organic compounds
6,6′-Dimethyl-2,2′-[oxalylbis(azanediyl)]dipyridinium dichloride acetonitrile solvate
aDepartment of Chemical and Materials Engineering, Nanya Institute of Technology, Chung-Li, Taiwan, and bDepartment of Chemistry, Chung-Yuan Christian University, Chung-Li, Taiwan
*Correspondence e-mail: jdchen@cycu.edu.tw
In the 14H16N4O22+·2Cl−·CH3CN, weak intermolecular N—H⋯Cl hydrogen bonds are found between the H atoms bound to the pyridine and amine N atoms and the chloride anions. The consits of one half cationic molecule which is located on a centre of inversion, one chloride anion in a general position and one half acetonitrile molecule which is located on a twofold axis. Because of symmetry, the C—H hydrogens of the acetonitrile solvent molecule are disordered over two orientations.
of the title compound, CRelated literature
For Ag(I) complexes incorporating N,N′-bis(2-pyridyl)oxamide ligands which show one- and two-dimensional structures, see: Hsu & Chen (2004); Hu et al. (2004). For the synthesis of the starting reactant, see: Cheng et al. (2009).
Experimental
Crystal data
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Refinement
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Data collection: XSCANS (Siemens, 1995); cell XSCANS; data reduction: XSCANS; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.
Supporting information
https://doi.org/10.1107/S1600536810033519/nc2195sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536810033519/nc2195Isup2.hkl
N,N'-bis(6-methyl-2-pyridyl)oxamide (0.30 g, 1.1 mmol) (Cheng, et al., 2009) and CuCl2 (0.15 g, 1.1 mmol) were placed in a flask containing 10 ml CH2Cl2, which was refluxed for 8 h. The precipitate was then filtered and dried in vacuum. Coloress plate crystals of the title compound suitable for X-ray crystallography were obtained by slow evaporization of the solvent from a solution of the precipitate in CH3CN.
All the hydrogen atoms were placed into idealized positions (methyl H atoms allowed to rotate but not to tip) and constrained by the riding atom approximation with C—H = 0.93 — 0.96 Å, N—H = 0.86 Å and Uiso(H) = 1.2 Ueq(C, N) (1.5 for methyl H atoms).
Several Ag(I) complexes containg N,N'-bis(2-pyridyl)oxamide ligands have been prepared, which show one-dimensional and two-dimensional structures (Hsu, et al., 2004; Hu, et al., 2004). To investigate the
of the on the structural type of such complexes, we have synthesized N,N'-bis(6-methyl-2-pyridyl)oxamide (Cheng, et al., 2009) and reacted with metal salts. Within this project the of the title compound was determined.In the
the cationic molecules are almost planar and the O atoms are trans-oriented (Fig. 1). The N,N'-Bis(6-methyl-2-pyridinium)oxamide cations and the chloride anions are connected by weak intermolecular N—H···Cl hydrogen bonding (Tab. 1).For Ag(I) complexes containg N,N'-bis(2-pyridyl)oxamide ligands which show one- and two-dimensional structures, see: Hsu et al. (2004); Hu et al. (2004). For the synthesis of the starting reactand, see: Cheng et al. (2009).
Data collection: XSCANS (Siemens, 1995); cell
XSCANS (Siemens, 1995); data reduction: SHELXTL (Sheldrick, 2008); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).C14H16N4O22+·2Cl−·C2H3N | F(000) = 400 |
Mr = 384.26 | Dx = 1.399 Mg m−3 |
Monoclinic, P2/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2yc | Cell parameters from 28 reflections |
a = 10.6740 (19) Å | θ = 4.7–12.5° |
b = 8.7637 (5) Å | µ = 0.38 mm−1 |
c = 10.370 (3) Å | T = 295 K |
β = 109.83 (2)° | Plate, colourless |
V = 912.5 (3) Å3 | 0.6 × 0.2 × 0.1 mm |
Z = 2 |
Bruker P4 diffractometer | 1308 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.023 |
Graphite monochromator | θmax = 25.0°, θmin = 2.0° |
ω scans | h = −12→12 |
Absorption correction: ψ scan (XSCANS; Siemens, 1995) | k = −10→1 |
Tmin = 0.823, Tmax = 0.922 | l = −12→1 |
2165 measured reflections | 3 standard reflections every 97 reflections |
1619 independent reflections | intensity decay: none |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.035 | H-atom parameters constrained |
wR(F2) = 0.094 | w = 1/[σ2(Fo2) + (0.0401P)2 + 0.2279P] where P = (Fo2 + 2Fc2)/3 |
S = 1.07 | (Δ/σ)max < 0.001 |
1619 reflections | Δρmax = 0.20 e Å−3 |
118 parameters | Δρmin = −0.17 e Å−3 |
0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.0090 (15) |
C14H16N4O22+·2Cl−·C2H3N | V = 912.5 (3) Å3 |
Mr = 384.26 | Z = 2 |
Monoclinic, P2/c | Mo Kα radiation |
a = 10.6740 (19) Å | µ = 0.38 mm−1 |
b = 8.7637 (5) Å | T = 295 K |
c = 10.370 (3) Å | 0.6 × 0.2 × 0.1 mm |
β = 109.83 (2)° |
Bruker P4 diffractometer | 1308 reflections with I > 2σ(I) |
Absorption correction: ψ scan (XSCANS; Siemens, 1995) | Rint = 0.023 |
Tmin = 0.823, Tmax = 0.922 | 3 standard reflections every 97 reflections |
2165 measured reflections | intensity decay: none |
1619 independent reflections |
R[F2 > 2σ(F2)] = 0.035 | 0 restraints |
wR(F2) = 0.094 | H-atom parameters constrained |
S = 1.07 | Δρmax = 0.20 e Å−3 |
1619 reflections | Δρmin = −0.17 e Å−3 |
118 parameters |
Experimental. 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. |
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 | Occ. (<1) | |
Cl | 0.23722 (6) | 0.11398 (6) | 0.09664 (5) | 0.0569 (2) | |
O | 0.55710 (15) | 0.81506 (16) | 0.54656 (14) | 0.0542 (4) | |
N1 | 0.27012 (15) | 0.78055 (18) | 0.15297 (15) | 0.0400 (4) | |
H1A | 0.2513 | 0.8715 | 0.1212 | 0.048* | |
N2 | 0.39872 (16) | 0.90108 (18) | 0.34987 (15) | 0.0424 (4) | |
H2A | 0.3653 | 0.9837 | 0.3073 | 0.051* | |
N3 | 1.0000 | 0.6381 (4) | 0.2500 | 0.0953 (12) | |
C1 | 0.1214 (2) | 0.7019 (3) | −0.0703 (2) | 0.0596 (6) | |
H1B | 0.0933 | 0.6103 | −0.1230 | 0.089* | |
H1C | 0.1660 | 0.7672 | −0.1153 | 0.089* | |
H1D | 0.0450 | 0.7538 | −0.0626 | 0.089* | |
C2 | 0.2141 (2) | 0.6624 (2) | 0.0687 (2) | 0.0443 (5) | |
C3 | 0.2463 (2) | 0.5175 (2) | 0.1183 (2) | 0.0521 (5) | |
H3A | 0.2118 | 0.4336 | 0.0627 | 0.062* | |
C4 | 0.3305 (2) | 0.4971 (3) | 0.2514 (2) | 0.0567 (6) | |
H4A | 0.3514 | 0.3985 | 0.2851 | 0.068* | |
C5 | 0.3847 (2) | 0.6201 (2) | 0.3363 (2) | 0.0522 (5) | |
H5A | 0.4406 | 0.6054 | 0.4262 | 0.063* | |
C6 | 0.35325 (19) | 0.7650 (2) | 0.28310 (18) | 0.0395 (4) | |
C7 | 0.4915 (2) | 0.9157 (2) | 0.47672 (19) | 0.0420 (5) | |
C8 | 1.0000 | 0.7663 (4) | 0.2500 | 0.0583 (8) | |
C9 | 1.0000 | 0.9293 (4) | 0.2500 | 0.0666 (9) | |
H9B | 1.0894 | 0.9658 | 0.2704 | 0.100* | 0.50 |
H9A | 0.9650 | 0.9658 | 0.3182 | 0.100* | 0.50 |
H9C | 0.9456 | 0.9658 | 0.1614 | 0.100* | 0.50 |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cl | 0.0769 (4) | 0.0307 (3) | 0.0530 (3) | 0.0030 (2) | 0.0089 (3) | 0.0052 (2) |
O | 0.0635 (9) | 0.0404 (9) | 0.0450 (7) | 0.0124 (7) | 0.0005 (7) | 0.0022 (6) |
N1 | 0.0498 (9) | 0.0268 (8) | 0.0401 (8) | 0.0023 (7) | 0.0112 (7) | 0.0022 (6) |
N2 | 0.0546 (10) | 0.0297 (9) | 0.0373 (8) | 0.0057 (7) | 0.0082 (7) | 0.0012 (6) |
N3 | 0.107 (3) | 0.052 (2) | 0.136 (3) | 0.000 | 0.054 (3) | 0.000 |
C1 | 0.0696 (15) | 0.0438 (13) | 0.0510 (12) | −0.0032 (11) | 0.0017 (11) | −0.0076 (10) |
C2 | 0.0499 (11) | 0.0326 (10) | 0.0494 (11) | −0.0034 (9) | 0.0155 (9) | −0.0053 (8) |
C3 | 0.0604 (14) | 0.0300 (11) | 0.0625 (13) | −0.0045 (9) | 0.0166 (11) | −0.0053 (10) |
C4 | 0.0689 (14) | 0.0289 (10) | 0.0680 (14) | 0.0042 (10) | 0.0178 (12) | 0.0110 (10) |
C5 | 0.0639 (13) | 0.0361 (11) | 0.0491 (11) | 0.0044 (10) | 0.0095 (10) | 0.0071 (9) |
C6 | 0.0465 (10) | 0.0334 (10) | 0.0382 (9) | 0.0016 (8) | 0.0140 (8) | 0.0010 (8) |
C7 | 0.0472 (11) | 0.0398 (11) | 0.0364 (10) | 0.0059 (9) | 0.0109 (8) | −0.0008 (8) |
C8 | 0.0587 (19) | 0.053 (2) | 0.066 (2) | 0.000 | 0.0248 (16) | 0.000 |
C9 | 0.080 (2) | 0.0492 (19) | 0.068 (2) | 0.000 | 0.0212 (18) | 0.000 |
O—C7 | 1.204 (2) | C2—C3 | 1.370 (3) |
N1—C6 | 1.347 (2) | C3—C4 | 1.380 (3) |
N1—C2 | 1.356 (2) | C3—H3A | 0.9300 |
N1—H1A | 0.8600 | C4—C5 | 1.388 (3) |
N2—C7 | 1.358 (2) | C4—H4A | 0.9300 |
N2—C6 | 1.382 (2) | C5—C6 | 1.379 (3) |
N2—H2A | 0.8600 | C5—H5A | 0.9300 |
N3—C8 | 1.123 (5) | C7—C7i | 1.545 (4) |
C1—C2 | 1.486 (3) | C8—C9 | 1.429 (5) |
C1—H1B | 0.9600 | C9—H9B | 0.9600 |
C1—H1C | 0.9600 | C9—H9A | 0.9600 |
C1—H1D | 0.9600 | C9—H9C | 0.9600 |
C6—N1—C2 | 124.41 (17) | C3—C4—H4A | 119.2 |
C6—N1—H1A | 117.8 | C5—C4—H4A | 119.2 |
C2—N1—H1A | 117.8 | C6—C5—C4 | 117.98 (19) |
C7—N2—C6 | 125.72 (16) | C6—C5—H5A | 121.0 |
C7—N2—H2A | 117.1 | C4—C5—H5A | 121.0 |
C6—N2—H2A | 117.1 | N1—C6—C5 | 118.82 (18) |
C2—C1—H1B | 109.5 | N1—C6—N2 | 114.49 (16) |
C2—C1—H1C | 109.5 | C5—C6—N2 | 126.69 (17) |
H1B—C1—H1C | 109.5 | O—C7—N2 | 126.70 (18) |
C2—C1—H1D | 109.5 | O—C7—C7i | 122.0 (2) |
H1B—C1—H1D | 109.5 | N2—C7—C7i | 111.3 (2) |
H1C—C1—H1D | 109.5 | N3—C8—C9 | 180.000 (2) |
N1—C2—C3 | 117.77 (18) | C8—C9—H9B | 109.5 |
N1—C2—C1 | 116.77 (18) | C8—C9—H9A | 109.5 |
C3—C2—C1 | 125.46 (19) | H9B—C9—H9A | 109.5 |
C2—C3—C4 | 119.4 (2) | C8—C9—H9C | 109.5 |
C2—C3—H3A | 120.3 | H9B—C9—H9C | 109.5 |
C4—C3—H3A | 120.3 | H9A—C9—H9C | 109.5 |
C3—C4—C5 | 121.6 (2) |
Symmetry code: (i) −x+1, −y+2, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1A···Clii | 0.86 | 2.14 | 2.9772 (16) | 165 |
N2—H2A···Clii | 0.86 | 2.43 | 3.2057 (17) | 150 |
Symmetry code: (ii) x, y+1, z. |
Experimental details
Crystal data | |
Chemical formula | C14H16N4O22+·2Cl−·C2H3N |
Mr | 384.26 |
Crystal system, space group | Monoclinic, P2/c |
Temperature (K) | 295 |
a, b, c (Å) | 10.6740 (19), 8.7637 (5), 10.370 (3) |
β (°) | 109.83 (2) |
V (Å3) | 912.5 (3) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 0.38 |
Crystal size (mm) | 0.6 × 0.2 × 0.1 |
Data collection | |
Diffractometer | Bruker P4 |
Absorption correction | ψ scan (XSCANS; Siemens, 1995) |
Tmin, Tmax | 0.823, 0.922 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 2165, 1619, 1308 |
Rint | 0.023 |
(sin θ/λ)max (Å−1) | 0.595 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.035, 0.094, 1.07 |
No. of reflections | 1619 |
No. of parameters | 118 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.20, −0.17 |
Computer programs: XSCANS (Siemens, 1995), SHELXTL (Sheldrick, 2008), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1A···Cli | 0.86 | 2.14 | 2.9772 (16) | 164.6 |
N2—H2A···Cli | 0.86 | 2.43 | 3.2057 (17) | 149.8 |
Symmetry code: (i) x, y+1, z. |
Acknowledgements
We are grateful to the National Science Council of the Republic of China for support. This research was also supported by the project of the specific research fields in Chung-Yuan Christian University, Taiwan, under grant No. CYCU-98-CR—CH.
References
Cheng, P.-C., Wu, C.-J. & Chen, J.-D. (2009). Acta Cryst. E65, o2734. Web of Science CrossRef IUCr Journals Google Scholar
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Several Ag(I) complexes containg N,N'-bis(2-pyridyl)oxamide ligands have been prepared, which show one-dimensional and two-dimensional structures (Hsu, et al., 2004; Hu, et al., 2004). To investigate the steric effect of the alkyl groups on the structural type of such complexes, we have synthesized N,N'-bis(6-methyl-2-pyridyl)oxamide (Cheng, et al., 2009) and reacted with metal salts. Within this project the crystal structure of the title compound was determined.
In the crystal structure the cationic molecules are almost planar and the O atoms are trans-oriented (Fig. 1). The N,N'-Bis(6-methyl-2-pyridinium)oxamide cations and the chloride anions are connected by weak intermolecular N—H···Cl hydrogen bonding (Tab. 1).