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The title complex, [CdNi(CN)4(C6H7N)2]n, adopts a slightly distorted octahedral geometry around the Cd centre. Four cyanide N atoms occupy the equatorial coordination sites around the Cd centre. The structure consists of corrugated and cyanide-bridged polymeric networks made up of tetracyano­nickelate ions coordinated to cadmium, with the Ni ion coordinated by four cyanide ligands in a square-planar arrangement. The Cd and Ni atoms occupy special positions of 2/m site symmetry. The 3-methyl­pyridine group, except for two methyl H atoms, lies on a crystallographic mirror plane. The 3-methyl­pyridine molecules, bound to cadmium in trans positions, are located on both sides of the network. The bonding in the networks occurs because of a departure of the Ni—C—N—Cd sequence of atoms from linearity at the C and N atoms.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270105000636/gd1364sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270105000636/gd1364Isup2.hkl
Contains datablock I

CCDC reference: 268076

Comment top

Hofmann-type complexes with the formula ML2Ni(CN)4, where M is a divalent transition metal and L is an N-donor ligand molecule, have a structure consisting of polymeric two-dimensional networks formed by [Ni(CN)4]2− anions bridged by [ML2]2+ cations. Metal coordination polymers with one- and two-dimensional structures are of current interest due to their possible relevance to material science (Yoghi et al., 1996). There is still much to be explored in the crystal engineering of Hofmann-type and analogous structures that are built up by CN linkages between square-planar or tetrahedral tetracyanometallate(II) complexes on the one hand, and octahedral metal(II) complexes ligated with complementary ligands on the other (Iwamoto et al., 1984).

The molecule of the title complex, (I) adopts a slightly distorted octahedral geometry around the Cd centre, as shown in Fig. 1. The equatorial and axial coordination sites are occupied by four N atoms of the bridging cyano groups and two N atoms of the two chelating 3-methylpyridine ligands, respectively. The structure consists of corrugated and cyanide-bridged polymeric networks made up of tetracyanonickelate ions coordinated to Cd, where the Ni ion is coordinated by four cyanide ligands in a square-planar arrangement. In this arrangement, two of the cyano groups are terminal, while the other two cyano groups, coordinated in a trans position about the Ni atom, constitute the bridges. The bonding in the networks occurs because of a departure of the Ni—C—N—Cd sequence of atoms from linearity at the C and N positions. The Ni1—C7—N2 and C7—N2—Cd bond angles are 177.2 (2) and 163.5 (2)°, respectively.

The Cd and Ni atoms of (I) lie at (0, 0, 0) and (0, 1/2, −1/2), respectively, on sites with 2/m symmetry. The non-H atoms of the 3-methylpyridine moiety lie on a mirror plane, chosen as that at y = 0. The [–Cd-{trans-NC—Ni(CN)2—CN–}] bridges run along the face diagonals of the bc plane, sharing the Cd atoms to form layers (Figs. 2 and 3). The distance between any two adjacent layers is a/2 (approximately 8.255 Å). Similar corrugated polymeric layers are also reported in some other related compounds (Erdönmez et al., 1998). The C—N and Ni—C bond distances of the square-planar Ni coordination environment are comparable with those in related Ni(CN)4 complexes (Karada~g et al., 2004; Yuge & Iwamoto, 1995; Yuge et al., 1996; Woodward et al., 2001).

The 3-methylpyridine ligands bound to the Cd atom in trans positions are located on both sides of the network and the whole 3-methylpyridine moiety, except for two H atoms of the methyl group, lies on a crystallographic mirror plane. By translation, the 3-methylpyridine aromatic rings stack in the b direction. The stacking is an offset face-to-face ππ interaction. The distance between ring centroids is 3.7789 (7) Å and the interplanar spacing is b/2.

Experimental top

The synthesis of the title compound and its characterization by IR spectroscopy have been described previously by Akyüz et al. (1994). Crystals of (I) were obtained from a solution in which solvent?

Refinement top

H atoms were treated as riding atoms, with C—H distances of 0.93 Å for aromatic H atoms and 0.96 Å for methyl H atoms, and with Uiso(H) = 1.5Ueq(C). Please check added text. Also, some H atoms have s.u.s in the CIF.

Computing details top

Data collection: CAD-4 EXPRESS (Enraf-Nonius, 1993); cell refinement: CAD-4 EXPRESS; data reduction: MolEN (Fair, 1990); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEPIII (Farrugia, 1997); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. A drawing of the molecule of (I), showing the atomic numbering scheme. Displacement ellipsoids are drawn at the 50% probability level and H atoms are shown as small spheres of arbitrary size. [Symmetry codes: (i) −x, −y, −z; (ii) x, −y, z; (iii) −x, y, −z].
[Figure 2] Fig. 2. Part of the crystal structure of (I), showing the formation of layers parallel to (100). For the sake of clarity, the 3-methylpyridine rings and their H atoms have been omitted.
[Figure 3] Fig. 3. Stereoview of the molecular packing in (I).
poly[[bis(3-methylpyridine)cadmium(II)]-tetra-µ-cyano-nickel(II)] top
Crystal data top
[CdNi(CN)4(C6H7N)2]F(000) = 456
Mr = 461.44Dx = 1.730 Mg m3
Monoclinic, C2/mMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2yCell parameters from 25 reflections
a = 16.5198 (16) Åθ = 10.6–18.7°
b = 7.3512 (7) ŵ = 2.27 mm1
c = 7.6309 (6) ÅT = 293 K
β = 107.06 (1)°Prismatic, orange
V = 885.92 (14) Å30.42 × 0.36 × 0.24 mm
Z = 2
Data collection top
Enraf-Nonius CAD-4
diffractometer
937 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.025
Graphite monochromatorθmax = 26.3°, θmin = 2.6°
ω/2θ scansh = 2020
Absorption correction: ψ scan
(North et al., 1968)
k = 09
Tmin = 0.427, Tmax = 0.580l = 99
1793 measured reflections3 standard reflections every 120 min
972 independent reflections intensity decay: 2.5%
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)] = 0.028Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.084H-atom parameters constrained
S = 1.07 w = 1/[σ2(Fo2) + (0.0623P)2 + 0.7317P]
where P = (Fo2 + 2Fc2)/3
972 reflections(Δ/σ)max < 0.001
73 parametersΔρmax = 1.40 e Å3
0 restraintsΔρmin = 0.60 e Å3
Crystal data top
[CdNi(CN)4(C6H7N)2]V = 885.92 (14) Å3
Mr = 461.44Z = 2
Monoclinic, C2/mMo Kα radiation
a = 16.5198 (16) ŵ = 2.27 mm1
b = 7.3512 (7) ÅT = 293 K
c = 7.6309 (6) Å0.42 × 0.36 × 0.24 mm
β = 107.06 (1)°
Data collection top
Enraf-Nonius CAD-4
diffractometer
937 reflections with I > 2σ(I)
Absorption correction: ψ scan
(North et al., 1968)
Rint = 0.025
Tmin = 0.427, Tmax = 0.5803 standard reflections every 120 min
1793 measured reflections intensity decay: 2.5%
972 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0280 restraints
wR(F2) = 0.084H-atom parameters constrained
S = 1.07Δρmax = 1.40 e Å3
972 reflectionsΔρmin = 0.60 e Å3
73 parameters
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)
Cd10.00000.00000.00000.02228 (18)
Ni10.00000.50000.50000.0199 (2)
N10.14144 (19)0.00000.0069 (4)0.0326 (6)
N20.02489 (17)0.2183 (3)0.2346 (3)0.0393 (5)
C10.2023 (3)0.00000.1650 (6)0.0484 (10)
H10.18750.00000.27360.046 (16)*
C20.2868 (3)0.00000.1739 (7)0.0628 (14)
H20.32820.00000.28690.09 (2)*
C30.3095 (3)0.00000.0147 (7)0.0516 (11)
H30.36640.00000.01880.09 (2)*
C40.2478 (3)0.00000.1496 (8)0.0405 (11)
C50.1641 (2)0.00000.1464 (5)0.0378 (8)
H50.12150.00000.25770.051 (13)*
C60.2670 (4)0.00000.3295 (10)0.072 (2)
H6A0.21500.00000.42770.109*
H6B0.29920.10660.33810.109*0.50
H6C0.29920.10660.33810.109*0.50
C70.01635 (16)0.3228 (3)0.3393 (3)0.0265 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cd10.0332 (3)0.0169 (2)0.0209 (2)0.0000.01449 (17)0.000
Ni10.0299 (4)0.0146 (3)0.0174 (3)0.0000.0105 (3)0.000
N10.0357 (15)0.0353 (16)0.0289 (14)0.0000.0126 (12)0.000
N20.0541 (14)0.0308 (12)0.0379 (12)0.0023 (11)0.0213 (11)0.0095 (11)
C10.046 (2)0.068 (3)0.0303 (18)0.0000.0099 (17)0.000
C20.040 (2)0.093 (4)0.045 (2)0.0000.003 (2)0.000
C30.0312 (19)0.061 (3)0.062 (3)0.0000.0129 (19)0.000
C40.039 (2)0.040 (2)0.049 (3)0.0000.023 (2)0.000
C50.0356 (19)0.049 (2)0.0316 (17)0.0000.0148 (15)0.000
C60.058 (4)0.108 (6)0.067 (4)0.0000.043 (3)0.000
C70.0356 (12)0.0209 (11)0.0252 (10)0.0022 (9)0.0123 (9)0.0007 (9)
Geometric parameters (Å, º) top
Cd1—N12.322 (3)C1—C21.378 (7)
Cd1—N1i2.322 (3)C1—H10.9300
Cd1—N2ii2.349 (2)C2—C31.373 (7)
Cd1—N2iii2.349 (2)C2—H20.9300
Cd1—N2i2.349 (2)C3—C41.365 (8)
Cd1—N22.349 (2)C3—H30.9300
Ni1—C7iv1.863 (2)C4—C51.390 (6)
Ni1—C7v1.863 (2)C4—C61.497 (11)
Ni1—C71.863 (2)C5—H50.9301
Ni1—C7vi1.863 (2)C6—H6A0.9600
N1—C11.324 (5)C6—H6B0.9600
N1—C51.329 (5)C6—H6C0.9600
N2—C71.146 (3)
N1—Cd1—N1i180.0C7—N2—Cd1163.5 (2)
N1—Cd1—N2ii91.87 (8)N1—C1—C2122.2 (4)
N1i—Cd1—N2ii88.13 (8)N1—C1—H1118.9
N1—Cd1—N2iii88.13 (8)C2—C1—H1118.9
N1i—Cd1—N2iii91.87 (8)C3—C2—C1119.5 (4)
N2ii—Cd1—N2iii180.00 (8)C3—C2—H2120.2
N1—Cd1—N2i88.13 (8)C1—C2—H2120.3
N1i—Cd1—N2i91.87 (8)C4—C3—C2119.3 (4)
N2ii—Cd1—N2i93.82 (12)C4—C3—H3120.4
N2iii—Cd1—N2i86.18 (12)C2—C3—H3120.4
N1—Cd1—N291.87 (8)C3—C4—C5117.6 (5)
N1i—Cd1—N288.13 (8)C3—C4—C6122.7 (6)
N2ii—Cd1—N286.18 (12)C5—C4—C6119.7 (6)
N2iii—Cd1—N293.82 (12)N1—C5—C4123.6 (4)
N2i—Cd1—N2180.0N1—C5—H5118.2
C7iv—Ni1—C7v180.00 (15)C4—C5—H5118.2
C7iv—Ni1—C788.77 (13)C4—C6—H6A109.5
C7v—Ni1—C791.23 (13)C4—C6—H6B109.5
C7iv—Ni1—C7vi91.23 (13)H6A—C6—H6B109.5
C7v—Ni1—C7vi88.77 (13)C4—C6—H6C109.5
C7—Ni1—C7vi180.00 (15)H6A—C6—H6C109.5
C1—N1—C5117.9 (3)H6B—C6—H6C109.5
C1—N1—Cd1120.7 (3)N2—C7—Ni1177.2 (2)
C5—N1—Cd1121.4 (2)
N2ii—Cd1—N1—C143.12 (6)N2iii—Cd1—N2—C785.9 (7)
N2iii—Cd1—N1—C1136.88 (6)C5—N1—C1—C20.0
N2i—Cd1—N1—C1136.88 (6)Cd1—N1—C1—C2180.0
N2—Cd1—N1—C143.12 (6)N1—C1—C2—C30.0
N2ii—Cd1—N1—C5136.88 (6)C1—C2—C3—C40.0
N2iii—Cd1—N1—C543.12 (6)C2—C3—C4—C50.0
N2i—Cd1—N1—C543.12 (6)C2—C3—C4—C6180.0
N2—Cd1—N1—C5136.88 (6)C1—N1—C5—C40.0
N1—Cd1—N2—C7174.1 (7)Cd1—N1—C5—C4180.0
N1i—Cd1—N2—C75.9 (7)C3—C4—C5—N10.0
N2ii—Cd1—N2—C794.1 (7)C6—C4—C5—N1180.0
Symmetry codes: (i) x, y, z; (ii) x, y, z; (iii) x, y, z; (iv) x, y+1, z; (v) x, y, z1; (vi) x, y+1, z1.

Experimental details

Crystal data
Chemical formula[CdNi(CN)4(C6H7N)2]
Mr461.44
Crystal system, space groupMonoclinic, C2/m
Temperature (K)293
a, b, c (Å)16.5198 (16), 7.3512 (7), 7.6309 (6)
β (°) 107.06 (1)
V3)885.92 (14)
Z2
Radiation typeMo Kα
µ (mm1)2.27
Crystal size (mm)0.42 × 0.36 × 0.24
Data collection
DiffractometerEnraf-Nonius CAD-4
diffractometer
Absorption correctionψ scan
(North et al., 1968)
Tmin, Tmax0.427, 0.580
No. of measured, independent and
observed [I > 2σ(I)] reflections
1793, 972, 937
Rint0.025
(sin θ/λ)max1)0.623
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.028, 0.084, 1.07
No. of reflections972
No. of parameters73
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)1.40, 0.60

Computer programs: CAD-4 EXPRESS (Enraf-Nonius, 1993), CAD-4 EXPRESS, MolEN (Fair, 1990), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), ORTEPIII (Farrugia, 1997), SHELXL97.

Selected geometric parameters (Å, º) top
Cd1—N12.322 (3)N2—C71.146 (3)
Ni1—C71.863 (2)
N1—Cd1—N1i180.0N2iii—Cd1—N293.82 (12)
N1—Cd1—N2ii91.87 (8)N2i—Cd1—N2180.0
N1i—Cd1—N2ii88.13 (8)C7—Ni1—C7iv180.00 (15)
N2ii—Cd1—N2iii180.00 (8)C1—N1—Cd1120.7 (3)
N2iii—Cd1—N2i86.18 (12)C5—N1—Cd1121.4 (2)
N2ii—Cd1—N286.18 (12)
Symmetry codes: (i) x, y, z; (ii) x, y, z; (iii) x, y, z; (iv) x, y+1, z1.
 

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