Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807043024/ng2324sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536807043024/ng2324Isup2.hkl |
CCDC reference: 223965
AgNO3 (0.68 g, 4.0 mmol), NH4SCN (0.61 g, 4.0 mmol) and hmt (1.4 g, 10 mmol) were added to a stired CoCl2.6H2O (0.47 g, 2.0 mmol) solution in acetonitrile, respectively. The mixture was stirred in r.t. for 12 h. After filtration, the filtrate was disposed to stand in the air. A few days later, purple-red single crystals suitable for X-ray diffraction were obtained.
The positions of hydrogen atoms were generated geometrically (C—H bond fixed at 0.96 Å) expect those connected to O1w atoms which are generated according to the fourier map, assigned isotropic thermal parameters and allowed to ride on their respective parent C atoms before the final cycle of least-squares refinement.
Thiocyanate ion has played an important role in constructing heteronuclear complexes in our systems. (Li, Tong et al.,2004; Li, Zhao et al., 2004). Herein is described a crystal structure of thiocyanate complex, [Co(NCS)2(H2O)4].2(C6H12N4). The cell contains two same units of the title compound. A perspective drawing of the complex with atomic numbering scheme is depicted in Fig. 1 and selected bonding parameters are presented in Table 1.
The cobalt atom locates in a slightly disordered CoN2O4 octahedral coordination geometry. Each hmt connects with four [Co(NCS)2(H2O)4] units and each [Co(NCS)2(H2O)4] unit connects with eight hmt molecules through O—H···N hydrogen bonds leading to 3-D network.
For related compounds, see Li, Tong et al. (2004); Li, Zhao et al. (2004).
Data collection: SMART (Siemens, 1996); cell refinement: SAINT (Siemens, 1996); data reduction: SAINT (Siemens, 1996); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1996); molecular graphics: SHELXTL (Bruker, 1999); software used to prepare material for publication: SHELXTL (Bruker, 1999).
Fig. 1. A view of the complex with the atomic numbering scheme. Displacement ellipsoids are drawn at the 30% probability level. |
[Co(H2O)4(NCS)2]·2C6H12N4 | Dx = 1.418 Mg m−3 |
Mr = 527.55 | Mo Kα radiation, λ = 0.71073 Å |
Tetragonal, P42/mnm | Cell parameters from 200 reflections |
Hall symbol: -P 4n 2n | θ = 2.6–25.1° |
a = 9.4846 (4) Å | µ = 0.90 mm−1 |
c = 13.7339 (6) Å | T = 293 K |
V = 1235.47 (7) Å3 | Prism, purple-red |
Z = 2 | 0.43 × 0.40 × 0.25 mm |
F(000) = 554 |
Siemens SMART diffractometer | 625 independent reflections |
Radiation source: fine-focus sealed tube | 554 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.024 |
φ and ω scans | θmax = 25.1°, θmin = 2.6° |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −7→11 |
Tmin = 0.685, Tmax = 0.798 | k = −11→11 |
2871 measured reflections | l = −16→10 |
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)] = 0.034 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.100 | w = 1/[σ2(Fo2) + (0.0614P)2 + 0.8126P] where P = (Fo2 + 2Fc2)/3 |
S = 1.06 | (Δ/σ)max = 0.01 |
626 reflections | Δρmax = 0.33 e Å−3 |
58 parameters | Δρmin = −0.46 e Å−3 |
0 restraints | Extinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.052 (5) |
[Co(H2O)4(NCS)2]·2C6H12N4 | Z = 2 |
Mr = 527.55 | Mo Kα radiation |
Tetragonal, P42/mnm | µ = 0.90 mm−1 |
a = 9.4846 (4) Å | T = 293 K |
c = 13.7339 (6) Å | 0.43 × 0.40 × 0.25 mm |
V = 1235.47 (7) Å3 |
Siemens SMART diffractometer | 625 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | 554 reflections with I > 2σ(I) |
Tmin = 0.685, Tmax = 0.798 | Rint = 0.024 |
2871 measured reflections |
R[F2 > 2σ(F2)] = 0.034 | 0 restraints |
wR(F2) = 0.100 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.06 | Δρmax = 0.33 e Å−3 |
626 reflections | Δρmin = −0.46 e Å−3 |
58 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 | ||
Co | 0.5000 | 0.5000 | 0.5000 | 0.0295 (4) | |
S1 | 0.86349 (9) | 0.86349 (9) | 0.5000 | 0.0606 (5) | |
O1W | 0.3901 (3) | 0.6099 (3) | 0.3938 (3) | 0.0960 (13) | |
H1 | 0.3990 | 0.7114 | 0.3810 | 0.115* | |
N1 | 0.6560 (3) | 0.6560 (3) | 0.5000 | 0.0413 (9) | |
C1 | 0.7427 (3) | 0.7427 (3) | 0.5000 | 0.0348 (10) | |
N2 | 0.1198 (3) | 0.5440 (3) | 0.31207 (17) | 0.0558 (7) | |
C2 | 0.0000 | 0.5000 | 0.3713 (3) | 0.0637 (13) | |
H2 | −0.023 (4) | 0.572 (4) | 0.409 (2) | 0.081 (11)* | |
C3 | 0.1598 (3) | 0.4253 (4) | 0.2505 (3) | 0.0632 (9) | |
H3A | 0.179 (4) | 0.350 (4) | 0.293 (3) | 0.078 (11)* | |
H3B | 0.243 (4) | 0.457 (4) | 0.212 (3) | 0.079 (10)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Co | 0.0285 (4) | 0.0285 (4) | 0.0315 (5) | −0.0055 (3) | 0.000 | 0.000 |
S1 | 0.0445 (6) | 0.0445 (6) | 0.0930 (11) | −0.0205 (6) | 0.000 | 0.000 |
O1W | 0.0788 (14) | 0.0788 (14) | 0.131 (3) | −0.0392 (18) | −0.0664 (18) | 0.0664 (18) |
N1 | 0.0391 (14) | 0.0391 (14) | 0.046 (2) | −0.0050 (18) | 0.000 | 0.000 |
C1 | 0.0322 (15) | 0.0322 (15) | 0.040 (2) | −0.0018 (19) | 0.000 | 0.000 |
N2 | 0.0523 (14) | 0.0631 (15) | 0.0520 (13) | 0.0067 (11) | −0.0179 (11) | −0.0131 (11) |
C2 | 0.095 (4) | 0.065 (3) | 0.0310 (18) | 0.031 (2) | 0.000 | 0.000 |
C3 | 0.0467 (17) | 0.071 (2) | 0.072 (2) | 0.0158 (15) | 0.0021 (14) | −0.0125 (17) |
Co—O1Wi | 2.074 (3) | N2—C2 | 1.459 (3) |
Co—O1Wii | 2.074 (3) | N2—C3iv | 1.459 (4) |
Co—O1W | 2.074 (3) | N2—C3 | 1.458 (4) |
Co—O1Wiii | 2.074 (3) | C2—N2v | 1.459 (3) |
Co—N1ii | 2.092 (4) | C2—H2 | 0.88 (3) |
Co—N1 | 2.092 (4) | C3—N2vi | 1.459 (4) |
S1—C1 | 1.621 (5) | C3—H3A | 0.94 (4) |
O1W—H1 | 0.9821 | C3—H3B | 0.99 (4) |
N1—C1 | 1.163 (6) | ||
O1Wi—Co—O1Wii | 89.4 (3) | Co—O1W—H1 | 125.1 |
O1Wi—Co—O1W | 90.6 (3) | C1—N1—Co | 180.0 |
O1Wii—Co—O1W | 180.0 | N1—C1—S1 | 179.999 (1) |
O1Wi—Co—O1Wiii | 180.0 | C2—N2—C3iv | 108.4 (2) |
O1Wii—Co—O1Wiii | 90.6 (3) | C2—N2—C3 | 107.8 (2) |
O1W—Co—O1Wiii | 89.4 (3) | C3iv—N2—C3 | 108.44 (18) |
O1Wi—Co—N1ii | 90.0 | N2—C2—N2v | 112.2 (3) |
O1Wii—Co—N1ii | 90.0 | N2—C2—H2 | 107 (2) |
O1W—Co—N1ii | 90.0 | N2v—C2—H2 | 111 (2) |
O1Wiii—Co—N1ii | 90.0 | N2vi—C3—N2 | 111.8 (3) |
O1Wi—Co—N1 | 90.0 | N2vi—C3—H3A | 107 (2) |
O1Wii—Co—N1 | 90.0 | N2—C3—H3A | 106 (2) |
O1W—Co—N1 | 90.0 | N2vi—C3—H3B | 112 (2) |
O1Wiii—Co—N1 | 90.0 | N2—C3—H3B | 106 (2) |
N1ii—Co—N1 | 180.0 | H3A—C3—H3B | 114 (3) |
Symmetry codes: (i) −x+1, −y+1, z; (ii) −x+1, −y+1, −z+1; (iii) x, y, −z+1; (iv) −y+1/2, x+1/2, −z+1/2; (v) −x, −y+1, z; (vi) y−1/2, −x+1/2, −z+1/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
O1W—H1···N2vii | 0.98 | 1.94 | 2.867 (3) | 157.1 |
Symmetry code: (vii) −y+1, −x+1, z. |
Experimental details
Crystal data | |
Chemical formula | [Co(H2O)4(NCS)2]·2C6H12N4 |
Mr | 527.55 |
Crystal system, space group | Tetragonal, P42/mnm |
Temperature (K) | 293 |
a, c (Å) | 9.4846 (4), 13.7339 (6) |
V (Å3) | 1235.47 (7) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 0.90 |
Crystal size (mm) | 0.43 × 0.40 × 0.25 |
Data collection | |
Diffractometer | Siemens SMART diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 1996) |
Tmin, Tmax | 0.685, 0.798 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 2871, 625, 554 |
Rint | 0.024 |
(sin θ/λ)max (Å−1) | 0.596 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.034, 0.100, 1.06 |
No. of reflections | 626 |
No. of parameters | 58 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.33, −0.46 |
Computer programs: SMART (Siemens, 1996), SAINT (Siemens, 1996), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1996), SHELXTL (Bruker, 1999).
O1Wi—Co—O1W | 90.6 (3) | C1—N1—Co | 180.0 |
O1W—Co—O1Wii | 89.4 (3) | N1—C1—S1 | 179.999 (1) |
Symmetry codes: (i) −x+1, −y+1, z; (ii) x, y, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
O1W—H1···N2iii | 0.98 | 1.94 | 2.867 (3) | 157.1 |
Symmetry code: (iii) −y+1, −x+1, z. |
Thiocyanate ion has played an important role in constructing heteronuclear complexes in our systems. (Li, Tong et al.,2004; Li, Zhao et al., 2004). Herein is described a crystal structure of thiocyanate complex, [Co(NCS)2(H2O)4].2(C6H12N4). The cell contains two same units of the title compound. A perspective drawing of the complex with atomic numbering scheme is depicted in Fig. 1 and selected bonding parameters are presented in Table 1.
The cobalt atom locates in a slightly disordered CoN2O4 octahedral coordination geometry. Each hmt connects with four [Co(NCS)2(H2O)4] units and each [Co(NCS)2(H2O)4] unit connects with eight hmt molecules through O—H···N hydrogen bonds leading to 3-D network.