supplementary materials


Acta Cryst. (2009). E65, m425    [ doi:10.1107/S1600536809009660 ]

Bis[[mu]-5-(5-carboxylato-3-pyridyl)tetrazolato-[kappa]3N1,N5:N2]bis[triaquazinc(II)]

H. Yin, L. Wang and Q. Nie

Abstract top

In the title complex, [Zn2(C7H3N5O2)2(H2O)6], the 5-(5-carboxylato-3-pyridyl)tetrazolate ligand chelates the ZnII center through one pyridyl N and one tetrazolate N atom, and uses another N atom to bridge to the second Zn atom, forming a centrosymmetric dinuclear unit. Three coordinated water molecules complete the distorted octahedral geometry of the ZnII atom. O-H...O and O-H...N hydrogen bonds involving the coordinated water molecules, tetrazolate N atoms and the carboxylate group result in a three-dimensional structure.

Comment top

Metal complexes based on tetrazol ligands have attracted great interests (Li et al. 2005; Sun et al. 2009). In the contribution, we report the title binuclear complex (I) based on tetrazol ligand obtained by in situ ligand synthesis.

In the structure of (I), 3-carboxylatopyridyl-6-tetrazolato ligand chelates ZnII center through one pyridyl N and one tetrazolato N and another bridging tetrazolato N atom results in a centrosymmetrical binuclear unit. Three coordinated water molecules complete the distorted octahedral geometry of ZnII center (Fig.1). There exist various hydrogen-bonding interactions between coordinated water molecules and tetrazol N, carboxylate group of the ligand (Table. 2). The hydrogen bonds connect binuclear complex into a three-dimensional structure (Fig.2).

Related literature top

For background, see: Li et al. (2005); Sun et al. (2009).

Experimental top

A mixture of Zn(NO3)2.6H2O (149 mg, 0.5 mmol), sodium azide(33 mg, 0.5 mmol) and 6-cyanopyridine-3-carboxylic acid (74 mg, 0.5 mmol) was suspended in water (10 ml) and heated in a teflon-lined steel bomb at 160 ° C for 3 days. The colorless crystals were obtained.

Refinement top

H atoms bonded to C were located geometrically (C—H = 0.95 Å) with Uiso(H) = 1.2 Ueq(C). H atoms bonded to O were located by difference maps and refined with a distance restraint of O—H = 0.85 (1) Å. The displacement factors were freely refined.

Computing details top

Data collection: CrystalClear (Rigaku, 2000); cell refinement: CrystalClear (Rigaku, 2000); data reduction: CrystalClear (Rigaku, 2000); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: X-SEED (Barbour, 2001); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. ORTEP of complex (I) with 30% thermal ellipsoids. [Symmetry code: (A) -x, 1-y, -z.]
[Figure 2] Fig. 2. The packing structure viewed along a axis.
Bis[µ-5-(5-carboxylato-3-pyridyl)tetrazolato- κ3N1,N5:N2]bis[triaquazinc(II)] top
Crystal data top
[Zn2(C7H3N5O2)2(H2O)6]F(000) = 624
Mr = 617.12Dx = 1.875 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 2535 reflections
a = 12.751 (5) Åθ = 3.2–27.5°
b = 12.685 (4) ŵ = 2.27 mm1
c = 6.992 (3) ÅT = 295 K
β = 104.914 (4)°Prism, colorless
V = 1092.9 (7) Å30.12 × 0.08 × 0.08 mm
Z = 2
Data collection top
Rigaku Mercury CCD
diffractometer
2502 independent reflections
Radiation source: fine-focus sealed tube2146 reflections with I > 2σ(I)
graphiteRint = 0.031
Detector resolution: 14.6306 pixels mm-1θmax = 27.5°, θmin = 2.3°
CCD_Profile_fitting scansh = 1316
Absorption correction: multi-scan
(CrystalClear; Rigaku, 2000)
k = 1613
Tmin = 0.880, Tmax = 1.000l = 98
8378 measured reflections
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)] = 0.032Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.064H atoms treated by a mixture of independent and constrained refinement
S = 1.10 w = 1/[σ2(Fo2) + (0.0236P)2 + 0.4632P]
where P = (Fo2 + 2Fc2)/3
2502 reflections(Δ/σ)max = 0.001
187 parametersΔρmax = 0.44 e Å3
6 restraintsΔρmin = 0.31 e Å3
Crystal data top
[Zn2(C7H3N5O2)2(H2O)6]V = 1092.9 (7) Å3
Mr = 617.12Z = 2
Monoclinic, P21/cMo Kα radiation
a = 12.751 (5) ŵ = 2.27 mm1
b = 12.685 (4) ÅT = 295 K
c = 6.992 (3) Å0.12 × 0.08 × 0.08 mm
β = 104.914 (4)°
Data collection top
Rigaku Mercury CCD
diffractometer
2502 independent reflections
Absorption correction: multi-scan
(CrystalClear; Rigaku, 2000)
2146 reflections with I > 2σ(I)
Tmin = 0.880, Tmax = 1.000Rint = 0.031
8378 measured reflectionsθmax = 27.5°
Refinement top
R[F2 > 2σ(F2)] = 0.032H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.064Δρmax = 0.44 e Å3
S = 1.10Δρmin = 0.31 e Å3
2502 reflectionsAbsolute structure: ?
187 parametersFlack parameter: ?
6 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
Zn10.16114 (2)0.451195 (18)0.04261 (4)0.01891 (9)
N10.29843 (15)0.55236 (13)0.1954 (3)0.0199 (4)
O20.62383 (14)0.48266 (13)0.2838 (3)0.0345 (4)
O10.67185 (13)0.64838 (12)0.3616 (2)0.0273 (4)
N20.08352 (15)0.59050 (14)0.1144 (3)0.0184 (4)
C10.60194 (19)0.57469 (18)0.3163 (3)0.0219 (5)
C40.3458 (2)0.72742 (18)0.3169 (4)0.0258 (5)
H40.32390.79530.34910.031*
C60.26966 (19)0.65036 (16)0.2412 (3)0.0196 (5)
C30.4544 (2)0.70372 (18)0.3447 (4)0.0260 (5)
H30.50790.75570.39580.031*
C20.48558 (18)0.60427 (17)0.2980 (3)0.0193 (5)
C50.40336 (19)0.53119 (17)0.2249 (3)0.0217 (5)
H50.42360.46240.19440.026*
O30.26729 (15)0.34205 (13)0.0178 (3)0.0278 (4)
O40.16780 (16)0.52386 (13)0.2289 (3)0.0277 (4)
C70.15272 (19)0.66661 (16)0.1971 (3)0.0184 (5)
O50.16098 (16)0.37901 (15)0.3062 (3)0.0353 (5)
N50.01525 (15)0.63182 (14)0.0916 (3)0.0195 (4)
N40.00558 (16)0.72963 (15)0.1574 (3)0.0250 (4)
N30.09973 (16)0.75412 (15)0.2242 (3)0.0245 (4)
H4A0.141 (2)0.5845 (12)0.254 (4)0.041 (9)*
H3A0.289 (2)0.2851 (13)0.042 (4)0.040 (8)*
H4B0.2293 (14)0.527 (2)0.254 (5)0.047 (9)*
H3B0.279 (2)0.339 (2)0.132 (2)0.045 (9)*
H5A0.114 (2)0.336 (2)0.320 (5)0.058 (10)*
H5B0.2086 (18)0.383 (2)0.415 (2)0.040 (8)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Zn10.01593 (16)0.01373 (14)0.02694 (15)0.00018 (10)0.00528 (11)0.00126 (10)
N10.0160 (10)0.0159 (9)0.0274 (10)0.0006 (7)0.0051 (8)0.0027 (8)
O20.0210 (10)0.0243 (9)0.0606 (12)0.0007 (7)0.0146 (9)0.0065 (8)
O10.0170 (9)0.0271 (9)0.0372 (10)0.0048 (7)0.0059 (8)0.0073 (7)
N20.0140 (10)0.0172 (9)0.0240 (10)0.0005 (7)0.0051 (8)0.0017 (7)
C10.0166 (13)0.0276 (13)0.0222 (12)0.0001 (9)0.0061 (10)0.0008 (9)
C40.0196 (13)0.0194 (11)0.0382 (14)0.0004 (9)0.0071 (11)0.0072 (10)
C60.0188 (13)0.0170 (11)0.0228 (11)0.0007 (9)0.0051 (10)0.0022 (9)
C30.0206 (13)0.0215 (12)0.0344 (14)0.0052 (10)0.0042 (11)0.0072 (10)
C20.0146 (12)0.0207 (11)0.0222 (12)0.0003 (9)0.0039 (9)0.0007 (9)
C50.0173 (13)0.0192 (11)0.0288 (12)0.0011 (9)0.0063 (10)0.0016 (9)
O30.0332 (11)0.0185 (9)0.0347 (10)0.0079 (7)0.0141 (9)0.0029 (8)
O40.0258 (11)0.0238 (9)0.0367 (10)0.0053 (7)0.0139 (9)0.0075 (8)
C70.0168 (12)0.0167 (10)0.0218 (11)0.0013 (8)0.0050 (9)0.0036 (9)
O50.0301 (12)0.0394 (11)0.0302 (10)0.0183 (9)0.0033 (9)0.0129 (8)
N50.0135 (10)0.0175 (9)0.0273 (10)0.0009 (7)0.0050 (8)0.0028 (8)
N40.0185 (11)0.0199 (10)0.0363 (12)0.0006 (8)0.0067 (9)0.0077 (8)
N30.0170 (11)0.0202 (10)0.0353 (11)0.0011 (8)0.0048 (9)0.0089 (8)
Geometric parameters (Å, °) top
Zn1—O32.0547 (18)C6—C71.457 (3)
Zn1—O52.0587 (19)C3—C21.386 (3)
Zn1—O42.1317 (18)C3—H30.9500
Zn1—N5i2.1333 (19)C2—C51.394 (3)
Zn1—N22.1470 (18)C5—H50.9500
Zn1—N12.2114 (19)O3—H3A0.846 (10)
N1—C51.328 (3)O3—H3B0.849 (10)
N1—C61.358 (3)O4—H4A0.841 (10)
O2—C11.235 (3)O4—H4B0.846 (10)
O1—C11.274 (3)C7—N31.338 (3)
N2—C71.335 (3)O5—H5A0.841 (10)
N2—N51.335 (2)O5—H5B0.844 (10)
C1—C21.504 (3)N5—N41.318 (3)
C4—C31.381 (3)N5—Zn1i2.1333 (19)
C4—C61.384 (3)N4—N31.340 (3)
C4—H40.9500
O3—Zn1—O592.12 (8)N1—C6—C7113.79 (19)
O3—Zn1—O485.92 (7)C4—C6—C7124.1 (2)
O5—Zn1—O4177.71 (8)C4—C3—C2120.2 (2)
O3—Zn1—N5i97.06 (7)C4—C3—H3119.9
O5—Zn1—N5i88.43 (7)C2—C3—H3119.9
O4—Zn1—N5i92.97 (7)C3—C2—C5117.2 (2)
O3—Zn1—N2166.01 (7)C3—C2—C1122.9 (2)
O5—Zn1—N292.86 (8)C5—C2—C1119.8 (2)
O4—Zn1—N288.79 (7)N1—C5—C2123.7 (2)
N5i—Zn1—N296.13 (7)N1—C5—H5118.1
O3—Zn1—N190.51 (7)C2—C5—H5118.1
O5—Zn1—N190.49 (7)Zn1—O3—H3A128.6 (19)
O4—Zn1—N188.35 (7)Zn1—O3—H3B121 (2)
N5i—Zn1—N1172.39 (7)H3A—O3—H3B108 (3)
N2—Zn1—N176.39 (7)Zn1—O4—H4A118.2 (19)
C5—N1—C6118.12 (19)Zn1—O4—H4B117 (2)
C5—N1—Zn1126.76 (14)H4A—O4—H4B105 (3)
C6—N1—Zn1114.64 (15)N2—C7—N3111.1 (2)
C7—N2—N5105.42 (17)N2—C7—C6121.04 (19)
C7—N2—Zn1113.79 (15)N3—C7—C6127.8 (2)
N5—N2—Zn1140.58 (14)Zn1—O5—H5A124 (2)
O2—C1—O1124.2 (2)Zn1—O5—H5B128 (2)
O2—C1—C2119.0 (2)H5A—O5—H5B108 (3)
O1—C1—C2116.8 (2)N4—N5—N2109.10 (17)
C3—C4—C6118.7 (2)N4—N5—Zn1i127.65 (14)
C3—C4—H4120.7N2—N5—Zn1i123.21 (13)
C6—C4—H4120.7N5—N4—N3109.59 (17)
N1—C6—C4122.1 (2)C7—N3—N4104.80 (18)
Symmetry codes: (i) −x, −y+1, −z.
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O4—H4B···O2ii0.85 (1)1.94 (1)2.782 (3)172 (3)
O4—H4A···N3iii0.84 (1)2.11 (1)2.940 (3)169 (3)
O3—H3B···O1ii0.85 (1)1.88 (1)2.712 (3)169 (3)
O3—H3A···O1iv0.85 (1)1.88 (1)2.719 (2)171 (3)
O5—H5B···O1v0.84 (1)1.92 (1)2.740 (3)163 (3)
O5—H5A···N4vi0.84 (1)1.96 (1)2.800 (3)177 (3)
Symmetry codes: (ii) −x+1, −y+1, −z; (iii) x, −y+3/2, z−1/2; (iv) −x+1, y−1/2, −z+1/2; (v) −x+1, −y+1, −z+1; (vi) −x, y−1/2, −z+1/2.
Table 1
Selected geometric parameters (Å, °)
top
Zn1—O32.0547 (18)Zn1—N5i2.1333 (19)
Zn1—O52.0587 (19)Zn1—N22.1470 (18)
Zn1—O42.1317 (18)Zn1—N12.2114 (19)
O3—Zn1—O592.12 (8)O5—Zn1—O4177.71 (8)
O3—Zn1—O485.92 (7)
Symmetry codes: (i) −x, −y+1, −z.
Table 2
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
O4—H4B···O2ii0.85 (1)1.94 (1)2.782 (3)172 (3)
O4—H4A···N3iii0.84 (1)2.11 (1)2.940 (3)169 (3)
O3—H3B···O1ii0.85 (1)1.88 (1)2.712 (3)169 (3)
O3—H3A···O1iv0.85 (1)1.88 (1)2.719 (2)171 (3)
O5—H5B···O1v0.84 (1)1.92 (1)2.740 (3)163 (3)
O5—H5A···N4vi0.84 (1)1.96 (1)2.800 (3)177 (3)
Symmetry codes: (ii) −x+1, −y+1, −z; (iii) x, −y+3/2, z−1/2; (iv) −x+1, y−1/2, −z+1/2; (v) −x+1, −y+1, −z+1; (vi) −x, y−1/2, −z+1/2.
Acknowledgements top

The authors acknowledge financial support from Zhejiang Provincial Natural Science Foundation of China (Y4080093 and Y407189).

references
References top

Barbour, L. J. (2001). J. Supramol. Chem. 1, 189–191.

Li, J.-T., Tao, J., Huang, R.-B. & Zhang, L.-S. (2005). Acta Cryst. E61, m984–m985.

Rigaku (2000). CrystalClear. Rigaku Corporation, Tokyo, Japan.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.

Sun, Z.-H., Meng, L.-B. & Lin, H. (2009). Acta Cryst. E65, m280.