008 (9)0.0047 (10)
C60.0270 (12)0.0273 (11)0.0232 (11)0.0020 (9)0.0031 (9)0.0018 (9)
C70.0207 (12)0.0256 (11)0.0260 (11)0.0022 (8)0.0035 (8)0.0069 (10)
C80.0182 (10)0.0280 (11)0.0283 (12)0.0004 (9)0.0016 (9)0.0063 (10)
C90.0214 (12)0.0285 (11)0.0279 (12)0.0024 (8)0.0000 (8)0.0035 (10)
C100.0276 (12)0.0443 (13)0.0355 (13)0.0050 (10)0.0006 (10)0.0096 (11)
N10.0229 (10)0.0336 (10)0.0288 (10)0.0018 (7)0.0004 (7)0.0040 (9)
N20.0158 (9)0.0362 (10)0.0318 (10)0.0014 (8)0.0008 (8)0.0042 (9)
N30.0205 (10)0.0311 (9)0.0291 (10)0.0004 (7)0.0017 (7)0.0034 (8)
N40.0202 (9)0.0308 (9)0.0249 (10)0.0016 (7)0.0032 (7)0.0013 (8)
N50.0177 (9)0.0248 (9)0.0269 (10)0.0015 (7)0.0005 (7)0.0046 (8)
O10.0243 (9)0.0600 (11)0.0381 (9)0.0026 (7)0.0004 (7)0.0150 (9)
Geometric parameters (Å, º) top
C1—C61.389 (3)C8—N31.322 (3)
C1—C21.390 (3)C8—N21.333 (3)
C1—C71.461 (3)C8—N51.346 (2)
C2—C31.375 (3)C9—N41.337 (3)
C2—H20.9500C9—N31.365 (3)
C3—C41.380 (3)C9—C101.485 (3)
C3—H30.9500C10—H10A0.9800
C4—C51.386 (3)C10—H10B0.9800
C4—H40.9500C10—H10C0.9800
C5—O11.351 (3)N1—N21.377 (2)
C5—C61.391 (3)N2—H2N0.93 (2)
C6—H60.9500N4—N51.389 (2)
C7—N11.308 (3)O1—H1O0.92 (3)
C7—N51.390 (2)
C6—C1—C2120.19 (19)N3—C8—N5112.32 (16)
C6—C1—C7121.89 (18)N2—C8—N5106.88 (18)
C2—C1—C7117.88 (18)N4—C9—N3116.55 (18)
C3—C2—C1119.6 (2)N4—C9—C10122.58 (17)
C3—C2—H2120.2N3—C9—C10120.86 (19)
C1—C2—H2120.2C9—C10—H10A109.5
C2—C3—C4120.7 (2)C9—C10—H10B109.5
C2—C3—H3119.7H10A—C10—H10B109.5
C4—C3—H3119.7C9—C10—H10C109.5
C3—C4—C5120.2 (2)H10A—C10—H10C109.5
C3—C4—H4119.9H10B—C10—H10C109.5
C5—C4—H4119.9C7—N1—N2107.25 (17)
O1—C5—C4117.43 (18)C8—N2—N1109.62 (16)
O1—C5—C6122.95 (18)C8—N2—H2N130.9 (13)
C4—C5—C6119.60 (19)N1—N2—H2N119.3 (13)
C1—C6—C5119.72 (19)C8—N3—C9101.32 (16)
C1—C6—H6120.1C9—N4—N5100.98 (15)
C5—C6—H6120.1C8—N5—N4108.83 (16)
N1—C7—N5108.30 (17)C8—N5—C7107.94 (15)
N1—C7—C1123.56 (19)N4—N5—C7143.23 (16)
N5—C7—C1128.14 (17)C5—O1—H1O109.4 (15)
N3—C8—N2140.80 (18)
C6—C1—C2—C31.2 (3)C7—N1—N2—C80.6 (2)
C7—C1—C2—C3176.81 (18)N2—C8—N3—C9179.7 (3)
C1—C2—C3—C41.3 (3)N5—C8—N3—C90.5 (2)
C2—C3—C4—C50.0 (3)N4—C9—N3—C80.3 (2)
C3—C4—C5—O1179.8 (2)C10—C9—N3—C8179.31 (18)
C3—C4—C5—C61.5 (3)N3—C9—N4—N50.0 (2)
C2—C1—C6—C50.3 (3)C10—C9—N4—N5179.02 (18)
C7—C1—C6—C5178.19 (17)N3—C8—N5—N40.5 (2)
O1—C5—C6—C1179.72 (19)N2—C8—N5—N4179.65 (15)
C4—C5—C6—C11.6 (3)N3—C8—N5—C7179.00 (16)
C6—C1—C7—N1175.36 (19)N2—C8—N5—C70.9 (2)
C2—C1—C7—N12.6 (3)C9—N4—N5—C80.25 (19)
C6—C1—C7—N54.1 (3)C9—N4—N5—C7178.9 (2)
C2—C1—C7—N5177.93 (19)N1—C7—N5—C81.3 (2)
N5—C7—N1—N21.2 (2)C1—C7—N5—C8179.16 (19)
C1—C7—N1—N2179.26 (17)N1—C7—N5—N4179.5 (2)
N3—C8—N2—N1179.6 (2)C1—C7—N5—N40.0 (4)
N5—C8—N2—N10.2 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C6—H6···N40.952.683.352 (3)128
C10—H10A···N1i0.982.383.338 (3)167
N2—H2N···N4ii0.93 (2)1.97 (2)2.891 (3)172.6 (19)
O1—H1O···N3i0.92 (3)1.86 (3)2.765 (2)167 (2)
Symmetry codes: (i) x1/2, y+1/2, z; (ii) x+1/2, y+1/2, z.
 

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