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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2009 Oct 10;65(Pt 11):o2676–o2677. doi: 10.1107/S1600536809040446

(E)-1-Methyl-4-styrylpyridinium iodide monohydrate

Hoong-Kun Fun a,*,, Suchada Chantrapromma b,§, Chanasuk Surasit b, Kullapa Chanawanno b
PMCID: PMC2971221  PMID: 21578284

Abstract

In the title compound, C14H14N+·I·H2O, the cation is essentially planar, with a dihedral angle of 2.55 (7)° between the pyridinium and phenyl rings, and exists in an E configuration with respect to the ethenyl bond. In the crystal structure, the cations are stacked in an anti­parallel manner along the a axis. The cation is linked to the water mol­ecule by a weak C—H⋯O inter­action, and the water mol­ecule is further linked to the I ion by O—H⋯I hydrogen bonds. The crystal structure is consolidated by these inter­actions and is further stabilized by a π–π inter­action between the pyridinium and phenyl rings with a centroid–centroid distance of 3.6850 (8) Å.

Related literature

For bond-length data, see: Allen et al. (1987). For background to non-linear optical materials research, see: Chemla & Zyss (1987); Chia et al. (1995); Dittrich et al. (2003); Lin et al. (2002); Prasad & Williams (1991). For related structures, see: Chanawanno et al. (2008); Chantrapromma, Jindawong & Fun (2007); Chantrapromma, Jindawong, Fun & Patil (2007). For the stability of the temperature controller used in the data collection, see: Cosier & Glazer (1986).graphic file with name e-65-o2676-scheme1.jpg

Experimental

Crystal data

  • C14H14N+·I·H2O

  • M r = 341.18

  • Monoclinic, Inline graphic

  • a = 7.3636 (1) Å

  • b = 10.5929 (1) Å

  • c = 18.2807 (2) Å

  • β = 106.770 (1)°

  • V = 1365.29 (3) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 2.33 mm−1

  • T = 100 K

  • 0.32 × 0.22 × 0.20 mm

Data collection

  • Bruker APEXII CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2005) T min = 0.524, T max = 0.649

  • 27548 measured reflections

  • 6004 independent reflections

  • 5307 reflections with I > 2σ(I)

  • R int = 0.021

Refinement

  • R[F 2 > 2σ(F 2)] = 0.023

  • wR(F 2) = 0.058

  • S = 1.05

  • 6004 reflections

  • 163 parameters

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 1.32 e Å−3

  • Δρmin = −0.56 e Å−3

Data collection: APEX2 (Bruker, 2005); cell refinement: SAINT (Bruker, 2005); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 2009).

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809040446/is2467sup1.cif

e-65-o2676-sup1.cif (17.6KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809040446/is2467Isup2.hkl

e-65-o2676-Isup2.hkl (293.9KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
O1W—H1W1⋯I1i 0.94 (3) 2.70 (3) 3.6458 (14) 177 (3)
O1W—H2W1⋯I1ii 0.93 (3) 2.66 (2) 3.5826 (12) 174 (2)
C14—H14A⋯O1Wii 0.96 2.52 3.3775 (19) 149

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Acknowledgments

The authors thank the Malaysian Government and Universiti Sains Malaysia for the Research University Golden Goose grant No. 1001/PFIZIK/811012. KC thanks the Development and Promotion of Science and Technology Talents Project (DPST) for a study grant. The authors also thank the Prince of Songkla University for financial support.

supplementary crystallographic information

Comment

The design and synthesis of nonlinear optical (NLO) materials have been receiving much attention due to their numerous applications (Chemla & Zyss, 1987; Prasad & Williams, 1991). In the search for new organic NLO materials, aromatic compounds with extended π-conjugation system are extensively studied (Chia et al., 1995; Dittrich et al., 2003). Such materials require molecular hyperpolarizability and orientation in a noncentrosymmetric arrangement of the bulk material (Lin et al., 2002; Prasad & Williams, 1991). During the course of our systematic studies of organic NLO materials, we have previously synthesized and reported the crystal structures of pyridinium and quinolinium iodide (Chanawanno et al., 2008; Chantrapromma, Jindawong & Fun, 2007; Chantrapromma, Jindawong, Fun & Patil, 2007). Herein we report the crystal structure of the title pyridinium derivative (I). However (I) crystallizes in centrosymmetric P21/c space group which precludes the second-order nonlinear optical properties.

The title compound consists of a C14H14N+ cation, an I- anion and one water molecule (Fig. 1). The cation exists in an E configuration with respect to the C6═C7 ethenyl bond [1.3429 (18) Å] with the torsion angle of C5–C6–C7–C8 = -179.95 (13)°. The cation is essentially planar with the dihedral angles between the pyridinium [C1–C5/N1] and benzene rings being 2.55 (7)°. The ethenyl unit is co-planar with the pyridinium and benzene rings as indicated by the torsion angles C1–C5–C6–C7 = -1.4 (2)° and C6–C7–C8–C9 = 1.6 (2)°. The rms deviation from the plane through the cation is 0.027 (15) Å. The bond distances in the cation have normal values (Allen et al., 1987) and comparable with the closely related compounds (Chanawanno et al., 2008; Chantrapromma, Jindawong & Fun, 2007; Chantrapromma, Jindawong, Fun & Patil, 2007).

In the crystal packing (Fig. 2), the cations are stacked in an antiparallel manner along the a axis. The cation is linked with the water molecule by a C—H···O weak interaction. The water molecule is further linked with the I- ion by O—H···I hydrogen bonds, forming a 3D network (Table 1). The crystal is consolidated by these interactions and further stabilized by π–π interactions with a distance of Cg1···Cg2iii = 3.6850 (8) Å [symmetry code: (iii) -x, 1-y, 2-z]; Cg1 and Cg2 are the centroids of the C1–C5/N1 and C8–C13 rings, respectively.

Experimental

(E)-1-Methyl-4-styrylpyridinium iodide was prepared by mixing 1:1:1 molar ratio solutions of 1,4-dimethylpyridinium iodide (2 g, 8.5 mmol), benzaldehyde (0.86 ml, 8.5 mmol) and piperidine (0.84 ml, 8.5 mmol) in methanol (40 ml). The resulting solution was refluxed for 3 h under a nitrogen atmosphere. The yellow solid which formed was filtered and washed with diethylether. Yellow block-shaped single crystals of the title compound suitable for x-ray structure determination were recrystallized from methanol by slow evaporation at room temperature over a few weeks (m.p. 489-490 K).

Refinement

Water H atoms were located in a difference map and refined isotropically. The remaining H atoms were positioned geometrically and allowed to ride on their parent atoms, with d(C—H) = 0.93 Å for aromatic and CH and 0.96 Å for CH3 atoms. The Uiso values were constrained to be 1.5Ueq of the carrier atom for methyl H atoms and 1.2Ueq for the remaining H atoms. A rotating group model was used for the methyl groups. The highest residual electron density peak is located at 0.70 Å from I1 and the deepest hole is located at 0.54 Å from I1.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound, with 50% probability displacement ellipsoids and the atom-numbering scheme.

Fig. 2.

Fig. 2.

The crystal packing of the title compound viewed down the c axis. O—H···I hydrogen bonds and C—H···O interactions are shown as dashed lines.

Crystal data

C14H14N+·I·H2O F(000) = 672
Mr = 341.18 Dx = 1.660 Mg m3
Monoclinic, P21/c Melting point = 489–490 K
Hall symbol: -P 2ybc Mo Kα radiation, λ = 0.71073 Å
a = 7.3636 (1) Å Cell parameters from 6004 reflections
b = 10.5929 (1) Å θ = 2.3–35.0°
c = 18.2807 (2) Å µ = 2.33 mm1
β = 106.770 (1)° T = 100 K
V = 1365.29 (3) Å3 Block, yellow
Z = 4 0.32 × 0.22 × 0.20 mm

Data collection

Bruker APEXII CCD area-detector diffractometer 6004 independent reflections
Radiation source: sealed tube 5307 reflections with I > 2σ(I)
graphite Rint = 0.021
φ and ω scans θmax = 35.0°, θmin = 2.3°
Absorption correction: multi-scan (SADABS; Bruker, 2005) h = −11→11
Tmin = 0.524, Tmax = 0.649 k = −17→16
27548 measured reflections l = −29→28

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.023 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.058 H atoms treated by a mixture of independent and constrained refinement
S = 1.05 w = 1/[σ2(Fo2) + (0.0248P)2 + 0.8184P] where P = (Fo2 + 2Fc2)/3
6004 reflections (Δ/σ)max = 0.004
163 parameters Δρmax = 1.32 e Å3
0 restraints Δρmin = −0.56 e Å3

Special details

Experimental. The crystal was placed in the cold stream of an Oxford Cryosystems Cobra open-flow nitrogen cryostat (Cosier & Glazer, 1986) operating at 100.0 (1) K.
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)

x y z Uiso*/Ueq
I1 0.742589 (15) 0.831113 (9) 0.885210 (5) 0.02548 (3)
O1W 0.20711 (19) 0.98174 (12) 0.94686 (7) 0.0308 (2)
H1W1 0.086 (4) 0.944 (3) 0.9327 (16) 0.060 (8)*
H2W1 0.210 (4) 1.028 (2) 0.9901 (15) 0.048 (7)*
N1 0.53960 (16) 0.74866 (11) 1.12888 (6) 0.01776 (19)
C1 0.3622 (2) 0.68934 (13) 1.00380 (8) 0.0219 (2)
H1A 0.3146 0.7096 0.9523 0.026*
C2 0.4699 (2) 0.77624 (13) 1.05393 (8) 0.0218 (2)
H2A 0.4948 0.8546 1.0360 0.026*
C3 0.5064 (2) 0.63509 (12) 1.15607 (7) 0.0185 (2)
H3A 0.5556 0.6174 1.2079 0.022*
C4 0.4006 (2) 0.54563 (12) 1.10806 (7) 0.0187 (2)
H4A 0.3796 0.4676 1.1275 0.022*
C5 0.32393 (19) 0.57076 (12) 1.02979 (7) 0.0176 (2)
C6 0.2111 (2) 0.47325 (12) 0.98062 (7) 0.0191 (2)
H6A 0.1960 0.3967 1.0031 0.023*
C7 0.12773 (19) 0.48617 (12) 0.90531 (7) 0.0188 (2)
H7A 0.1434 0.5629 0.8832 0.023*
C8 0.01415 (19) 0.38969 (12) 0.85514 (7) 0.0175 (2)
C9 −0.0249 (2) 0.27106 (12) 0.88126 (8) 0.0195 (2)
H9A 0.0259 0.2496 0.9324 0.023*
C10 −0.1394 (2) 0.18542 (12) 0.83081 (9) 0.0214 (2)
H10A −0.1634 0.1065 0.8482 0.026*
C11 −0.2182 (2) 0.21752 (13) 0.75423 (8) 0.0214 (2)
H11A −0.2975 0.1609 0.7210 0.026*
C12 −0.1783 (2) 0.33396 (13) 0.72750 (8) 0.0226 (2)
H12A −0.2297 0.3551 0.6763 0.027*
C13 −0.0616 (2) 0.41849 (13) 0.77750 (8) 0.0206 (2)
H13A −0.0331 0.4956 0.7592 0.025*
C14 0.6473 (2) 0.84639 (13) 1.18135 (8) 0.0234 (3)
H14A 0.7349 0.8866 1.1588 0.035*
H14B 0.7160 0.8079 1.2288 0.035*
H14C 0.5611 0.9082 1.1906 0.035*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
I1 0.03493 (6) 0.02076 (4) 0.01682 (4) −0.00883 (3) 0.00120 (3) 0.00305 (3)
O1W 0.0324 (6) 0.0315 (6) 0.0294 (5) 0.0025 (5) 0.0103 (5) −0.0004 (4)
N1 0.0178 (5) 0.0184 (4) 0.0172 (4) −0.0012 (4) 0.0054 (4) −0.0003 (3)
C1 0.0249 (7) 0.0220 (6) 0.0176 (5) −0.0017 (5) 0.0043 (5) 0.0029 (4)
C2 0.0247 (7) 0.0209 (6) 0.0199 (5) −0.0022 (5) 0.0065 (5) 0.0038 (4)
C3 0.0203 (6) 0.0177 (5) 0.0183 (5) 0.0011 (4) 0.0068 (4) 0.0015 (4)
C4 0.0207 (6) 0.0174 (5) 0.0191 (5) 0.0005 (4) 0.0074 (4) 0.0018 (4)
C5 0.0166 (5) 0.0181 (5) 0.0182 (5) 0.0008 (4) 0.0055 (4) 0.0011 (4)
C6 0.0202 (6) 0.0177 (5) 0.0194 (5) 0.0002 (4) 0.0060 (4) 0.0017 (4)
C7 0.0193 (6) 0.0181 (5) 0.0192 (5) 0.0008 (4) 0.0058 (4) 0.0025 (4)
C8 0.0159 (5) 0.0178 (5) 0.0188 (5) 0.0006 (4) 0.0051 (4) 0.0005 (4)
C9 0.0186 (6) 0.0181 (5) 0.0212 (5) 0.0024 (4) 0.0049 (4) 0.0033 (4)
C10 0.0207 (6) 0.0158 (5) 0.0281 (6) 0.0012 (4) 0.0077 (5) 0.0023 (4)
C11 0.0198 (6) 0.0208 (6) 0.0238 (6) −0.0012 (5) 0.0068 (5) −0.0047 (4)
C12 0.0243 (7) 0.0251 (6) 0.0178 (5) −0.0005 (5) 0.0054 (5) 0.0005 (4)
C13 0.0212 (6) 0.0207 (5) 0.0200 (5) −0.0015 (5) 0.0064 (5) 0.0026 (4)
C14 0.0248 (7) 0.0228 (6) 0.0224 (6) −0.0050 (5) 0.0065 (5) −0.0044 (4)

Geometric parameters (Å, °)

O1W—H1W1 0.94 (3) C7—C8 1.4637 (18)
O1W—H2W1 0.93 (3) C7—H7A 0.9300
N1—C2 1.3491 (17) C8—C13 1.4005 (18)
N1—C3 1.3507 (17) C8—C9 1.4032 (19)
N1—C14 1.4772 (18) C9—C10 1.391 (2)
C1—C2 1.377 (2) C9—H9A 0.9300
C1—C5 1.4003 (19) C10—C11 1.394 (2)
C1—H1A 0.9300 C10—H10A 0.9300
C2—H2A 0.9300 C11—C12 1.389 (2)
C3—C4 1.3711 (19) C11—H11A 0.9300
C3—H3A 0.9300 C12—C13 1.387 (2)
C4—C5 1.4039 (18) C12—H12A 0.9300
C4—H4A 0.9300 C13—H13A 0.9300
C5—C6 1.4608 (19) C14—H14A 0.9600
C6—C7 1.3429 (18) C14—H14B 0.9600
C6—H6A 0.9300 C14—H14C 0.9600
H1W1—O1W—H2W1 104 (2) C13—C8—C9 118.63 (12)
C2—N1—C3 120.69 (12) C13—C8—C7 118.12 (12)
C2—N1—C14 118.90 (12) C9—C8—C7 123.24 (11)
C3—N1—C14 120.37 (11) C10—C9—C8 120.19 (12)
C2—C1—C5 120.49 (12) C10—C9—H9A 119.9
C2—C1—H1A 119.8 C8—C9—H9A 119.9
C5—C1—H1A 119.8 C9—C10—C11 120.24 (12)
N1—C2—C1 120.55 (12) C9—C10—H10A 119.9
N1—C2—H2A 119.7 C11—C10—H10A 119.9
C1—C2—H2A 119.7 C12—C11—C10 120.06 (13)
N1—C3—C4 120.65 (12) C12—C11—H11A 120.0
N1—C3—H3A 119.7 C10—C11—H11A 120.0
C4—C3—H3A 119.7 C13—C12—C11 119.69 (13)
C3—C4—C5 120.56 (12) C13—C12—H12A 120.2
C3—C4—H4A 119.7 C11—C12—H12A 120.2
C5—C4—H4A 119.7 C12—C13—C8 121.14 (12)
C1—C5—C4 117.05 (12) C12—C13—H13A 119.4
C1—C5—C6 124.05 (12) C8—C13—H13A 119.4
C4—C5—C6 118.90 (12) N1—C14—H14A 109.5
C7—C6—C5 124.71 (12) N1—C14—H14B 109.5
C7—C6—H6A 117.6 H14A—C14—H14B 109.5
C5—C6—H6A 117.6 N1—C14—H14C 109.5
C6—C7—C8 125.51 (12) H14A—C14—H14C 109.5
C6—C7—H7A 117.2 H14B—C14—H14C 109.5
C8—C7—H7A 117.2
C3—N1—C2—C1 0.5 (2) C5—C6—C7—C8 −179.95 (13)
C14—N1—C2—C1 −177.34 (14) C6—C7—C8—C13 −179.47 (14)
C5—C1—C2—N1 −0.2 (2) C6—C7—C8—C9 1.6 (2)
C2—N1—C3—C4 −0.2 (2) C13—C8—C9—C10 −1.1 (2)
C14—N1—C3—C4 177.64 (13) C7—C8—C9—C10 177.78 (13)
N1—C3—C4—C5 −0.4 (2) C8—C9—C10—C11 −0.9 (2)
C2—C1—C5—C4 −0.3 (2) C9—C10—C11—C12 1.8 (2)
C2—C1—C5—C6 179.97 (14) C10—C11—C12—C13 −0.7 (2)
C3—C4—C5—C1 0.7 (2) C11—C12—C13—C8 −1.3 (2)
C3—C4—C5—C6 −179.63 (13) C9—C8—C13—C12 2.2 (2)
C1—C5—C6—C7 −1.4 (2) C7—C8—C13—C12 −176.72 (13)
C4—C5—C6—C7 178.88 (14)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O1W—H1W1···I1i 0.94 (3) 2.70 (3) 3.6458 (14) 177 (3)
O1W—H2W1···I1ii 0.93 (3) 2.66 (2) 3.5826 (12) 174 (2)
C14—H14A···O1Wii 0.96 2.52 3.3775 (19) 149

Symmetry codes: (i) x−1, y, z; (ii) −x+1, −y+2, −z+2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: IS2467).

References

  1. Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1–19.
  2. Bruker (2005). APEX2, SAINT and SADABS Bruker AXS Inc., Madison, Wisconsin, USA.
  3. Chanawanno, K., Chantrapromma, S. & Fun, H.-K. (2008). Acta Cryst. E64, o1882–o1883. [DOI] [PMC free article] [PubMed]
  4. Chantrapromma, S., Jindawong, B. & Fun, H.-K. (2007). Acta Cryst. E63, o2020–o2022.
  5. Chantrapromma, S., Jindawong, B., Fun, H.-K. & Patil, P. S. (2007). Acta Cryst E63, o2321–o2323.
  6. Chemla, D. S. & Zyss, J. (1987). Nonlinear Optical Properties of Organic Molecules and Crystals, pp. 32–198. New York: Academic Press.
  7. Chia, W.-L., Chen, C.-N. & Sheu, H.-J. (1995). Mater. Res. Bull.30, 1421–1430.
  8. Cosier, J. & Glazer, A. M. (1986). J. Appl. Cryst.19, 105–107.
  9. Dittrich, Ph., Bartlome, R., Montemezzani, G. & Günter, P. (2003). Appl. Surf. Sci.220, 88–95.
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  11. Prasad, P. N. & Williams, D. J. (1991). Introduction to Nonlinear Optical Effects in Molecules and Polymers New York: John Wiley.
  12. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  13. Spek, A. L. (2009). Acta Cryst D65, 148–155. [DOI] [PMC free article] [PubMed]

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809040446/is2467sup1.cif

e-65-o2676-sup1.cif (17.6KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809040446/is2467Isup2.hkl

e-65-o2676-Isup2.hkl (293.9KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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