metal-organic compounds
Diaquabis[2,6-bis(4H-1,2,4-triazol-4-yl)pyridine-κN2]bis(selenocyanato-κN)cobalt(II)
aTianjin Key Laboratory of Structure and Performance for Functional Molecule, Tianjin Normal University, Tianjin 300071, People's Republic of China
*Correspondence e-mail: liuyuanyuan1973@yahoo.com.cn
In the title compound, [Co(NCSe)2(C9H7N7)2(H2O)2], the Co2+ cation is coordinated by two selenocyanate anions, two 2,6-bis(4H-1,2,4-triazol-4-yl)pyridine ligands and two water molecules within a slightly distorted N4O2 octahedron. The consists of one Co2+ cation, which is located on a center of inversion, as well as one selenocyanate anion, one 2,6-bis(4H-1,2,4-triazol-4-yl)pyridine ligand and one water molecule in general positions. Intermolecular O—H⋯N hydrogen bonds join the complex molecules into layers parallel to the bc plane. The layers are linked by C—H⋯N and C—H⋯Se hydrogen bonds into a three-dimensional supramolecular architecture.
Related literature
For general background to this work, see: Liu et al. (2007). Previous research on compounds with Co(II) as cation have found a slow relaxation of the magnetization, see: Boeckmann & Näther (2010, 2011, 2012). For related structures, see: Du et al. (2009); Yang et al. (2008).
Experimental
Crystal data
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Refinement
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Data collection: APEX2 (Bruker, 2007); cell SAINT (Bruker, 2007); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL and DIAMOND (Brandenburg, 1999); software used to prepare material for publication: publCIF (Westrip, 2010).
Supporting information
https://doi.org/10.1107/S1600536812032461/zj2088sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536812032461/zj2088Isup2.hkl
The compound was synthesized under hydrothermal conditions. A mixture of L (L = 1,4-Bis(2,6-Bis(4H-1,2,4-triazol-4-yl)pyridine) (0.3 mmol, 0.0636 g), CoSO4.7H2O (0.1 mmol, 0.028 g), KSeCN (0.2 mmol, 0.029 g) and water (10 ml) was placed in a 25 ml acid digestion bomb and heated at 393 K for two days, then equably cooled to room temperature for three days. After washed by 5 ml water for twice, Red block crystals of the compound were obtained..
The water H atoms were located in a Fourier difference map and refined subject to an O—H restraint 0.88 (1) Å and an H···H restraint of 1.42 (2) Å. Other H atoms were allowed to ride on their parent atoms with C—H distances of 0.93 Å (Uiso(H) = 1.2Ueq(C)). All of the non-hydrogen atoms were refined anisotropically..
Previously we have reported on the a series of novel zinc(II) and cadmium(II) compounds based on 2,6-di-(1,2,4-triazole-4-yl)pyridine (Liu et al., 2007). On the other hand, dependent on the nature of the metal cation, anti- or ferromagnetic ordering is observed and for the compounds with Co(II) as cation preivous resrarch have found a slow relaxation of the magnetization (Boeckmann & Näther 2010, 2011, 2012). To investigate the influence of the co-ligand on the magnetic properties for the compounds with Co(II), we tried to prepare cobalt(II) compounds based on 2,6-di-(1,2,4-triazole-4-yl)pyridine, which resulted in the formation of the title compound in which the neutral ligands are only terminal N-coordinated. This compound was characterized only by single-crystal X-ray diffraction. In the
the cobalt(II) cations are coordinated by four nitrogen atoms of two terminal N-bonded seleno-cyanato anions and two terminal bonded 2,6-di-(1,2,4-triazole-4-yl)pyridine co-ligands as well as two water molecules into discrete complexes (Fig. 1). The of the Co cations can be described as a slightly distorted octahedron with the Co cation located on a centre of inversion. The discrete cobalt complexes are bridged by intermolecular O—H···N, C—H···N and C—H···Se hydrogen bonds (Yang et al., 2008; Du et al., 2009), wich assemble (I) into a three-dimensional supra-molecular architecture(Fig. 2 and Table 1).Perspective drawing with the atomic numbering scheme is illustrated in figure 1. Selected geometric parameters (Å, °) for (I) are listed in table 1. Selected hydrogen-bonding geometric parameters (Å, °) for (I) are listed in table 2. The two-dimensional supramolecular framework of (I) is shown in Figure 2.
For general background to this work, see: Liu et al. (2007). Previous research on compounds with Co(II) as cation have found a slow relaxation of the magnetization, see: Boeckmann & Näther (2010, 2011, 2012). For related structures, see: Du et al. (2009); Yang et al. (2008).
Data collection: APEX2 (Bruker, 2007); cell
SAINT (Bruker, 2007); data reduction: SAINT (Bruker, 2007); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL and DIAMOND (Brandenburg, 1999); software used to prepare material for publication: publCIF (Westrip, 2010).[Co(NCSe)2(C9H7N7)2(H2O)2] | Z = 4 |
Mr = 731.35 | F(000) = 1444 |
Monoclinic, C2/c | Dx = 1.883 Mg m−3 |
Hall symbol: -C 2yc | Mo Kα radiation, λ = 0.71073 Å |
a = 17.5460 (16) Å | µ = 3.54 mm−1 |
b = 7.2752 (7) Å | T = 173 K |
c = 20.3148 (19) Å | Block, red |
β = 95.691 (2)° | 0.15 × 0.14 × 0.13 mm |
V = 2580.4 (4) Å3 |
Bruker APEXII CCD diffractometer | 2280 independent reflections |
Radiation source: fine-focus sealed tube | 2083 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.026 |
φ and ω scans | θmax = 25.0°, θmin = 2.3° |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −20→9 |
Tmin = 0.619, Tmax = 0.656 | k = −8→8 |
6336 measured reflections | l = −23→24 |
Refinement on F2 | 0 restraints |
Least-squares matrix: full | H-atom parameters constrained |
R[F2 > 2σ(F2)] = 0.026 | w = 1/[σ2(Fo2) + (0.0325P)2 + 4.1522P] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.065 | (Δ/σ)max = 0.002 |
S = 1.05 | Δρmax = 0.59 e Å−3 |
2280 reflections | Δρmin = −0.58 e Å−3 |
186 parameters |
[Co(NCSe)2(C9H7N7)2(H2O)2] | V = 2580.4 (4) Å3 |
Mr = 731.35 | Z = 4 |
Monoclinic, C2/c | Mo Kα radiation |
a = 17.5460 (16) Å | µ = 3.54 mm−1 |
b = 7.2752 (7) Å | T = 173 K |
c = 20.3148 (19) Å | 0.15 × 0.14 × 0.13 mm |
β = 95.691 (2)° |
Bruker APEXII CCD diffractometer | 2280 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | 2083 reflections with I > 2σ(I) |
Tmin = 0.619, Tmax = 0.656 | Rint = 0.026 |
6336 measured reflections |
R[F2 > 2σ(F2)] = 0.026 | 0 restraints |
wR(F2) = 0.065 | H-atom parameters constrained |
S = 1.05 | Δρmax = 0.59 e Å−3 |
2280 reflections | Δρmin = −0.58 e Å−3 |
186 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 | ||
Co1 | 1.0000 | 0.85337 (6) | 0.2500 | 0.01309 (13) | |
Se1 | 1.238743 (15) | 0.51140 (3) | 0.329458 (13) | 0.02053 (11) | |
O1 | 1.08413 (10) | 1.0675 (2) | 0.26203 (8) | 0.0171 (4) | |
H1A | 1.1136 | 1.0578 | 0.2321 | 0.026* | |
H1B | 1.1116 | 1.0623 | 0.2983 | 0.026* | |
N1 | 1.01232 (11) | 0.7890 (3) | 0.04271 (10) | 0.0134 (4) | |
N2 | 1.08763 (12) | 0.9006 (3) | 0.12643 (10) | 0.0171 (5) | |
N3 | 1.01748 (11) | 0.8524 (3) | 0.14815 (10) | 0.0143 (4) | |
N4 | 0.91149 (11) | 0.6660 (3) | −0.02481 (10) | 0.0125 (4) | |
N5 | 0.80409 (12) | 0.5469 (3) | −0.08553 (10) | 0.0136 (4) | |
N6 | 0.69319 (13) | 0.4701 (3) | −0.05234 (12) | 0.0217 (5) | |
N7 | 0.68675 (13) | 0.4682 (3) | −0.12169 (11) | 0.0182 (5) | |
N8 | 1.09050 (12) | 0.6689 (3) | 0.27341 (10) | 0.0180 (5) | |
C1 | 1.08281 (14) | 0.8611 (3) | 0.06371 (12) | 0.0156 (5) | |
H1 | 1.1228 | 0.8797 | 0.0361 | 0.019* | |
C2 | 0.97369 (14) | 0.7874 (3) | 0.09813 (12) | 0.0139 (5) | |
H2 | 0.9227 | 0.7452 | 0.0998 | 0.017* | |
C3 | 0.98360 (13) | 0.7256 (3) | −0.02156 (12) | 0.0114 (5) | |
C4 | 0.88145 (14) | 0.6091 (3) | −0.08405 (12) | 0.0135 (5) | |
C5 | 0.91929 (15) | 0.6072 (3) | −0.14054 (12) | 0.0160 (5) | |
H5 | 0.8949 | 0.5656 | −0.1817 | 0.019* | |
C6 | 0.99442 (14) | 0.6689 (3) | −0.13447 (12) | 0.0163 (5) | |
H6 | 1.0226 | 0.6702 | −0.1720 | 0.020* | |
C7 | 1.02849 (14) | 0.7287 (3) | −0.07389 (12) | 0.0150 (5) | |
H7 | 1.0801 | 0.7698 | −0.0685 | 0.018* | |
C8 | 0.76306 (16) | 0.5177 (3) | −0.03236 (14) | 0.0199 (6) | |
H8 | 0.7829 | 0.5305 | 0.0126 | 0.024* | |
C9 | 0.75337 (15) | 0.5140 (3) | −0.13963 (13) | 0.0171 (6) | |
H9 | 0.7651 | 0.5233 | −0.1842 | 0.020* | |
C10 | 1.14850 (15) | 0.6077 (3) | 0.29588 (12) | 0.0167 (5) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Co1 | 0.0104 (2) | 0.0163 (2) | 0.0123 (2) | 0.000 | −0.00015 (19) | 0.000 |
Se1 | 0.01776 (16) | 0.02176 (16) | 0.02165 (17) | 0.00585 (11) | −0.00019 (12) | 0.00176 (10) |
O1 | 0.0126 (8) | 0.0238 (9) | 0.0150 (9) | −0.0010 (8) | 0.0014 (7) | −0.0007 (7) |
N1 | 0.0111 (10) | 0.0154 (10) | 0.0138 (11) | −0.0007 (8) | 0.0017 (8) | −0.0003 (8) |
N2 | 0.0118 (11) | 0.0201 (10) | 0.0192 (12) | −0.0021 (9) | 0.0015 (9) | −0.0001 (9) |
N3 | 0.0113 (10) | 0.0159 (10) | 0.0158 (11) | −0.0006 (8) | 0.0020 (9) | 0.0017 (8) |
N4 | 0.0110 (10) | 0.0127 (9) | 0.0138 (10) | 0.0004 (8) | 0.0017 (8) | 0.0005 (8) |
N5 | 0.0101 (10) | 0.0156 (10) | 0.0150 (11) | −0.0016 (8) | 0.0012 (9) | −0.0010 (8) |
N6 | 0.0156 (11) | 0.0293 (12) | 0.0205 (12) | −0.0058 (10) | 0.0033 (10) | −0.0008 (10) |
N7 | 0.0151 (11) | 0.0208 (11) | 0.0185 (12) | −0.0006 (9) | 0.0005 (9) | −0.0004 (9) |
N8 | 0.0191 (12) | 0.0200 (10) | 0.0151 (11) | 0.0031 (10) | 0.0023 (9) | −0.0022 (9) |
C1 | 0.0121 (12) | 0.0177 (12) | 0.0171 (13) | −0.0028 (10) | 0.0017 (10) | −0.0015 (10) |
C2 | 0.0122 (11) | 0.0159 (12) | 0.0140 (12) | −0.0007 (10) | 0.0032 (10) | 0.0016 (10) |
C3 | 0.0105 (11) | 0.0089 (11) | 0.0145 (12) | 0.0003 (9) | −0.0002 (10) | 0.0012 (9) |
C4 | 0.0106 (12) | 0.0108 (11) | 0.0189 (13) | −0.0008 (10) | 0.0007 (10) | 0.0007 (10) |
C5 | 0.0182 (13) | 0.0155 (11) | 0.0145 (12) | −0.0021 (10) | 0.0021 (10) | −0.0032 (10) |
C6 | 0.0174 (13) | 0.0181 (12) | 0.0140 (12) | 0.0005 (10) | 0.0055 (10) | 0.0013 (10) |
C7 | 0.0104 (11) | 0.0157 (12) | 0.0190 (13) | 0.0000 (10) | 0.0021 (10) | 0.0022 (10) |
C8 | 0.0171 (14) | 0.0266 (14) | 0.0161 (14) | −0.0047 (11) | 0.0019 (11) | −0.0026 (10) |
C9 | 0.0157 (13) | 0.0193 (13) | 0.0160 (14) | −0.0017 (10) | 0.0002 (11) | −0.0005 (10) |
C10 | 0.0198 (14) | 0.0157 (12) | 0.0152 (13) | 0.0000 (11) | 0.0052 (11) | −0.0036 (10) |
Co1—N8i | 2.097 (2) | N5—C8 | 1.373 (3) |
Co1—N8 | 2.097 (2) | N5—C4 | 1.428 (3) |
Co1—N3i | 2.122 (2) | N6—C8 | 1.300 (4) |
Co1—N3 | 2.122 (2) | N6—N7 | 1.402 (3) |
Co1—O1 | 2.1434 (18) | N7—C9 | 1.302 (3) |
Co1—O1i | 2.1433 (17) | N8—C10 | 1.162 (3) |
Se1—C10 | 1.803 (3) | C1—H1 | 0.9500 |
O1—H1A | 0.8400 | C2—H2 | 0.9500 |
O1—H1B | 0.8400 | C3—C7 | 1.385 (3) |
N1—C2 | 1.371 (3) | C4—C5 | 1.382 (3) |
N1—C1 | 1.372 (3) | C5—C6 | 1.387 (4) |
N1—C3 | 1.429 (3) | C5—H5 | 0.9500 |
N2—C1 | 1.301 (3) | C6—C7 | 1.384 (3) |
N2—N3 | 1.393 (3) | C6—H6 | 0.9500 |
N3—C2 | 1.300 (3) | C7—H7 | 0.9500 |
N4—C4 | 1.331 (3) | C8—H8 | 0.9500 |
N4—C3 | 1.333 (3) | C9—H9 | 0.9500 |
N5—C9 | 1.365 (3) | ||
N8i—Co1—N8 | 100.44 (12) | C9—N7—N6 | 107.1 (2) |
N8i—Co1—N3i | 92.26 (8) | C10—N8—Co1 | 161.5 (2) |
N8—Co1—N3i | 87.48 (8) | N2—C1—N1 | 111.0 (2) |
N8i—Co1—N3 | 87.48 (8) | N2—C1—H1 | 124.5 |
N8—Co1—N3 | 92.26 (8) | N1—C1—H1 | 124.5 |
N3i—Co1—N3 | 179.60 (11) | N3—C2—N1 | 109.7 (2) |
N8i—Co1—O1 | 171.22 (7) | N3—C2—H2 | 125.2 |
N8—Co1—O1 | 86.66 (7) | N1—C2—H2 | 125.2 |
N3i—Co1—O1 | 93.20 (7) | N4—C3—C7 | 125.2 (2) |
N3—Co1—O1 | 87.09 (7) | N4—C3—N1 | 113.4 (2) |
N8i—Co1—O1i | 86.66 (7) | C7—C3—N1 | 121.4 (2) |
N8—Co1—O1i | 171.22 (7) | N4—C4—C5 | 125.0 (2) |
N3i—Co1—O1i | 87.09 (7) | N4—C4—N5 | 114.1 (2) |
N3—Co1—O1i | 93.20 (7) | C5—C4—N5 | 120.9 (2) |
O1—Co1—O1i | 86.76 (9) | C4—C5—C6 | 117.0 (2) |
Co1—O1—H1A | 108.8 | C4—C5—H5 | 121.5 |
Co1—O1—H1B | 113.3 | C6—C5—H5 | 121.5 |
H1A—O1—H1B | 106.9 | C7—C6—C5 | 120.2 (2) |
C2—N1—C1 | 104.6 (2) | C7—C6—H6 | 119.9 |
C2—N1—C3 | 126.1 (2) | C5—C6—H6 | 119.9 |
C1—N1—C3 | 129.3 (2) | C6—C7—C3 | 116.7 (2) |
C1—N2—N3 | 106.3 (2) | C6—C7—H7 | 121.6 |
C2—N3—N2 | 108.43 (19) | C3—C7—H7 | 121.6 |
C2—N3—Co1 | 129.19 (17) | N6—C8—N5 | 110.3 (2) |
N2—N3—Co1 | 121.72 (15) | N6—C8—H8 | 124.8 |
C4—N4—C3 | 115.8 (2) | N5—C8—H8 | 124.8 |
C9—N5—C8 | 104.8 (2) | N7—C9—N5 | 110.6 (2) |
C9—N5—C4 | 127.9 (2) | N7—C9—H9 | 124.7 |
C8—N5—C4 | 127.2 (2) | N5—C9—H9 | 124.7 |
C8—N6—N7 | 107.2 (2) | N8—C10—Se1 | 179.1 (2) |
C1—N2—N3—C2 | −0.3 (3) | C4—N4—C3—C7 | −1.3 (3) |
C1—N2—N3—Co1 | 171.20 (16) | C4—N4—C3—N1 | 178.59 (19) |
N8i—Co1—N3—C2 | 12.0 (2) | C2—N1—C3—N4 | 2.0 (3) |
N8—Co1—N3—C2 | 112.4 (2) | C1—N1—C3—N4 | −179.1 (2) |
N3i—Co1—N3—C2 | 62.2 (3) | C2—N1—C3—C7 | −178.1 (2) |
O1—Co1—N3—C2 | −161.1 (2) | C1—N1—C3—C7 | 0.8 (4) |
O1i—Co1—N3—C2 | −74.5 (2) | C3—N4—C4—C5 | 0.3 (3) |
N8i—Co1—N3—N2 | −157.53 (17) | C3—N4—C4—N5 | −179.81 (19) |
N8—Co1—N3—N2 | −57.18 (17) | C9—N5—C4—N4 | 166.4 (2) |
N3i—Co1—N3—N2 | −107.3 (3) | C8—N5—C4—N4 | −9.4 (3) |
O1—Co1—N3—N2 | 29.36 (17) | C9—N5—C4—C5 | −13.7 (4) |
O1i—Co1—N3—N2 | 115.95 (17) | C8—N5—C4—C5 | 170.5 (2) |
C8—N6—N7—C9 | 0.3 (3) | N4—C4—C5—C6 | 0.3 (4) |
N8i—Co1—N8—C10 | −156.3 (7) | N5—C4—C5—C6 | −179.6 (2) |
N3i—Co1—N8—C10 | −64.4 (6) | C4—C5—C6—C7 | 0.1 (4) |
N3—Co1—N8—C10 | 115.9 (6) | C5—C6—C7—C3 | −0.9 (3) |
O1—Co1—N8—C10 | 28.9 (6) | N4—C3—C7—C6 | 1.6 (4) |
O1i—Co1—N8—C10 | −12.6 (10) | N1—C3—C7—C6 | −178.2 (2) |
N3—N2—C1—N1 | 0.2 (3) | N7—N6—C8—N5 | −0.3 (3) |
C2—N1—C1—N2 | 0.0 (3) | C9—N5—C8—N6 | 0.3 (3) |
C3—N1—C1—N2 | −179.1 (2) | C4—N5—C8—N6 | 176.8 (2) |
N2—N3—C2—N1 | 0.3 (3) | N6—N7—C9—N5 | −0.1 (3) |
Co1—N3—C2—N1 | −170.33 (15) | C8—N5—C9—N7 | −0.1 (3) |
C1—N1—C2—N3 | −0.2 (3) | C4—N5—C9—N7 | −176.6 (2) |
C3—N1—C2—N3 | 178.9 (2) | Co1—N8—C10—Se1 | −132 (15) |
Symmetry code: (i) −x+2, y, −z+1/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1A···N2 | 0.84 | 2.43 | 3.017 (3) | 127 |
O1—H1B···N7ii | 0.84 | 2.00 | 2.837 (3) | 173 |
C1—H1···N6iii | 0.95 | 2.37 | 3.293 (3) | 163 |
C5—H5···N8iv | 0.95 | 2.56 | 3.356 (3) | 142 |
C7—H7···N6iii | 0.95 | 2.46 | 3.373 (3) | 162 |
C9—H9···Se1iv | 0.95 | 2.96 | 3.877 (3) | 164 |
Symmetry codes: (ii) x+1/2, −y+3/2, z+1/2; (iii) x+1/2, y+1/2, z; (iv) −x+2, −y+1, −z. |
Experimental details
Crystal data | |
Chemical formula | [Co(NCSe)2(C9H7N7)2(H2O)2] |
Mr | 731.35 |
Crystal system, space group | Monoclinic, C2/c |
Temperature (K) | 173 |
a, b, c (Å) | 17.5460 (16), 7.2752 (7), 20.3148 (19) |
β (°) | 95.691 (2) |
V (Å3) | 2580.4 (4) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 3.54 |
Crystal size (mm) | 0.15 × 0.14 × 0.13 |
Data collection | |
Diffractometer | Bruker APEXII CCD |
Absorption correction | Multi-scan (SADABS; Sheldrick, 1996) |
Tmin, Tmax | 0.619, 0.656 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 6336, 2280, 2083 |
Rint | 0.026 |
(sin θ/λ)max (Å−1) | 0.595 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.026, 0.065, 1.05 |
No. of reflections | 2280 |
No. of parameters | 186 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.59, −0.58 |
Computer programs: APEX2 (Bruker, 2007), SAINT (Bruker, 2007), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL and DIAMOND (Brandenburg, 1999), publCIF (Westrip, 2010).
Co1—N8i | 2.097 (2) | Co1—N3 | 2.122 (2) |
Co1—N8 | 2.097 (2) | Co1—O1 | 2.1434 (18) |
Co1—N3i | 2.122 (2) | Co1—O1i | 2.1433 (17) |
Symmetry code: (i) −x+2, y, −z+1/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1A···N2 | 0.84 | 2.43 | 3.017 (3) | 127.1 |
O1—H1B···N7ii | 0.84 | 2.00 | 2.837 (3) | 172.5 |
C1—H1···N6iii | 0.95 | 2.37 | 3.293 (3) | 163.1 |
C5—H5···N8iv | 0.95 | 2.56 | 3.356 (3) | 141.7 |
C7—H7···N6iii | 0.95 | 2.46 | 3.373 (3) | 161.8 |
C9—H9···Se1iv | 0.95 | 2.96 | 3.877 (3) | 163.6 |
Symmetry codes: (ii) x+1/2, −y+3/2, z+1/2; (iii) x+1/2, y+1/2, z; (iv) −x+2, −y+1, −z. |
Acknowledgements
This work was supported financially by Tianjin Educational Committee (20090504, 20110301) and Tianjin Normal University (1E0402B).
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Previously we have reported on the a series of novel zinc(II) and cadmium(II) compounds based on 2,6-di-(1,2,4-triazole-4-yl)pyridine (Liu et al., 2007). On the other hand, dependent on the nature of the metal cation, anti- or ferromagnetic ordering is observed and for the compounds with Co(II) as cation preivous resrarch have found a slow relaxation of the magnetization (Boeckmann & Näther 2010, 2011, 2012). To investigate the influence of the co-ligand on the magnetic properties for the compounds with Co(II), we tried to prepare cobalt(II) compounds based on 2,6-di-(1,2,4-triazole-4-yl)pyridine, which resulted in the formation of the title compound in which the neutral ligands are only terminal N-coordinated. This compound was characterized only by single-crystal X-ray diffraction. In the crystal structure the cobalt(II) cations are coordinated by four nitrogen atoms of two terminal N-bonded seleno-cyanato anions and two terminal bonded 2,6-di-(1,2,4-triazole-4-yl)pyridine co-ligands as well as two water molecules into discrete complexes (Fig. 1). The coordination polyhedron of the Co cations can be described as a slightly distorted octahedron with the Co cation located on a centre of inversion. The discrete cobalt complexes are bridged by intermolecular O—H···N, C—H···N and C—H···Se hydrogen bonds (Yang et al., 2008; Du et al., 2009), wich assemble (I) into a three-dimensional supra-molecular architecture(Fig. 2 and Table 1).
Perspective drawing with the atomic numbering scheme is illustrated in figure 1. Selected geometric parameters (Å, °) for (I) are listed in table 1. Selected hydrogen-bonding geometric parameters (Å, °) for (I) are listed in table 2. The two-dimensional supramolecular framework of (I) is shown in Figure 2.