Abstract
The title dinuclear complex, [Cu2Br2(C12H14N4S2)2], is located about an inversion center. The CuI ion is coordinated in a distorted tetrahedral geometry by two bridging Br atoms in addition to an N and an S atom from the 2-[(4,6-dimethylpyrimidin-2-yl)disulfanyl]-4,6-dimethylpyrimidine ligand. In the crystal, π–π stacking interactions are observed with a centroid–centroid distance of 3.590 (2) Å.
Related literature
For potential applications of heterocyclic thioamides and their metal complexes, see: Battistuzzi & Peyronel (1981 ▶); Holm & Solomon (1996 ▶); Cox et al. (2006 ▶); Falcomer et al. (2006 ▶); Sevier & Kaiser (2006 ▶); Saxena et al. (2009 ▶). For related structures, see: Lemos et al. (2001 ▶); Aslanidis et al. (2004 ▶); Freeman et al. (2008 ▶).
Experimental
Crystal data
[Cu2Br2(C12H14N4S2)2]
M r = 843.68
Monoclinic,
a = 15.3351 (7) Å
b = 15.3898 (7) Å
c = 14.3398 (7) Å
β = 109.178 (1)°
V = 3196.4 (3) Å3
Z = 4
Mo Kα radiation
μ = 4.12 mm−1
T = 293 K
0.21 × 0.18 × 0.10 mm
Data collection
Bruker SMART CCD diffractometer
Absorption correction: integration (SADABS; Bruker, 2003 ▶) T min = 0.425, T max = 0.662
12339 measured reflections
2732 independent reflections
2344 reflections with I > 2σ(I)
R int = 0.024
Refinement
R[F 2 > 2σ(F 2)] = 0.028
wR(F 2) = 0.077
S = 1.04
2732 reflections
181 parameters
55 restraints
H-atom parameters constrained
Δρmax = 0.37 e Å−3
Δρmin = −0.31 e Å−3
Data collection: SMART (Bruker, 1998 ▶); cell refinement: SAINT (Bruker, 2003 ▶); 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: SHELXL97 and publCIF (Westrip, 2010 ▶).
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812016315/lh5449sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812016315/lh5449Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Acknowledgments
We gratefully acknowledge financial support from the Center for Innovation in Chemistry (PERCH–CIC), the Commission on Higher Education, Ministry of Education, the Department of Chemistry and the Graduate School, Prince of Songkla University.
supplementary crystallographic information
Comment
The studies of cooordination multidentate ligands such as heterocyclic thioamides, in complexes of closed-shell d10 metal ions, have been shown attention from a number of researchers (Saxena et al., 2009; Cox et al., 2006; Falcomer et al., 2006) because of their interesting biochemical properties and presence in active sites of many metalloproteins (Holm & Solomon, 1996; Battistuzzi & Peyronel, 1981). Particularly, the formation of disulfide bonds is an essential step in the folding and assembly of the extracellular domains of many membrane and secreted proteins which are important features of the structure of many proteins (Sevier & Kaiser, 2006).
The molecular structure of the title compound is shown in Fig. 1. The complex is dinuclear in which the CuI ions adopt distorted tetrahedral geometries. There is a binuclear µ,µ'-dibromobridged CuBr2Cu core. The Cu—S and Cu—N distances are similar to those reported for other thioamide containing complexes (Aslanidis et al., 2004; Lemos et al., 2001) and the disulfide bond distances is shorter than that reported in a related compound with a disulfide bond (Freeman et al., 2008). The 'bite' angle S—Cu—N angle is 90.77 (7)°. The molecule lies on a crystallographic inversion center which is at the center of the CuBr2Cu core with a Cu···Cu separation of 2.7802 (7) Å. This value is close the sum of the van der Waals radii for two Cu atoms (2.8 Å). In the crystal π–π stacking interactions with a centroid to centroid distance of 3.590 (2) Å are observed (Fig. 2). In addition, fairly short C(sp3)—H···N intermolecular distances (H···N = 2.67 Å, C(sp3)—N = 3.41 Å and C(sp3)—H···N = 134.2°) are observed (Fig. 3).
Experimental
4,6-Dimethyl-2-pyrimidinethiol, dmpymtH, (0.07 g, 0.50 mmol) was dissolved in 30 cm3 of methanol at 343-348K. CuBr (0.1 g, 0.70 mmol) was added and the mixture was stirred for 5 h. The resulting clear solution was filtered off and left to evaporate at room temperature. The crystalline complex, which was deposited upon standing for several days, was filtered off and dried in vacuo (yield 75%).
Refinement
The H atoms bonded to C atoms were constrained with a riding model of C—H = 0.93–0.96 Å and with Uiso(H) = 1.2Ueq(C). The DELU instruction in SHELXL (Sheldrick, 2008) was used without any further parameters. This sets up 'rigid bond' restraints for all non-hydrogen atom. The dafault standard deviation values are 0.01 and 0.01. This appears to have little effect but it does affect the no of restraints (55) listed in the CIF.
Figures
Fig. 1.
The molecular structure with displacement ellipsoids drawn at the 50% probability level. Unlabeled atoms are related by (-x+1/2, -y+1/2, -z+1).
Fig. 2.
Part of the crystal structure with π–π stacking interactions shown as dashed lines.
Fig. 3.
Part of the crystal structure with weak C—H···N hydrogen bonds shown as dashed lines.
Crystal data
| [Cu2Br2(C12H14N4S2)2] | F(000) = 1680 |
| Mr = 843.68 | Dx = 1.753 Mg m−3 |
| Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -C 2yc | Cell parameters from 16645 reflections |
| a = 15.3351 (7) Å | θ = 1.9–24.7° |
| b = 15.3898 (7) Å | µ = 4.12 mm−1 |
| c = 14.3398 (7) Å | T = 293 K |
| β = 109.178 (1)° | Plate, colorless |
| V = 3196.4 (3) Å3 | 0.21 × 0.18 × 0.10 mm |
| Z = 4 |
Data collection
| Bruker SMART CCD diffractometer | 2732 independent reflections |
| Radiation source: fine-focus sealed tube | 2344 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.024 |
| φ and ω scans | θmax = 24.7°, θmin = 1.9° |
| Absorption correction: integration (SADABS; Bruker, 2003) | h = −18→18 |
| Tmin = 0.425, Tmax = 0.662 | k = −18→17 |
| 12339 measured reflections | l = −16→16 |
Refinement
| 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)] = 0.028 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.077 | H-atom parameters constrained |
| S = 1.04 | w = 1/[σ2(Fo2) + (0.0412P)2 + 3.1838P] where P = (Fo2 + 2Fc2)/3 |
| 2732 reflections | (Δ/σ)max = 0.001 |
| 181 parameters | Δρmax = 0.37 e Å−3 |
| 55 restraints | Δρmin = −0.31 e Å−3 |
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 > 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)
| x | y | z | Uiso*/Ueq | ||
| C1A | 0.12116 (19) | 0.06625 (19) | 0.6388 (2) | 0.0437 (7) | |
| C2A | 0.0939 (2) | −0.0746 (2) | 0.5935 (3) | 0.0541 (8) | |
| C3A | 0.1153 (2) | −0.0561 (2) | 0.5100 (3) | 0.0559 (8) | |
| H1A | 0.1118 | −0.0994 | 0.4637 | 0.067* | |
| C4A | 0.1417 (2) | 0.0265 (2) | 0.4949 (2) | 0.0491 (7) | |
| C5A | 0.0690 (3) | −0.1640 (2) | 0.6172 (4) | 0.0806 (12) | |
| H2A | 0.0531 | −0.1622 | 0.6766 | 0.097* | |
| H4A | 0.1206 | −0.2022 | 0.6264 | 0.097* | |
| H3A | 0.0172 | −0.1849 | 0.5637 | 0.097* | |
| C6A | 0.1667 (3) | 0.0518 (3) | 0.4062 (3) | 0.0738 (11) | |
| H7A | 0.1835 | 0.1121 | 0.4107 | 0.089* | |
| H5A | 0.1147 | 0.0423 | 0.3477 | 0.089* | |
| H6A | 0.2178 | 0.0173 | 0.4033 | 0.089* | |
| C1B | 0.0927 (2) | 0.3281 (2) | 0.6662 (2) | 0.0444 (7) | |
| C2B | 0.0657 (2) | 0.4721 (2) | 0.6545 (2) | 0.0535 (8) | |
| C3B | −0.0270 (2) | 0.4533 (2) | 0.6114 (2) | 0.0572 (8) | |
| H1B | −0.0700 | 0.4979 | 0.5910 | 0.069* | |
| C4B | −0.0549 (2) | 0.3680 (2) | 0.5989 (2) | 0.0534 (8) | |
| C5B | 0.1020 (3) | 0.5630 (2) | 0.6741 (3) | 0.0741 (11) | |
| H2B | 0.1679 | 0.5614 | 0.7044 | 0.089* | |
| H4B | 0.0749 | 0.5914 | 0.7174 | 0.089* | |
| H3B | 0.0866 | 0.5943 | 0.6129 | 0.089* | |
| C6B | −0.1546 (2) | 0.3429 (3) | 0.5541 (3) | 0.0743 (11) | |
| H5B | −0.1599 | 0.2807 | 0.5516 | 0.089* | |
| H6B | −0.1787 | 0.3661 | 0.4885 | 0.089* | |
| H7B | −0.1890 | 0.3658 | 0.5937 | 0.089* | |
| Cu1 | 0.20241 (3) | 0.20852 (2) | 0.55473 (3) | 0.05128 (14) | |
| N1A | 0.09541 (17) | −0.01146 (17) | 0.65843 (19) | 0.0522 (6) | |
| N2A | 0.14596 (16) | 0.09016 (15) | 0.56177 (17) | 0.0420 (5) | |
| N1B | 0.12747 (18) | 0.40741 (17) | 0.68337 (19) | 0.0515 (6) | |
| N2B | 0.00657 (18) | 0.30262 (16) | 0.62617 (19) | 0.0491 (6) | |
| S1A | 0.12183 (7) | 0.14055 (6) | 0.73360 (6) | 0.0591 (2) | |
| S1B | 0.18435 (6) | 0.24973 (5) | 0.70698 (6) | 0.0506 (2) | |
| Br1 | 0.13259 (2) | 0.31106 (2) | 0.42440 (3) | 0.05795 (13) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1A | 0.0383 (15) | 0.0440 (16) | 0.0466 (16) | 0.0048 (12) | 0.0110 (13) | 0.0077 (13) |
| C2A | 0.0375 (17) | 0.0438 (17) | 0.072 (2) | −0.0002 (13) | 0.0056 (15) | 0.0108 (16) |
| C3A | 0.0514 (19) | 0.0434 (17) | 0.066 (2) | −0.0011 (14) | 0.0099 (16) | −0.0083 (15) |
| C4A | 0.0506 (18) | 0.0460 (17) | 0.0482 (17) | 0.0027 (14) | 0.0127 (14) | −0.0042 (14) |
| C5A | 0.070 (3) | 0.049 (2) | 0.113 (3) | −0.0075 (18) | 0.017 (2) | 0.017 (2) |
| C6A | 0.107 (3) | 0.062 (2) | 0.063 (2) | −0.011 (2) | 0.042 (2) | −0.0166 (18) |
| C1B | 0.0487 (17) | 0.0486 (17) | 0.0411 (16) | 0.0076 (13) | 0.0216 (13) | −0.0017 (13) |
| C2B | 0.070 (2) | 0.0468 (18) | 0.0517 (18) | 0.0055 (15) | 0.0303 (16) | −0.0021 (14) |
| C3B | 0.060 (2) | 0.0566 (19) | 0.059 (2) | 0.0166 (15) | 0.0256 (16) | 0.0068 (16) |
| C4B | 0.0501 (18) | 0.063 (2) | 0.0504 (18) | 0.0081 (15) | 0.0211 (14) | 0.0066 (15) |
| C5B | 0.092 (3) | 0.051 (2) | 0.083 (3) | 0.0023 (19) | 0.034 (2) | −0.0080 (19) |
| C6B | 0.051 (2) | 0.090 (3) | 0.082 (3) | 0.0056 (19) | 0.0231 (18) | 0.018 (2) |
| Cu1 | 0.0570 (3) | 0.0424 (2) | 0.0616 (3) | 0.00037 (16) | 0.0292 (2) | 0.00422 (17) |
| N1A | 0.0473 (14) | 0.0483 (15) | 0.0595 (16) | −0.0005 (12) | 0.0157 (12) | 0.0126 (13) |
| N2A | 0.0429 (13) | 0.0409 (13) | 0.0426 (13) | −0.0011 (10) | 0.0146 (10) | 0.0018 (10) |
| N1B | 0.0565 (16) | 0.0476 (15) | 0.0552 (15) | 0.0014 (12) | 0.0249 (12) | −0.0074 (12) |
| N2B | 0.0477 (15) | 0.0521 (15) | 0.0501 (15) | 0.0017 (12) | 0.0197 (12) | 0.0034 (12) |
| S1A | 0.0828 (6) | 0.0531 (5) | 0.0510 (5) | 0.0106 (4) | 0.0351 (4) | 0.0078 (4) |
| S1B | 0.0495 (4) | 0.0485 (5) | 0.0521 (4) | 0.0070 (3) | 0.0142 (3) | −0.0062 (4) |
| Br1 | 0.0467 (2) | 0.0548 (2) | 0.0746 (3) | 0.01020 (14) | 0.02299 (17) | 0.02122 (16) |
Geometric parameters (Å, º)
| C1A—N1A | 1.319 (4) | C2B—C3B | 1.381 (5) |
| C1A—N2A | 1.332 (4) | C2B—C5B | 1.498 (5) |
| C1A—S1A | 1.774 (3) | C3B—C4B | 1.375 (5) |
| C2A—N1A | 1.341 (4) | C3B—H1B | 0.9300 |
| C2A—C3A | 1.371 (5) | C4B—N2B | 1.346 (4) |
| C2A—C5A | 1.496 (4) | C4B—C6B | 1.501 (5) |
| C3A—C4A | 1.372 (4) | C5B—H2B | 0.9600 |
| C3A—H1A | 0.9300 | C5B—H4B | 0.9600 |
| C4A—N2A | 1.358 (4) | C5B—H3B | 0.9600 |
| C4A—C6A | 1.495 (5) | C6B—H5B | 0.9600 |
| C5A—H2A | 0.9600 | C6B—H6B | 0.9600 |
| C5A—H4A | 0.9600 | C6B—H7B | 0.9600 |
| C5A—H3A | 0.9600 | Cu1—N2A | 2.033 (2) |
| C6A—H7A | 0.9600 | Cu1—S1B | 2.3754 (9) |
| C6A—H5A | 0.9600 | Cu1—Br1 | 2.4114 (5) |
| C6A—H6A | 0.9600 | Cu1—Br1i | 2.4669 (5) |
| C1B—N2B | 1.315 (4) | Cu1—Cu1i | 2.7801 (7) |
| C1B—N1B | 1.323 (4) | S1A—S1B | 2.0318 (13) |
| C1B—S1B | 1.798 (3) | Br1—Cu1i | 2.4668 (5) |
| C2B—N1B | 1.342 (4) | ||
| N1A—C1A—N2A | 127.9 (3) | C3B—C4B—C6B | 122.1 (3) |
| N1A—C1A—S1A | 110.3 (2) | C2B—C5B—H2B | 109.5 |
| N2A—C1A—S1A | 121.7 (2) | C2B—C5B—H4B | 109.5 |
| N1A—C2A—C3A | 120.0 (3) | H2B—C5B—H4B | 109.5 |
| N1A—C2A—C5A | 117.2 (3) | C2B—C5B—H3B | 109.5 |
| C3A—C2A—C5A | 122.8 (3) | H2B—C5B—H3B | 109.5 |
| C2A—C3A—C4A | 119.9 (3) | H4B—C5B—H3B | 109.5 |
| C2A—C3A—H1A | 120.0 | C4B—C6B—H5B | 109.5 |
| C4A—C3A—H1A | 120.0 | C4B—C6B—H6B | 109.5 |
| N2A—C4A—C3A | 120.3 (3) | H5B—C6B—H6B | 109.5 |
| N2A—C4A—C6A | 116.5 (3) | C4B—C6B—H7B | 109.5 |
| C3A—C4A—C6A | 123.2 (3) | H5B—C6B—H7B | 109.5 |
| C2A—C5A—H2A | 109.5 | H6B—C6B—H7B | 109.5 |
| C2A—C5A—H4A | 109.5 | N2A—Cu1—S1B | 90.77 (7) |
| H2A—C5A—H4A | 109.5 | N2A—Cu1—Br1 | 122.47 (7) |
| C2A—C5A—H3A | 109.5 | S1B—Cu1—Br1 | 112.43 (3) |
| H2A—C5A—H3A | 109.5 | N2A—Cu1—Br1i | 108.72 (7) |
| H4A—C5A—H3A | 109.5 | S1B—Cu1—Br1i | 110.22 (3) |
| C4A—C6A—H7A | 109.5 | Br1—Cu1—Br1i | 110.523 (16) |
| C4A—C6A—H5A | 109.5 | N2A—Cu1—Cu1i | 138.63 (7) |
| H7A—C6A—H5A | 109.5 | S1B—Cu1—Cu1i | 129.62 (3) |
| C4A—C6A—H6A | 109.5 | Br1—Cu1—Cu1i | 56.200 (16) |
| H7A—C6A—H6A | 109.5 | Br1i—Cu1—Cu1i | 54.323 (15) |
| H5A—C6A—H6A | 109.5 | C1A—N1A—C2A | 116.6 (3) |
| N2B—C1B—N1B | 129.9 (3) | C1A—N2A—C4A | 115.2 (3) |
| N2B—C1B—S1B | 120.5 (2) | C1A—N2A—Cu1 | 122.05 (19) |
| N1B—C1B—S1B | 109.5 (2) | C4A—N2A—Cu1 | 122.3 (2) |
| N1B—C2B—C3B | 120.1 (3) | C1B—N1B—C2B | 115.2 (3) |
| N1B—C2B—C5B | 116.9 (3) | C1B—N2B—C4B | 114.3 (3) |
| C3B—C2B—C5B | 123.0 (3) | C1A—S1A—S1B | 105.86 (11) |
| C4B—C3B—C2B | 119.3 (3) | C1B—S1B—S1A | 104.42 (11) |
| C4B—C3B—H1B | 120.4 | C1B—S1B—Cu1 | 101.24 (10) |
| C2B—C3B—H1B | 120.4 | S1A—S1B—Cu1 | 99.01 (4) |
| N2B—C4B—C3B | 121.2 (3) | Cu1—Br1—Cu1i | 69.476 (16) |
| N2B—C4B—C6B | 116.7 (3) |
Symmetry code: (i) −x+1/2, −y+1/2, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: LH5449).
References
- Aslanidis, P., Cox, P. J., Divanidis, S. & Karagiannidis, P. (2004). Inorg. Chim. Acta, 357, 4231–4239.
- Battistuzzi, R. & Peyronel, G. (1981). Can. J. Chem. 59, 591–596.
- Bruker (1998). SMART Bruker AXS Inc., Madison, Wisconsin, USA.
- Bruker (2003). SAINT and SADABS Bruker AXS Inc., Madison, Wisconsin, USA.
- Cox, P. J., Kaltzoglou, A. & Aslanidis, P. (2006). Inorg. Chim. Acta, 359, 3183–3190.
- Falcomer, V. A. S., Lemos, S. S., Batista, A. A., Ellena, A. & Castellano, E. E. (2006). Inorg. Chim. Acta, 359, 1064–1070.
- Freeman, F., Po, H. N., Ho, T. S. & Wang, X. (2008). J. Phys. Chem. A, 112, 1643–1655. [DOI] [PubMed]
- Holm, R. H. & Solomon, E. J. (1996). Chem. Rev. 96, 2239–2341. [DOI] [PubMed]
- Lemos, S. S., Camargo, M. A., Cadoso, Z. Z., Deflon, V. M., Försterling, F. H. & Hagenbach, A. (2001). Polyhedron, 20, 849–854.
- Saxena, A., Dugan, E. C., Liaw, J., Dembo, M. D. & Pike, R. D. (2009). Polyhedron, 28, 4017–4031.
- Sevier, C. S. & Kaiser, C. A. (2006). Antioxid. Redox Signal. 8, 797–811. [DOI] [PubMed]
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812016315/lh5449sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812016315/lh5449Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report



