supplementary materials


cv2646 scheme

Acta Cryst. (2009). E65, o2977    [ doi:10.1107/S1600536809045450 ]

cis-1,2-Bis{[4-(4-pyridyl)pyrimidin-2-yl]sulfanylmethyl}benzene

H.-Z. Dong, H.-B. Zhu and S.-H. Gou

Abstract top

The molecular skeleton of the title molecule, C26H20N6S2, adopts a cis conformation with the two arms positioned on one side of the benzene ring plane. Intramolecular [pi]-[pi] interactions between the pyrimidine rings [centroid-centroid distance = 3.654 (2) Å] and between the pyridine rings [centroid-centroid distance = 3.775 (2) Å] help to set the molecular conformation; the pyrimidine rings, as well as the pyridine rings, are nearly parallel, forming dihedral angles of 4.12 (14) and 2.46 (14)°, respectively.

Comment top

Remarkable attention has been paid to the rational design and assembly of new coordination polymers with heterocyclic thiolates or thioethers in recent years. In our previous work, we reported aserials dithioether ligands (Dong et al., 2008; 2009; Huang et al., 2007). As our continuing study, herein we report the molecular structure of the title compound - the newly synthesized ligand derived from 4-(4-pyridinyl)pyrimidine-2-thiol.

The molecular structure of the title compound is shown in Fig. 1. The molecule adopts a cis conformation with two arms positioned on one side of the benzene ring plane. It is noted that intramolecular π-π interactions between the pyrimidinyl rings [centroid-centroid distance of 3.654 (2) Å] and between the pyridinyl rings [centroid-centroid distance of 3.775 (2) Å] set the molecular conformation - the pyrimidinyl rings, as well as the pyridinyl ones, are nearly parallel forming dihedral angles of 4.12 (14)° and 2.46 (14)°, respectively.

Related literature top

For related compounds, see: Dong et al. (2008, 2009); Huang et al. (2007).

Experimental top

All solvents and chemicals were of analytical grade and were used without further purification. The title compound was prepared by similar procedure reported in the literature (Dong et al., 2008; 2009), To a solution of 4-(4-pyridinyl)pyrimidine-2-thiol (3.78 g, 20 mmol) and sodium hydroxide (0.80 g, 20 mmol) in dry ethanol (300 ml), 1,2-bis(bromomethyl)benzene (2.64 g, 10 mmol) in CCl4 (30 ml) was added. The mixture was stirred and refluxed for 8 h. After cooling, precipitates were filtered, washed in water and ethanol, and dried in vacuum. Anal. Calcd for C26H20N6S2: C, 64.98; H, 4.19; N, 17.49%. Found: C, 65.07; H, 4.52; N, 17.34%. Single crystals of ligang suitable for X-ray diffraction were grown from methanol solution by slow evaporation in air at room temperature.

Refinement top

All hydrogen atoms were geometrically positioned (C—H 0.93–0.97 Å) and refined as riding, with Uiso(H)=1.2Ueq(C).

Computing details top

Data collection: SMART (Bruker, 2000); cell refinement: SAINT (Bruker, 2000); data reduction: SAINT (Bruker, 2000); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound showing 30% probability displacement ellipsoids and the atom-numbering scheme.
cis-1,2-Bis{[4-(4-pyridyl)pyrimidin-2-yl]sulfanylmethyl}benzene top
Crystal data top
C26H20N6S2F(000) = 1000.0
Mr = 480.62Dx = 1.404 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 4903 reflections
a = 8.6078 (11) Åθ = 2.2–27.0°
b = 27.102 (3) ŵ = 0.26 mm1
c = 10.0282 (12) ÅT = 291 K
β = 103.661 (2)°Block, pale yellow
V = 2273.3 (5) Å30.32 × 0.18 × 0.16 mm
Z = 4
Data collection top
Bruker SMART CCD area-detector
diffractometer
4903 independent reflections
Radiation source: fine-focus sealed tube3067 reflections with I > 2σ(I)
graphiteRint = 0.052
φ and ω scansθmax = 27.0°, θmin = 2.2°
Absorption correction: multi-scan
(SADABS; Bruker, 2000)
h = 108
Tmin = 0.917, Tmax = 0.966k = 3431
13064 measured reflectionsl = 1212
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)] = 0.052Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.108H-atom parameters constrained
S = 0.90 w = 1/[σ2(Fo2) + (0.0421P)2]
where P = (Fo2 + 2Fc2)/3
4903 reflections(Δ/σ)max = 0.001
307 parametersΔρmax = 0.32 e Å3
0 restraintsΔρmin = 0.22 e Å3
Crystal data top
C26H20N6S2V = 2273.3 (5) Å3
Mr = 480.62Z = 4
Monoclinic, P21/nMo Kα radiation
a = 8.6078 (11) ŵ = 0.26 mm1
b = 27.102 (3) ÅT = 291 K
c = 10.0282 (12) Å0.32 × 0.18 × 0.16 mm
β = 103.661 (2)°
Data collection top
Bruker SMART CCD area-detector
diffractometer
4903 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2000)
3067 reflections with I > 2σ(I)
Tmin = 0.917, Tmax = 0.966Rint = 0.052
13064 measured reflectionsθmax = 27.0°
Refinement top
R[F2 > 2σ(F2)] = 0.052H-atom parameters constrained
wR(F2) = 0.108Δρmax = 0.32 e Å3
S = 0.90Δρmin = 0.22 e Å3
4903 reflectionsAbsolute structure: ?
307 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
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
C10.7345 (3)0.22381 (8)0.8229 (2)0.0384 (5)
C20.9748 (3)0.25202 (9)0.9324 (2)0.0494 (6)
H21.07990.24690.98070.059*
C30.9230 (3)0.29935 (8)0.9059 (2)0.0474 (6)
H30.99090.32590.93510.057*
C40.7668 (3)0.30680 (8)0.8343 (2)0.0411 (6)
C50.6967 (3)0.35654 (8)0.8048 (2)0.0436 (6)
C60.7521 (3)0.39620 (9)0.8867 (3)0.0623 (8)
H60.83550.39220.96400.075*
C70.6845 (4)0.44177 (10)0.8545 (3)0.0774 (9)
H70.72400.46800.91250.093*
C80.5126 (3)0.41215 (9)0.6685 (3)0.0690 (8)
H80.42910.41720.59190.083*
C90.5716 (3)0.36519 (8)0.6935 (3)0.0529 (7)
H90.52750.33940.63570.063*
C100.6875 (3)0.12421 (7)0.8693 (2)0.0472 (6)
H10A0.78170.11240.84180.057*
H10B0.71880.13420.96480.057*
C110.5630 (3)0.08400 (8)0.8510 (2)0.0443 (6)
C120.5488 (3)0.05264 (9)0.7392 (3)0.0592 (7)
H120.61830.05600.68150.071*
C130.4334 (4)0.01686 (9)0.7133 (3)0.0687 (8)
H130.42480.00380.63790.082*
C140.3317 (3)0.01133 (9)0.7966 (3)0.0660 (8)
H140.25190.01260.77770.079*
C150.3473 (3)0.04123 (8)0.9091 (3)0.0566 (7)
H150.27940.03670.96770.068*
C160.4617 (3)0.07813 (8)0.9376 (2)0.0446 (6)
C170.4698 (3)0.11019 (7)1.0609 (2)0.0502 (6)
H17A0.58050.11841.10170.060*
H17B0.42830.09211.12850.060*
C180.4950 (3)0.21357 (8)1.0767 (2)0.0380 (5)
C190.7376 (3)0.24131 (9)1.1805 (2)0.0484 (6)
H190.84420.23581.22380.058*
C200.6847 (3)0.28872 (8)1.1637 (2)0.0446 (6)
H200.75230.31511.19550.053*
C210.5267 (3)0.29608 (8)1.0977 (2)0.0393 (5)
C220.4562 (3)0.34572 (8)1.0709 (2)0.0399 (5)
C230.5154 (3)0.38590 (9)1.1509 (3)0.0589 (7)
H230.60240.38231.22530.071*
C240.4452 (4)0.43133 (9)1.1201 (3)0.0701 (9)
H240.48680.45791.17610.084*
C250.3284 (3)0.35403 (8)0.9626 (2)0.0497 (6)
H250.28350.32820.90520.060*
C260.2679 (3)0.40072 (9)0.9402 (3)0.0597 (7)
H260.18160.40540.86560.072*
N10.8822 (2)0.21295 (7)0.89261 (18)0.0458 (5)
N20.6713 (2)0.26820 (6)0.79073 (17)0.0405 (5)
N30.5667 (3)0.45081 (8)0.7465 (3)0.0771 (8)
N40.6443 (2)0.20240 (7)1.13813 (19)0.0463 (5)
N50.4294 (2)0.25802 (6)1.05275 (17)0.0394 (5)
N60.3221 (3)0.43947 (7)1.0157 (2)0.0640 (6)
S10.60063 (8)0.17575 (2)0.76342 (6)0.04810 (19)
S20.35623 (8)0.16649 (2)1.01669 (6)0.04634 (19)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0353 (14)0.0411 (13)0.0382 (13)0.0043 (11)0.0074 (11)0.0000 (10)
C20.0363 (16)0.0586 (16)0.0487 (15)0.0038 (12)0.0005 (12)0.0005 (12)
C30.0409 (16)0.0496 (15)0.0480 (15)0.0112 (12)0.0031 (12)0.0033 (11)
C40.0424 (15)0.0443 (13)0.0377 (13)0.0058 (12)0.0116 (11)0.0023 (10)
C50.0423 (16)0.0436 (14)0.0462 (14)0.0055 (11)0.0131 (12)0.0066 (11)
C60.068 (2)0.0518 (16)0.0583 (17)0.0030 (15)0.0019 (14)0.0126 (13)
C70.090 (3)0.0455 (17)0.086 (2)0.0035 (16)0.001 (2)0.0243 (15)
C80.063 (2)0.0504 (16)0.081 (2)0.0088 (14)0.0070 (16)0.0122 (15)
C90.0461 (17)0.0422 (14)0.0656 (17)0.0020 (12)0.0036 (14)0.0122 (12)
C100.0394 (15)0.0401 (13)0.0559 (15)0.0036 (11)0.0010 (12)0.0066 (11)
C110.0447 (16)0.0305 (12)0.0509 (15)0.0019 (11)0.0025 (12)0.0012 (11)
C120.064 (2)0.0480 (15)0.0640 (18)0.0002 (14)0.0131 (15)0.0030 (13)
C130.079 (2)0.0455 (16)0.072 (2)0.0027 (15)0.0014 (18)0.0151 (14)
C140.058 (2)0.0367 (15)0.094 (2)0.0075 (13)0.0005 (17)0.0006 (15)
C150.0512 (18)0.0380 (14)0.079 (2)0.0012 (12)0.0129 (15)0.0064 (13)
C160.0457 (16)0.0304 (12)0.0526 (15)0.0027 (11)0.0016 (12)0.0056 (11)
C170.0563 (17)0.0387 (13)0.0527 (16)0.0057 (12)0.0071 (13)0.0101 (11)
C180.0354 (15)0.0429 (13)0.0355 (13)0.0000 (11)0.0084 (11)0.0030 (10)
C190.0335 (15)0.0601 (16)0.0471 (15)0.0018 (13)0.0005 (12)0.0007 (12)
C200.0357 (15)0.0464 (14)0.0473 (14)0.0037 (11)0.0014 (12)0.0047 (11)
C210.0379 (14)0.0453 (13)0.0340 (13)0.0012 (11)0.0070 (11)0.0043 (10)
C220.0364 (14)0.0410 (13)0.0417 (13)0.0033 (11)0.0080 (11)0.0054 (10)
C230.0475 (17)0.0524 (16)0.0654 (18)0.0002 (13)0.0096 (14)0.0141 (13)
C240.065 (2)0.0455 (16)0.088 (2)0.0040 (14)0.0062 (17)0.0218 (14)
C250.0514 (17)0.0407 (14)0.0511 (15)0.0003 (12)0.0003 (13)0.0089 (11)
C260.0584 (19)0.0521 (16)0.0590 (17)0.0073 (14)0.0057 (14)0.0017 (13)
N10.0354 (13)0.0505 (12)0.0475 (12)0.0011 (10)0.0016 (10)0.0037 (9)
N20.0357 (12)0.0397 (11)0.0440 (11)0.0041 (9)0.0054 (9)0.0016 (9)
N30.079 (2)0.0508 (14)0.0889 (19)0.0089 (13)0.0057 (15)0.0148 (13)
N40.0392 (13)0.0472 (11)0.0494 (12)0.0050 (10)0.0041 (10)0.0038 (9)
N50.0350 (12)0.0394 (11)0.0420 (11)0.0016 (9)0.0053 (9)0.0027 (8)
N60.0645 (17)0.0434 (13)0.0754 (16)0.0052 (11)0.0007 (13)0.0055 (11)
S10.0409 (4)0.0417 (3)0.0538 (4)0.0057 (3)0.0044 (3)0.0051 (3)
S20.0425 (4)0.0402 (3)0.0539 (4)0.0003 (3)0.0067 (3)0.0024 (3)
Geometric parameters (Å, °) top
C1—N21.328 (2)C13—H130.9300
C1—N11.331 (3)C14—C151.369 (3)
C1—S11.748 (2)C14—H140.9300
C2—N11.329 (3)C15—C161.385 (3)
C2—C31.364 (3)C15—H150.9300
C2—H20.9300C16—C171.500 (3)
C3—C41.381 (3)C17—S21.810 (2)
C3—H30.9300C17—H17A0.9700
C4—N21.338 (2)C17—H17B0.9700
C4—C51.478 (3)C18—N41.323 (3)
C5—C61.369 (3)C18—N51.328 (2)
C5—C91.375 (3)C18—S21.754 (2)
C6—C71.371 (3)C19—N41.333 (3)
C6—H60.9300C19—C201.360 (3)
C7—N31.320 (3)C19—H190.9300
C7—H70.9300C20—C211.379 (3)
C8—N31.324 (3)C20—H200.9300
C8—C91.372 (3)C21—N51.339 (2)
C8—H80.9300C21—C221.474 (3)
C9—H90.9300C22—C251.369 (3)
C10—C111.509 (3)C22—C231.377 (3)
C10—S11.807 (2)C23—C241.374 (3)
C10—H10A0.9700C23—H230.9300
C10—H10B0.9700C24—N61.321 (3)
C11—C161.377 (3)C24—H240.9300
C11—C121.389 (3)C25—C261.367 (3)
C12—C131.368 (3)C25—H250.9300
C12—H120.9300C26—N61.314 (3)
C13—C141.354 (4)C26—H260.9300
N2—C1—N1127.8 (2)C14—C15—H15119.2
N2—C1—S1113.12 (17)C16—C15—H15119.2
N1—C1—S1119.04 (17)C11—C16—C15118.6 (2)
N1—C2—C3123.0 (2)C11—C16—C17122.7 (2)
N1—C2—H2118.5C15—C16—C17118.7 (2)
C3—C2—H2118.5C16—C17—S2111.68 (15)
C2—C3—C4118.2 (2)C16—C17—H17A109.3
C2—C3—H3120.9S2—C17—H17A109.3
C4—C3—H3120.9C16—C17—H17B109.3
N2—C4—C3120.2 (2)S2—C17—H17B109.3
N2—C4—C5117.2 (2)H17A—C17—H17B107.9
C3—C4—C5122.6 (2)N4—C18—N5128.1 (2)
C6—C5—C9116.6 (2)N4—C18—S2120.10 (17)
C6—C5—C4121.9 (2)N5—C18—S2111.83 (17)
C9—C5—C4121.5 (2)N4—C19—C20123.3 (2)
C5—C6—C7119.8 (2)N4—C19—H19118.4
C5—C6—H6120.1C20—C19—H19118.4
C7—C6—H6120.1C19—C20—C21117.4 (2)
N3—C7—C6124.2 (2)C19—C20—H20121.3
N3—C7—H7117.9C21—C20—H20121.3
C6—C7—H7117.9N5—C21—C20121.2 (2)
N3—C8—C9124.2 (2)N5—C21—C22116.3 (2)
N3—C8—H8117.9C20—C21—C22122.4 (2)
C9—C8—H8117.9C25—C22—C23116.7 (2)
C8—C9—C5119.5 (2)C25—C22—C21120.9 (2)
C8—C9—H9120.3C23—C22—C21122.4 (2)
C5—C9—H9120.3C24—C23—C22119.7 (2)
C11—C10—S1107.66 (15)C24—C23—H23120.1
C11—C10—H10A110.2C22—C23—H23120.1
S1—C10—H10A110.2N6—C24—C23123.7 (2)
C11—C10—H10B110.2N6—C24—H24118.1
S1—C10—H10B110.2C23—C24—H24118.1
H10A—C10—H10B108.5C26—C25—C22119.1 (2)
C16—C11—C12119.3 (2)C26—C25—H25120.4
C16—C11—C10122.9 (2)C22—C25—H25120.4
C12—C11—C10117.7 (2)N6—C26—C25125.1 (2)
C13—C12—C11120.6 (3)N6—C26—H26117.4
C13—C12—H12119.7C25—C26—H26117.4
C11—C12—H12119.7C2—N1—C1114.35 (19)
C14—C13—C12120.5 (3)C1—N2—C4116.4 (2)
C14—C13—H13119.8C7—N3—C8115.6 (2)
C12—C13—H13119.8C18—N4—C19114.42 (19)
C13—C14—C15119.4 (3)C18—N5—C21115.62 (19)
C13—C14—H14120.3C26—N6—C24115.6 (2)
C15—C14—H14120.3C1—S1—C10103.16 (11)
C14—C15—C16121.6 (3)C18—S2—C17104.16 (11)
Acknowledgements top

The authors are indebted to the National Natural Science Foundationof China (grant No. 20801011) for financial support.

references
References top

Bruker (2000). SADABS, SMART and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.

Dong, H. Z., Zhao, J., Zhu, H. B. & Gou, S. H. (2009). Polyhedron, 28, 1040–1048.

Dong, H. Z., Zhu, H. B., Tong, T. F. & Gou, S. H. (2008). J. Mol. Struct. 891, 266–271.

Huang, C. H., Gou, S. H., Zhu, H. B. & Huang, W. (2007). Inorg. Chem. 46, 5537–5543.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.