organic compounds
4,4′-Di-4-pyridyl-2,2′-dithiodipyrimidine
aSchool of Chemistry and Chemical Engineering, Southeast University, Nanjing, People's Republic of China
*Correspondence e-mail: zhuhaibin@seu.edu.cn
In the title molecule, C18H12N6S2, the C—S—S—C torsion angle is 96.12 (9)°. The dihedral angles between the pyridyl and pyrimidinyl rings are 16.7 (1) and 1.27 (9)°. In the crystal, intermolecular π–π interactions between the aromatic rings [centroid–centroid distances = 3.888 (2) and 3.572 (1) Å] link molecules into chains propagating in [011].
Related literature
For related crystal structures, see: Ji et al. (2009); Higashi et al. (1978); Tabellion et al. (2001). For general background to heterocyclic disulfides, see: Horikoshi & Mochida (2006).
Experimental
Crystal data
|
Data collection: APEX2 (Bruker, 2007); cell SAINT-Plus (Bruker, 2007); data reduction: SAINT-Plus; 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.
Supporting information
10.1107/S1600536809022004/cv2571sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536809022004/cv2571Isup2.hkl
A solution of SO2Cl2 (0.5 ml) in CH2Cl2 (20 ml) was added dropwise into the suspension containing 4-(pyridin-4-yl)pyrimidine-2-thiol (1.89 g) and 30 ml of CH2Cl2. Upon addition, the mixture was stirred at room temperature for 30 min. The solid was collected by filtration and dissolved into 30 ml of H2O. The solution PH was adjusted into the range of 8–9 to give white precipitates. Single crystals suitable for X-ray
were obtained by slow evaporation of the CH2Cl2 solution of the title compound.All H atoms were positioned geometrically and allowed to ride on their parent atoms, with C—H = 0.93 Å and Uiso(H) = 1.2Ueq(C).
Data collection: APEX2 (Bruker, 2007); cell
SAINT-Plus (Bruker, 2007); data reduction: SAINT-Plus (Bruker, 2007); 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 (Sheldrick, 2008).Fig. 1. The molecular structure of the title compound showing the atomic numbering and 30% probability displacement ellipsoids. |
C18H12N6S2 | Z = 2 |
Mr = 376.48 | F(000) = 388 |
Triclinic, P1 | Dx = 1.452 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 9.1060 (8) Å | Cell parameters from 3982 reflections |
b = 9.3861 (9) Å | θ = 2.3–25.5° |
c = 10.9176 (10) Å | µ = 0.32 mm−1 |
α = 84.228 (1)° | T = 298 K |
β = 74.926 (1)° | Block, yellow |
γ = 72.983 (1)° | 0.14 × 0.12 × 0.10 mm |
V = 861.27 (14) Å3 |
Bruker APEXII CCD area-detector diffractometer | 3982 independent reflections |
Radiation source: fine-focus sealed tube | 3283 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.093 |
ϕ and ω scans | θmax = 28.3°, θmin = 1.9° |
Absorption correction: multi-scan (SADABS; Bruker, 2001) | h = −11→12 |
Tmin = 0.884, Tmax = 0.920 | k = −10→11 |
5665 measured reflections | l = −14→13 |
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)] = 0.056 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.158 | H-atom parameters constrained |
S = 1.12 | w = 1/[σ2(Fo2) + (0.092P)2] where P = (Fo2 + 2Fc2)/3 |
3982 reflections | (Δ/σ)max = 0.026 |
235 parameters | Δρmax = 0.63 e Å−3 |
0 restraints | Δρmin = −0.50 e Å−3 |
C18H12N6S2 | γ = 72.983 (1)° |
Mr = 376.48 | V = 861.27 (14) Å3 |
Triclinic, P1 | Z = 2 |
a = 9.1060 (8) Å | Mo Kα radiation |
b = 9.3861 (9) Å | µ = 0.32 mm−1 |
c = 10.9176 (10) Å | T = 298 K |
α = 84.228 (1)° | 0.14 × 0.12 × 0.10 mm |
β = 74.926 (1)° |
Bruker APEXII CCD area-detector diffractometer | 3982 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2001) | 3283 reflections with I > 2σ(I) |
Tmin = 0.884, Tmax = 0.920 | Rint = 0.093 |
5665 measured reflections |
R[F2 > 2σ(F2)] = 0.056 | 0 restraints |
wR(F2) = 0.158 | H-atom parameters constrained |
S = 1.12 | Δρmax = 0.63 e Å−3 |
3982 reflections | Δρmin = −0.50 e Å−3 |
235 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
S1 | 0.17317 (7) | 0.15307 (5) | 0.45673 (4) | 0.04865 (18) | |
S2 | 0.04746 (6) | 0.10746 (6) | 0.34511 (5) | 0.05008 (19) | |
N5 | 0.33888 (18) | −0.04716 (16) | 0.21420 (13) | 0.0350 (3) | |
N3 | 0.23093 (18) | 0.39811 (16) | 0.49060 (14) | 0.0390 (3) | |
C13 | 0.4305 (2) | −0.12822 (18) | 0.11230 (16) | 0.0350 (4) | |
C10 | 0.1865 (2) | 0.00258 (19) | 0.21737 (17) | 0.0372 (4) | |
C14 | 0.6028 (2) | −0.18393 (19) | 0.10565 (16) | 0.0359 (4) | |
N4 | 0.1100 (2) | −0.01902 (19) | 0.13474 (17) | 0.0465 (4) | |
N2 | 0.1638 (2) | 0.39133 (19) | 0.29373 (16) | 0.0488 (4) | |
C18 | 0.7094 (2) | −0.2658 (2) | 0.00391 (19) | 0.0450 (4) | |
H18A | 0.6733 | −0.2889 | −0.0618 | 0.054* | |
C9 | 0.1901 (2) | 0.3355 (2) | 0.40474 (17) | 0.0391 (4) | |
C15 | 0.6663 (2) | −0.1528 (2) | 0.19982 (18) | 0.0445 (4) | |
H15A | 0.6009 | −0.0976 | 0.2695 | 0.053* | |
C6 | 0.2505 (2) | 0.53454 (19) | 0.45950 (17) | 0.0382 (4) | |
C5 | 0.2986 (2) | 0.6052 (2) | 0.55342 (17) | 0.0398 (4) | |
N6 | 0.9295 (2) | −0.2845 (2) | 0.09198 (18) | 0.0547 (5) | |
C1 | 0.3575 (2) | 0.7282 (2) | 0.5210 (2) | 0.0477 (5) | |
H1A | 0.3689 | 0.7692 | 0.4391 | 0.057* | |
C17 | 0.8683 (3) | −0.3123 (3) | 0.0009 (2) | 0.0537 (5) | |
H17A | 0.9372 | −0.3662 | −0.0684 | 0.064* | |
C11 | 0.2021 (2) | −0.0998 (2) | 0.03537 (19) | 0.0481 (5) | |
H11A | 0.1556 | −0.1189 | −0.0254 | 0.058* | |
C7 | 0.2231 (3) | 0.6050 (2) | 0.3465 (2) | 0.0510 (5) | |
H7A | 0.2337 | 0.7005 | 0.3253 | 0.061* | |
C12 | 0.3641 (2) | −0.1563 (2) | 0.01909 (19) | 0.0445 (4) | |
H12A | 0.4265 | −0.2112 | −0.0517 | 0.053* | |
C16 | 0.8274 (3) | −0.2050 (3) | 0.1883 (2) | 0.0525 (5) | |
H16A | 0.8673 | −0.1831 | 0.2522 | 0.063* | |
C4 | 0.2837 (3) | 0.5510 (3) | 0.6763 (2) | 0.0586 (6) | |
H4B | 0.2450 | 0.4686 | 0.7018 | 0.070* | |
N1 | 0.3860 (3) | 0.7375 (2) | 0.7322 (2) | 0.0695 (6) | |
C8 | 0.1796 (3) | 0.5286 (2) | 0.2664 (2) | 0.0546 (5) | |
H8A | 0.1605 | 0.5747 | 0.1904 | 0.066* | |
C2 | 0.3989 (3) | 0.7884 (3) | 0.6135 (2) | 0.0584 (6) | |
H2B | 0.4387 | 0.8704 | 0.5905 | 0.070* | |
C3 | 0.3270 (4) | 0.6206 (3) | 0.7623 (2) | 0.0737 (8) | |
H3B | 0.3142 | 0.5837 | 0.8455 | 0.088* |
U11 | U22 | U33 | U12 | U13 | U23 | |
S1 | 0.0729 (4) | 0.0372 (3) | 0.0380 (3) | −0.0224 (2) | −0.0072 (2) | −0.0058 (2) |
S2 | 0.0442 (3) | 0.0486 (3) | 0.0559 (3) | −0.0174 (2) | 0.0021 (2) | −0.0188 (2) |
N5 | 0.0447 (8) | 0.0311 (7) | 0.0309 (7) | −0.0148 (6) | −0.0068 (6) | −0.0009 (6) |
N3 | 0.0498 (9) | 0.0321 (7) | 0.0342 (7) | −0.0121 (6) | −0.0061 (6) | −0.0053 (6) |
C13 | 0.0472 (9) | 0.0291 (8) | 0.0291 (8) | −0.0153 (7) | −0.0047 (7) | −0.0005 (6) |
C10 | 0.0462 (10) | 0.0306 (8) | 0.0372 (9) | −0.0179 (7) | −0.0061 (7) | −0.0008 (7) |
C14 | 0.0467 (10) | 0.0302 (8) | 0.0311 (8) | −0.0141 (7) | −0.0065 (7) | 0.0013 (6) |
N4 | 0.0465 (9) | 0.0481 (9) | 0.0506 (9) | −0.0194 (7) | −0.0123 (7) | −0.0064 (7) |
N2 | 0.0622 (11) | 0.0463 (9) | 0.0425 (9) | −0.0183 (8) | −0.0164 (8) | −0.0035 (7) |
C18 | 0.0487 (11) | 0.0450 (10) | 0.0391 (9) | −0.0091 (8) | −0.0082 (8) | −0.0087 (8) |
C9 | 0.0438 (9) | 0.0359 (9) | 0.0345 (8) | −0.0099 (7) | −0.0032 (7) | −0.0071 (7) |
C15 | 0.0516 (11) | 0.0480 (11) | 0.0344 (9) | −0.0162 (8) | −0.0078 (8) | −0.0036 (8) |
C6 | 0.0430 (9) | 0.0324 (8) | 0.0372 (9) | −0.0090 (7) | −0.0062 (7) | −0.0047 (7) |
C5 | 0.0448 (10) | 0.0307 (8) | 0.0414 (9) | −0.0081 (7) | −0.0061 (8) | −0.0084 (7) |
N6 | 0.0498 (10) | 0.0580 (11) | 0.0529 (10) | −0.0117 (8) | −0.0121 (8) | 0.0037 (8) |
C1 | 0.0515 (11) | 0.0438 (10) | 0.0470 (11) | −0.0161 (8) | −0.0045 (8) | −0.0085 (8) |
C17 | 0.0528 (12) | 0.0509 (12) | 0.0489 (11) | −0.0052 (9) | −0.0055 (9) | −0.0087 (9) |
C11 | 0.0554 (11) | 0.0548 (12) | 0.0429 (10) | −0.0236 (9) | −0.0148 (9) | −0.0085 (9) |
C7 | 0.0694 (13) | 0.0378 (10) | 0.0502 (11) | −0.0189 (9) | −0.0198 (10) | 0.0054 (8) |
C12 | 0.0541 (11) | 0.0462 (11) | 0.0367 (9) | −0.0179 (8) | −0.0092 (8) | −0.0101 (8) |
C16 | 0.0558 (12) | 0.0634 (13) | 0.0444 (11) | −0.0225 (10) | −0.0180 (9) | 0.0042 (9) |
C4 | 0.0924 (17) | 0.0458 (12) | 0.0475 (12) | −0.0306 (11) | −0.0207 (11) | −0.0032 (9) |
N1 | 0.0925 (16) | 0.0651 (13) | 0.0639 (13) | −0.0318 (11) | −0.0235 (12) | −0.0193 (10) |
C8 | 0.0737 (14) | 0.0501 (12) | 0.0465 (11) | −0.0202 (10) | −0.0255 (11) | 0.0069 (9) |
C2 | 0.0635 (14) | 0.0516 (13) | 0.0656 (15) | −0.0244 (10) | −0.0103 (11) | −0.0161 (11) |
C3 | 0.120 (2) | 0.0663 (16) | 0.0496 (13) | −0.0387 (16) | −0.0302 (15) | −0.0036 (11) |
S1—C9 | 1.7867 (19) | C5—C4 | 1.374 (3) |
S1—S2 | 2.0238 (7) | C5—C1 | 1.388 (3) |
S2—C10 | 1.7734 (19) | N6—C17 | 1.339 (3) |
N5—C10 | 1.321 (2) | N6—C16 | 1.331 (3) |
N5—C13 | 1.352 (2) | C1—C2 | 1.385 (3) |
N3—C9 | 1.335 (2) | C1—H1A | 0.9300 |
N3—C6 | 1.342 (2) | C17—H17A | 0.9300 |
C13—C12 | 1.392 (2) | C11—C12 | 1.384 (3) |
C13—C14 | 1.486 (3) | C11—H11A | 0.9300 |
C10—N4 | 1.336 (2) | C7—C8 | 1.382 (3) |
C14—C18 | 1.393 (3) | C7—H7A | 0.9300 |
C14—C15 | 1.395 (3) | C12—H12A | 0.9300 |
N4—C11 | 1.332 (3) | C16—H16A | 0.9300 |
N2—C8 | 1.333 (3) | C4—C3 | 1.389 (3) |
N2—C9 | 1.323 (2) | C4—H4B | 0.9300 |
C18—C17 | 1.377 (3) | N1—C2 | 1.323 (3) |
C18—H18A | 0.9300 | N1—C3 | 1.335 (3) |
C15—C16 | 1.380 (3) | C8—H8A | 0.9300 |
C15—H15A | 0.9300 | C2—H2B | 0.9300 |
C6—C7 | 1.386 (3) | C3—H3B | 0.9300 |
C6—C5 | 1.491 (2) | ||
Cg1···Cg2i | 3.888 (2) | Cg3···Cg4ii | 3.572 (1) |
C9—S1—S2 | 104.02 (6) | C2—C1—C5 | 118.5 (2) |
C10—S2—S1 | 106.81 (6) | C2—C1—H1A | 120.8 |
C10—N5—C13 | 115.68 (14) | C5—C1—H1A | 120.8 |
C9—N3—C6 | 115.86 (16) | N6—C17—C18 | 123.76 (19) |
N5—C13—C12 | 120.70 (17) | N6—C17—H17A | 118.1 |
N5—C13—C14 | 116.75 (15) | C18—C17—H17A | 118.1 |
C12—C13—C14 | 122.55 (16) | N4—C11—C12 | 122.50 (16) |
N5—C10—N4 | 128.71 (17) | N4—C11—H11A | 118.8 |
N5—C10—S2 | 122.14 (13) | C12—C11—H11A | 118.7 |
N4—C10—S2 | 109.10 (13) | C8—C7—C6 | 117.84 (19) |
C18—C14—C15 | 116.68 (17) | C8—C7—H7A | 121.1 |
C18—C14—C13 | 121.97 (16) | C6—C7—H7A | 121.1 |
C15—C14—C13 | 121.33 (16) | C11—C12—C13 | 117.66 (17) |
C10—N4—C11 | 114.73 (16) | C11—C12—H12A | 121.2 |
C8—N2—C9 | 114.58 (16) | C13—C12—H12A | 121.2 |
C17—C18—C14 | 119.77 (18) | N6—C16—C15 | 124.43 (18) |
C17—C18—H18A | 120.1 | N6—C16—H16A | 117.8 |
C14—C18—H18A | 120.1 | C15—C16—H16A | 117.8 |
N3—C9—N2 | 128.50 (18) | C5—C4—C3 | 119.3 (2) |
N3—C9—S1 | 111.00 (14) | C5—C4—H4B | 120.4 |
N2—C9—S1 | 120.50 (14) | C3—C4—H4B | 120.4 |
C16—C15—C14 | 119.14 (18) | C2—N1—C3 | 116.0 (2) |
C16—C15—H15A | 120.4 | N2—C8—C7 | 122.63 (19) |
C14—C15—H15A | 120.4 | N2—C8—H8A | 118.7 |
N3—C6—C7 | 120.54 (17) | C7—C8—H8A | 118.7 |
N3—C6—C5 | 116.60 (16) | N1—C2—C1 | 124.7 (2) |
C7—C6—C5 | 122.84 (17) | N1—C2—H2B | 117.6 |
C4—C5—C1 | 117.73 (18) | C1—C2—H2B | 117.6 |
C4—C5—C6 | 120.55 (18) | N1—C3—C4 | 123.8 (2) |
C1—C5—C6 | 121.71 (18) | N1—C3—H3B | 118.1 |
C17—N6—C16 | 116.21 (18) | C4—C3—H3B | 118.1 |
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) −x+1, −y, −z. |
Experimental details
Crystal data | |
Chemical formula | C18H12N6S2 |
Mr | 376.48 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 298 |
a, b, c (Å) | 9.1060 (8), 9.3861 (9), 10.9176 (10) |
α, β, γ (°) | 84.228 (1), 74.926 (1), 72.983 (1) |
V (Å3) | 861.27 (14) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 0.32 |
Crystal size (mm) | 0.14 × 0.12 × 0.10 |
Data collection | |
Diffractometer | Bruker APEXII CCD area-detector diffractometer |
Absorption correction | Multi-scan (SADABS; Bruker, 2001) |
Tmin, Tmax | 0.884, 0.920 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 5665, 3982, 3283 |
Rint | 0.093 |
(sin θ/λ)max (Å−1) | 0.667 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.056, 0.158, 1.12 |
No. of reflections | 3982 |
No. of parameters | 235 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.63, −0.50 |
Computer programs: APEX2 (Bruker, 2007), SAINT-Plus (Bruker, 2007), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
Acknowledgements
The authors acknowledge the support of the National Natural Science Foundation of China (grant No. 20801011).
References
Bruker (2001). SADABS. Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Bruker (2007). APEX2 and SAINT-Plus. Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Higashi, L. S., Lundeen, M. & Seff, J. (1978). J. Am. Chem. Soc. 100, 8101–8106. CSD CrossRef CAS Web of Science Google Scholar
Horikoshi, R. & Mochida, T. (2006). Coord. Chem. Rev. 250, 2595–2609. Web of Science CrossRef CAS Google Scholar
Ji, J.-F., Li, L. & Zhu, H.-B. (2009). Acta Cryst. E65, o1253. Web of Science CSD CrossRef IUCr Journals Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Tabellion, F. M., Seidel, S. R., Arif, A. M. & Stang, P. J. (2001). J. Am Chem. Soc. 123, 7740–7741. Web of Science CSD CrossRef PubMed CAS Google Scholar
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.
Heterocylic disulfide ligands have been considerably studied in the field of supramolecular chemistry over past years (Horikoshi & Mochida, 2006). Herein, we report the molecular structure of the title compound (I) - the newly synthesized disulfide ligand.
In (I) (Fig. 1), the C—S—S—C torsion angle of 96.12 (9)° is much larger than that in its analogue, namely 2,2'-dithiobis(4-pyridin-3-yl-pyrimidine) (Ji et al., 2009).The S—S bond length of 2.0239 (8) Å in (I) is within the normal range (Higashi et al., 1978; Tabellion et al., 2001). In the crystal, molecules are linked into chains through intermolecular aromatic π-π interactions (Table 1) .