organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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ISSN: 2056-9890

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

(Received 2 August 2010; accepted 19 August 2010; online 25 August 2010)

In the crystal structure of the title compound, C14H16N4O22+·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 asymmetric unit 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.

Related literature

For Ag(I) complexes incorporating N,N′-bis­(2-pyrid­yl)oxamide ligands which show one- and two-dimensional structures, see: Hsu & Chen (2004[Hsu, Y.-F. & Chen, J.-D. (2004). Eur. J. Inorg. Chem. pp. 1488-1493.]); Hu et al. (2004[Hu, H.-L., Yeh, C.-W. & Chen, J.-D. (2004). Eur. J. Inorg. Chem. pp. 4696-4701.]). For the synthesis of the starting reactant, see: Cheng et al. (2009[Cheng, P.-C., Wu, C.-J. & Chen, J.-D. (2009). Acta Cryst. E65, o2734.]).

[Scheme 1]

Experimental

Crystal data
  • C14H16N4O22+·2Cl·C2H3N

  • Mr = 384.26

  • Monoclinic, P 2/c

  • a = 10.6740 (19) Å

  • b = 8.7637 (5) Å

  • c = 10.370 (3) Å

  • β = 109.83 (2)°

  • V = 912.5 (3) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.38 mm−1

  • T = 295 K

  • 0.6 × 0.2 × 0.1 mm

Data collection
  • Bruker P4 diffractometer

  • Absorption correction: ψ scan (XSCANS; Siemens, 1995[Siemens (1995). XSCANS. Siemens Analytical X-ray Instruments Inc., Madison, Wisconsin, USA.]) Tmin = 0.823, Tmax = 0.922

  • 2165 measured reflections

  • 1619 independent reflections

  • 1308 reflections with I > 2σ(I)

  • Rint = 0.023

  • 3 standard reflections every 97 reflections intensity decay: none

Refinement
  • R[F2 > 2σ(F2)] = 0.035

  • wR(F2) = 0.094

  • S = 1.07

  • 1619 reflections

  • 118 parameters

  • H-atom parameters constrained

  • Δρmax = 0.20 e Å−3

  • Δρmin = −0.17 e Å−3

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1A⋯Cli 0.86 2.14 2.9772 (16) 165
N2—H2A⋯Cli 0.86 2.43 3.2057 (17) 150
Symmetry code: (i) x, y+1, z.

Data collection: XSCANS (Siemens, 1995[Siemens (1995). XSCANS. Siemens Analytical X-ray Instruments Inc., Madison, Wisconsin, USA.]); cell refinement: XSCANS; data reduction: XSCANS; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); molecular graphics: SHELXTL (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); software used to prepare material for publication: SHELXTL.

Supporting information


Comment top

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).

Related literature top

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).

Experimental top

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.

Refinement top

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).

Structure description top

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).

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).

Computing details top

Data collection: XSCANS (Siemens, 1995); cell refinement: 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).

Figures top
[Figure 1] Fig. 1. Crystal structure of the title compound with labeling and displacement ellipsoids drawn at the 30% probability level. Symmetry code: i = -x + 1,-y + 2,-z + 1. Disordering is shown as full and open bonds.
6,6'-Dimethyl-2,2'-[oxalylbis(azanediyl)]dipyridinium dichloride acetonitrile solvate top
Crystal data top
C14H16N4O22+·2Cl·C2H3NF(000) = 400
Mr = 384.26Dx = 1.399 Mg m3
Monoclinic, P2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ycCell parameters from 28 reflections
a = 10.6740 (19) Åθ = 4.7–12.5°
b = 8.7637 (5) ŵ = 0.38 mm1
c = 10.370 (3) ÅT = 295 K
β = 109.83 (2)°Plate, colourless
V = 912.5 (3) Å30.6 × 0.2 × 0.1 mm
Z = 2
Data collection top
Bruker P4
diffractometer
1308 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.023
Graphite monochromatorθmax = 25.0°, θmin = 2.0°
ω scansh = 1212
Absorption correction: ψ scan
(XSCANS; Siemens, 1995)
k = 101
Tmin = 0.823, Tmax = 0.922l = 121
2165 measured reflections3 standard reflections every 97 reflections
1619 independent reflections intensity decay: none
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)] = 0.035H-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 reflectionsΔρmax = 0.20 e Å3
118 parametersΔρmin = 0.17 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0090 (15)
Crystal data top
C14H16N4O22+·2Cl·C2H3NV = 912.5 (3) Å3
Mr = 384.26Z = 2
Monoclinic, P2/cMo Kα radiation
a = 10.6740 (19) ŵ = 0.38 mm1
b = 8.7637 (5) ÅT = 295 K
c = 10.370 (3) Å0.6 × 0.2 × 0.1 mm
β = 109.83 (2)°
Data collection top
Bruker P4
diffractometer
1308 reflections with I > 2σ(I)
Absorption correction: ψ scan
(XSCANS; Siemens, 1995)
Rint = 0.023
Tmin = 0.823, Tmax = 0.9223 standard reflections every 97 reflections
2165 measured reflections intensity decay: none
1619 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0350 restraints
wR(F2) = 0.094H-atom parameters constrained
S = 1.07Δρmax = 0.20 e Å3
1619 reflectionsΔρmin = 0.17 e Å3
118 parameters
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Cl0.23722 (6)0.11398 (6)0.09664 (5)0.0569 (2)
O0.55710 (15)0.81506 (16)0.54656 (14)0.0542 (4)
N10.27012 (15)0.78055 (18)0.15297 (15)0.0400 (4)
H1A0.25130.87150.12120.048*
N20.39872 (16)0.90108 (18)0.34987 (15)0.0424 (4)
H2A0.36530.98370.30730.051*
N31.00000.6381 (4)0.25000.0953 (12)
C10.1214 (2)0.7019 (3)0.0703 (2)0.0596 (6)
H1B0.09330.61030.12300.089*
H1C0.16600.76720.11530.089*
H1D0.04500.75380.06260.089*
C20.2141 (2)0.6624 (2)0.0687 (2)0.0443 (5)
C30.2463 (2)0.5175 (2)0.1183 (2)0.0521 (5)
H3A0.21180.43360.06270.062*
C40.3305 (2)0.4971 (3)0.2514 (2)0.0567 (6)
H4A0.35140.39850.28510.068*
C50.3847 (2)0.6201 (2)0.3363 (2)0.0522 (5)
H5A0.44060.60540.42620.063*
C60.35325 (19)0.7650 (2)0.28310 (18)0.0395 (4)
C70.4915 (2)0.9157 (2)0.47672 (19)0.0420 (5)
C81.00000.7663 (4)0.25000.0583 (8)
C91.00000.9293 (4)0.25000.0666 (9)
H9B1.08940.96580.27040.100*0.50
H9A0.96500.96580.31820.100*0.50
H9C0.94560.96580.16140.100*0.50
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl0.0769 (4)0.0307 (3)0.0530 (3)0.0030 (2)0.0089 (3)0.0052 (2)
O0.0635 (9)0.0404 (9)0.0450 (7)0.0124 (7)0.0005 (7)0.0022 (6)
N10.0498 (9)0.0268 (8)0.0401 (8)0.0023 (7)0.0112 (7)0.0022 (6)
N20.0546 (10)0.0297 (9)0.0373 (8)0.0057 (7)0.0082 (7)0.0012 (6)
N30.107 (3)0.052 (2)0.136 (3)0.0000.054 (3)0.000
C10.0696 (15)0.0438 (13)0.0510 (12)0.0032 (11)0.0017 (11)0.0076 (10)
C20.0499 (11)0.0326 (10)0.0494 (11)0.0034 (9)0.0155 (9)0.0053 (8)
C30.0604 (14)0.0300 (11)0.0625 (13)0.0045 (9)0.0166 (11)0.0053 (10)
C40.0689 (14)0.0289 (10)0.0680 (14)0.0042 (10)0.0178 (12)0.0110 (10)
C50.0639 (13)0.0361 (11)0.0491 (11)0.0044 (10)0.0095 (10)0.0071 (9)
C60.0465 (10)0.0334 (10)0.0382 (9)0.0016 (8)0.0140 (8)0.0010 (8)
C70.0472 (11)0.0398 (11)0.0364 (10)0.0059 (9)0.0109 (8)0.0008 (8)
C80.0587 (19)0.053 (2)0.066 (2)0.0000.0248 (16)0.000
C90.080 (2)0.0492 (19)0.068 (2)0.0000.0212 (18)0.000
Geometric parameters (Å, º) top
O—C71.204 (2)C2—C31.370 (3)
N1—C61.347 (2)C3—C41.380 (3)
N1—C21.356 (2)C3—H3A0.9300
N1—H1A0.8600C4—C51.388 (3)
N2—C71.358 (2)C4—H4A0.9300
N2—C61.382 (2)C5—C61.379 (3)
N2—H2A0.8600C5—H5A0.9300
N3—C81.123 (5)C7—C7i1.545 (4)
C1—C21.486 (3)C8—C91.429 (5)
C1—H1B0.9600C9—H9B0.9600
C1—H1C0.9600C9—H9A0.9600
C1—H1D0.9600C9—H9C0.9600
C6—N1—C2124.41 (17)C3—C4—H4A119.2
C6—N1—H1A117.8C5—C4—H4A119.2
C2—N1—H1A117.8C6—C5—C4117.98 (19)
C7—N2—C6125.72 (16)C6—C5—H5A121.0
C7—N2—H2A117.1C4—C5—H5A121.0
C6—N2—H2A117.1N1—C6—C5118.82 (18)
C2—C1—H1B109.5N1—C6—N2114.49 (16)
C2—C1—H1C109.5C5—C6—N2126.69 (17)
H1B—C1—H1C109.5O—C7—N2126.70 (18)
C2—C1—H1D109.5O—C7—C7i122.0 (2)
H1B—C1—H1D109.5N2—C7—C7i111.3 (2)
H1C—C1—H1D109.5N3—C8—C9180.000 (2)
N1—C2—C3117.77 (18)C8—C9—H9B109.5
N1—C2—C1116.77 (18)C8—C9—H9A109.5
C3—C2—C1125.46 (19)H9B—C9—H9A109.5
C2—C3—C4119.4 (2)C8—C9—H9C109.5
C2—C3—H3A120.3H9B—C9—H9C109.5
C4—C3—H3A120.3H9A—C9—H9C109.5
C3—C4—C5121.6 (2)
Symmetry code: (i) x+1, y+2, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···Clii0.862.142.9772 (16)165
N2—H2A···Clii0.862.433.2057 (17)150
Symmetry code: (ii) x, y+1, z.

Experimental details

Crystal data
Chemical formulaC14H16N4O22+·2Cl·C2H3N
Mr384.26
Crystal system, space groupMonoclinic, P2/c
Temperature (K)295
a, b, c (Å)10.6740 (19), 8.7637 (5), 10.370 (3)
β (°) 109.83 (2)
V3)912.5 (3)
Z2
Radiation typeMo Kα
µ (mm1)0.38
Crystal size (mm)0.6 × 0.2 × 0.1
Data collection
DiffractometerBruker P4
Absorption correctionψ scan
(XSCANS; Siemens, 1995)
Tmin, Tmax0.823, 0.922
No. of measured, independent and
observed [I > 2σ(I)] reflections
2165, 1619, 1308
Rint0.023
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.035, 0.094, 1.07
No. of reflections1619
No. of parameters118
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.20, 0.17

Computer programs: XSCANS (Siemens, 1995), SHELXTL (Sheldrick, 2008), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···Cli0.862.142.9772 (16)164.6
N2—H2A···Cli0.862.433.2057 (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

First citationCheng, P.-C., Wu, C.-J. & Chen, J.-D. (2009). Acta Cryst. E65, o2734.  Web of Science CrossRef IUCr Journals Google Scholar
First citationHsu, Y.-F. & Chen, J.-D. (2004). Eur. J. Inorg. Chem. pp. 1488–1493.  Web of Science CSD CrossRef Google Scholar
First citationHu, H.-L., Yeh, C.-W. & Chen, J.-D. (2004). Eur. J. Inorg. Chem. pp. 4696–4701.  Web of Science CSD CrossRef Google Scholar
First citationSheldrick, G. M. (2008). Acta Cryst. A64, 112–122.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationSiemens (1995). XSCANS. Siemens Analytical X-ray Instruments Inc., Madison, Wisconsin, USA.  Google Scholar

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