supplementary materials


Acta Cryst. (2007). E63, m1591    [ doi:10.1107/S1600536807021393 ]

Diaquabis[5-(pyrazin-2-yl)tetrazolato]cobalt(II)

R.-H. Zeng, Y.-C. Qiu, Z.-H. Liu, Y.-H. Li and H. Deng

Abstract top

In the title complex, [Co(C5H3N3)2(H2O)2], prepared in a one-pot synthesis, the CoII atom (site symmetry \overline{1}), is coordinated by four N atoms from two 5-(2-pyrazinyl)tetrazolate ligands and by two water molecules in a distorted trans-CoO2N4 octahedral geometry. A supramolecular network is formed via intermolecular O-H...N hydrogen bonds.

Comment top

The design, synthesis, characterization, and properties of supramolecular networks formed by using functionalized organic molecules as bridges between metal centers are of great interest (Rizk et al., 2005; Eddaoudi et al., 2001). The reports on tetrazoles is expanding rapidly, since tetrazoles have an important role in coordination chemistry as a ligand (Deng et al., 2006). Recently, 5-substituted 1H-tetrazoles have been synthesized by a facile approach (Demko & Sharpless, 2001a, 2001b). In the general reaction, the tetrazoles are prepared by the addition of azide to nitriles in water with the aid of a lewis acid such a Zn2+. In this paper, we selected 2-cyanopyrazine, NaN3 and a Lewis acid CoCl2 as reagent, to yield in one step the mononuclear structure (I) under hydrothermal condition.

In (I), the CoII atom, located on an inversion center, is coordinated by four N atoms from two 5-(2-pyrazinyl)tetrazolate ligands and two water molecules in a distorted octahedral geometry (Fig. 1; Table 1). In the ligand, the pyrazinyl and tetrazolyl rings are almost coplanar, with a dihedral angle of 3.53 (4)°. Intermolecular O—H···N hydrogen bonds (Table 2) form a supramolecular network (Fig. 2).

Related literature top

For related literature, see: Demko & Sharpless (2001a, 2001b); Deng et al. (2007); Eddaoudi et al. (2001); Rizk et al. (2005).

Experimental top

Hydrothermal treatment of CoCl2.6H2O (1.0 mmol, 0.237 g), 2-cyanopyrazine (1 mmol, 0.105 g), NaN3 (1 mmol, 0.065 g), and water (3 ml) over 50 h at 422 K yielded red prisms of (I) (yield 78%).

Refinement top

The water H atoms were located in a difference Fourier map and their positions were freely refined with Uiso(H) = 1.2Ueq(O). The other H atoms were placed

in calculated positions (C—H = 0.93 Å) refined using a riding model with Uiso(H) = 1.2Ueq(C).

Computing details top

Data collection: APEX2 (Bruker, 2004); cell refinement: SAINT (Bruker, 2004); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 2004); software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. The structure of (I), showing the atomic numbering scheme. Non-H atoms are shown as 50% probability displacement ellipsoids. Unlabelled atoms are related to the labelled atoms by the symmetry operator (1 - x, 1 - y, -z).
[Figure 2] Fig. 2. A packing diagram of (I). Hydrogen bonds are depicted as broken lines.
Diaquabis[5-(pyrazin-2-yl)tetrazolate]cobalt(II) top
Crystal data top
[Co(C5H3N3)2(H2O)2]F(000) = 394
Mr = 389.23Dx = 1.809 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 5700 reflections
a = 6.0676 (1) Åθ = 1.7–28.0°
b = 11.4221 (2) ŵ = 1.24 mm1
c = 10.7096 (2) ÅT = 293 K
β = 105.652 (1)°Prism, red
V = 714.70 (2) Å30.18 × 0.16 × 0.15 mm
Z = 2
Data collection top
Bruker APEXII area-detector
diffractometer
1693 independent reflections
Radiation source: fine-focus sealed tube1325 reflections with I > 2σ(I)
graphiteRint = 0.035
φ and ω scansθmax = 27.9°, θmin = 2.7°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 77
Tmin = 0.808, Tmax = 0.836k = 1514
6011 measured reflectionsl = 1412
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)] = 0.034Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.083H atoms treated by a mixture of independent and constrained refinement
S = 1.06 w = 1/[σ2(Fo2) + (0.0392P)2 + 0.1286P]
where P = (Fo2 + 2Fc2)/3
1693 reflections(Δ/σ)max < 0.001
121 parametersΔρmax = 0.33 e Å3
3 restraintsΔρmin = 0.30 e Å3
Crystal data top
[Co(C5H3N3)2(H2O)2]V = 714.70 (2) Å3
Mr = 389.23Z = 2
Monoclinic, P21/nMo Kα radiation
a = 6.0676 (1) ŵ = 1.24 mm1
b = 11.4221 (2) ÅT = 293 K
c = 10.7096 (2) Å0.18 × 0.16 × 0.15 mm
β = 105.652 (1)°
Data collection top
Bruker APEXII area-detector
diffractometer
1693 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
1325 reflections with I > 2σ(I)
Tmin = 0.808, Tmax = 0.836Rint = 0.035
6011 measured reflectionsθmax = 27.9°
Refinement top
R[F2 > 2σ(F2)] = 0.034H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.083Δρmax = 0.33 e Å3
S = 1.06Δρmin = 0.30 e Å3
1693 reflectionsAbsolute structure: ?
121 parametersFlack parameter: ?
3 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
C10.5209 (3)0.24786 (18)0.0722 (2)0.0292 (5)
C20.4676 (4)0.13095 (19)0.0833 (3)0.0422 (6)
H20.58040.08130.13140.051*
C30.1084 (4)0.1622 (2)0.0407 (3)0.0437 (6)
H30.03790.13510.08130.052*
C40.1588 (4)0.2787 (2)0.0534 (2)0.0355 (5)
H40.04590.32770.10250.043*
C50.7458 (3)0.29806 (18)0.1328 (2)0.0292 (5)
Co10.50000.50000.00000.02720 (14)
H1W0.305 (3)0.5142 (18)0.182 (2)0.053*
H2W0.457 (4)0.5988 (15)0.212 (2)0.053*
N10.3655 (3)0.32279 (14)0.00284 (17)0.0286 (4)
N20.2619 (3)0.08721 (18)0.0278 (2)0.0507 (6)
N30.9254 (3)0.24591 (16)0.21020 (19)0.0355 (4)
N41.0867 (3)0.32889 (18)0.2402 (2)0.0427 (5)
N51.0062 (3)0.42684 (17)0.1815 (2)0.0393 (5)
N60.7895 (3)0.41001 (15)0.11191 (18)0.0306 (4)
O1W0.4169 (3)0.53856 (16)0.17002 (18)0.0428 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0287 (11)0.0243 (10)0.0337 (12)0.0012 (8)0.0066 (9)0.0007 (9)
C20.0394 (13)0.0269 (12)0.0563 (17)0.0021 (10)0.0057 (12)0.0062 (11)
C30.0346 (12)0.0398 (14)0.0532 (16)0.0101 (10)0.0061 (12)0.0053 (12)
C40.0295 (11)0.0368 (12)0.0378 (13)0.0004 (9)0.0053 (10)0.0005 (10)
C50.0292 (11)0.0241 (10)0.0343 (12)0.0034 (8)0.0086 (9)0.0032 (9)
Co10.0264 (2)0.0196 (2)0.0336 (2)0.00012 (16)0.00481 (16)0.00184 (17)
N10.0296 (9)0.0247 (9)0.0310 (10)0.0007 (7)0.0072 (8)0.0009 (7)
N20.0447 (12)0.0308 (11)0.0706 (16)0.0105 (9)0.0055 (11)0.0010 (11)
N30.0286 (9)0.0329 (10)0.0419 (11)0.0020 (8)0.0041 (8)0.0081 (9)
N40.0323 (10)0.0448 (12)0.0461 (12)0.0013 (9)0.0024 (9)0.0063 (10)
N50.0310 (10)0.0365 (11)0.0465 (12)0.0049 (8)0.0039 (9)0.0003 (9)
N60.0249 (9)0.0261 (9)0.0382 (11)0.0014 (7)0.0042 (8)0.0007 (8)
O1W0.0455 (10)0.0381 (9)0.0503 (11)0.0154 (8)0.0225 (9)0.0143 (8)
Geometric parameters (Å, °) top
C1—N11.340 (2)Co1—O1W2.0638 (18)
C1—C21.386 (3)Co1—O1Wi2.0638 (18)
C1—C51.461 (3)Co1—N6i2.1076 (17)
C2—N21.327 (3)Co1—N62.1076 (17)
C2—H20.9300Co1—N1i2.1856 (16)
C3—N21.330 (3)Co1—N12.1856 (16)
C3—C41.381 (3)N3—N41.338 (3)
C3—H30.9300N4—N51.311 (3)
C4—N11.335 (3)N5—N61.339 (2)
C4—H40.9300O1W—H1W0.777 (15)
C5—N31.320 (3)O1W—H2W0.819 (15)
C5—N61.337 (3)
N1—C1—C2121.15 (19)O1Wi—Co1—N1i90.25 (7)
N1—C1—C5115.39 (18)N6i—Co1—N1i78.31 (6)
C2—C1—C5123.46 (19)N6—Co1—N1i101.69 (6)
N2—C2—C1122.5 (2)O1W—Co1—N190.25 (7)
N2—C2—H2118.8O1Wi—Co1—N189.75 (7)
C1—C2—H2118.8N6i—Co1—N1101.69 (6)
N2—C3—C4122.3 (2)N6—Co1—N178.31 (6)
N2—C3—H3118.9N1i—Co1—N1180.0
C4—C3—H3118.9C4—N1—C1116.36 (18)
N1—C4—C3121.7 (2)C4—N1—Co1130.69 (15)
N1—C4—H4119.2C1—N1—Co1112.94 (13)
C3—C4—H4119.2C2—N2—C3116.0 (2)
N3—C5—N6111.69 (19)C5—N3—N4104.92 (17)
N3—C5—C1128.00 (19)N5—N4—N3109.61 (17)
N6—C5—C1120.31 (18)N4—N5—N6109.10 (17)
O1W—Co1—O1Wi180.0C5—N6—N5104.68 (17)
O1W—Co1—N6i91.90 (7)C5—N6—Co1112.91 (13)
O1Wi—Co1—N6i88.10 (7)N5—N6—Co1142.10 (14)
O1W—Co1—N688.10 (7)Co1—O1W—H1W120.3 (18)
O1Wi—Co1—N691.90 (7)Co1—O1W—H2W123.5 (16)
N6i—Co1—N6180.0H1W—O1W—H2W111 (2)
O1W—Co1—N1i89.75 (7)
Symmetry codes: (i) −x+1, −y+1, −z.
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O1W—H1W···N5ii0.78 (2)2.07 (2)2.832 (2)168 (2)
O1W—H2W···N3iii0.82 (2)1.93 (2)2.740 (2)171 (2)
Symmetry codes: (ii) x−1, y, z; (iii) −x+3/2, y+1/2, −z+1/2.
Table 1
Selected geometric parameters (Å)
top
Co1—O1W2.0638 (18)Co1—N12.1856 (16)
Co1—N62.1076 (17)
Table 2
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
O1W—H1W···N5i0.78 (2)2.07 (2)2.832 (2)168 (2)
O1W—H2W···N3ii0.82 (2)1.93 (2)2.740 (2)171 (2)
Symmetry codes: (i) x−1, y, z; (ii) −x+3/2, y+1/2, −z+1/2.
Acknowledgements top

The authors acknowledge South China Normal University for supporting this work.

references
References top

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Rizk, A. T., Kilner, C. A. & Halcrow, M. A. (2005). CrystEngComm, 7, 359–362.

Sheldrick, G. M. (1996). SADABS. University of Göttingen, Germany.

Sheldrick, G. M. (1997). SHELXS97 and SHELXL97. University of Göttingen, Germany.