metal-organic compounds
Diaquabis(nicotinamide-κN1)bis(thiocyanato-κN)nickel(II)
aDepartment of Chemistry, Motilal Nehru National Institute of Technology, Allahabad 211 004, India, and bDepartment of Chemistry, Howard University, 2400 Sixth Street, N.W. Washington, DC 20059, USA
*Correspondence e-mail: deepanjalipandey.1@gmail.com
In the title complex, [Ni(NCS)2(C6H6N2O)2(H2O)2], the NiII ion is located on an inversion center and is coordinated in a distorted octahedral environment by two N atoms from two nicotinamide ligands and two water molecules in the equatorial plane, and two N atoms from two thiocyanate anions in the axial positions, all acting as monodentate ligands. In the crystal, weak N—H⋯S hydrogen bonds between the amino groups and the thiocyanate anions form an R42(8) motif. The complex molecules are linked by O—H⋯O, O—H⋯S, and N—H⋯S hydrogen bonds into a three-dimensional supramolecular structure. Weak π–π interactions between the pyridine rings is also found [centroid–centroid distance = 3.8578 (14) Å].
CCDC reference: 993930
Related literature
For background to the applications of transition metal complexes with biochemically active ligands, see: Antolini et al. (1982); Krishnamachari (1974). For related structures, see: Hökelek, Dal et al. (2009); Hökelek, Yilmaz et al. (2009); Özbek et al. (2009); Zhu et al. (2006).
Experimental
Crystal data
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Data collection: CrysAlis PRO (Agilent, 2012); cell CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008) and Mercury (Macrae et al., 2008); software used to prepare material for publication: SHELXTL.
Supporting information
CCDC reference: 993930
10.1107/S1600536814006771/hy2643sup1.cif
contains datablock I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536814006771/hy2643Isup2.hkl
An aqueous solution (10 ml) of nickel acetate tetrahydrate (0.246 g, 1 mmol) and potassium thiocyanate (0.196 g, 2 mmol) was slowly added drop wise to a hot aqueous solution (10 ml) of nicotinamide (0.244 g, 2 mmol) with stirring. Greenish blue colour solution was obtained. After filtration the final clear solution left undisturbed at room temperature for slow evaporation. Next day, needle shaped greenish blue crystals were collected and dried in vacuo over silica gel. Crystals suitable for single crystal X-ray diffraction were manually selected and immersed in silicon oil.
H atoms bound to C and N atoms were placed in calculated positions and refined as riding atoms, with C—H = 0.95 and N—H = 0.88 Å and with Uiso(H) = 1.2Ueq(C, N). H atoms of the water molecule were located from a difference Fourier map and refined isotropically.
Data collection: CrysAlis PRO (Agilent, 2012); cell
CrysAlis PRO (Agilent, 2012); data reduction: CrysAlis PRO (Agilent, 2012); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008) and Mercury (Macrae et al., 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).Fig. 1. Molecular structure of the title complex, showing the 50% probability level ellipsoids. [Symmetry code: (i) 1-x, 1-y, 2-z.] | |
Fig. 2. Packing diagram of the title complex. Hydrogen bonds are shown as dashed lines. |
[Ni(NCS)2(C6H6N2O)2(H2O)2] | Z = 1 |
Mr = 455.16 | F(000) = 234 |
Triclinic, P1 | Dx = 1.587 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 7.5574 (15) Å | Cell parameters from 1387 reflections |
b = 8.2683 (19) Å | θ = 5.2–37.4° |
c = 9.0056 (15) Å | µ = 1.27 mm−1 |
α = 73.010 (18)° | T = 123 K |
β = 69.698 (17)° | Prism, green-blue |
γ = 66.51 (2)° | 0.48 × 0.32 × 0.26 mm |
V = 476.23 (18) Å3 |
Agilent Xcalibur Ruby CCD diffractometer | 4752 independent reflections |
Radiation source: Enhance (Mo) X-ray Source | 3477 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.032 |
Detector resolution: 10.5081 pixels mm-1 | θmax = 37.8°, θmin = 5.1° |
ω scans | h = −12→11 |
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2012) | k = −13→14 |
Tmin = 0.690, Tmax = 1.000 | l = −15→15 |
8114 measured reflections |
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)] = 0.046 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.125 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.03 | w = 1/[σ2(Fo2) + (0.0525P)2 + 0.1045P] where P = (Fo2 + 2Fc2)/3 |
4752 reflections | (Δ/σ)max < 0.001 |
132 parameters | Δρmax = 0.50 e Å−3 |
3 restraints | Δρmin = −0.71 e Å−3 |
[Ni(NCS)2(C6H6N2O)2(H2O)2] | γ = 66.51 (2)° |
Mr = 455.16 | V = 476.23 (18) Å3 |
Triclinic, P1 | Z = 1 |
a = 7.5574 (15) Å | Mo Kα radiation |
b = 8.2683 (19) Å | µ = 1.27 mm−1 |
c = 9.0056 (15) Å | T = 123 K |
α = 73.010 (18)° | 0.48 × 0.32 × 0.26 mm |
β = 69.698 (17)° |
Agilent Xcalibur Ruby CCD diffractometer | 4752 independent reflections |
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2012) | 3477 reflections with I > 2σ(I) |
Tmin = 0.690, Tmax = 1.000 | Rint = 0.032 |
8114 measured reflections |
R[F2 > 2σ(F2)] = 0.046 | 3 restraints |
wR(F2) = 0.125 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.03 | Δρmax = 0.50 e Å−3 |
4752 reflections | Δρmin = −0.71 e Å−3 |
132 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 | ||
Ni | 0.5000 | 0.5000 | 1.0000 | 0.02711 (9) | |
S1 | −0.10823 (7) | 0.89262 (6) | 0.85626 (6) | 0.03634 (11) | |
O1 | 0.3352 (3) | 0.1975 (2) | 0.47112 (16) | 0.0455 (4) | |
O1W | 0.5790 (2) | 0.7206 (2) | 0.85157 (16) | 0.0386 (3) | |
H1W1 | 0.671 (3) | 0.737 (4) | 0.859 (3) | 0.061 (9)* | |
H1W2 | 0.588 (4) | 0.737 (4) | 0.759 (2) | 0.056 (8)* | |
N3 | 0.2125 (2) | 0.6286 (2) | 0.9666 (2) | 0.0371 (3) | |
N1 | 0.5789 (2) | 0.38229 (19) | 0.78909 (16) | 0.0268 (3) | |
N2 | 0.2320 (3) | 0.1178 (2) | 0.73701 (18) | 0.0365 (3) | |
H2A | 0.1431 | 0.0801 | 0.7281 | 0.044* | |
H2B | 0.2439 | 0.1106 | 0.8327 | 0.044* | |
C7 | 0.0784 (3) | 0.7361 (2) | 0.92131 (19) | 0.0281 (3) | |
C1 | 0.4532 (2) | 0.3212 (2) | 0.76502 (18) | 0.0260 (3) | |
H1A | 0.3295 | 0.3278 | 0.8439 | 0.031* | |
C2 | 0.4940 (2) | 0.2486 (2) | 0.63092 (17) | 0.0246 (3) | |
C3 | 0.3476 (3) | 0.1854 (2) | 0.60664 (19) | 0.0279 (3) | |
C4 | 0.6734 (3) | 0.2419 (3) | 0.5151 (2) | 0.0327 (3) | |
H4A | 0.7051 | 0.1966 | 0.4202 | 0.039* | |
C5 | 0.8053 (3) | 0.3020 (3) | 0.5400 (2) | 0.0363 (4) | |
H5A | 0.9301 | 0.2968 | 0.4631 | 0.044* | |
C6 | 0.7533 (3) | 0.3700 (2) | 0.6787 (2) | 0.0314 (3) | |
H6A | 0.8457 | 0.4095 | 0.6956 | 0.038* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Ni | 0.02907 (15) | 0.03414 (16) | 0.02262 (14) | −0.01311 (12) | −0.00883 (11) | −0.00525 (11) |
S1 | 0.0317 (2) | 0.0386 (2) | 0.0394 (2) | −0.01499 (18) | −0.01464 (18) | 0.00316 (18) |
O1 | 0.0661 (10) | 0.0612 (9) | 0.0270 (6) | −0.0368 (8) | −0.0189 (6) | −0.0029 (6) |
O1W | 0.0531 (8) | 0.0506 (8) | 0.0262 (6) | −0.0332 (7) | −0.0161 (6) | 0.0029 (5) |
N3 | 0.0325 (7) | 0.0469 (9) | 0.0357 (8) | −0.0099 (7) | −0.0125 (6) | −0.0129 (7) |
N1 | 0.0285 (6) | 0.0331 (6) | 0.0231 (5) | −0.0131 (5) | −0.0071 (5) | −0.0068 (5) |
N2 | 0.0404 (8) | 0.0497 (9) | 0.0279 (7) | −0.0266 (7) | −0.0045 (6) | −0.0078 (6) |
C7 | 0.0286 (7) | 0.0367 (8) | 0.0241 (6) | −0.0158 (6) | −0.0050 (6) | −0.0079 (6) |
C1 | 0.0276 (7) | 0.0333 (7) | 0.0203 (6) | −0.0130 (6) | −0.0041 (5) | −0.0077 (5) |
C2 | 0.0299 (7) | 0.0275 (6) | 0.0189 (6) | −0.0118 (6) | −0.0060 (5) | −0.0049 (5) |
C3 | 0.0341 (8) | 0.0289 (7) | 0.0238 (6) | −0.0114 (6) | −0.0082 (6) | −0.0073 (5) |
C4 | 0.0367 (8) | 0.0396 (9) | 0.0223 (6) | −0.0152 (7) | −0.0007 (6) | −0.0110 (6) |
C5 | 0.0308 (8) | 0.0472 (10) | 0.0309 (8) | −0.0167 (8) | 0.0017 (7) | −0.0136 (7) |
C6 | 0.0283 (7) | 0.0384 (8) | 0.0303 (7) | −0.0131 (7) | −0.0073 (6) | −0.0077 (7) |
Ni—O1W | 2.0876 (15) | N2—H2A | 0.8800 |
Ni—N3 | 2.0899 (17) | N2—H2B | 0.8800 |
Ni—N1 | 2.1776 (14) | C1—C2 | 1.389 (2) |
S1—C7 | 1.6377 (18) | C1—H1A | 0.9500 |
O1—C3 | 1.228 (2) | C2—C4 | 1.386 (2) |
O1W—H1W1 | 0.79 (2) | C2—C3 | 1.497 (2) |
O1W—H1W2 | 0.79 (2) | C4—C5 | 1.380 (3) |
N3—C7 | 1.158 (2) | C4—H4A | 0.9500 |
N1—C6 | 1.334 (2) | C5—C6 | 1.387 (2) |
N1—C1 | 1.340 (2) | C5—H5A | 0.9500 |
N2—C3 | 1.322 (2) | C6—H6A | 0.9500 |
O1Wi—Ni—O1W | 180.00 (6) | C3—N2—H2A | 120.0 |
O1Wi—Ni—N3i | 88.85 (7) | C3—N2—H2B | 120.0 |
O1W—Ni—N3i | 91.15 (7) | H2A—N2—H2B | 120.0 |
O1Wi—Ni—N3 | 91.15 (7) | N3—C7—S1 | 178.30 (17) |
O1W—Ni—N3 | 88.85 (7) | N1—C1—C2 | 123.52 (15) |
N3i—Ni—N3 | 180.0 | N1—C1—H1A | 118.2 |
O1Wi—Ni—N1 | 90.25 (6) | C2—C1—H1A | 118.2 |
O1W—Ni—N1 | 89.75 (6) | C4—C2—C1 | 117.97 (16) |
N3i—Ni—N1 | 92.52 (6) | C4—C2—C3 | 120.08 (14) |
N3—Ni—N1 | 87.48 (6) | C1—C2—C3 | 121.91 (15) |
O1Wi—Ni—N1i | 89.75 (6) | O1—C3—N2 | 121.81 (17) |
O1W—Ni—N1i | 90.25 (6) | O1—C3—C2 | 121.07 (16) |
N3i—Ni—N1i | 87.48 (6) | N2—C3—C2 | 117.12 (14) |
N3—Ni—N1i | 92.52 (6) | C5—C4—C2 | 118.94 (15) |
N1—Ni—N1i | 180.000 (1) | C5—C4—H4A | 120.5 |
Ni—O1W—H1W1 | 118 (2) | C2—C4—H4A | 120.5 |
Ni—O1W—H1W2 | 119 (2) | C4—C5—C6 | 119.16 (17) |
H1W1—O1W—H1W2 | 107 (2) | C4—C5—H5A | 120.4 |
C7—N3—Ni | 160.38 (17) | C6—C5—H5A | 120.4 |
C6—N1—C1 | 117.68 (14) | N1—C6—C5 | 122.70 (17) |
C6—N1—Ni | 121.18 (12) | N1—C6—H6A | 118.7 |
C1—N1—Ni | 121.14 (11) | C5—C6—H6A | 118.7 |
O1Wi—Ni—N3—C7 | −179.4 (4) | Ni—N1—C1—C2 | 178.49 (12) |
O1W—Ni—N3—C7 | 0.6 (4) | N1—C1—C2—C4 | −1.0 (2) |
N1—Ni—N3—C7 | −89.2 (4) | N1—C1—C2—C3 | −178.64 (14) |
N1i—Ni—N3—C7 | 90.8 (4) | C4—C2—C3—O1 | −30.6 (2) |
O1Wi—Ni—N1—C6 | −130.61 (14) | C1—C2—C3—O1 | 147.02 (17) |
O1W—Ni—N1—C6 | 49.39 (14) | C4—C2—C3—N2 | 149.97 (17) |
N3i—Ni—N1—C6 | −41.75 (14) | C1—C2—C3—N2 | −32.4 (2) |
N3—Ni—N1—C6 | 138.25 (14) | C1—C2—C4—C5 | 1.9 (3) |
O1Wi—Ni—N1—C1 | 50.01 (13) | C3—C2—C4—C5 | 179.63 (16) |
O1W—Ni—N1—C1 | −129.99 (13) | C2—C4—C5—C6 | −1.0 (3) |
N3i—Ni—N1—C1 | 138.87 (13) | C1—N1—C6—C5 | 1.9 (3) |
N3—Ni—N1—C1 | −41.13 (13) | Ni—N1—C6—C5 | −177.55 (14) |
C6—N1—C1—C2 | −0.9 (2) | C4—C5—C6—N1 | −0.9 (3) |
Symmetry code: (i) −x+1, −y+1, −z+2. |
D—H···A | D—H | H···A | D···A | D—H···A |
O1W—H1W1···S1ii | 0.79 (3) | 2.47 (3) | 3.224 (2) | 161 (3) |
O1W—H1W2···O1iii | 0.79 (2) | 1.92 (2) | 2.686 (2) | 164 (3) |
N2—H2A···S1iv | 0.88 | 2.67 | 3.459 (2) | 150 |
N2—H2B···S1v | 0.88 | 2.62 | 3.435 (2) | 154 |
Symmetry codes: (ii) x+1, y, z; (iii) −x+1, −y+1, −z+1; (iv) x, y−1, z; (v) −x, −y+1, −z+2. |
D—H···A | D—H | H···A | D···A | D—H···A |
O1W—H1W1···S1i | 0.79 (3) | 2.47 (3) | 3.224 (2) | 161 (3) |
O1W—H1W2···O1ii | 0.79 (2) | 1.92 (2) | 2.686 (2) | 164 (3) |
N2—H2A···S1iii | 0.88 | 2.67 | 3.459 (2) | 150 |
N2—H2B···S1iv | 0.88 | 2.62 | 3.435 (2) | 154 |
Symmetry codes: (i) x+1, y, z; (ii) −x+1, −y+1, −z+1; (iii) x, y−1, z; (iv) −x, −y+1, −z+2. |
Acknowledgements
The authors wish to extend their gratitude to Professor P. Chakrabarti, Director, MNNIT, Allahabad, for providing a Institute Research Fellowship to DP.
References
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This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
Transition metal complexes with biochemically active ligands frequently show interesting physical and/or chemical properties, as a result they may find applications in biological systems (Antolini et al., 1982). As ligands, nicotinamide (NA) and thiocyanate are interesting due to their potential formation of metal coordination complexes as they exhibit multifunctional coordination modes due to the presence of S and N donor atoms. With reference to the hard and soft acids and bases concept, the soft cations show a pronounced affinity for coordination with the softer ligands, while hard cations prefer coordination with harder ligands (Hökelek, Dal et al., 2009; Hökelek, Yilmaz et al., 2009; Özbek et al., 2009; Zhu et al., 2006). NA is one form of niacin and a deficiency of this vitamin leads to loss of copper from body, known as pellagra disease. The nicotinic acid derivative N,N-diethylnicotinamide (DENA) is an important respiratory stimulant.
In the title complex, the NiII ion is located on an inversion center and coordinated by two equatorial N atoms from two NA ligands and two equatorial O atoms from water molecules, and two axial N donor from thiocyanate ligands, as can be seen in Fig. 1. The Ni—O1W bond distance is 2.088 (2) Å, which is very close to the Ni—N3(thiocyanate) distance of 2.090 (2) Å. The bond distance of Ni—N1(NA) is longer at 2.178 (1) Å. The N—Ni–N, O—Ni–N angles indicate a slightly distorted octahedral coordination for the NiII ion. The thiocyanate anion is almost linear with an N—C—S bond angle being 178.3 (2)°, coordinating in a little bent fashion to Ni with an Ni—N3—C7 angle of 160.38 (17)°. The two terminal N–bonded thiocyanate anions around the NiII ion are trans arranged. The Ni···Ni distance spaced by the thiocyanate ligand is 7.5574 (15) Å.
As can be seen from the packing diagram (Fig. 2), the complex molecules are linked by intermolecular O—H···O, O—H···S and N—H···S hydrogen bonds (Table 1), forming a supramolecular structure. The discrete molecules are connected by O1W—H···O1 and O1W—H···S1 hydrogen bonds into a two-dimensional layer parallel to (010). The thiocyanate S1 atom also accepts the other two hydrogen bonds from two different amide N atoms, completing an overall three-dimensional supramolecular structure.