organic compounds
1,1′-Dimethyl-4,4′-bipyridinium bis(triiodide)
aDepartment of Chemistry, North University of China, Taiyuan, Shanxi 030051, People's Republic of China
*Correspondence e-mail: hutuopingsx@yahoo.com.cn
In the title compound, C12H14N22+·2I3−, the 1,1′-dimethyl-4,4′-bipyridinium (DMBP) dication is charge balanced by two triiodide ions. The DMBP dication is planar within 0.010 (5) Å. The contains only half of the dication, the other half being generated by an inversion center. Weak C—H⋯I interactions link the ions into sheets parallel to (121).
Related literature
For a dication with similar geometry, see: Russell & Wallwork (1972). For anions with comparable geometry, see: Marsh (2004); Madsen et al. (1999).
Experimental
Crystal data
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Refinement
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Data collection: SMART (Bruker, 2007); cell SAINT-Plus (Bruker, 2007); data reduction: SAINT-Plus; 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
10.1107/S1600536809015207/ez2167sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536809015207/ez2167Isup2.hkl
C12H14N2.4Cl (0.5 mmol, 128 mg) and KI (10 mmol, 1660 mg) were added to 50 ml of CH3CN. After stirring and refluxing for 12 h, the mixture was filtered, and the clear solution was allowed to evaporate slowly under inert atmosphere. Prismatic crystals of the title compound were obtained after 5 days. The crystals were filtered, washed by cool EtOH and dried in air.
All of the H atoms were positioned geometrically and refined using a riding model with C—H = 0.930 Å and 0.96 Å, with Uiso(H) = 1.2 and 1.5 times Ueq(C), for aromatic and methyl hydrogens, respectively.
Data collection: SMART (Bruker, 2007); cell
SAINT-Plus (Bruker, 2007); data reduction: SAINT-Plus (Bruker, 2007); 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).C12H14N22+·2I3− | Z = 1 |
Mr = 947.65 | F(000) = 418 |
Triclinic, P1 | Dx = 2.893 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 7.5457 (4) Å | Cell parameters from 4412 reflections |
b = 7.9541 (6) Å | θ = 2.6–27.6° |
c = 9.3029 (6) Å | µ = 8.56 mm−1 |
α = 90.306 (5)° | T = 296 K |
β = 94.192 (4)° | Prism, black |
γ = 102.332 (5)° | 0.22 × 0.16 × 0.08 mm |
V = 543.88 (6) Å3 |
Bruker SMART CCD area-detector diffractometer | 2683 independent reflections |
Radiation source: fine-focus sealed tube | 1468 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.052 |
ϕ and ω scans | θmax = 28.3°, θmin = 3.9° |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −10→10 |
Tmin = 0.211, Tmax = 0.504 | k = −10→10 |
12956 measured reflections | l = −11→12 |
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)] = 0.040 | H-atom parameters constrained |
wR(F2) = 0.073 | w = 1/[σ2(Fo2) + (0.005P)2 + 2.2853P] where P = (Fo2 + 2Fc2)/3 |
S = 1.02 | (Δ/σ)max < 0.001 |
2683 reflections | Δρmax = 0.97 e Å−3 |
93 parameters | Δρmin = −0.86 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: 0.0028 (3) |
C12H14N22+·2I3− | γ = 102.332 (5)° |
Mr = 947.65 | V = 543.88 (6) Å3 |
Triclinic, P1 | Z = 1 |
a = 7.5457 (4) Å | Mo Kα radiation |
b = 7.9541 (6) Å | µ = 8.56 mm−1 |
c = 9.3029 (6) Å | T = 296 K |
α = 90.306 (5)° | 0.22 × 0.16 × 0.08 mm |
β = 94.192 (4)° |
Bruker SMART CCD area-detector diffractometer | 2683 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | 1468 reflections with I > 2σ(I) |
Tmin = 0.211, Tmax = 0.504 | Rint = 0.052 |
12956 measured reflections |
R[F2 > 2σ(F2)] = 0.040 | 0 restraints |
wR(F2) = 0.073 | H-atom parameters constrained |
S = 1.02 | Δρmax = 0.97 e Å−3 |
2683 reflections | Δρmin = −0.86 e Å−3 |
93 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 | ||
I1 | 0.11371 (7) | 0.64766 (7) | 0.84204 (6) | 0.0705 (2) | |
I2 | 0.19121 (6) | 0.80427 (6) | 0.56237 (6) | 0.05927 (17) | |
I3 | 0.25337 (8) | 0.96496 (8) | 0.28546 (6) | 0.0816 (2) | |
N1 | 0.3773 (9) | 0.2800 (7) | 0.8128 (7) | 0.0588 (16) | |
C1 | 0.3276 (13) | 0.1852 (11) | 0.9438 (9) | 0.085 (3) | |
H1A | 0.4248 | 0.2166 | 1.0179 | 0.128* | |
H1B | 0.3064 | 0.0638 | 0.9235 | 0.128* | |
H1C | 0.2190 | 0.2131 | 0.9758 | 0.128* | |
C2 | 0.5358 (12) | 0.3875 (11) | 0.8116 (9) | 0.074 (2) | |
H2 | 0.6149 | 0.4034 | 0.8944 | 0.088* | |
C3 | 0.2652 (11) | 0.2566 (10) | 0.6956 (10) | 0.072 (2) | |
H3 | 0.1526 | 0.1813 | 0.6969 | 0.086* | |
C4 | 0.5864 (9) | 0.4764 (10) | 0.6903 (8) | 0.061 (2) | |
H4 | 0.6984 | 0.5532 | 0.6924 | 0.074* | |
C5 | 0.3120 (10) | 0.3414 (10) | 0.5722 (8) | 0.066 (2) | |
H5 | 0.2309 | 0.3216 | 0.4906 | 0.079* | |
C6 | 0.4743 (8) | 0.4540 (7) | 0.5658 (7) | 0.0396 (14) |
U11 | U22 | U33 | U12 | U13 | U23 | |
I1 | 0.0689 (4) | 0.0899 (4) | 0.0576 (3) | 0.0291 (3) | 0.0010 (3) | 0.0076 (3) |
I2 | 0.0503 (3) | 0.0648 (3) | 0.0672 (3) | 0.0224 (2) | 0.0040 (2) | 0.0045 (2) |
I3 | 0.0838 (4) | 0.0895 (4) | 0.0816 (4) | 0.0335 (3) | 0.0267 (3) | 0.0292 (3) |
N1 | 0.066 (4) | 0.051 (4) | 0.063 (4) | 0.016 (3) | 0.016 (4) | 0.010 (3) |
C1 | 0.106 (7) | 0.076 (6) | 0.075 (6) | 0.017 (5) | 0.017 (5) | 0.015 (5) |
C2 | 0.071 (6) | 0.088 (6) | 0.061 (5) | 0.020 (5) | −0.011 (4) | 0.015 (5) |
C3 | 0.062 (5) | 0.066 (5) | 0.078 (6) | −0.010 (4) | 0.011 (5) | −0.003 (5) |
C4 | 0.039 (4) | 0.077 (5) | 0.058 (5) | −0.004 (4) | −0.016 (3) | 0.006 (4) |
C5 | 0.052 (5) | 0.080 (6) | 0.054 (5) | −0.007 (4) | −0.003 (4) | −0.001 (4) |
C6 | 0.031 (3) | 0.032 (3) | 0.054 (4) | 0.005 (3) | −0.002 (3) | −0.003 (3) |
I1—I2 | 2.9341 (8) | C2—H2 | 0.9300 |
I2—I3 | 2.9061 (8) | C3—C5 | 1.364 (10) |
N1—C2 | 1.314 (9) | C3—H3 | 0.9300 |
N1—C3 | 1.317 (9) | C4—C6 | 1.371 (8) |
N1—C1 | 1.467 (9) | C4—H4 | 0.9300 |
C1—H1A | 0.9600 | C5—C6 | 1.359 (9) |
C1—H1B | 0.9600 | C5—H5 | 0.9300 |
C1—H1C | 0.9600 | C6—C6i | 1.464 (12) |
C2—C4 | 1.370 (10) | ||
I3—I2—I1 | 177.49 (2) | N1—C3—C5 | 120.9 (7) |
C2—N1—C3 | 119.7 (7) | N1—C3—H3 | 119.5 |
C2—N1—C1 | 119.8 (7) | C5—C3—H3 | 119.5 |
C3—N1—C1 | 120.5 (7) | C2—C4—C6 | 121.0 (6) |
N1—C1—H1A | 109.5 | C2—C4—H4 | 119.5 |
N1—C1—H1B | 109.5 | C6—C4—H4 | 119.5 |
H1A—C1—H1B | 109.5 | C6—C5—C3 | 121.6 (7) |
N1—C1—H1C | 109.5 | C6—C5—H5 | 119.2 |
H1A—C1—H1C | 109.5 | C3—C5—H5 | 119.2 |
H1B—C1—H1C | 109.5 | C5—C6—C4 | 115.9 (6) |
N1—C2—C4 | 121.0 (7) | C5—C6—C6i | 122.1 (7) |
N1—C2—H2 | 119.5 | C4—C6—C6i | 122.1 (7) |
C4—C2—H2 | 119.5 | ||
C3—N1—C2—C4 | 0.3 (12) | N1—C3—C5—C6 | −0.7 (13) |
C1—N1—C2—C4 | 179.4 (7) | C3—C5—C6—C4 | 0.0 (11) |
C2—N1—C3—C5 | 0.6 (12) | C3—C5—C6—C6i | −179.8 (8) |
C1—N1—C3—C5 | −178.5 (7) | C2—C4—C6—C5 | 0.9 (11) |
N1—C2—C4—C6 | −1.0 (12) | C2—C4—C6—C6i | −179.3 (8) |
Symmetry code: (i) −x+1, −y+1, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
C3—H3···I3ii | 0.93 | 3.05 | 3.951 (8) | 163 |
C2—H2···I1iii | 0.93 | 3.16 | 4.066 (8) | 164 |
C5—H5···I2ii | 0.93 | 3.13 | 3.839 (7) | 135 |
Symmetry codes: (ii) −x, −y+1, −z+1; (iii) −x+1, −y+1, −z+2. |
Experimental details
Crystal data | |
Chemical formula | C12H14N22+·2I3− |
Mr | 947.65 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 296 |
a, b, c (Å) | 7.5457 (4), 7.9541 (6), 9.3029 (6) |
α, β, γ (°) | 90.306 (5), 94.192 (4), 102.332 (5) |
V (Å3) | 543.88 (6) |
Z | 1 |
Radiation type | Mo Kα |
µ (mm−1) | 8.56 |
Crystal size (mm) | 0.22 × 0.16 × 0.08 |
Data collection | |
Diffractometer | Bruker SMART CCD area-detector diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 1996) |
Tmin, Tmax | 0.211, 0.504 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 12956, 2683, 1468 |
Rint | 0.052 |
(sin θ/λ)max (Å−1) | 0.667 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.040, 0.073, 1.02 |
No. of reflections | 2683 |
No. of parameters | 93 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.97, −0.86 |
Computer programs: SMART (Bruker, 2007), SAINT-Plus (Bruker, 2007), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
C3—H3···I3i | 0.93 | 3.05 | 3.951 (8) | 162.8 |
C2—H2···I1ii | 0.93 | 3.16 | 4.066 (8) | 164.4 |
C5—H5···I2i | 0.93 | 3.13 | 3.839 (7) | 134.5 |
Symmetry codes: (i) −x, −y+1, −z+1; (ii) −x+1, −y+1, −z+2. |
Acknowledgements
The author is grateful for funding support from the Natural Science Foundation of Shanxi Province (2007011033), the Program of Technological Industrialization at the University of Shanxi Province (20070308) and the start-up fund of North University of China.
References
Bruker (2007). SMART and SAINT-Plus. Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Madsen, D., Burghammer, M., Fiedler, S. & Müller, H. (1999). Acta Cryst. B55, 601–606. Web of Science CSD CrossRef CAS IUCr Journals Google Scholar
Marsh, R. E. (2004). Acta Cryst. B60, 252–253. Web of Science CSD CrossRef CAS IUCr Journals Google Scholar
Russell, J. H. & Wallwork, S. C. (1972). Acta Cryst. B28, 1527–1533. CSD CrossRef CAS IUCr Journals Web of Science Google Scholar
Sheldrick, G. M. (1996). SADABS. University of Göttingen, Germany. Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
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The title compound, (I), was obtained by chance when we tried to prepare the salt of the Pb(II) cation and DMBP in MeOH. This paper provides the first crystal structure of the DMBP dication with two triiodide anions.
Only half of the dication of DMBP is contained in the asymmetric unit, while the other half is generated by the inversion center at (1/2,1/2,1/2) (Fig 1.). The N,N'-dimethyl-4,4'bipyridylium(II) dication has an essentially planar conformation, the maximum deviation of the C1 atom (the methyl group) from its mean plane being 0.010 (5) Å. The geometry of the dication is similar to the one observed in Russell & Wallwork (1972). Meanwhile, the geometry of the anion is comparable to that described in Marsh (2004) and Madsen et al. (1999).
Weak C3—H3···I3 interactions link two I3 anions to each dication. A weaker C2—I2···H1 interaction links each anion to a further DMBP cation, to form sheets parallel to (121). Adjacent sheets are packed into a three-dimensional motif (Fig. 2).