Literature DB >> 22412559

3-(Adamantan-1-yl)-4-(prop-2-en-1-yl)-1H-1,2,4-triazole-5(4H)-thione.

Maha S Almutairi, Mona M Al-Shehri, Ali A El-Emam, Seik Weng Ng, Edward R T Tiekink.   

Abstract

The title mol-ecule, C(15)H(21)N(3)S, exists as the thione tautomer in the solid state. The 1,2,4-triazole ring is almost planar (r.m.s. deviation = 0.004 Å) and the prop-2-en-1-yl chain is close to being perpendicular to this plane [C-N-C-C torsion angle = 77.1 (5)°]. In the crystal, centrosymmetric dimeric aggregates are formed by pairs of N-H⋯S hydrogen bonds as parts of eight-membered (⋯HNCS)(2) synthons. These are connected into layers parallel to (101) via C-H⋯π inter-actions, where the π-system is the triazole ring. The investigated sample was a nonmerohedral twin; the refined domain ratio was 0.655 (4):0.345 (4).

Entities:  

Year:  2012        PMID: 22412559      PMCID: PMC3295448          DOI: 10.1107/S1600536812005065

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For the biological activity of adamantyl derivatives, see: Vernier et al. (1969 ▶); El-Emam et al. (2004 ▶). Kadi et al. (2007 ▶, 2010 ▶). For the biological activity of adamantyl-1,2,4-triazole derivatives, see: Al-Deeb et al. (2006 ▶). For the separation of diffraction data into twin domains, see: Spek (2009 ▶).

Experimental

Crystal data

C15H21N3S M = 275.41 Monoclinic, a = 13.5833 (17) Å b = 8.6483 (6) Å c = 13.6973 (14) Å β = 115.938 (14)° V = 1447.0 (3) Å3 Z = 4 Mo Kα radiation μ = 0.22 mm−1 T = 100 K 0.35 × 0.15 × 0.10 mm

Data collection

Agilent SuperNova Dual diffractometer with Atlas detector Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011 ▶) T min = 0.929, T max = 0.979 10998 measured reflections 3324 independent reflections 2875 reflections with I > 2σ(I) R int = 0.077

Refinement

R[F 2 > 2σ(F 2)] = 0.081 wR(F 2) = 0.230 S = 1.17 3324 reflections 173 parameters H-atom parameters constrained Δρmax = 0.71 e Å−3 Δρmin = −0.66 e Å−3 Data collection: CrysAlis PRO (Agilent, 2011 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶) and DIAMOND (Brandenburg, 2006 ▶); software used to prepare material for publication: publCIF (Westrip, 2010 ▶). Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812005065/hb6626sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812005065/hb6626Isup2.hkl Supplementary material file. DOI: 10.1107/S1600536812005065/hb6626Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C15H21N3SF(000) = 592
Mr = 275.41Dx = 1.264 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 1371 reflections
a = 13.5833 (17) Åθ = 2.4–27.5°
b = 8.6483 (6) ŵ = 0.22 mm1
c = 13.6973 (14) ÅT = 100 K
β = 115.938 (14)°Prism, colourless
V = 1447.0 (3) Å30.35 × 0.15 × 0.10 mm
Z = 4
Agilent SuperNova Dual diffractometer with Atlas detector3324 independent reflections
Radiation source: SuperNova (Mo) X-ray Source2875 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.077
Detector resolution: 10.4041 pixels mm-1θmax = 27.6°, θmin = 2.8°
ω scansh = −17→15
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011)k = −11→11
Tmin = 0.929, Tmax = 0.979l = −6→17
10998 measured reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.081Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.230H-atom parameters constrained
S = 1.17w = 1/[σ2(Fo2) + (0.0882P)2 + 4.0546P] where P = (Fo2 + 2Fc2)/3
3324 reflections(Δ/σ)max < 0.001
173 parametersΔρmax = 0.71 e Å3
0 restraintsΔρmin = −0.66 e Å3
Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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.
xyzUiso*/Ueq
S10.60052 (9)0.72236 (11)0.51878 (8)0.0170 (3)
N10.6426 (3)0.7440 (4)0.7336 (3)0.0115 (6)
N20.5548 (3)0.5391 (4)0.6557 (3)0.0137 (7)
H2N0.52030.46850.60620.016*
N30.5707 (3)0.5286 (4)0.7620 (3)0.0141 (7)
C10.5976 (3)0.6683 (5)0.6357 (3)0.0127 (7)
C20.6240 (3)0.6536 (4)0.8078 (3)0.0124 (7)
C30.6643 (3)0.6857 (5)0.9271 (3)0.0124 (7)
C40.7912 (3)0.6936 (5)0.9857 (3)0.0152 (8)
H4A0.82240.59540.97470.018*
H4B0.81730.77840.95440.018*
C50.8298 (4)0.7216 (5)1.1068 (3)0.0190 (9)
H50.91150.72861.14350.023*
C60.7923 (4)0.5877 (6)1.1559 (3)0.0238 (10)
H6A0.81760.60521.23460.029*
H6B0.82450.48951.14620.029*
C70.6670 (4)0.5770 (6)1.0993 (3)0.0222 (9)
H70.64290.48851.13070.027*
C80.6281 (3)0.5500 (5)0.9779 (3)0.0176 (8)
H8A0.54730.54110.94190.021*
H8B0.65920.45200.96650.021*
C90.6144 (3)0.8368 (5)0.9470 (3)0.0170 (8)
H9A0.63610.92540.91490.020*
H9B0.53350.82960.91130.020*
C100.6547 (4)0.8630 (6)1.0692 (3)0.0228 (10)
H100.62330.96181.08130.027*
C110.7803 (4)0.8738 (6)1.1234 (3)0.0232 (9)
H11A0.80690.89411.20200.028*
H11B0.80370.96051.09140.028*
C120.6173 (4)0.7278 (6)1.1179 (4)0.0263 (11)
H12A0.53640.72081.08260.032*
H12B0.64190.74471.19660.032*
C130.6875 (3)0.9016 (5)0.7431 (3)0.0157 (8)
H13A0.73160.90790.70170.019*
H13B0.73650.92370.82020.019*
C140.5979 (4)1.0210 (5)0.7008 (3)0.0180 (8)
H140.54091.00800.62950.022*
C150.5939 (4)1.1433 (5)0.7573 (4)0.0234 (10)
H15A0.64971.15930.82880.035*
H15B0.53531.21490.72640.035*
U11U22U33U12U13U23
S10.0220 (6)0.0180 (5)0.0114 (5)−0.0044 (4)0.0077 (4)−0.0016 (4)
N10.0121 (15)0.0121 (14)0.0112 (15)−0.0009 (13)0.0058 (12)0.0001 (12)
N20.0165 (16)0.0116 (15)0.0109 (14)−0.0005 (13)0.0039 (12)−0.0013 (12)
N30.0173 (16)0.0125 (16)0.0114 (15)0.0001 (13)0.0051 (12)−0.0014 (12)
C10.0131 (17)0.0137 (18)0.0104 (16)0.0001 (15)0.0043 (13)−0.0016 (14)
C20.0137 (18)0.0119 (17)0.0127 (17)−0.0005 (14)0.0067 (14)0.0010 (14)
C30.0135 (18)0.0150 (18)0.0108 (16)−0.0018 (15)0.0073 (14)0.0003 (14)
C40.0156 (19)0.0188 (19)0.0121 (17)−0.0012 (16)0.0070 (14)0.0014 (15)
C50.0162 (19)0.025 (2)0.0129 (18)−0.0087 (17)0.0038 (15)0.0021 (16)
C60.023 (2)0.031 (2)0.0132 (18)−0.0073 (19)0.0042 (16)0.0063 (17)
C70.023 (2)0.029 (2)0.0146 (18)−0.0090 (19)0.0088 (16)0.0029 (17)
C80.0174 (19)0.019 (2)0.0155 (18)−0.0065 (16)0.0063 (15)0.0016 (15)
C90.0181 (19)0.0167 (19)0.0173 (19)−0.0002 (16)0.0087 (16)−0.0039 (15)
C100.026 (2)0.030 (2)0.0175 (19)−0.0006 (19)0.0137 (17)−0.0061 (17)
C110.027 (2)0.029 (2)0.0150 (18)−0.0116 (19)0.0107 (17)−0.0096 (17)
C120.024 (2)0.043 (3)0.016 (2)−0.009 (2)0.0134 (17)−0.0073 (19)
C130.0161 (19)0.015 (2)0.0144 (17)−0.0059 (15)0.0054 (15)−0.0007 (14)
C140.021 (2)0.0132 (18)0.0178 (18)−0.0031 (16)0.0071 (16)0.0015 (15)
C150.030 (2)0.015 (2)0.024 (2)−0.0007 (18)0.0103 (18)0.0003 (17)
S1—C11.685 (4)C7—C121.539 (7)
N1—C11.372 (5)C7—H71.0000
N1—C21.390 (5)C8—H8A0.9900
N1—C131.476 (5)C8—H8B0.9900
N2—C11.342 (5)C9—C101.534 (6)
N2—N31.379 (5)C9—H9A0.9900
N2—H2N0.8800C9—H9B0.9900
N3—C21.300 (5)C10—C111.537 (6)
C2—C31.504 (5)C10—C121.538 (7)
C3—C81.550 (5)C10—H101.0000
C3—C91.551 (6)C11—H11A0.9900
C3—C41.552 (5)C11—H11B0.9900
C4—C51.525 (5)C12—H12A0.9900
C4—H4A0.9900C12—H12B0.9900
C4—H4B0.9900C13—C141.506 (6)
C5—C61.533 (6)C13—H13A0.9900
C5—C111.539 (7)C13—H13B0.9900
C5—H51.0000C14—C151.326 (6)
C6—C71.534 (6)C14—H140.9500
C6—H6A0.9900C15—H15A0.9500
C6—H6B0.9900C15—H15B0.9500
C7—C81.527 (6)
C1—N1—C2107.5 (3)C7—C8—C3110.3 (3)
C1—N1—C13121.1 (3)C7—C8—H8A109.6
C2—N1—C13131.0 (3)C3—C8—H8A109.6
C1—N2—N3112.9 (3)C7—C8—H8B109.6
C1—N2—H2N123.6C3—C8—H8B109.6
N3—N2—H2N123.6H8A—C8—H8B108.1
C2—N3—N2104.6 (3)C10—C9—C3110.0 (3)
N2—C1—N1104.2 (3)C10—C9—H9A109.7
N2—C1—S1128.1 (3)C3—C9—H9A109.7
N1—C1—S1127.7 (3)C10—C9—H9B109.7
N3—C2—N1110.8 (3)C3—C9—H9B109.7
N3—C2—C3122.6 (3)H9A—C9—H9B108.2
N1—C2—C3126.4 (3)C9—C10—C11109.1 (3)
C2—C3—C8108.2 (3)C9—C10—C12109.4 (4)
C2—C3—C9111.5 (3)C11—C10—C12110.1 (4)
C8—C3—C9108.1 (3)C9—C10—H10109.4
C2—C3—C4111.4 (3)C11—C10—H10109.4
C8—C3—C4107.5 (3)C12—C10—H10109.4
C9—C3—C4110.1 (3)C10—C11—C5110.0 (4)
C5—C4—C3110.2 (3)C10—C11—H11A109.7
C5—C4—H4A109.6C5—C11—H11A109.7
C3—C4—H4A109.6C10—C11—H11B109.7
C5—C4—H4B109.6C5—C11—H11B109.7
C3—C4—H4B109.6H11A—C11—H11B108.2
H4A—C4—H4B108.1C10—C12—C7108.7 (4)
C4—C5—C6109.6 (3)C10—C12—H12A110.0
C4—C5—C11109.4 (3)C7—C12—H12A110.0
C6—C5—C11109.3 (4)C10—C12—H12B110.0
C4—C5—H5109.5C7—C12—H12B110.0
C6—C5—H5109.5H12A—C12—H12B108.3
C11—C5—H5109.5N1—C13—C14111.4 (3)
C5—C6—C7109.4 (4)N1—C13—H13A109.3
C5—C6—H6A109.8C14—C13—H13A109.3
C7—C6—H6A109.8N1—C13—H13B109.3
C5—C6—H6B109.8C14—C13—H13B109.3
C7—C6—H6B109.8H13A—C13—H13B108.0
H6A—C6—H6B108.2C15—C14—C13123.7 (4)
C8—C7—C6109.7 (4)C15—C14—H14118.2
C8—C7—C12110.0 (4)C13—C14—H14118.2
C6—C7—C12109.6 (4)C14—C15—H15A120.0
C8—C7—H7109.2C14—C15—H15B120.0
C6—C7—H7109.2H15A—C15—H15B120.0
C12—C7—H7109.2
C1—N2—N3—C20.0 (4)C11—C5—C6—C760.0 (5)
N3—N2—C1—N1−0.1 (4)C5—C6—C7—C859.5 (5)
N3—N2—C1—S1177.5 (3)C5—C6—C7—C12−61.4 (5)
C2—N1—C1—N20.2 (4)C6—C7—C8—C3−60.4 (5)
C13—N1—C1—N2−173.0 (3)C12—C7—C8—C360.3 (5)
C2—N1—C1—S1−177.5 (3)C2—C3—C8—C7−179.9 (3)
C13—N1—C1—S19.3 (6)C9—C3—C8—C7−59.1 (4)
N2—N3—C2—N10.1 (4)C4—C3—C8—C759.7 (4)
N2—N3—C2—C3−176.5 (3)C2—C3—C9—C10178.3 (3)
C1—N1—C2—N3−0.2 (5)C8—C3—C9—C1059.6 (4)
C13—N1—C2—N3172.1 (4)C4—C3—C9—C10−57.5 (4)
C1—N1—C2—C3176.2 (4)C3—C9—C10—C1159.2 (5)
C13—N1—C2—C3−11.5 (7)C3—C9—C10—C12−61.3 (5)
N3—C2—C3—C8−1.5 (5)C9—C10—C11—C5−61.2 (5)
N1—C2—C3—C8−177.5 (4)C12—C10—C11—C558.9 (4)
N3—C2—C3—C9−120.2 (4)C4—C5—C11—C1061.1 (4)
N1—C2—C3—C963.8 (5)C6—C5—C11—C10−58.9 (4)
N3—C2—C3—C4116.4 (4)C9—C10—C12—C760.6 (5)
N1—C2—C3—C4−59.6 (5)C11—C10—C12—C7−59.3 (4)
C2—C3—C4—C5−178.4 (3)C8—C7—C12—C10−60.2 (4)
C8—C3—C4—C5−60.1 (4)C6—C7—C12—C1060.6 (4)
C9—C3—C4—C557.4 (4)C1—N1—C13—C1477.1 (5)
C3—C4—C5—C661.0 (5)C2—N1—C13—C14−94.3 (5)
C3—C4—C5—C11−58.8 (4)N1—C13—C14—C15126.8 (4)
C4—C5—C6—C7−59.8 (5)
D—H···AD—HH···AD···AD—H···A
N2—H2N···S1i0.882.433.296 (3)170
C5—H5···Cg1ii1.002.603.529 (6)155
C13—H13A···Cg1iii0.992.813.351 (5)115
Table 1

Hydrogen-bond geometry (Å, °)

Cg1 is the centroid of the C1/C2/N1/N2/N3 ring.

D—H⋯AD—HH⋯ADAD—H⋯A
N2—H2N⋯S1i0.882.433.296 (3)170
C5—H5⋯Cg1ii1.002.603.529 (6)155
C13—H13ACg1iii0.992.813.351 (5)115

Symmetry codes: (i) ; (ii) ; (iii) .

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Journal:  Acta Crystallogr Sect E Struct Rep Online       Date:  2013-04-10

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Journal:  Acta Crystallogr Sect E Struct Rep Online       Date:  2013-12-14
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