metal-organic compounds
catena-Poly[[[tetraaquairon(II)]-μ-5,5′-diazenediylditetrazolido] dihydrate]
aDepartment of Chemistry and Chemical Engineering, Xi'an University of Arts & Science, Xi'an 710065, Shaanxi, People's Republic of China, bCollege of Chemistry and Chemical Engineering, Xianyang Normal University, Xianyang 712000, Shaanxi, People's Republic of China, and cCollege of Chemistry and Materials Science, Northwest University, Xi'an 710069, Shaanxi, People's Republic of China
*Correspondence e-mail: sanpingchen@126.com
In the title compound, {[Fe(C2N10)(H2O)4]·2H2O}n, the coordination geometry around the Fe(II) atom, which lies on a center of inversion, is distorted octahedral, with bonds to four O atoms and two N atoms. The azotetrazolate ligand displays a bridging coordination mode, forming an infinite zigzag chain. Intermolecular O—H⋯O and O—H⋯N hydrogen bonding and offset face-to-face π–π stacking interactions [centroid–centroid distance = 3.4738 (13) Å] lead to a three-dimensional network.
Experimental
Crystal data
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Refinement
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Data collection: SMART (Bruker, 2002); cell SAINT (Bruker, 2002); data reduction: SAINT; 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: SHELXL97.
Supporting information
https://doi.org/10.1107/S1600536810039632/ng5036sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536810039632/ng5036Isup2.hkl
Brown block-like crystal for X-ray
was obtained from the mixture of (NH4)2Fe(SO4)2.6H2O (0.392 g, 1 mmol), Na2AT.5H2O (0.304 g,1 mmol) and distilled H2O (20 ml), which was allowed to evaporate at room temperature for one week.H atoms attached to O atoms were placed in calculated positions, with O—H distances of 0.86 Å. The Uiso(H) values were constrained to be -1.5Ueq of the carrier atom.
After Thiele prepared metallic salts of azotetrazole and claimed these for use in initiators, salts of AT2- (AT = 5,5'-azotetrazolate) have been extensively investigated and have often been considered for practical use as a class of energetic materials. We report here the
of the title compound, [Fe(C2N10)(H20)4.2H20]n, (I).Single-crystal analysis shows that (I) exists as a one-dimensional infinite chain. As shown in Figure 1, the coordination geometry around Fe2+ cation can be described a disordered octahedral arrangement with
of 6, where O1, O2, O1A and O2A form the equatorial plane, and axial positions are occupied by N1 and N1A. Additionally, each AT2- provides two terminal nitrogen atoms (N1 and N1A) acting as bridging ligand to connect two [Fe(H2O)4]2+ to form an infinite zigzag chain.In the π-π stacking interactions of the terazole rings link the complex to a three dimensional structure, as shown in Figure 2.
the interactions of hydrogen bonding between the water molecules and the N atoms in the terazole rings, the off-set face to faceFor related literature [on what subject?], see: Hammerl et al. (2001, 2002); Jiao et al. (2007).
Data collection: SMART (Bruker, 2002); cell
SAINT (Bruker, 2002); data reduction: SAINT (Bruker, 2002); 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: SHELXL97 (Sheldrick, 2008).Fig. 1. A view of the molecular structure of (I) with the atom-labling scheme. Displacement ellipsoids are drawn at the 30% probability level and H atoms are shown as small spheres of arbitrary radii. | |
Fig. 2. Three dimensional network of the title complex. |
[Fe(C2N10)(H2O)4]·2H2O | Z = 1 |
Mr = 328.07 | F(000) = 168 |
Triclinic, P1 | Dx = 1.791 Mg m−3 |
a = 6.2449 (5) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 6.9764 (6) Å | Cell parameters from 1061 reflections |
c = 7.8256 (6) Å | θ = 2.7–25.1° |
α = 76.424 (1)° | µ = 1.29 mm−1 |
β = 74.135 (1)° | T = 273 K |
γ = 69.844 (1)° | Block, brown |
V = 304.11 (4) Å3 | 0.30 × 0.18 × 0.12 mm |
Bruker SMART APEX CCD diffractometer | 1061 independent reflections |
Radiation source: fine-focus sealed tube | 973 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.012 |
φ and ω scans | θmax = 25.1°, θmin = 2.7° |
Absorption correction: multi-scan (SADABS; Bruker, 2002) | h = −7→6 |
Tmin = 0.699, Tmax = 0.861 | k = −7→8 |
1564 measured reflections | l = −8→9 |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.026 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.070 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.13 | w = 1/[σ2(Fo2) + (0.0447P)2 + 0.0115P] where P = (Fo2 + 2Fc2)/3 |
1061 reflections | (Δ/σ)max = 0.007 |
106 parameters | Δρmax = 0.24 e Å−3 |
6 restraints | Δρmin = −0.35 e Å−3 |
[Fe(C2N10)(H2O)4]·2H2O | γ = 69.844 (1)° |
Mr = 328.07 | V = 304.11 (4) Å3 |
Triclinic, P1 | Z = 1 |
a = 6.2449 (5) Å | Mo Kα radiation |
b = 6.9764 (6) Å | µ = 1.29 mm−1 |
c = 7.8256 (6) Å | T = 273 K |
α = 76.424 (1)° | 0.30 × 0.18 × 0.12 mm |
β = 74.135 (1)° |
Bruker SMART APEX CCD diffractometer | 1061 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2002) | 973 reflections with I > 2σ(I) |
Tmin = 0.699, Tmax = 0.861 | Rint = 0.012 |
1564 measured reflections |
R[F2 > 2σ(F2)] = 0.026 | 6 restraints |
wR(F2) = 0.070 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.13 | Δρmax = 0.24 e Å−3 |
1061 reflections | Δρmin = −0.35 e Å−3 |
106 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 | ||
Fe1 | 0.5000 | 0.5000 | 1.0000 | 0.02375 (17) | |
N1 | 0.5314 (3) | 0.6482 (3) | 0.7101 (2) | 0.0240 (4) | |
N2 | 0.3404 (3) | 0.7685 (3) | 0.6503 (2) | 0.0287 (4) | |
N3 | 0.3949 (3) | 0.8147 (3) | 0.4742 (2) | 0.0323 (4) | |
N4 | 0.6210 (3) | 0.7259 (3) | 0.4135 (2) | 0.0287 (4) | |
N5 | 0.9299 (3) | 0.5062 (3) | 0.5738 (2) | 0.0253 (4) | |
O1 | 0.8288 (3) | 0.2802 (3) | 0.9369 (2) | 0.0340 (4) | |
O2 | 0.6617 (3) | 0.6912 (3) | 1.0508 (2) | 0.0403 (4) | |
O3 | 0.8598 (3) | 0.9497 (3) | 0.7946 (2) | 0.0342 (4) | |
C1 | 0.7009 (3) | 0.6250 (3) | 0.5618 (3) | 0.0228 (4) | |
H1A | 0.829 (4) | 0.172 (3) | 0.903 (3) | 0.034* | |
H2A | 0.710 (4) | 0.784 (3) | 0.975 (3) | 0.034* | |
H3A | 1.002 (2) | 0.886 (3) | 0.754 (3) | 0.034* | |
H1B | 0.922 (4) | 0.329 (4) | 0.851 (2) | 0.034* | |
H2B | 0.658 (4) | 0.707 (4) | 1.1563 (18) | 0.034* | |
H3B | 0.797 (4) | 1.008 (3) | 0.705 (2) | 0.034* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Fe1 | 0.0192 (2) | 0.0327 (3) | 0.0151 (2) | −0.00481 (17) | −0.00252 (16) | −0.00163 (17) |
N1 | 0.0186 (9) | 0.0307 (9) | 0.0172 (9) | −0.0021 (7) | −0.0026 (7) | −0.0026 (7) |
N2 | 0.0214 (9) | 0.0379 (10) | 0.0198 (9) | −0.0024 (8) | −0.0035 (7) | −0.0022 (8) |
N3 | 0.0273 (10) | 0.0406 (10) | 0.0218 (10) | −0.0020 (8) | −0.0073 (8) | −0.0014 (8) |
N4 | 0.0242 (9) | 0.0389 (10) | 0.0168 (9) | −0.0043 (8) | −0.0021 (7) | −0.0034 (8) |
N5 | 0.0211 (9) | 0.0336 (9) | 0.0162 (8) | −0.0053 (7) | −0.0002 (6) | −0.0033 (7) |
O1 | 0.0260 (8) | 0.0398 (9) | 0.0283 (9) | −0.0044 (7) | −0.0020 (7) | −0.0033 (7) |
O2 | 0.0526 (11) | 0.0589 (11) | 0.0188 (9) | −0.0333 (9) | −0.0034 (8) | −0.0035 (8) |
O3 | 0.0234 (8) | 0.0433 (9) | 0.0255 (9) | −0.0014 (7) | −0.0055 (7) | 0.0017 (7) |
C1 | 0.0210 (10) | 0.0285 (10) | 0.0154 (10) | −0.0059 (8) | −0.0023 (8) | −0.0010 (8) |
Fe1—O2 | 2.0868 (15) | N4—C1 | 1.335 (3) |
Fe1—O2i | 2.0868 (15) | N5—N5ii | 1.245 (3) |
Fe1—O1i | 2.1081 (16) | N5—C1 | 1.400 (3) |
Fe1—O1 | 2.1081 (16) | O1—H1A | 0.854 (10) |
Fe1—N1 | 2.2474 (16) | O1—H1B | 0.851 (10) |
Fe1—N1i | 2.2474 (16) | O2—H2A | 0.848 (10) |
N1—N2 | 1.333 (2) | O2—H2B | 0.850 (10) |
N1—C1 | 1.338 (3) | O3—H3A | 0.852 (10) |
N2—N3 | 1.315 (3) | O3—H3B | 0.844 (10) |
N3—N4 | 1.331 (3) | ||
O2—Fe1—O2i | 180.0 | N2—N1—Fe1 | 119.64 (12) |
O2—Fe1—O1i | 90.39 (7) | C1—N1—Fe1 | 134.93 (13) |
O2i—Fe1—O1i | 89.61 (7) | N3—N2—N1 | 109.13 (16) |
O2—Fe1—O1 | 89.61 (7) | N2—N3—N4 | 110.32 (16) |
O2i—Fe1—O1 | 90.39 (7) | N3—N4—C1 | 104.10 (16) |
O1i—Fe1—O1 | 180.0 | N5ii—N5—C1 | 114.3 (2) |
O2—Fe1—N1 | 91.16 (6) | Fe1—O1—H1A | 116.1 (17) |
O2i—Fe1—N1 | 88.84 (6) | Fe1—O1—H1B | 112.4 (17) |
O1i—Fe1—N1 | 89.55 (6) | H1A—O1—H1B | 104 (2) |
O1—Fe1—N1 | 90.45 (6) | Fe1—O2—H2A | 126.3 (16) |
O2—Fe1—N1i | 88.84 (6) | Fe1—O2—H2B | 123.0 (16) |
O2i—Fe1—N1i | 91.16 (6) | H2A—O2—H2B | 109 (2) |
O1i—Fe1—N1i | 90.45 (6) | H3A—O3—H3B | 107 (2) |
O1—Fe1—N1i | 89.55 (6) | N4—C1—N1 | 111.80 (17) |
N1—Fe1—N1i | 180.0 | N4—C1—N5 | 127.64 (18) |
N2—N1—C1 | 104.65 (15) | N1—C1—N5 | 120.57 (17) |
Symmetry codes: (i) −x+1, −y+1, −z+2; (ii) −x+2, −y+1, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
O2—H2A···O3 | 0.85 (1) | 1.86 (1) | 2.699 (2) | 170 (2) |
O1—H1A···O3iii | 0.85 (1) | 1.87 (1) | 2.715 (2) | 171 (3) |
O1—H1B···N5 | 0.85 (1) | 2.23 (2) | 2.926 (2) | 139 (2) |
O3—H3B···N3iv | 0.84 (1) | 2.01 (1) | 2.839 (2) | 169 (2) |
O3—H3A···N2v | 0.85 (1) | 2.00 (1) | 2.843 (2) | 173 (2) |
O2—H2B···N3vi | 0.85 (1) | 2.69 (2) | 3.439 (2) | 148 (2) |
O2—H2B···N4vi | 0.85 (1) | 1.99 (1) | 2.840 (2) | 173 (2) |
Symmetry codes: (iii) x, y−1, z; (iv) −x+1, −y+2, −z+1; (v) x+1, y, z; (vi) x, y, z+1. |
Experimental details
Crystal data | |
Chemical formula | [Fe(C2N10)(H2O)4]·2H2O |
Mr | 328.07 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 273 |
a, b, c (Å) | 6.2449 (5), 6.9764 (6), 7.8256 (6) |
α, β, γ (°) | 76.424 (1), 74.135 (1), 69.844 (1) |
V (Å3) | 304.11 (4) |
Z | 1 |
Radiation type | Mo Kα |
µ (mm−1) | 1.29 |
Crystal size (mm) | 0.30 × 0.18 × 0.12 |
Data collection | |
Diffractometer | Bruker SMART APEX CCD |
Absorption correction | Multi-scan (SADABS; Bruker, 2002) |
Tmin, Tmax | 0.699, 0.861 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 1564, 1061, 973 |
Rint | 0.012 |
(sin θ/λ)max (Å−1) | 0.597 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.026, 0.070, 1.13 |
No. of reflections | 1061 |
No. of parameters | 106 |
No. of restraints | 6 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.24, −0.35 |
Computer programs: SMART (Bruker, 2002), SAINT (Bruker, 2002), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
O2—H2A···O3 | 0.848 (10) | 1.860 (11) | 2.699 (2) | 170 (2) |
O1—H1A···O3i | 0.854 (10) | 1.868 (11) | 2.715 (2) | 171 (3) |
O1—H1B···N5 | 0.851 (10) | 2.226 (18) | 2.926 (2) | 139 (2) |
O3—H3B···N3ii | 0.844 (10) | 2.007 (11) | 2.839 (2) | 169 (2) |
O3—H3A···N2iii | 0.852 (10) | 1.996 (10) | 2.843 (2) | 173 (2) |
O2—H2B···N3iv | 0.850 (10) | 2.691 (16) | 3.439 (2) | 148 (2) |
O2—H2B···N4iv | 0.850 (10) | 1.994 (11) | 2.840 (2) | 173 (2) |
Symmetry codes: (i) x, y−1, z; (ii) −x+1, −y+2, −z+1; (iii) x+1, y, z; (iv) x, y, z+1. |
Acknowledgements
We gratefully acknowledge the National Science Foundation of China (No. 20873100), the Natural Science Foundation of Shaanxi Province (2009JQ2015), the Special Foundation of the Education Department of Shaanxi Province (09 J K798) and the Research Foundation of Xi'an University of Arts and Science (kyc201026).
References
Bruker (2002). SADABS, SAINT and SMART. Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Hammerl, A., Gerhard, H., Klapötke, T. M., Mayer, P., Nöth, H., Piotrowski, H. & Warchhold, M. (2002). Eur. J. Inorg. Chem. pp. 834–845. CSD CrossRef Google Scholar
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After Thiele prepared metallic salts of azotetrazole and claimed these for use in initiators, salts of AT2- (AT = 5,5'-azotetrazolate) have been extensively investigated and have often been considered for practical use as a class of energetic materials. We report here the crystal structure of the title compound, [Fe(C2N10)(H20)4.2H20]n, (I).
Single-crystal analysis shows that (I) exists as a one-dimensional infinite chain. As shown in Figure 1, the coordination geometry around Fe2+ cation can be described a disordered octahedral arrangement with coordination number of 6, where O1, O2, O1A and O2A form the equatorial plane, and axial positions are occupied by N1 and N1A. Additionally, each AT2- provides two terminal nitrogen atoms (N1 and N1A) acting as bridging ligand to connect two [Fe(H2O)4]2+ to form an infinite zigzag chain.
In the crystal structure, the interactions of hydrogen bonding between the water molecules and the N atoms in the terazole rings, the off-set face to face π-π stacking interactions of the terazole rings link the complex to a three dimensional structure, as shown in Figure 2.