supplementary materials

[
-N1,N2-Bis(pyridin-2-yl)hydrazine-1,2-dicarbothioamidato]bis[chloridocopper(II)]
The ligand (L),
N,N'-di(pyridin-2-yl)hydrazine-1,2-bis(carbothioamide,)
was prepared by the literature method (Szecsenyi et al., 2006).
L (0.05 mmol) was solved in DMF (5 ml) in a test tube, then an 8 ml
solvent mixture of CH3OH and DMF (v/v = 1:1) was added as a buffer layer. A
solution of CuCl2(0.10 mmol) in CH3OH (3 ml) was then carefully layered on
top. The system was sealed and kept for a week, after which black block-like
single crystals, suitable for X-ray analysis, were obtained. Anal. Calcd for
C12H10Cl2Cu2N6S2: C 28.80, H 2.01, N16.80. Found: C 29.23; H,
2.40; N, 16.44.
The NH and C-bound H atoms were included in calculated positions and treated
as riding atoms: N–H = 0.86 Å and C–H = 0.93 Å ,
with Uiso(H) = 1.2Ueq(N,C).
Data collection: SMART (Bruker, 2003); cell refinement: SAINT-Plus (Bruker, 2003); data reduction: SAINT-Plus (Bruker, 2003); 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).
[µ-
N1,
N2-Bis(pyridin-2-yl)hydrazine-1,2-
dicarbothioamidato]bis[chloridocopper(II)]
top
Crystal data top
| [Cu2(C12H10N6S2)Cl2] | F(000) = 992 |
| Mr = 500.36 | Dx = 2.073 Mg m−3 |
| Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -C 2yc | Cell parameters from 253 reflections |
| a = 15.825 (3) Å | θ = 2.9–29.5° |
| b = 7.6190 (13) Å | µ = 3.26 mm−1 |
| c = 15.082 (4) Å | T = 293 K |
| β = 118.179 (2)° | Block, black |
| V = 1602.9 (6) Å3 | 0.32 × 0.28 × 0.27 mm |
| Z = 4 | |
Data collection top
Bruker SMART APEX CCD diffractometer | 1561 independent reflections |
| Radiation source: fine-focus sealed tube | 1445 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.018 |
| φ and ω scans | θmax = 26.0°, θmin = 2.9° |
Absorption correction: multi-scan (SADABS; Bruker, 2003) | h = −19→18 |
| Tmin = 0.422, Tmax = 0.474 | k = −9→7 |
| 4270 measured reflections | l = −18→17 |
Refinement top
| 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) + (0.0374P)2 + 2.3083P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.07 | (Δ/σ)max < 0.001 |
| 1561 reflections | Δρmax = 0.73 e Å−3 |
| 110 parameters | Δρmin = −0.34 e Å−3 |
| 0 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: 0.0018 (3) |
Crystal data top
| [Cu2(C12H10N6S2)Cl2] | V = 1602.9 (6) Å3 |
| Mr = 500.36 | Z = 4 |
| Monoclinic, C2/c | Mo Kα radiation |
| a = 15.825 (3) Å | µ = 3.26 mm−1 |
| b = 7.6190 (13) Å | T = 293 K |
| c = 15.082 (4) Å | 0.32 × 0.28 × 0.27 mm |
| β = 118.179 (2)° | |
Data collection top
Bruker SMART APEX CCD diffractometer | 1561 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2003) | 1445 reflections with I > 2σ(I) |
| Tmin = 0.422, Tmax = 0.474 | Rint = 0.018 |
| 4270 measured reflections | θmax = 26.0° |
Refinement top
| R[F2 > 2σ(F2)] = 0.024 | H-atom parameters constrained |
| wR(F2) = 0.068 | Δρmax = 0.73 e Å−3 |
| S = 1.07 | Δρmin = −0.34 e Å−3 |
| 1561 reflections | Absolute structure: ? |
| 110 parameters | Flack parameter: ? |
| 0 restraints | Rogers parameter: ? |
Special details top
Geometry. Bond distances, angles etc. have been calculated using the
rounded fractional coordinates. All su's are estimated
from the variances of the (full) variance-covariance matrix.
The cell esds are taken into account in the estimation of
distances, angles and torsion angles |
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| | x | y | z | Uiso*/Ueq | |
| Cu1 | 0.12780 (2) | 0.63445 (4) | 0.20890 (2) | 0.0266 (1) | |
| Cl1 | 0.25399 (4) | 0.50248 (9) | 0.20491 (5) | 0.0355 (2) | |
| S2 | 0.18501 (4) | 0.59737 (10) | 0.37400 (5) | 0.0336 (2) | |
| N1 | 0.07304 (14) | 0.7259 (3) | 0.06931 (14) | 0.0267 (6) | |
| N2 | 0.08612 (15) | 0.6577 (3) | 0.46876 (15) | 0.0297 (6) | |
| N3 | −0.00303 (14) | 0.6631 (3) | 0.29480 (15) | 0.0258 (6) | |
| C1 | −0.02056 (17) | 0.7259 (3) | 0.00390 (18) | 0.0265 (7) | |
| C2 | −0.05668 (19) | 0.7912 (4) | −0.09283 (19) | 0.0356 (8) | |
| C3 | 0.0058 (2) | 0.8611 (4) | −0.1223 (2) | 0.0452 (10) | |
| C4 | 0.1031 (2) | 0.8622 (4) | −0.0559 (2) | 0.0434 (10) | |
| C5 | 0.13323 (19) | 0.7951 (4) | 0.03822 (19) | 0.0340 (8) | |
| C6 | 0.07986 (17) | 0.6433 (3) | 0.37555 (18) | 0.0248 (7) | |
| H2 | −0.12210 | 0.78770 | −0.13690 | 0.0430* | |
| H2A | 0.13840 | 0.61870 | 0.51760 | 0.0360* | |
| H3 | −0.01690 | 0.90740 | −0.18660 | 0.0540* | |
| H4 | 0.14670 | 0.90750 | −0.07490 | 0.0520* | |
| H5 | 0.19850 | 0.79710 | 0.08320 | 0.0410* | |
Atomic displacement parameters (Å2) top| | U11 | U22 | U33 | U12 | U13 | U23 |
| Cu1 | 0.0178 (2) | 0.0406 (2) | 0.0238 (2) | 0.0017 (1) | 0.0118 (1) | 0.0002 (1) |
| Cl1 | 0.0250 (3) | 0.0472 (4) | 0.0381 (3) | 0.0039 (3) | 0.0181 (3) | −0.0055 (3) |
| S2 | 0.0188 (3) | 0.0567 (4) | 0.0270 (3) | 0.0091 (3) | 0.0123 (3) | 0.0067 (3) |
| N1 | 0.0221 (10) | 0.0354 (12) | 0.0249 (10) | −0.0031 (8) | 0.0131 (8) | −0.0023 (9) |
| N2 | 0.0190 (10) | 0.0477 (13) | 0.0217 (10) | 0.0072 (9) | 0.0090 (9) | 0.0026 (9) |
| N3 | 0.0191 (10) | 0.0392 (12) | 0.0213 (9) | −0.0001 (8) | 0.0113 (8) | 0.0005 (8) |
| C1 | 0.0251 (12) | 0.0323 (13) | 0.0260 (11) | −0.0019 (10) | 0.0152 (10) | −0.0031 (10) |
| C2 | 0.0294 (13) | 0.0508 (17) | 0.0245 (12) | −0.0022 (12) | 0.0109 (11) | 0.0020 (11) |
| C3 | 0.0462 (18) | 0.064 (2) | 0.0302 (14) | −0.0015 (14) | 0.0221 (14) | 0.0078 (13) |
| C4 | 0.0428 (17) | 0.0564 (19) | 0.0422 (16) | −0.0074 (13) | 0.0294 (15) | 0.0031 (13) |
| C5 | 0.0268 (13) | 0.0445 (15) | 0.0354 (13) | −0.0062 (11) | 0.0186 (12) | −0.0029 (12) |
| C6 | 0.0204 (12) | 0.0304 (13) | 0.0252 (11) | 0.0001 (9) | 0.0121 (10) | 0.0007 (9) |
Geometric parameters (Å, º) top
| Cu1—Cl1 | 2.2619 (10) | N3—N3i | 1.399 (3) |
| Cu1—S2 | 2.2295 (9) | N2—H2A | 0.8600 |
| Cu1—N1 | 1.986 (2) | C1—C2 | 1.384 (4) |
| Cu1—N3i | 1.961 (3) | C2—C3 | 1.369 (5) |
| S2—C6 | 1.711 (3) | C3—C4 | 1.385 (4) |
| N1—C1 | 1.337 (4) | C4—C5 | 1.366 (4) |
| N1—C5 | 1.352 (4) | C2—H2 | 0.9300 |
| N2—C6 | 1.366 (3) | C3—H3 | 0.9300 |
| N2—C1i | 1.386 (4) | C4—H4 | 0.9300 |
| N3—C6 | 1.311 (3) | C5—H5 | 0.9300 |
| | | |
| Cl1—Cu1—S2 | 94.32 (3) | N1—C1—C2 | 122.7 (3) |
| Cl1—Cu1—N1 | 94.39 (7) | N1—C1—N2i | 120.3 (2) |
| Cl1—Cu1—N3i | 159.80 (7) | C1—C2—C3 | 118.7 (3) |
| S2—Cu1—N1 | 166.41 (7) | C2—C3—C4 | 119.6 (3) |
| S2—Cu1—N3i | 85.31 (6) | C3—C4—C5 | 118.2 (3) |
| N1—Cu1—N3i | 90.08 (9) | N1—C5—C4 | 123.3 (3) |
| Cu1—S2—C6 | 96.01 (9) | N2—C6—N3 | 120.1 (3) |
| Cu1—N1—C1 | 123.98 (19) | S2—C6—N2 | 115.6 (2) |
| Cu1—N1—C5 | 118.58 (18) | S2—C6—N3 | 124.3 (2) |
| C1—N1—C5 | 117.4 (2) | C1—C2—H2 | 121.00 |
| C1i—N2—C6 | 129.5 (2) | C3—C2—H2 | 121.00 |
| Cu1i—N3—C6 | 124.48 (19) | C2—C3—H3 | 120.00 |
| N3i—N3—C6 | 113.7 (2) | C4—C3—H3 | 120.00 |
| Cu1i—N3—N3i | 119.99 (16) | C3—C4—H4 | 121.00 |
| C6—N2—H2A | 115.00 | C5—C4—H4 | 121.00 |
| C1i—N2—H2A | 115.00 | N1—C5—H5 | 118.00 |
| N2i—C1—C2 | 117.0 (3) | C4—C5—H5 | 118.00 |
| | | |
| Cl1—Cu1—S2—C6 | −165.43 (8) | C5—N1—C1—N2i | −179.7 (2) |
| N3i—Cu1—S2—C6 | −5.68 (11) | Cu1—N1—C5—C4 | −179.7 (2) |
| Cl1—Cu1—N1—C1 | 138.8 (2) | C1i—N2—C6—S2 | 166.0 (2) |
| Cl1—Cu1—N1—C5 | −42.3 (2) | C6i—N2i—C1—N1 | 26.4 (4) |
| N3i—Cu1—N1—C1 | −21.5 (2) | C6i—N2i—C1—C2 | −154.0 (3) |
| N3i—Cu1—N1—C5 | 157.5 (2) | C1i—N2—C6—N3 | −14.5 (4) |
| Cl1—Cu1—N3i—N3 | 94.0 (2) | N3i—N3—C6—N2 | 173.7 (2) |
| Cl1—Cu1—N3i—C6i | −69.8 (3) | Cu1i—N3—C6—S2 | 157.76 (14) |
| S2—Cu1—N3i—N3 | 4.18 (18) | Cu1i—N3—C6—N2 | −21.7 (3) |
| S2—Cu1—N3i—C6i | −159.6 (2) | C6—N3—N3i—Cu1 | 0.2 (3) |
| N1—Cu1—N3i—N3 | −163.03 (19) | C6—N3—N3i—C6i | 165.6 (2) |
| N1—Cu1—N3i—C6i | 33.2 (2) | Cu1i—N3—N3i—Cu1 | −165.23 (11) |
| Cu1—S2—C6—N2 | −171.77 (17) | N3i—N3—C6—S2 | −6.9 (3) |
| Cu1—S2—C6—N3 | 8.8 (2) | N1—C1—C2—C3 | −1.0 (4) |
| C1—N1—C5—C4 | −0.7 (4) | N2i—C1—C2—C3 | 179.4 (3) |
| Cu1—N1—C1—C2 | 179.7 (2) | C1—C2—C3—C4 | 1.1 (4) |
| C5—N1—C1—C2 | 0.8 (4) | C2—C3—C4—C5 | −1.0 (5) |
| Cu1—N1—C1—N2i | −0.7 (3) | C3—C4—C5—N1 | 0.8 (5) |
| Symmetry code: (i) −x, y, −z+1/2. |
Hydrogen-bond geometry (Å, º) top
| D—H···A | D—H | H···A | D···A | D—H···A |
| N2—H2A···Cl1ii | 0.86 | 2.70 | 3.507 (2) | 156 |
| C2—H2···Cl1iii | 0.93 | 2.77 | 3.482 (3) | 134 |
| C5—H5···S2iv | 0.93 | 2.82 | 3.425 (3) | 124 |
| Symmetry codes: (ii) x, −y+1, z+1/2; (iii) x−1/2, −y+3/2, z−1/2; (iv) −x+1/2, y+1/2, −z+1/2. |
Selected bond lengths (Å) top| Cu1—Cl1 | 2.2619 (10) | Cu1—N1 | 1.986 (2) |
| Cu1—S2 | 2.2295 (9) | Cu1—N3i | 1.961 (3) |
| Symmetry code: (i) −x, y, −z+1/2. |
Hydrogen-bond geometry (Å, º) top
| D—H···A | D—H | H···A | D···A | D—H···A |
| N2—H2A···Cl1ii | 0.86 | 2.70 | 3.507 (2) | 156 |
| C2—H2···Cl1iii | 0.93 | 2.77 | 3.482 (3) | 134 |
| C5—H5···S2iv | 0.93 | 2.82 | 3.425 (3) | 124 |
| Symmetry codes: (ii) x, −y+1, z+1/2; (iii) x−1/2, −y+3/2, z−1/2; (iv) −x+1/2, y+1/2, −z+1/2. |
This work was sponsored by the National Natural Science Foundation of China
(No. 20977115).
Akinchan, N. T., Drozdzewski, P. M. & Battagli, L. P. (2002). J. Chem. Crystallogr. 32, 91–97.
Bruker (2003). SADABS, SMART and SAINT-Plus. Bruker AXS Inc., Madison, Wisconsin, USA.
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.
Szecsenyi, K. M., Leovac, V. M. & Evans, I. R. (2006). J. Coord. Chem. 59, 523–530.
Wang, H. Y., Zhao, P. S., Song, J. & Li, R. Q. (2011). J. Chem. Crystallogr. 41, 379–385.
West, D. X., Liberta, A. E., Padhye, S. B., Chikate, R. C., Sonawane, P. B., Kumbhar, A. S. & Yerande, R. G. (1993). Coord. Chem. Rev. 123, 49–71.
Yamin, B. M. & Yusof, M. S. M. (2003). Acta Cryst. E59, o358–o359.
Thiosemicarbazide and their metal complexes have attracked considerable interest due to their biological activities, such as antiviral, antibacterial, antimalarial, antifungal, and antitumoral activities (West et al., 1993). Thiosemicarbazide are versatile ligands that can coordinate as neutral ligands or in the deprotonated form. They can also be used as flexible spacers with potential multiple binding sites to construct coordination polymers with multiple dimensions and various topologies. In the present paper, the synthesis and crystal structure of the title thiosemicarbazide binuclear copper(II) compound is reported.
The title compound possesses twofold rotational symmetry (Fig.1). Each CuII center occupies a four-coordinated pseudotetrahedral environment bound to one sulfur atom, one imine nitrogen atom, and one pyridine nitrogen atom from one N,N'-di(pyridin-2-yl)hydrazine-1,2-bis(carbothioamide) ligand, and one chlorine anion. The metal centres are connected via the hexadentate ligand into a binuclear structure. The molecule is bow-shaped. The thiosemicarbazide moiety (S2/N2(N3/N6) is twisted by 20.14 (13)° from the pyridine ring to which it is attached. The two thiosemicarbazide moieties, (S2/N2/N3/N6) and (S2A/N2A/N3A/N6A), are inclined to one another by 23.36 (13) °, while the pyrdine rings make a dihedral angle of 51.56 (14)°.
The Cu—S distance is 2.2295 (9) Å, and the Cu—N distances vary between 1.961 (3)–1.986 (2) Å. The C—S bond distances of 1.711 (3) Å are within the normal range for a C—S single bond, indicating that the thiosemicarbazide moieties adopt the thiol tautomeric form, acting as a doubly charged negative ligand. The C6—N distances of 1.311 (3)–1.366 (3) Å and the N3—N3A distance of 1.399 (3) Å are intermediate between formal single and double bonds, pointing to extensive electron delocalization over the entire ligand skeleton. This agrees well with the same distances observed in related compounds (Wang et al., 2011; Yamin & Yusof, 2003; Akinchan et al., 2002).
In the crystal, there are N-H···Cl hydrogen bonds, leading to the formation of ribbons propagating along [001], and C-H···Cl and C-H···S interactions (Table 1). The latter link the ribbons and together with π–π interactions lead to the formation of a three-dimensional structure [Cg1···Cg1i 3.6146 (19) Å; perpendicular separation 3.5312 (11) Å; slippage 0.772 Å; Cg1 is the centroid of pyrdine ring N1/C1-C5; symmetry code: (i) -x, -y+2, -z].