supplementary materials


Acta Cryst. (2007). E63, m2176    [ doi:10.1107/S1600536807034472 ]

Hexakis(1H-imidazole-[kappa]N3)nickel(II) sulfate dihydrate

X.-C. Sun, G.-P. Zhou, Z.-B. Liu and Y. Xu

Abstract top

The title compound, [Ni(C3H4N2)6]SO4·2H2O, was prepared by hydrothermal synthesis. The NiII atom lies on a site of \overline{3} point symmetry and is coordinated by six imidazole ligands in a regular octahedral geometry. The sulfate anion is disordered about a site of 32 point symmetry; water molecules lie on sites of 32 point symmetry and on general positions. The coordinated imidazole molecules make N-H...O hydrogen bonds with the sulfate anions.

Comment top

The title compound was obtained during an attempted synthesis of a metal-organic framework (MOF) incorporating NiII and imidazole. The unit cell has been reported previously (Phung et al., 1976), although complete space group information and atomic coordinates were not given.

The structure comprises discrete [Ni(C3N2H4)6]2+ cations (Figure 1). The NiII atom lies on a site of 3 point symmetry and is coordinated by six N atoms from six imidazole molecules in a regular octahedral geometry with Ni—N = 2.1216 (17) Å. The Ni—N bond lengths and angles are comparable to those in similar reported NiII compounds (for example, Fu et al., 2007). The sulfate anion is disordered about a site of 32 point symmetry. As shown in Figure 2, the non-coordinated N atoms of imidazole are involved in hydrogen-bonding interactions with O atoms of the sulfate groups.

Related literature top

The unit-cell dimensions of this compound have been reported previously (Phung et al., 1976), although complete space-group information and atomic coordinates were not given. For examples of other structures containing [Ni(C3N2H4)6]2+ cations, see: Fu et al. (2007); Gao et al. (2004); Wang et al. (2000).

Experimental top

Light purple block crystals were synthesized hydrothermally from a complex reaction mixture. In a typical synthesis, GeO2 (0.1054 g), NH4VO3 (0.1079) and NiSO4 (0.5278 g) were dissolved in the mixed solvent of dimethyl formamide (0.5162 g) and water (1.8388 g) followed by addition of imidazole (0.4551 g) with constant stirring. The mixture was kept in a 25 ml Teflon-lined steel autoclave at 443 K for 7 days then slowly cooled to room temperature. The product was filtered, washed with distilled water, and dried at room temperature.

Refinement top

H atoms bound to C or N atoms were placed geometrically and allowed to ride with C—H = 0.93 Å or N—H = 0.86 Å, and with Uiso(H) = 1.2Ueq(C/N). H atoms of the water molecules were located in difference Fourier maps and refined with O—H distances restrained to be 0.85 (1)Å and with Uiso(H) = 1.2Ueq(O). The displacement parameters of the O atoms of the water molecules were restrained to approximate isotropic behaviour and the S—O distances in the disordered sulfate anion were restrained to be 1.420 (2) Å.

Computing details top

Data collection: APEX2 (Bruker, 2005); cell refinement: SAINT (Bruker, 2005); 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, 1997); software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. The molecular structure of title compound showing displacement ellipsoids at the 70% probability level for non-H atoms.
[Figure 2] Fig. 2. Unit-cell contents for title compound. Dashed lines denote hydrogen bonds.
Hexakis(1H-imidazole-κN3)nickel(II) sulfate dihydrate top
Crystal data top
[Ni(C3H4N2)6]SO4·2H2ODx = 1.236 Mg m3
Mr = 599.29Mo Kα radiation, λ = 0.71073 Å
Trigonal, P31cCell parameters from 7600 reflections
Hall symbol: -P 3 2cθ = 2.6–25.0°
a = 9.0029 (9) ŵ = 0.72 mm1
c = 22.937 (4) ÅT = 293 K
V = 1610.0 (4) Å3Block, blue
Z = 20.13 × 0.12 × 0.12 mm
F(000) = 624
Data collection top
Bruker APEXII CCD
diffractometer
949 independent reflections
Radiation source: fine-focus sealed tube794 reflections with I > 2σ(I)
graphiteRint = 0.023
ω scansθmax = 25.0°, θmin = 2.6°
Absorption correction: multi-scan
(SADABS; Sheldrick, 2003)
h = 109
Tmin = 0.913, Tmax = 0.919k = 109
7600 measured reflectionsl = 1527
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)] = 0.056Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.183H atoms treated by a mixture of independent and constrained refinement
S = 1.16 w = 1/[σ2(Fo2) + (0.13P)2 + 0.1485P]
where P = (Fo2 + 2Fc2)/3
949 reflections(Δ/σ)max = 0.032
82 parametersΔρmax = 0.49 e Å3
17 restraintsΔρmin = 0.48 e Å3
Crystal data top
[Ni(C3H4N2)6]SO4·2H2OZ = 2
Mr = 599.29Mo Kα radiation
Trigonal, P31cµ = 0.72 mm1
a = 9.0029 (9) ÅT = 293 K
c = 22.937 (4) Å0.13 × 0.12 × 0.12 mm
V = 1610.0 (4) Å3
Data collection top
Bruker APEXII CCD
diffractometer
949 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 2003)
794 reflections with I > 2σ(I)
Tmin = 0.913, Tmax = 0.919Rint = 0.023
7600 measured reflectionsθmax = 25.0°
Refinement top
R[F2 > 2σ(F2)] = 0.056H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.183Δρmax = 0.49 e Å3
S = 1.16Δρmin = 0.48 e Å3
949 reflectionsAbsolute structure: ?
82 parametersFlack parameter: ?
17 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*/UeqOcc. (<1)
Ni10.00000.00000.00000.04666 (14)
S10.33330.33330.25000.0660 (3)
N10.3116 (2)0.0743 (2)0.12231 (8)0.0878 (5)
H3A0.32350.12430.15240.105*
N20.18871 (19)0.00718 (14)0.05341 (7)0.0557 (4)
C10.4392 (3)0.0428 (3)0.08892 (12)0.0901 (8)
H1A0.55620.08720.09450.108*
C20.3650 (2)0.0825 (3)0.04641 (10)0.0746 (6)
H4A0.42290.15920.01630.090*
C30.1628 (2)0.0995 (2)0.10058 (8)0.0693 (5)
H6A0.05570.17250.11670.083*
O10.33330.33330.18837 (15)0.108 (2)0.50
O20.3702 (8)0.4468 (6)0.2181 (3)0.211 (2)0.50
O1W0.00001.00000.25000.313 (5)0.50
H1W0.0255 (4)1.0713 (3)0.2645 (3)0.375*0.17
O2W0.3549 (10)0.7269 (11)0.2078 (5)0.137 (3)0.25
H2WB0.460 (2)0.647 (6)0.211 (6)0.165*0.25
H2WA0.271 (3)0.799 (6)0.2284 (17)0.165*0.25
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ni10.05113 (18)0.05113 (18)0.0377 (3)0.02556 (9)0.0000.000
S10.0785 (4)0.0785 (4)0.0412 (5)0.0392 (2)0.0000.000
N10.1061 (8)0.1020 (9)0.0739 (10)0.0660 (7)0.0246 (9)0.0081 (8)
N20.0600 (7)0.0609 (6)0.0504 (8)0.0334 (5)0.0035 (7)0.0022 (5)
C10.0703 (9)0.1121 (11)0.0945 (17)0.0506 (9)0.0056 (11)0.0219 (12)
C20.0606 (7)0.0906 (11)0.0753 (12)0.0398 (7)0.0016 (9)0.0088 (10)
C30.0742 (8)0.0729 (9)0.0624 (11)0.0380 (6)0.0110 (8)0.0046 (8)
O10.135 (3)0.135 (3)0.054 (3)0.0674 (15)0.0000.000
O20.317 (4)0.165 (3)0.196 (5)0.155 (2)0.079 (4)0.024 (3)
O1W0.315 (6)0.315 (6)0.307 (8)0.158 (3)0.0000.000
O2W0.155 (4)0.141 (4)0.143 (5)0.095 (3)0.018 (4)0.003 (4)
Geometric parameters (Å, °) top
Ni1—N2i2.1216 (17)N1—C11.344 (3)
Ni1—N2ii2.1216 (17)N1—H3A0.860
Ni1—N2iii2.1216 (17)N2—C31.312 (2)
Ni1—N22.1216 (17)N2—C21.384 (2)
Ni1—N2iv2.1216 (17)C1—C21.328 (3)
Ni1—N2v2.1216 (17)C1—H1A0.930
S1—O1vi1.414 (3)C2—H4A0.930
S1—O11.414 (3)C3—H6A0.930
S1—O2vii1.423 (6)O1—O2ix1.400 (7)
S1—O2viii1.423 (6)O1—O2viii1.400 (7)
S1—O2ix1.423 (6)O1—O21.400 (7)
S1—O2x1.423 (6)O2—O2vi1.616 (13)
S1—O21.423 (6)O1W—H1W0.850 (3)
S1—O2vi1.423 (6)O2W—H2WB0.855 (18)
N1—C31.338 (3)O2W—H2WA0.853 (19)
N2i—Ni1—N2ii180.00 (11)O2ix—S1—O296.0 (4)
N2i—Ni1—N2iii89.99 (7)O2x—S1—O2103.2 (4)
N2ii—Ni1—N2iii90.01 (7)O1vi—S1—O2vi59.1 (3)
N2i—Ni1—N289.99 (7)O1—S1—O2vi120.9 (3)
N2ii—Ni1—N290.01 (7)O2vii—S1—O2vi96.0 (4)
N2iii—Ni1—N289.99 (7)O2viii—S1—O2vi103.2 (4)
N2i—Ni1—N2iv90.01 (7)O2ix—S1—O2vi156.7 (5)
N2ii—Ni1—N2iv89.99 (7)O2x—S1—O2vi96.0 (4)
N2iii—Ni1—N2iv90.01 (7)O2—S1—O2vi69.2 (6)
N2—Ni1—N2iv180.00 (9)C3—N1—C1108.16 (18)
N2i—Ni1—N2v90.01 (7)C3—N1—H3A125.9
N2ii—Ni1—N2v89.99 (7)C1—N1—H3A125.9
N2iii—Ni1—N2v180.00 (10)C3—N2—C2104.71 (17)
N2—Ni1—N2v90.01 (7)C3—N2—Ni1127.15 (12)
N2iv—Ni1—N2v89.99 (7)C2—N2—Ni1128.14 (14)
O1vi—S1—O1180.0C2—C1—N1106.35 (19)
O1vi—S1—O2vii59.1 (3)C2—C1—H1A126.8
O1—S1—O2vii120.9 (3)N1—C1—H1A126.8
O1vi—S1—O2viii120.9 (3)C1—C2—N2110.03 (19)
O1—S1—O2viii59.1 (3)C1—C2—H4A125.0
O2vii—S1—O2viii69.2 (6)N2—C2—H4A125.0
O1vi—S1—O2ix120.9 (3)N2—C3—N1110.71 (16)
O1—S1—O2ix59.1 (3)N2—C3—H6A124.6
O2vii—S1—O2ix103.2 (4)N1—C3—H6A124.6
O2viii—S1—O2ix96.0 (4)O2ix—O1—O2viii98.2 (3)
O1vi—S1—O2x59.1 (3)O2ix—O1—O298.2 (3)
O1—S1—O2x120.9 (3)O2viii—O1—O298.2 (3)
O2vii—S1—O2x96.0 (4)O2ix—O1—S160.8 (3)
O2viii—S1—O2x156.7 (5)O2viii—O1—S160.8 (3)
O2ix—S1—O2x69.2 (6)O2—O1—S160.8 (3)
O1vi—S1—O2120.9 (3)O1—O2—S160.1 (3)
O1—S1—O259.1 (3)O1—O2—O2vi109.6 (3)
O2vii—S1—O2156.7 (5)S1—O2—O2vi55.4 (3)
O2viii—S1—O296.0 (4)H2WB—O2W—H2WA141 (10)
Symmetry codes: (i) −x+y, −x, z; (ii) xy, x, −z; (iii) −y, xy, z; (iv) −x, −y, −z; (v) y, −x+y, −z; (vi) −y, −x, −z−1/2; (vii) x, xy−1, −z−1/2; (viii) −y, xy−1, z; (ix) −x+y+1, −x, z; (x) −x+y+1, y, −z−1/2.
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N1—H3A···O10.862.102.868 (3)149
N1—H3A···O2viii0.862.092.908 (7)159
N1—H3A···O2ix0.862.443.191 (7)146
Symmetry codes: (viii) −y, xy−1, z; (ix) −x+y+1, −x, z.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
N1—H3A···O10.862.102.868 (3)149
N1—H3A···O2i0.862.092.908 (7)159
N1—H3A···O2ii0.862.443.191 (7)146
Symmetry codes: (i) −y, xy−1, z; (ii) −x+y+1, −x, z.
Acknowledgements top

This work was supported by the Education Office Foundation of Liaoning province (05 L220).

references
References top

Bruker (1997). SHELXTL. Version 5.10. Bruker AXS Inc., Madison, Wisconsin, USA.

Bruker (2005). APEX2 (Version 1.27) and SAINT (Version 7.06). Bruker AXS Inc., Madison, Wisconsin, USA.

Fu, H.-Y., Dou, J.-M., Li, D.-C. & Wang, D.-Q. (2007). Acta Cryst. E63, m1793–m1795.

Gao, S., Liu, J.-W., Dong, Y., Huo, L.-H. & Zhao, H. (2004). Acta Cryst. E60, m778–m780.

Phung, N. D., Tedenac, J.-C. & Maurin, M. (1976). J. Inorg. Nucl. Chem. 38, 2316–2317.

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

Sheldrick, G. M. (2003). SADABS. University of Göttingen, Germany.

Wang, Z.-X., Zhang, Y., Razak, I. A., Shanmuga Sundara Raj, S., Fun, H.-K., Li, F. & Song, H. (2000). Acta Cryst. C56, 161–162.