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In the title complex, [Zn(C10H10N4)3](NO3)2, the six-coordin­ate ZnII atom lies at the inter­section of three twofold axes in a slightly disorted octa­hedral coordination environment. The N atom of a nitrate anion is located on a threefold axis. In the crystal structure, inter­molecular N—H...N and N—H...O hydrogen bonds between cations and anions form a two-dimensional network perpendicular to the c axis.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807048192/lh2515sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807048192/lh2515Isup2.hkl
Contains datablock I

CCDC reference: 667120

Key indicators

  • Single-crystal X-ray study
  • T = 298 K
  • Mean [sigma](C-C) = 0.005 Å
  • R factor = 0.038
  • wR factor = 0.081
  • Data-to-parameter ratio = 13.7

checkCIF/PLATON results

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Alert level C PLAT042_ALERT_1_C Calc. and Rep. MoietyFormula Strings Differ .... ? PLAT094_ALERT_2_C Ratio of Maximum / Minimum Residual Density .... 2.65 PLAT152_ALERT_1_C Supplied and Calc Volume s.u. Inconsistent ..... ? PLAT764_ALERT_4_C Overcomplete CIF Bond List Detected (Rep/Expd) . 1.13 Ratio
Alert level G REFLT03_ALERT_4_G Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF. From the CIF: _diffrn_reflns_theta_max 25.98 From the CIF: _reflns_number_total 1072 Count of symmetry unique reflns 601 Completeness (_total/calc) 178.37% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 471 Fraction of Friedel pairs measured 0.784 Are heavy atom types Z>Si present yes PLAT794_ALERT_5_G Check Predicted Bond Valency for Zn1 (2) 1.83
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 4 ALERT level C = Check and explain 2 ALERT level G = General alerts; check 2 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 0 ALERT type 3 Indicator that the structure quality may be low 2 ALERT type 4 Improvement, methodology, query or suggestion 1 ALERT type 5 Informative message, check

Comment top

2,2'-Bipyridine and its derivatives play a pivotal role in the area of modern coordination chemistry. For example, some dye-sensitized solar cells deal with complexes of derivatives of 2,2'-bispyridine as a ligand (Kuang et al., 2006). We have an interest in complexes containing 3,3'-diamino-2,2'-bipyridine and have synthesized the complexes containing NiII, CdII, MnII and CuII ions (Shi et al., 2006a,b; Min et al., 2006; Zhang et al., 2007). Here we report the structure of the title complex (Fig. 1).

The ZnII atom, located on the intersection of a threefold axis and a twofold axis, assumes a slightly distorted octahedral ZnN6 coordination geometry. The nitrate anion lies on a threefold axis. In the 3,3'-diamino-2,2'-bipyridine ligand, each pyridine ring is essentially planar with a maximum deviation of -0.029 (4) Å for atom C1; the dihedral angle between the two pyridine rings is 34.77 (18), which is larger than that in the Ni(II) complex, but smaller than that in Cd(II) and Mn(II) complexes. Just as with the Ni(II), Mn(II) and Cd(II) complexes the deviation from planarity in the title compound is expected in terms of steric relief. The hydrogen bonds (Table 1) that arise from nitrate anions and amino group result in the connection of the cations and the nitrate anions and contribute to the formation of a supermolecular two-dimensional sheet parallel ab plane, as shown in Fig. 2.

Related literature top

For background information see: Kuang et al. (2006). For related structures, see: Shi et al. (2006a,b,c); Zhang et al. (2007).

Experimental top

Zn(NO3)2·6H2O (0.0354 g, 0.119 mmol) in H2O (10 ml) was added to 6,6'-diamino-2,2'-bipyridine (0.0110 g, 0.059 mmol) in acetonitrile (5 ml), and the solution was stirred for a few minutes. Colorless crystals were obtained after allowing the solution to stand at room temperature for one week. The infrared stretching vibrations of pyridine ring and amino groups appeared at 1638 cm-1, 1465 cm-1 and 1384 cm-1.

Refinement top

The H atoms were placed in calculated positions and refined as riding, with C—H = 0.93 Å, Uiso(H) = 1.2eq(C); N—H = 0.86 Å, Uiso(H) = 1.2eq(N) for amino group.

Structure description top

2,2'-Bipyridine and its derivatives play a pivotal role in the area of modern coordination chemistry. For example, some dye-sensitized solar cells deal with complexes of derivatives of 2,2'-bispyridine as a ligand (Kuang et al., 2006). We have an interest in complexes containing 3,3'-diamino-2,2'-bipyridine and have synthesized the complexes containing NiII, CdII, MnII and CuII ions (Shi et al., 2006a,b; Min et al., 2006; Zhang et al., 2007). Here we report the structure of the title complex (Fig. 1).

The ZnII atom, located on the intersection of a threefold axis and a twofold axis, assumes a slightly distorted octahedral ZnN6 coordination geometry. The nitrate anion lies on a threefold axis. In the 3,3'-diamino-2,2'-bipyridine ligand, each pyridine ring is essentially planar with a maximum deviation of -0.029 (4) Å for atom C1; the dihedral angle between the two pyridine rings is 34.77 (18), which is larger than that in the Ni(II) complex, but smaller than that in Cd(II) and Mn(II) complexes. Just as with the Ni(II), Mn(II) and Cd(II) complexes the deviation from planarity in the title compound is expected in terms of steric relief. The hydrogen bonds (Table 1) that arise from nitrate anions and amino group result in the connection of the cations and the nitrate anions and contribute to the formation of a supermolecular two-dimensional sheet parallel ab plane, as shown in Fig. 2.

For background information see: Kuang et al. (2006). For related structures, see: Shi et al. (2006a,b,c); Zhang et al. (2007).

Computing details top

Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT (Bruker, 1997); program(s) used to solve structure: SHELXTL (Bruker, 2001); program(s) used to refine structure: SHELXTL (Bruker, 2001); molecular graphics: SHELXTL (Bruker, 2001); software used to prepare material for publication: SHELXTL (Bruker, 2001).

Figures top
[Figure 1] Fig. 1. The molecular structure showing the atom numbering scheme with thermal ellipsoids drawn at the 30% probability level. [Symmetry codes: (i) x - y + 1, -y + 2, -z; (ii) -y + 1, x - y + 2, z; (iii) -x + y - 1, -x + 1, z; (iv) y - 1, x + 1, -z; (v) -x, -x + y, -z; (vi) -y + 1, x - y + 1, z; (vii) -x + y, -x + 1, z]. Only one of the two nitrate anions in the formula unit is showm.
[Figure 2] Fig. 2. Part of the crystal structure with hydrogen bonds shown as dashed lines.
Tris(3,3'-diamino-2,2'-bipyridine)zinc(II) bis(nitrate) top
Crystal data top
[Zn(C10H10N4)3](NO3)2Dx = 1.527 Mg m3
Mr = 748.05Mo Kα radiation, λ = 0.71073 Å
Trigonal, R32Cell parameters from 918 reflections
Hall symbol: R 3 2"θ = 2.2–19.0°
a = 14.6116 (19) ŵ = 0.82 mm1
c = 13.199 (4) ÅT = 298 K
V = 2440.4 (8) Å3Prism, colourless
Z = 30.20 × 0.14 × 0.10 mm
F(000) = 1158
Data collection top
Bruker SMART APEX CCD
diffractometer
1072 independent reflections
Radiation source: fine-focus sealed tube1005 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.051
φ and ω scansθmax = 26.0°, θmin = 2.2°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 1810
Tmin = 0.853, Tmax = 0.922k = 1518
4419 measured reflectionsl = 1615
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.038H-atom parameters constrained
wR(F2) = 0.081 w = 1/[σ2(Fo2) + (0.0391P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max < 0.001
1072 reflectionsΔρmax = 0.49 e Å3
78 parametersΔρmin = 0.18 e Å3
0 restraintsAbsolute structure: Flack (1983), with 469 Friedel pairs
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.03 (2)
Crystal data top
[Zn(C10H10N4)3](NO3)2Z = 3
Mr = 748.05Mo Kα radiation
Trigonal, R32µ = 0.82 mm1
a = 14.6116 (19) ÅT = 298 K
c = 13.199 (4) Å0.20 × 0.14 × 0.10 mm
V = 2440.4 (8) Å3
Data collection top
Bruker SMART APEX CCD
diffractometer
1072 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
1005 reflections with I > 2σ(I)
Tmin = 0.853, Tmax = 0.922Rint = 0.051
4419 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.038H-atom parameters constrained
wR(F2) = 0.081Δρmax = 0.49 e Å3
S = 1.05Δρmin = 0.18 e Å3
1072 reflectionsAbsolute structure: Flack (1983), with 469 Friedel pairs
78 parametersAbsolute structure parameter: 0.03 (2)
0 restraints
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*/Ueq
Zn10.00001.00000.00000.0332 (2)
N20.0862 (2)0.9399 (2)0.08301 (16)0.0354 (6)
C50.1754 (2)0.9566 (2)0.0369 (2)0.0363 (7)
C30.1693 (4)0.8141 (4)0.1330 (2)0.0585 (9)
H30.19690.77110.15050.070*
C10.0411 (3)0.8668 (3)0.1543 (3)0.0487 (8)
H10.02060.85640.18510.058*
C20.0846 (3)0.8054 (3)0.1838 (3)0.0593 (10)
H20.05590.75880.23800.071*
C40.2154 (3)0.8876 (2)0.0541 (3)0.0478 (8)
N10.33330.66670.0452 (2)0.0415 (8)
O10.3647 (2)0.6020 (2)0.04535 (17)0.0631 (7)
N30.2931 (3)0.8874 (3)0.0037 (3)0.0721 (10)
H3A0.31330.84250.00850.087*
H3B0.32170.93230.05220.087*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Zn10.0295 (3)0.0295 (3)0.0407 (4)0.01473 (14)0.0000.000
N20.0331 (16)0.0286 (15)0.0419 (12)0.0135 (13)0.0018 (12)0.0051 (12)
C50.0318 (15)0.0314 (16)0.0463 (18)0.0163 (13)0.0014 (13)0.0018 (13)
C30.065 (3)0.044 (2)0.077 (2)0.0356 (19)0.006 (3)0.011 (2)
C10.051 (2)0.047 (2)0.0494 (19)0.0249 (16)0.0071 (15)0.0095 (15)
C20.073 (3)0.048 (2)0.059 (2)0.031 (2)0.0009 (19)0.0202 (17)
C40.0407 (19)0.0358 (17)0.069 (2)0.0204 (15)0.0072 (16)0.0034 (16)
N10.0402 (13)0.0402 (13)0.044 (2)0.0201 (7)0.0000.000
O10.0538 (17)0.0466 (17)0.0985 (16)0.0322 (15)0.0023 (13)0.0010 (13)
N30.062 (2)0.059 (2)0.116 (3)0.0456 (18)0.022 (2)0.0168 (19)
Geometric parameters (Å, º) top
Zn1—N2i2.159 (2)C3—C41.404 (5)
Zn1—N2ii2.159 (2)C3—H30.9300
Zn1—N2iii2.159 (2)C1—C21.390 (5)
Zn1—N2iv2.159 (2)C1—H10.9300
Zn1—N22.159 (2)C2—H20.9300
Zn1—N2v2.159 (2)C4—N31.368 (4)
N2—C11.325 (4)N1—O1vi1.239 (2)
N2—C51.345 (4)N1—O1vii1.239 (2)
C5—C41.414 (4)N1—O11.239 (2)
C5—C5iii1.467 (6)N3—H3A0.8600
C3—C21.357 (5)N3—H3B0.8600
N2i—Zn1—N2ii169.86 (16)C4—C5—C5iii124.6 (2)
N2i—Zn1—N2iii96.53 (8)C2—C3—C4120.3 (3)
N2ii—Zn1—N2iii91.45 (14)C2—C3—H3119.8
N2i—Zn1—N2iv96.53 (8)C4—C3—H3119.8
N2ii—Zn1—N2iv76.28 (14)N2—C1—C2121.1 (3)
N2iii—Zn1—N2iv96.53 (8)N2—C1—H1119.5
N2i—Zn1—N291.45 (14)C2—C1—H1119.5
N2ii—Zn1—N296.53 (8)C3—C2—C1119.4 (3)
N2iii—Zn1—N276.28 (14)C3—C2—H2120.3
N2iv—Zn1—N2169.86 (16)C1—C2—H2120.3
N2i—Zn1—N2v76.28 (14)N3—C4—C3119.5 (3)
N2ii—Zn1—N2v96.53 (8)N3—C4—C5123.5 (3)
N2iii—Zn1—N2v169.86 (16)C3—C4—C5117.0 (3)
N2iv—Zn1—N2v91.45 (14)O1vi—N1—O1vii120.000 (2)
N2—Zn1—N2v96.53 (8)O1vi—N1—O1120.000 (2)
C1—N2—C5120.9 (3)O1vii—N1—O1120.000 (3)
C1—N2—Zn1122.1 (2)C4—N3—H3A120.0
C5—N2—Zn1113.92 (18)C4—N3—H3B120.0
N2—C5—C4120.4 (3)H3A—N3—H3B120.0
N2—C5—C5iii114.69 (17)
N2ii—Zn1—N2—C1101.6 (2)C5—N2—C1—C20.2 (5)
N2iii—Zn1—N2—C1168.5 (3)Zn1—N2—C1—C2159.3 (3)
N2v—Zn1—N2—C14.2 (3)C4—C3—C2—C12.7 (6)
N2ii—Zn1—N2—C598.0 (3)N2—C1—C2—C35.7 (6)
N2iii—Zn1—N2—C58.12 (15)C2—C3—C4—N3172.8 (4)
N2v—Zn1—N2—C5164.6 (2)C2—C3—C4—C55.2 (6)
C1—N2—C5—C48.2 (4)N2—C5—C4—N3167.3 (3)
Zn1—N2—C5—C4152.5 (2)C5iii—C5—C4—N36.8 (5)
C1—N2—C5—C5iii177.2 (3)N2—C5—C4—C310.7 (5)
Zn1—N2—C5—C5iii22.1 (4)C5iii—C5—C4—C3175.2 (4)
Symmetry codes: (i) x, x+y, z; (ii) y+1, xy+2, z; (iii) xy+1, y+2, z; (iv) y1, x+1, z; (v) x+y1, x+1, z; (vi) x+y, x+1, z; (vii) y+1, xy+1, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N3—H3A···O1vii0.862.142.980 (4)167
N3—H3B···N3iii0.862.402.851 (6)113
Symmetry codes: (iii) xy+1, y+2, z; (vii) y+1, xy+1, z.

Experimental details

Crystal data
Chemical formula[Zn(C10H10N4)3](NO3)2
Mr748.05
Crystal system, space groupTrigonal, R32
Temperature (K)298
a, c (Å)14.6116 (19), 13.199 (4)
V3)2440.4 (8)
Z3
Radiation typeMo Kα
µ (mm1)0.82
Crystal size (mm)0.20 × 0.14 × 0.10
Data collection
DiffractometerBruker SMART APEX CCD
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.853, 0.922
No. of measured, independent and
observed [I > 2σ(I)] reflections
4419, 1072, 1005
Rint0.051
(sin θ/λ)max1)0.616
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.038, 0.081, 1.05
No. of reflections1072
No. of parameters78
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.49, 0.18
Absolute structureFlack (1983), with 469 Friedel pairs
Absolute structure parameter0.03 (2)

Computer programs: SMART (Bruker, 1997), SAINT (Bruker, 1997), SHELXTL (Bruker, 2001).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N3—H3A···O1i0.862.142.980 (4)166.8
N3—H3B···N3ii0.862.402.851 (6)113.3
Symmetry codes: (i) y+1, xy+1, z; (ii) xy+1, y+2, z.
 

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