metal-organic compounds
Bis(1-amino-4-methylpyridinium) bis(1,2-dicyanoethene-1,2-dithiolato-κ2S,S′)nickelate(II)
aDepartment of Applied Chemistry, College of Science, Nanjing University of Technology, Nanjing 210009, People's Republic of China
*Correspondence e-mail: powdtech@njut.edu.cn
The 6H9N2)2[Ni(C4N2S2)2], contains one half of an [Ni(mnt)2]2− anion (mnt is maleonitriledithiolate or 1,2-dicyanoethene-1,2-dithiolate) and one 1-amino-4-methylpyridinium cation. The NiII atom is located on an inversion centre. In the intermolecular N—H⋯N hydrogen bonds link the molecules.
of the title compound, (CRelated literature
For general background, see: Cassoux et al. (1991). For bond-length data, see: Allen et al. (1987).
Experimental
Crystal data
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Refinement
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Data collection: SMART (Bruker, 2000); cell SAINT (Bruker, 2000); data reduction: SAINT=; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).
Supporting information
10.1107/S1600536808018886/hk2475sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536808018886/hk2475Isup2.hkl
For the preparation of the title compound, disodium maleonitriledithiolate (456 mg, 2.5 mmol) and nickel chloride hexahydrate (297 mg, 1.25 mmol) were mixed with water (20 ml) by stirring at room temperature. Subsequently, a solution of 1-amino-4-methylpyridinium iodide (590 mg, 2.5 mmol) in water (10 ml) was added to the mixture, and the red precipitate immediately formed was filtered off, and washed with water. The crude product was recrystallized in acetone (20 ml) to give red crystals. Crystals suitable for X-ray analysis were obtained by diffusing diethyl ether into the solution of (I) in acetone for 6 d. Anal. Calcd.: C, 43.10; H, 3.26; N, 20.10%. Found: C, 43.15; H, 3.29; N, 20.16%. FTIR data (KBr pellets, cm-1): 3025, 2928, 2920, 2199, 1577, 1490, 1399, 1125.
H atoms were positioned geometrically, with N-H = 0.86 Å (for NH2) and C-H= 0.93 and 0.96 Å for aromatic and methyl H, and constrained to ride on their parent atoms, with Uiso(H) = xUeq(C,N), where x = 1.5 for methyl H, and x = 1.2 for all other H atoms.
Data collection: SMART (Bruker, 2000); cell
SMART (Bruker, 2000); data reduction: SAINT (Bruker, 2000); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).(C6H9N2)2[Ni(C4N2S2)2] | Z = 1 |
Mr = 557.39 | F(000) = 286 |
Triclinic, P1 | Dx = 1.513 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 7.678 (5) Å | Cell parameters from 2479 reflections |
b = 9.095 (6) Å | θ = 2.3–22.2° |
c = 9.665 (6) Å | µ = 1.16 mm−1 |
α = 93.116 (7)° | T = 296 K |
β = 104.519 (8)° | Block, red |
γ = 108.813 (7)° | 0.30 × 0.20 × 0.10 mm |
V = 611.7 (7) Å3 |
Bruker SMART CCD area-detector diffractometer | 2097 independent reflections |
Radiation source: sealed tube | 1937 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.137 |
ϕ and ω scans | θmax = 25.0°, θmin = 2.2° |
Absorption correction: multi-scan (SADABS; Bruker, 2000) | h = −8→9 |
Tmin = 0.732, Tmax = 0.892 | k = −10→10 |
3040 measured reflections | l = −11→8 |
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)] = 0.065 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.173 | H-atom parameters constrained |
S = 1.04 | w = 1/[σ2(Fo2) + (0.1404P)2] where P = (Fo2 + 2Fc2)/3 |
2097 reflections | (Δ/σ)max < 0.001 |
152 parameters | Δρmax = 0.82 e Å−3 |
0 restraints | Δρmin = −1.48 e Å−3 |
(C6H9N2)2[Ni(C4N2S2)2] | γ = 108.813 (7)° |
Mr = 557.39 | V = 611.7 (7) Å3 |
Triclinic, P1 | Z = 1 |
a = 7.678 (5) Å | Mo Kα radiation |
b = 9.095 (6) Å | µ = 1.16 mm−1 |
c = 9.665 (6) Å | T = 296 K |
α = 93.116 (7)° | 0.30 × 0.20 × 0.10 mm |
β = 104.519 (8)° |
Bruker SMART CCD area-detector diffractometer | 2097 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2000) | 1937 reflections with I > 2σ(I) |
Tmin = 0.732, Tmax = 0.892 | Rint = 0.137 |
3040 measured reflections |
R[F2 > 2σ(F2)] = 0.065 | 0 restraints |
wR(F2) = 0.173 | H-atom parameters constrained |
S = 1.04 | Δρmax = 0.82 e Å−3 |
2097 reflections | Δρmin = −1.48 e Å−3 |
152 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 > 2sigma(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 | ||
Ni1 | 0.5000 | 1.0000 | 0.0000 | 0.0326 (2) | |
S1 | 0.53316 (12) | 0.82630 (9) | −0.14377 (8) | 0.0430 (3) | |
S2 | 0.62570 (12) | 0.89841 (9) | 0.18019 (8) | 0.0441 (3) | |
N1 | 0.3775 (6) | 0.6494 (4) | −0.5237 (4) | 0.0726 (10) | |
N2 | 0.8189 (5) | 0.9732 (4) | 0.5790 (3) | 0.0570 (7) | |
N3 | 0.8790 (4) | 0.6656 (3) | 0.8401 (3) | 0.0463 (6) | |
N4 | 0.8879 (5) | 0.6838 (4) | 0.6984 (4) | 0.0633 (8) | |
H4A | 0.8169 | 0.6097 | 0.6282 | 0.076* | |
H4B | 0.9644 | 0.7692 | 0.6817 | 0.076* | |
C1 | 0.4152 (4) | 0.8525 (4) | −0.3142 (3) | 0.0390 (6) | |
C2 | 0.3924 (5) | 0.7418 (4) | −0.4332 (3) | 0.0476 (7) | |
C3 | 0.6515 (4) | 1.0259 (3) | 0.3304 (3) | 0.0373 (6) | |
C4 | 0.7452 (4) | 0.9981 (4) | 0.4683 (3) | 0.0433 (7) | |
C5 | 0.8723 (7) | 0.6146 (5) | 1.2737 (4) | 0.0694 (11) | |
H5A | 0.9882 | 0.6007 | 1.3268 | 0.104* | |
H5B | 0.7639 | 0.5245 | 1.2731 | 0.104* | |
H5C | 0.8615 | 0.7068 | 1.3187 | 0.104* | |
C6 | 0.8775 (5) | 0.6333 (4) | 1.1208 (4) | 0.0488 (7) | |
C7 | 0.7604 (5) | 0.5155 (4) | 1.0066 (4) | 0.0508 (7) | |
H7 | 0.6800 | 0.4223 | 1.0251 | 0.061* | |
C8 | 0.7615 (5) | 0.5345 (4) | 0.8667 (4) | 0.0511 (8) | |
H8 | 0.6802 | 0.4556 | 0.7909 | 0.061* | |
C9 | 0.9972 (5) | 0.7824 (4) | 0.9466 (4) | 0.0516 (8) | |
H9 | 1.0795 | 0.8726 | 0.9252 | 0.062* | |
C10 | 0.9965 (5) | 0.7687 (4) | 1.0869 (4) | 0.0564 (9) | |
H10 | 1.0764 | 0.8509 | 1.1601 | 0.068* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Ni1 | 0.0304 (3) | 0.0274 (3) | 0.0316 (3) | 0.0051 (2) | 0.0022 (2) | −0.0029 (2) |
S1 | 0.0501 (5) | 0.0389 (4) | 0.0369 (4) | 0.0191 (3) | 0.0041 (3) | −0.0026 (3) |
S2 | 0.0558 (5) | 0.0376 (4) | 0.0348 (4) | 0.0194 (4) | 0.0031 (3) | −0.0010 (3) |
N1 | 0.091 (3) | 0.058 (2) | 0.0556 (18) | 0.0214 (18) | 0.0098 (17) | −0.0172 (15) |
N2 | 0.0604 (18) | 0.0588 (18) | 0.0416 (15) | 0.0165 (14) | 0.0021 (12) | 0.0067 (12) |
N3 | 0.0428 (14) | 0.0357 (13) | 0.0576 (15) | 0.0130 (11) | 0.0119 (11) | −0.0003 (11) |
N4 | 0.078 (2) | 0.0500 (17) | 0.0605 (18) | 0.0180 (16) | 0.0238 (16) | 0.0052 (13) |
C1 | 0.0360 (14) | 0.0370 (15) | 0.0354 (14) | 0.0068 (11) | 0.0052 (11) | −0.0055 (11) |
C2 | 0.0506 (18) | 0.0385 (16) | 0.0421 (16) | 0.0100 (13) | 0.0029 (13) | −0.0063 (12) |
C3 | 0.0334 (14) | 0.0344 (14) | 0.0342 (13) | 0.0058 (11) | 0.0020 (10) | −0.0028 (10) |
C4 | 0.0400 (16) | 0.0402 (15) | 0.0404 (15) | 0.0073 (12) | 0.0051 (12) | 0.0007 (12) |
C5 | 0.075 (3) | 0.064 (3) | 0.063 (2) | 0.027 (2) | 0.0076 (19) | 0.0050 (18) |
C6 | 0.0418 (17) | 0.0439 (16) | 0.0552 (18) | 0.0176 (13) | 0.0028 (13) | −0.0011 (13) |
C7 | 0.0487 (18) | 0.0321 (15) | 0.0605 (19) | 0.0042 (13) | 0.0111 (14) | −0.0011 (13) |
C8 | 0.0461 (18) | 0.0336 (15) | 0.0620 (19) | 0.0060 (13) | 0.0085 (14) | −0.0080 (13) |
C9 | 0.0404 (17) | 0.0317 (15) | 0.071 (2) | 0.0030 (12) | 0.0104 (15) | −0.0006 (14) |
C10 | 0.0464 (18) | 0.0393 (17) | 0.063 (2) | 0.0053 (14) | −0.0033 (15) | −0.0110 (14) |
Ni1—S1 | 2.1655 (12) | C5—H5C | 0.9600 |
Ni1—S1i | 2.1655 (12) | C6—C10 | 1.388 (5) |
Ni1—S2 | 2.1738 (11) | C6—C7 | 1.388 (5) |
Ni1—S2i | 2.1738 (11) | C7—C8 | 1.375 (5) |
S1—C1 | 1.739 (3) | C7—H7 | 0.9300 |
S2—C3 | 1.737 (3) | C8—N3 | 1.326 (4) |
C1—C3i | 1.361 (4) | C8—H8 | 0.9300 |
C1—C2 | 1.423 (4) | C9—N3 | 1.343 (4) |
C2—N1 | 1.137 (5) | C9—C10 | 1.369 (5) |
C3—C1i | 1.361 (4) | C9—H9 | 0.9300 |
C3—C4 | 1.426 (4) | C10—H10 | 0.9300 |
C4—N2 | 1.149 (4) | N3—N4 | 1.404 (4) |
C5—C6 | 1.506 (5) | N4—H4A | 0.8600 |
C5—H5A | 0.9600 | N4—H4B | 0.8600 |
C5—H5B | 0.9600 | ||
S1—Ni1—S1i | 180.00 (3) | C10—C6—C7 | 117.0 (3) |
S1—Ni1—S2 | 88.08 (5) | C10—C6—C5 | 122.0 (3) |
S1i—Ni1—S2 | 91.92 (5) | C7—C6—C5 | 121.0 (4) |
S1—Ni1—S2i | 91.92 (5) | C8—C7—C6 | 120.9 (3) |
S1i—Ni1—S2i | 88.08 (5) | C8—C7—H7 | 119.5 |
S2—Ni1—S2i | 180.0 | C6—C7—H7 | 119.5 |
C1—S1—Ni1 | 103.30 (12) | N3—C8—C7 | 119.8 (3) |
C3—S2—Ni1 | 103.34 (12) | N3—C8—H8 | 120.1 |
C3i—C1—C2 | 122.5 (3) | C7—C8—H8 | 120.1 |
C3i—C1—S1 | 120.5 (2) | N3—C9—C10 | 120.0 (3) |
C2—C1—S1 | 117.0 (3) | N3—C9—H9 | 120.0 |
N1—C2—C1 | 176.8 (4) | C10—C9—H9 | 120.0 |
C1i—C3—C4 | 122.4 (3) | C9—C10—C6 | 120.6 (3) |
C1i—C3—S2 | 120.3 (2) | C9—C10—H10 | 119.7 |
C4—C3—S2 | 117.4 (2) | C6—C10—H10 | 119.7 |
N2—C4—C3 | 178.9 (4) | C8—N3—C9 | 121.7 (3) |
C6—C5—H5A | 109.5 | C8—N3—N4 | 120.4 (3) |
C6—C5—H5B | 109.5 | C9—N3—N4 | 117.8 (3) |
H5A—C5—H5B | 109.5 | N3—N4—H4A | 120.0 |
C6—C5—H5C | 109.5 | N3—N4—H4B | 120.0 |
H5A—C5—H5C | 109.5 | H4A—N4—H4B | 120.0 |
H5B—C5—H5C | 109.5 |
Symmetry code: (i) −x+1, −y+2, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
N4—H4A···N1ii | 0.86 | 2.35 | 3.151 (6) | 155 |
N4—H4B···N2 | 0.86 | 2.58 | 3.075 (5) | 118 |
Symmetry code: (ii) −x+1, −y+1, −z. |
Experimental details
Crystal data | |
Chemical formula | (C6H9N2)2[Ni(C4N2S2)2] |
Mr | 557.39 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 296 |
a, b, c (Å) | 7.678 (5), 9.095 (6), 9.665 (6) |
α, β, γ (°) | 93.116 (7), 104.519 (8), 108.813 (7) |
V (Å3) | 611.7 (7) |
Z | 1 |
Radiation type | Mo Kα |
µ (mm−1) | 1.16 |
Crystal size (mm) | 0.30 × 0.20 × 0.10 |
Data collection | |
Diffractometer | Bruker SMART CCD area-detector diffractometer |
Absorption correction | Multi-scan (SADABS; Bruker, 2000) |
Tmin, Tmax | 0.732, 0.892 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 3040, 2097, 1937 |
Rint | 0.137 |
(sin θ/λ)max (Å−1) | 0.595 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.065, 0.173, 1.04 |
No. of reflections | 2097 |
No. of parameters | 152 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.82, −1.48 |
Computer programs: SMART (Bruker, 2000), SAINT (Bruker, 2000), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), ORTEP-3 for Windows (Farrugia, 1997), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
N4—H4A···N1i | 0.86 | 2.35 | 3.151 (6) | 155.2 |
N4—H4B···N2 | 0.86 | 2.58 | 3.075 (5) | 117.7 |
Symmetry code: (i) −x+1, −y+1, −z. |
Acknowledgements
The authors thank the Science and Technology Department of Jiangsu Province, People's Republic of China, and the Natural Science Foundation of China for financial support (grant No. 10774076).
References
Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1–19. CrossRef Web of Science Google Scholar
Bruker (2000). SMART, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Cassoux, P., Valade, L., Kobayashi, H., Kobayashi, A., Clark, R. A. & Underhill, A. E. (1991). Coord. Chem. Rev. 110, 115–160. CrossRef CAS Web of Science Google Scholar
Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565. CrossRef IUCr Journals Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
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Square-planar M[dithiolene]2 complexes have attracted extensive interests in the areas of conducting and magnetic materials, dyes, non-linear optics and catalysis (Cassoux et al., 1991). We report herein the crystal structure of the title compound, (I).
The asymmetric unit of (I) (Fig. 1) contains one-half [Ni(mnt)2]2- anion (where mnt is maleonitriledithiolate) and one 1-amino-4-methyl- pyridinium cation. The NiII atom is located at the inversion centre. The bond lengths (Allen et al., 1987) and angles are within normal ranges.
In the crystal structure, intra- and intermolecular N-H···N hydrogen bonds (Table 2) link the molecules (Fig. 2), in which they may be effective in the stabilization of the structure.