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The title compound, C15H9N9S3, was synthesized by the reaction of cyanuric chloride with the potassium salt of 2-mercapto­pyrimidine. The dihedral angles between the three pyrimidinyl rings and the central triazine plane are 94.1 (4), 105.5 (3) and 126.6 (5)°. The three S atoms are essentially coplanar with the triazine ring, while the orientations of the three pyrimidinyl rings are different, with one ring twisting in the opposite direction to the other two.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805008901/hg6159sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536805008901/hg6159Isup2.hkl
Contains datablock I

CCDC reference: 270451

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.004 Å
  • R factor = 0.035
  • wR factor = 0.090
  • Data-to-parameter ratio = 12.7

checkCIF/PLATON results

No syntax errors found


No errors found in this datablock

Computing details top

Data collection: SMART (Bruker, 1997); cell refinement: SMART; data reduction: SAINT (Bruker, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1997); software used to prepare material for publication: SHELXTL.

2,4,6-tris(pyrimidin-2-ylsulfanyl)-1,3,5-triazine top
Crystal data top
C15H9N9S3F(000) = 840
Mr = 411.49Dx = 1.557 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 1536 reflections
a = 9.020 (1) Åθ = 2.6–22.5°
b = 18.233 (3) ŵ = 0.44 mm1
c = 11.219 (2) ÅT = 293 K
β = 107.908 (2)°Plate, colourless
V = 1755.7 (5) Å30.42 × 0.20 × 0.04 mm
Z = 4
Data collection top
Bruker SMART CCD area-detector
diffractometer
3110 independent reflections
Radiation source: fine-focus sealed tube2177 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.033
φ and ω scansθmax = 25.0°, θmin = 2.2°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1997)
h = 109
Tmin = 0.845, Tmax = 0.978k = 2121
9470 measured reflectionsl = 713
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.035 w = 1/[σ2(Fo2) + (0.0309P)2 + 0.2133P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.090(Δ/σ)max = 0.001
S = 1.08Δρmax = 0.21 e Å3
3110 reflectionsΔρmin = 0.25 e Å3
244 parameters
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
S10.77586 (8)0.01474 (4)1.03672 (6)0.0507 (2)
S21.08865 (8)0.26117 (4)1.06110 (7)0.0564 (2)
S30.93995 (8)0.11367 (4)0.64794 (6)0.0555 (2)
N10.8560 (2)0.06905 (10)0.84431 (18)0.0395 (5)
N20.9960 (2)0.18121 (10)0.86156 (18)0.0424 (5)
N30.9280 (2)0.13492 (10)1.03606 (18)0.0432 (5)
N40.5224 (3)0.01067 (12)0.8402 (2)0.0548 (6)
N50.6692 (3)0.09927 (11)0.8906 (2)0.0581 (6)
N60.7258 (2)0.01102 (11)0.5618 (2)0.0545 (6)
N70.9866 (2)0.02890 (12)0.6531 (2)0.0567 (6)
N81.1053 (2)0.28886 (11)1.2938 (2)0.0517 (5)
N90.8510 (2)0.26506 (11)1.1554 (2)0.0505 (5)
C10.4180 (3)0.02472 (19)0.7484 (3)0.0656 (8)
H10.33060.00050.70000.079*
C20.4351 (4)0.0969 (2)0.7229 (3)0.0744 (9)
H20.36220.12070.65740.089*
C30.5615 (4)0.13216 (17)0.7963 (3)0.0751 (9)
H30.57450.18150.78070.090*
C40.6423 (3)0.02933 (13)0.9052 (2)0.0430 (6)
C50.8607 (2)0.07946 (12)0.9621 (2)0.0373 (5)
C60.9910 (2)0.18408 (12)0.9786 (2)0.0422 (6)
C71.0048 (3)0.27115 (12)1.1844 (2)0.0420 (6)
C80.7952 (3)0.27607 (14)1.2508 (3)0.0563 (7)
H80.68880.27011.23720.068*
C90.8860 (3)0.29559 (14)1.3670 (3)0.0611 (7)
H90.84380.30431.43160.073*
C101.0417 (3)0.30189 (15)1.3848 (3)0.0642 (8)
H101.10630.31581.46330.077*
C110.9286 (2)0.12106 (12)0.8007 (2)0.0389 (5)
C120.8766 (3)0.02106 (13)0.6174 (2)0.0439 (6)
C130.6825 (3)0.05894 (16)0.5448 (3)0.0641 (8)
H130.57800.06950.50520.077*
C140.7835 (3)0.11567 (15)0.5824 (3)0.0644 (8)
H140.74990.16420.57210.077*
C150.9358 (3)0.09824 (16)0.6359 (3)0.0661 (8)
H151.00780.13600.66170.079*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0534 (4)0.0590 (4)0.0418 (4)0.0152 (3)0.0179 (3)0.0023 (3)
S20.0562 (4)0.0555 (4)0.0674 (5)0.0183 (3)0.0335 (4)0.0181 (4)
S30.0730 (5)0.0536 (4)0.0475 (4)0.0110 (3)0.0300 (4)0.0001 (3)
N10.0396 (11)0.0410 (11)0.0420 (12)0.0032 (8)0.0189 (9)0.0002 (9)
N20.0397 (11)0.0444 (12)0.0481 (13)0.0041 (9)0.0208 (9)0.0029 (10)
N30.0424 (11)0.0465 (12)0.0455 (13)0.0057 (9)0.0203 (10)0.0041 (10)
N40.0477 (13)0.0655 (14)0.0505 (14)0.0007 (11)0.0144 (11)0.0041 (12)
N50.0719 (15)0.0459 (13)0.0537 (15)0.0032 (11)0.0153 (12)0.0003 (11)
N60.0476 (13)0.0578 (14)0.0540 (14)0.0002 (10)0.0097 (11)0.0018 (11)
N70.0502 (13)0.0591 (15)0.0583 (15)0.0059 (11)0.0129 (11)0.0005 (11)
N80.0422 (12)0.0568 (13)0.0559 (14)0.0096 (9)0.0146 (11)0.0119 (11)
N90.0377 (11)0.0599 (13)0.0541 (14)0.0053 (9)0.0146 (10)0.0033 (11)
C10.0499 (17)0.102 (3)0.0449 (18)0.0030 (16)0.0151 (14)0.0052 (17)
C20.076 (2)0.092 (2)0.0511 (19)0.0314 (19)0.0129 (17)0.0112 (18)
C30.100 (3)0.0556 (18)0.067 (2)0.0150 (18)0.021 (2)0.0108 (16)
C40.0439 (14)0.0507 (16)0.0402 (15)0.0082 (11)0.0214 (12)0.0053 (12)
C50.0321 (12)0.0416 (13)0.0402 (15)0.0005 (10)0.0143 (10)0.0001 (11)
C60.0364 (13)0.0430 (14)0.0501 (16)0.0000 (10)0.0175 (12)0.0057 (12)
C70.0421 (13)0.0336 (13)0.0516 (16)0.0015 (10)0.0163 (12)0.0044 (11)
C80.0423 (14)0.0581 (16)0.072 (2)0.0060 (12)0.0235 (15)0.0048 (15)
C90.0662 (19)0.0632 (18)0.0646 (19)0.0074 (14)0.0360 (16)0.0174 (15)
C100.0634 (19)0.075 (2)0.0532 (18)0.0159 (14)0.0174 (15)0.0155 (15)
C110.0347 (12)0.0430 (13)0.0418 (14)0.0036 (10)0.0159 (11)0.0023 (11)
C120.0499 (15)0.0537 (15)0.0309 (14)0.0013 (12)0.0167 (12)0.0019 (11)
C130.0537 (17)0.0687 (19)0.063 (2)0.0089 (15)0.0077 (14)0.0003 (16)
C140.073 (2)0.0528 (17)0.065 (2)0.0057 (15)0.0163 (16)0.0076 (15)
C150.068 (2)0.0547 (18)0.074 (2)0.0121 (14)0.0194 (16)0.0013 (15)
Geometric parameters (Å, º) top
S1—C51.753 (2)N8—C71.323 (3)
S1—C41.783 (2)N8—C101.337 (3)
S2—C61.763 (2)N9—C71.328 (3)
S2—C71.778 (2)N9—C81.331 (3)
S3—C111.754 (2)C1—C21.365 (4)
S3—C121.782 (2)C1—H10.9300
N1—C51.323 (3)C2—C31.347 (4)
N1—C111.328 (3)C2—H20.9300
N2—C61.329 (3)C3—H30.9300
N2—C111.335 (3)C8—C91.357 (4)
N3—C61.329 (3)C8—H80.9300
N3—C51.330 (3)C9—C101.361 (4)
N4—C41.322 (3)C9—H90.9300
N4—C11.330 (3)C10—H100.9300
N5—C41.318 (3)C13—C141.357 (4)
N5—C31.338 (4)C13—H130.9300
N6—C121.323 (3)C14—C151.357 (4)
N6—C131.330 (3)C14—H140.9300
N7—C121.316 (3)C15—H150.9300
N7—C151.338 (3)
C5—S1—C4101.04 (11)N2—C6—S2112.75 (17)
C6—S2—C7103.08 (11)N8—C7—N9127.9 (2)
C11—S3—C1298.56 (11)N8—C7—S2114.38 (17)
C5—N1—C11113.39 (19)N9—C7—S2117.58 (18)
C6—N2—C11112.86 (19)N9—C8—C9123.1 (2)
C6—N3—C5113.0 (2)N9—C8—H8118.4
C4—N4—C1115.1 (2)C9—C8—H8118.4
C4—N5—C3114.6 (2)C8—C9—C10117.0 (3)
C12—N6—C13114.5 (2)C8—C9—H9121.5
C12—N7—C15114.7 (2)C10—C9—H9121.5
C7—N8—C10114.8 (2)N8—C10—C9122.6 (3)
C7—N9—C8114.6 (2)N8—C10—H10118.7
N4—C1—C2122.1 (3)C9—C10—H10118.7
N4—C1—H1118.9N1—C11—N2126.7 (2)
C2—C1—H1118.9N1—C11—S3119.24 (17)
C3—C2—C1117.5 (3)N2—C11—S3114.09 (16)
C3—C2—H2121.3N7—C12—N6128.1 (2)
C1—C2—H2121.3N7—C12—S3115.48 (19)
N5—C3—C2122.8 (3)N6—C12—S3116.38 (18)
N5—C3—H3118.6N6—C13—C14123.2 (3)
C2—C3—H3118.6N6—C13—H13118.4
N5—C4—N4128.0 (2)C14—C13—H13118.4
N5—C4—S1115.82 (19)C15—C14—C13116.8 (3)
N4—C4—S1115.95 (19)C15—C14—H14121.6
N1—C5—N3126.9 (2)C13—C14—H14121.6
N1—C5—S1119.72 (16)N7—C15—C14122.7 (3)
N3—C5—S1113.35 (17)N7—C15—H15118.6
N3—C6—N2127.0 (2)C14—C15—H15118.6
N3—C6—S2120.16 (18)
C4—N4—C1—C20.7 (4)C8—N9—C7—N82.4 (4)
N4—C1—C2—C31.2 (4)C8—N9—C7—S2177.37 (18)
C4—N5—C3—C20.6 (4)C6—S2—C7—N8139.84 (18)
C1—C2—C3—N50.6 (5)C6—S2—C7—N944.5 (2)
C3—N5—C4—N41.3 (4)C7—N9—C8—C93.2 (4)
C3—N5—C4—S1175.8 (2)N9—C8—C9—C101.8 (4)
C1—N4—C4—N50.7 (4)C7—N8—C10—C91.6 (4)
C1—N4—C4—S1175.16 (18)C8—C9—C10—N80.8 (4)
C5—S1—C4—N5115.77 (19)C5—N1—C11—N23.0 (3)
C5—S1—C4—N469.05 (19)C5—N1—C11—S3177.48 (15)
C11—N1—C5—N30.3 (3)C6—N2—C11—N12.9 (3)
C11—N1—C5—S1178.09 (15)C6—N2—C11—S3177.59 (15)
C6—N3—C5—N12.0 (3)C12—S3—C11—N111.97 (19)
C6—N3—C5—S1179.47 (15)C12—S3—C11—N2168.48 (17)
C4—S1—C5—N121.7 (2)C15—N7—C12—N63.8 (4)
C4—S1—C5—N3159.71 (16)C15—N7—C12—S3176.4 (2)
C5—N3—C6—N22.2 (3)C13—N6—C12—N72.5 (4)
C5—N3—C6—S2179.02 (15)C13—N6—C12—S3177.74 (19)
C11—N2—C6—N30.0 (3)C11—S3—C12—N787.3 (2)
C11—N2—C6—S2177.00 (15)C11—S3—C12—N692.90 (19)
C7—S2—C6—N324.0 (2)C12—N6—C13—C140.8 (4)
C7—S2—C6—N2158.74 (16)N6—C13—C14—C152.3 (4)
C10—N8—C7—N90.1 (4)C12—N7—C15—C142.0 (4)
C10—N8—C7—S2175.19 (18)C13—C14—C15—N70.8 (4)
 

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