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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Mar 20;64(Pt 4):o722. doi: 10.1107/S1600536808006752

2-Propyl-4H-thia­zolo[3,2-a][1,3,5]triazine-4-thione

Uzma Yunus a,*, Muhammad Kalim Tahir a, Moazzam Hussain Bhatti a, Wai-Yeung Wong b
PMCID: PMC2961019  PMID: 21202112

Abstract

In the title compound, C8H9N3S2, the n-propyl chain is disordered over two orientations (site-occupancy ratio = 0.522:0.478) and is roughly perpendicular to the fused thia­zolotriazine system. The angle between the fused ring and the propyl chain is 83.6 (1)° [ 82.2 (1)° for the disordered chain]. The structure is stabilized by C—H⋯N hydrogen bonds.

Related literature

For related literature, see: Jiang et al. (2007); Pauling et al. (1960); Yunus et al. (2007).graphic file with name e-64-0o722-scheme1.jpg

Experimental

Crystal data

  • C8H9N3S2

  • M r = 211.32

  • Monoclinic, Inline graphic

  • a = 9.3240 (7) Å

  • b = 14.9973 (11) Å

  • c = 6.8063 (5) Å

  • β = 95.505 (1)°

  • V = 947.37 (12) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.52 mm−1

  • T = 173 (2) K

  • 0.32 × 0.25 × 0.22 mm

Data collection

  • Bruker SMART CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 1999) T min = 0.853, T max = 0.895

  • 5571 measured reflections

  • 2254 independent reflections

  • 2077 reflections with I > 2σ(I)

  • R int = 0.016

Refinement

  • R[F 2 > 2σ(F 2)] = 0.024

  • wR(F 2) = 0.068

  • S = 1.05

  • 2254 reflections

  • 161 parameters

  • 5 restraints

  • H-atom parameters constrained

  • Δρmax = 0.32 e Å−3

  • Δρmin = −0.28 e Å−3

Data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 1999); data reduction: SAINT; 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.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808006752/pk2086sup1.cif

e-64-0o722-sup1.cif (17KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808006752/pk2086Isup2.hkl

e-64-0o722-Isup2.hkl (110.8KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
C1—H1⋯N2i 0.95 2.38 3.3261 (16) 171

Symmetry code: (i) Inline graphic.

Acknowledgments

The authors gratefully acknowledge Allama Iqbal Open University, Islamabad, Pakistan, for providing research facilities.

supplementary crystallographic information

Comment

We have previously reported the crystal structure of 2-phenyl-4H-thiazolo[3,2,-a]- [1,3,5]triazine-4-thione with a phenyl group attached to the 1,3,5-triazine ring (Yunus et al., 2007). The molecule was essentially planar. In contrast, in the title compound the pendant n-propyl group is almost perpendicular to the fused thiazolo[3,2,-a][1,3,5]triazine ring, which are themselves co-planar (maximum deviation from mean plane is 0.0437 (1) Å from atom C4). The n-propyl chain is disordered over two orientations with a site occupancy ratio of 0.522:0.478 (Jiang et al., 2007). The CN bond distances of the 1,3,5-triazine ring are in the range 1.3191 (15) to 1.4093 (14) Å, in which N1—C5 bond length is slightly longer than that of N2—C5. These values are intermediate between those expected for single and double C—N bonds (1.47 and 1.27 Å, respectively). The C=S bond length of 1.6686 (12) Å is similar to that of the phenyl analog (Yunus et al., 2007) but is slightly longer then the pure double bond distance (1.61 Å) (Pauling 1960). The bond angles and bond lengths in the thiazole ring are within the normal ranges. The crystal structure is stabilized by weak C—H···N hydrogen bonding interactions.

Experimental

A mixture of ammonium thiocyanate (26 mmol) and butyryl chloride (26 mmol) in dry acetone (60 ml) was stirred for 30 min. Then 2-aminothiazole (26 mmol) was added and the reaction mixture was refluxed for 2 h. After cooling, the reaction mixture was poured into acidified cold water. The resulting yellow solid was filtered and washed with cold acetone. Single crystals of the title compound suitable for single-crystal x-ray analysis were obtained by recrystallization of the yellow solid from acetonitrile.

Refinement

H atoms were found in difference Fourier maps and subsequently placed in idealized positions with constrained C—H distances of 0.98 Å (RCH3), 0.99 Å (R2CH2) and 0.95 Å (CArH) with Uiso(H) values set to either 1.5Ueq (RCH3) or 1.2Ueq of the attached C atom.

Figures

Fig. 1.

Fig. 1.

: A view of the molecular structure. Displacement ellipsoids are drawn at the 50% probability level.

Crystal data

C8H9N3S2 F000 = 440
Mr = 211.32 Dx = 1.481 Mg m3
Monoclinic, P21/c Mo Kα radiation λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 5571 reflections
a = 9.3240 (7) Å θ = 2.6–28.3º
b = 14.9973 (11) Å µ = 0.52 mm1
c = 6.8063 (5) Å T = 173 (2) K
β = 95.505 (1)º Block, pale yellow
V = 947.37 (12) Å3 0.32 × 0.25 × 0.22 mm
Z = 4

Data collection

Bruker SMART CCD diffractometer 2254 independent reflections
Radiation source: fine-focus sealed tube 2077 reflections with I > 2σ(I)
Monochromator: graphite Rint = 0.016
T = 173(2) K θmax = 28.3º
ω and φ scans θmin = 2.6º
Absorption correction: multi-scan(SADABS; Bruker, 1999) h = −12→12
Tmin = 0.853, Tmax = 0.895 k = −19→14
5571 measured reflections l = −9→9

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.024 H-atom parameters constrained
wR(F2) = 0.068   w = 1/[σ2(Fo2) + (0.0392P)2 + 0.2601P] where P = (Fo2 + 2Fc2)/3
S = 1.05 (Δ/σ)max = 0.001
2254 reflections Δρmax = 0.32 e Å3
161 parameters Δρmin = −0.28 e Å3
5 restraints Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.0066 (12)

Special details

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 > 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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq Occ. (<1)
S1 0.20093 (3) 0.710163 (18) 0.27470 (4) 0.02095 (10)
S2 −0.15462 (3) 0.443002 (19) 0.21702 (4) 0.02265 (10)
N1 0.04853 (10) 0.56884 (6) 0.25767 (13) 0.01739 (19)
N2 0.12868 (11) 0.42185 (7) 0.29852 (15) 0.0235 (2)
N3 0.29929 (11) 0.54164 (7) 0.31895 (15) 0.0231 (2)
C1 0.01557 (13) 0.71890 (8) 0.23196 (17) 0.0224 (2)
H1 −0.0344 0.7739 0.2143 0.027*
C2 −0.04951 (12) 0.63902 (8) 0.22664 (17) 0.0211 (2)
H2 −0.1508 0.6311 0.2043 0.025*
C3 0.18861 (12) 0.59613 (7) 0.28536 (15) 0.0185 (2)
C5 0.01588 (12) 0.47711 (7) 0.25939 (15) 0.0187 (2)
C4 0.26174 (14) 0.45502 (8) 0.32834 (18) 0.0259 (3) 0.522 (4)
C6 0.3713 (6) 0.3883 (4) 0.4050 (7) 0.0221 (9) 0.522 (4)
H6A 0.3288 0.3278 0.4003 0.029 (8)* 0.522 (4)
H6B 0.4062 0.4022 0.5436 0.025 (7)* 0.522 (4)
C7 0.4958 (2) 0.39267 (16) 0.2751 (4) 0.0248 (6) 0.522 (4)
H7A 0.5357 0.4539 0.2799 0.021 (7)* 0.522 (4)
H7B 0.5730 0.3517 0.3292 0.036 (8)* 0.522 (4)
C8 0.4516 (9) 0.3679 (6) 0.0614 (6) 0.0357 (13) 0.522 (4)
H8A 0.5357 0.3714 −0.0143 0.030 (8)* 0.522 (4)
H8B 0.3773 0.4093 0.0055 0.045 (10)* 0.522 (4)
H8C 0.4134 0.3070 0.0552 0.061 (12)* 0.522 (4)
C4A 0.26174 (14) 0.45502 (8) 0.32834 (18) 0.0259 (3) 0.478 (4)
C6A 0.3938 (7) 0.3911 (4) 0.3487 (8) 0.0255 (12) 0.478 (4)
H6A1 0.4827 0.4276 0.3621 0.047 (11)* 0.478 (4)
H6A2 0.3913 0.3565 0.4722 0.038 (11)* 0.478 (4)
C7A 0.4034 (3) 0.32554 (16) 0.1781 (4) 0.0247 (7) 0.478 (4)
H7A1 0.4736 0.2781 0.2199 0.036 (9)* 0.478 (4)
H7A2 0.3083 0.2970 0.1461 0.037 (9)* 0.478 (4)
C8A 0.4491 (8) 0.3709 (6) −0.0056 (8) 0.0320 (11) 0.478 (4)
H8A1 0.4583 0.3263 −0.1087 0.064 (14)* 0.478 (4)
H8A2 0.5420 0.4007 0.0263 0.061 (13)* 0.478 (4)
H8A3 0.3764 0.4152 −0.0528 0.030 (9)* 0.478 (4)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
S1 0.02618 (16) 0.01417 (15) 0.02233 (16) −0.00294 (10) 0.00150 (11) 0.00001 (9)
S2 0.02469 (16) 0.01845 (15) 0.02542 (16) −0.00432 (10) 0.00559 (11) −0.00188 (10)
N1 0.0225 (4) 0.0139 (4) 0.0155 (4) −0.0004 (3) 0.0008 (3) 0.0001 (3)
N2 0.0307 (5) 0.0151 (4) 0.0231 (5) 0.0010 (4) −0.0059 (4) −0.0003 (4)
N3 0.0254 (5) 0.0183 (5) 0.0243 (5) 0.0009 (4) −0.0051 (4) −0.0020 (4)
C1 0.0273 (6) 0.0166 (5) 0.0236 (6) 0.0020 (4) 0.0037 (4) −0.0001 (4)
C2 0.0235 (5) 0.0172 (5) 0.0226 (5) 0.0024 (4) 0.0029 (4) 0.0003 (4)
C3 0.0247 (5) 0.0157 (5) 0.0147 (5) −0.0022 (4) 0.0000 (4) −0.0010 (4)
C5 0.0280 (5) 0.0148 (5) 0.0130 (5) −0.0015 (4) 0.0010 (4) −0.0015 (4)
C4 0.0301 (6) 0.0183 (5) 0.0266 (6) 0.0025 (4) −0.0106 (5) −0.0023 (4)
C6 0.0217 (16) 0.0211 (14) 0.023 (2) 0.0022 (11) −0.0009 (16) 0.0060 (18)
C7 0.0159 (11) 0.0253 (12) 0.0332 (13) 0.0029 (8) 0.0023 (9) −0.0008 (9)
C8 0.0347 (17) 0.039 (2) 0.034 (3) 0.0051 (15) 0.006 (3) −0.009 (3)
C4A 0.0301 (6) 0.0183 (5) 0.0266 (6) 0.0025 (4) −0.0106 (5) −0.0023 (4)
C6A 0.032 (3) 0.0196 (16) 0.023 (3) 0.0051 (16) −0.0085 (19) 0.0019 (19)
C7A 0.0224 (11) 0.0180 (12) 0.0337 (15) 0.0042 (9) 0.0030 (10) 0.0003 (10)
C8A 0.0268 (16) 0.0325 (18) 0.038 (3) −0.0014 (13) 0.009 (3) 0.004 (3)

Geometric parameters (Å, °)

S1—C3 1.7161 (11) C6—H6B 0.9900
S1—C1 1.7299 (13) C7—C8 1.519 (5)
S2—C5 1.6686 (12) C7—H7A 0.9900
N1—C3 1.3644 (14) C7—H7B 0.9900
N1—C2 1.3967 (14) C8—H8A 0.9800
N1—C5 1.4093 (14) C8—H8B 0.9800
N2—C4 1.3340 (16) C8—H8C 0.9800
N2—C5 1.3455 (15) C6A—C7A 1.531 (6)
N3—C3 1.3191 (15) C6A—H6A1 0.9900
N3—C4 1.3485 (15) C6A—H6A2 0.9900
C1—C2 1.3418 (17) C7A—C8A 1.520 (6)
C1—H1 0.9500 C7A—H7A1 0.9900
C2—H2 0.9500 C7A—H7A2 0.9900
C4—C6 1.488 (6) C8A—H8A1 0.9800
C6—C7 1.526 (5) C8A—H8A2 0.9800
C6—H6A 0.9900 C8A—H8A3 0.9800
C3—S1—C1 90.73 (6) C8—C7—C6 113.1 (4)
C3—N1—C2 113.50 (9) C8—C7—H7A 109.0
C3—N1—C5 119.76 (9) C6—C7—H7A 109.0
C2—N1—C5 126.73 (10) C8—C7—H7B 109.0
C4—N2—C5 119.89 (10) C6—C7—H7B 109.0
C3—N3—C4 113.74 (10) H7A—C7—H7B 107.8
C2—C1—S1 112.26 (9) C7—C8—H8A 109.5
C2—C1—H1 123.9 C7—C8—H8B 109.5
S1—C1—H1 123.9 H8A—C8—H8B 109.5
C1—C2—N1 112.39 (10) C7—C8—H8C 109.5
C1—C2—H2 123.8 H8A—C8—H8C 109.5
N1—C2—H2 123.8 H8B—C8—H8C 109.5
N3—C3—N1 124.11 (10) C7A—C6A—H6A1 108.4
N3—C3—S1 124.77 (9) C7A—C6A—H6A2 108.4
N1—C3—S1 111.11 (8) H6A1—C6A—H6A2 107.5
N2—C5—N1 115.95 (10) C8A—C7A—C6A 112.2 (4)
N2—C5—S2 123.99 (9) C8A—C7A—H7A1 109.2
N1—C5—S2 120.05 (8) C6A—C7A—H7A1 109.2
N2—C4—N3 126.44 (11) C8A—C7A—H7A2 109.2
N2—C4—C6 113.6 (3) C6A—C7A—H7A2 109.2
N3—C4—C6 119.4 (3) H7A1—C7A—H7A2 107.9
C4—C6—C7 107.7 (3) C7A—C8A—H8A1 109.5
C4—C6—H6A 110.2 C7A—C8A—H8A2 109.5
C7—C6—H6A 110.2 H8A1—C8A—H8A2 109.5
C4—C6—H6B 110.2 C7A—C8A—H8A3 109.5
C7—C6—H6B 110.2 H8A1—C8A—H8A3 109.5
H6A—C6—H6B 108.5 H8A2—C8A—H8A3 109.5
C3—S1—C1—C2 −0.03 (9) C4—N2—C5—S2 179.23 (9)
S1—C1—C2—N1 0.23 (13) C3—N1—C5—N2 3.03 (15)
C3—N1—C2—C1 −0.38 (14) C2—N1—C5—N2 −178.04 (10)
C5—N1—C2—C1 −179.36 (10) C3—N1—C5—S2 −177.64 (8)
C4—N3—C3—N1 −1.45 (16) C2—N1—C5—S2 1.28 (15)
C4—N3—C3—S1 177.43 (9) C5—N2—C4—N3 −1.78 (19)
C2—N1—C3—N3 179.37 (10) C5—N2—C4—C6 169.6 (2)
C5—N1—C3—N3 −1.58 (16) C3—N3—C4—N2 3.24 (19)
C2—N1—C3—S1 0.35 (11) C3—N3—C4—C6 −167.7 (2)
C5—N1—C3—S1 179.41 (7) N2—C4—C6—C7 129.4 (3)
C1—S1—C3—N3 −179.19 (10) N3—C4—C6—C7 −58.6 (4)
C1—S1—C3—N1 −0.19 (8) C4—C6—C7—C8 −62.5 (5)
C4—N2—C5—N1 −1.48 (16)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C1—H1···N2i 0.95 2.38 3.3261 (16) 171

Symmetry codes: (i) −x, y+1/2, −z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: PK2086).

References

  1. Bruker (1998). SMART Bruker AXS Inc., Madison, Wisconsin, USA.
  2. Bruker (1999). SAINT and SADABS Bruker AXS Inc., Madison, Wisconsin, USA.
  3. Jiang, Y.-P., Qiu, T., Wang, L.-E. & Wang, J.-N. (2007). Acta Cryst. E63, o3096.
  4. Pauling, L. (1960). The Nature of the Chemical Bond, 3rd ed. Ithaca: Cornell University Press.
  5. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  6. Yunus, U., Tahir, M. K., Bhatti, M. H., Ali, S. & Helliwell, M. (2007). Acta Cryst. E63, o3690.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808006752/pk2086sup1.cif

e-64-0o722-sup1.cif (17KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808006752/pk2086Isup2.hkl

e-64-0o722-Isup2.hkl (110.8KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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