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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Jun 18;67(Pt 7):o1701. doi: 10.1107/S1600536811022094

1-Carb­oxy­methyl-3-octylimidazolium bromide

Nassir N Al-Mohammed a, Yatimah Alias a, Zanariah Abdullah a, Hamid Khaledi a,*
PMCID: PMC3152140  PMID: 21837097

Abstract

In the title compound, C13H23N2O2 +·Br, the octyl chain has an all-trans conformation. In the crystal, the cations are linked by C—H⋯O bonds into a zigzag chain along the b axis. The bromide anions further link the chains via C—H⋯Br inter­actions into a two-dimensional array parallel to the ab plane. An O—H⋯Br interaction is also observed.

Related literature

For related structures, see: Wei et al. (2009); Chen et al. (2009).graphic file with name e-67-o1701-scheme1.jpg

Experimental

Crystal data

  • C13H23N2O2+·Br

  • M r = 319.24

  • Monoclinic, Inline graphic

  • a = 7.6745 (2) Å

  • b = 4.6176 (1) Å

  • c = 41.8663 (9) Å

  • β = 92.167 (1)°

  • V = 1482.59 (6) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 2.77 mm−1

  • T = 100 K

  • 0.21 × 0.19 × 0.06 mm

Data collection

  • Bruker APEXII CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996) T min = 0.594, T max = 0.851

  • 10905 measured reflections

  • 2761 independent reflections

  • 2678 reflections with I > 2σ(I)

  • R int = 0.023

Refinement

  • R[F 2 > 2σ(F 2)] = 0.049

  • wR(F 2) = 0.095

  • S = 1.43

  • 2761 reflections

  • 167 parameters

  • 1 restraint

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

  • Δρmax = 1.25 e Å−3

  • Δρmin = −2.19 e Å−3

Data collection: APEX2 (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: X-SEED (Barbour, 2001); software used to prepare material for publication: SHELXL97 and publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) I, New_Global_Publ_Block. DOI: 10.1107/S1600536811022094/is2721sup1.cif

e-67-o1701-sup1.cif (16.8KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811022094/is2721Isup2.hkl

e-67-o1701-Isup2.hkl (135.6KB, 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
C6—H6B⋯Br1i 0.99 2.89 3.772 (4) 148
C5—H5⋯Br1ii 0.95 2.91 3.681 (4) 139
C4—H4⋯O2iii 0.95 2.25 3.151 (5) 158
C3—H3⋯Br1i 0.95 2.82 3.593 (4) 139
C2—H2B⋯Br1iv 0.99 2.90 3.676 (4) 136
C2—H2A⋯O2v 0.99 2.44 3.328 (5) 150
O1—H1⋯Br1 0.84 (2) 2.33 (2) 3.153 (3) 168 (4)

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic; (iv) Inline graphic; (v) Inline graphic.

Acknowledgments

The authors thank the University of Malaya for funding this study (FRGS grant No. FP001/2010 A).

supplementary crystallographic information

Comment

The imidazolium ring is N-bound to a long alkyl chain, namely an octyl chain, and a carboxymethyl group. The alkyl chain adopts an all-trans conformation, as observed in similar structures (Wei et al., 2009; Chen et al., 2009). The carboxy group and the imidazolium ring subtend an N1—C2—C1 angle of 110.7 (3)°. In the crystal, the cationic moieties are bonded via C—H···O interactions (Table 1) into infinite chains along the b axis. The bromide anions link the cationic chains through C—H···Br interactions into layers parallel to the ab plane (Fig. 2).

Experimental

A solution of bromoacetic acid (1 g, 7.2 mmol) and octylimidazole (1.29 g, 7.2 mmol) in dry 1,4-dioxane (10 ml) was stirred under nitrogen atmosphere at 70 °C for 7 hr. The solution was then poured into dichloromethane (25 ml) and extracted with distilled water (50 ml). The aqueous solution was evaporated under vacuum to give a viscous oil which crystallized from THF to yield the colorless crystals of the title compound.

Refinement

The C-bound H atoms were placed at calculated positions [C—H distances of 0.95 (Ar), 0.98 (methyl) and 0.99 (methylene) Å] and refined as riding atoms, with Uiso(H) set to 1.2(1.5 for methyl)Ueq(C). The carboxylic hydrogen atom was located in a difference Fourier map and refind with a dinstance restraint of O—H 0.84 (2) Å. The maximum and minimum residual electron density peaks of 1.25 and -2.19 e Å-3, respectively, were located 2.06 and 1.85 Å from atom Br1.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound with displacement ellipsoids drawn at 50% probability level. Hydrogen atoms are drawn as spheres of arbitrary radius.

Fig. 2.

Fig. 2.

Packing view looking down the crystallographic b axis.

Crystal data

C13H23N2O2+·Br F(000) = 664
Mr = 319.24 Dx = 1.430 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 9093 reflections
a = 7.6745 (2) Å θ = 2.7–30.4°
b = 4.6176 (1) Å µ = 2.77 mm1
c = 41.8663 (9) Å T = 100 K
β = 92.167 (1)° Plate, colorless
V = 1482.59 (6) Å3 0.21 × 0.19 × 0.06 mm
Z = 4

Data collection

Bruker APEXII CCD diffractometer 2761 independent reflections
Radiation source: fine-focus sealed tube 2678 reflections with I > 2σ(I)
graphite Rint = 0.023
φ and ω scans θmax = 25.5°, θmin = 2.7°
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) h = −9→9
Tmin = 0.594, Tmax = 0.851 k = −5→5
10905 measured reflections l = −50→50

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)] = 0.049 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.095 H atoms treated by a mixture of independent and constrained refinement
S = 1.43 w = 1/[σ2(Fo2) + (0.P)2 + 5.6415P] where P = (Fo2 + 2Fc2)/3
2761 reflections (Δ/σ)max < 0.001
167 parameters Δρmax = 1.25 e Å3
1 restraint Δρmin = −2.19 e Å3

Special details

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)

x y z Uiso*/Ueq
Br1 0.10811 (5) 0.60448 (9) 0.158623 (9) 0.01633 (12)
O1 0.1327 (4) 0.9207 (7) 0.22540 (7) 0.0206 (6)
H1 0.140 (6) 0.823 (9) 0.2087 (7) 0.025*
O2 0.3056 (4) 0.5633 (7) 0.24528 (7) 0.0223 (7)
N1 0.3042 (4) 0.7879 (7) 0.30550 (7) 0.0135 (7)
N2 0.3636 (4) 0.4977 (8) 0.34476 (7) 0.0141 (7)
C1 0.2224 (5) 0.7809 (9) 0.24846 (9) 0.0145 (8)
C2 0.2071 (6) 0.9390 (9) 0.27999 (9) 0.0179 (9)
H2A 0.2530 1.1383 0.2780 0.021*
H2B 0.0829 0.9524 0.2853 0.021*
C3 0.2346 (5) 0.6121 (9) 0.32676 (9) 0.0144 (8)
H3 0.1137 0.5747 0.3287 0.017*
C4 0.4832 (5) 0.7869 (10) 0.31017 (10) 0.0191 (9)
H4 0.5648 0.8927 0.2983 0.023*
C5 0.5201 (5) 0.6074 (10) 0.33479 (9) 0.0191 (9)
H5 0.6328 0.5640 0.3437 0.023*
C6 0.3422 (5) 0.3118 (9) 0.37260 (9) 0.0168 (9)
H6A 0.4475 0.1900 0.3759 0.020*
H6B 0.2413 0.1816 0.3686 0.020*
C7 0.3137 (5) 0.4881 (9) 0.40246 (9) 0.0163 (8)
H7A 0.2055 0.6032 0.3994 0.020*
H7B 0.4120 0.6248 0.4059 0.020*
C8 0.2994 (5) 0.2982 (9) 0.43200 (9) 0.0172 (8)
H8A 0.4069 0.1809 0.4348 0.021*
H8B 0.2002 0.1632 0.4286 0.021*
C9 0.2731 (5) 0.4719 (9) 0.46238 (9) 0.0158 (8)
H9A 0.3717 0.6083 0.4656 0.019*
H9B 0.1651 0.5879 0.4596 0.019*
C10 0.2602 (6) 0.2852 (10) 0.49212 (10) 0.0195 (9)
H10A 0.3684 0.1697 0.4949 0.023*
H10B 0.1618 0.1484 0.4889 0.023*
C11 0.2332 (5) 0.4592 (9) 0.52259 (9) 0.0162 (9)
H11A 0.3315 0.5965 0.5258 0.019*
H11B 0.1250 0.5744 0.5198 0.019*
C12 0.2207 (6) 0.2733 (10) 0.55249 (9) 0.0196 (9)
H12A 0.3290 0.1586 0.5554 0.023*
H12B 0.1225 0.1359 0.5494 0.023*
C13 0.1934 (6) 0.4506 (10) 0.58268 (9) 0.0215 (10)
H13A 0.2926 0.5814 0.5864 0.032*
H13B 0.1840 0.3199 0.6010 0.032*
H13C 0.0860 0.5643 0.5800 0.032*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Br1 0.0160 (2) 0.0183 (2) 0.01477 (19) 0.00006 (18) 0.00112 (13) −0.00132 (18)
O1 0.0278 (15) 0.0187 (17) 0.0153 (14) 0.0039 (14) 0.0000 (12) 0.0001 (13)
O2 0.0315 (16) 0.0190 (18) 0.0164 (14) 0.0086 (14) 0.0024 (12) −0.0021 (13)
N1 0.0177 (16) 0.0132 (17) 0.0098 (15) −0.0009 (14) 0.0026 (13) −0.0002 (13)
N2 0.0145 (16) 0.0162 (17) 0.0118 (16) −0.0005 (14) 0.0018 (13) 0.0000 (13)
C1 0.0155 (19) 0.015 (2) 0.0131 (19) −0.0032 (17) 0.0029 (15) 0.0017 (16)
C2 0.027 (2) 0.010 (2) 0.0162 (19) 0.0048 (18) 0.0005 (16) 0.0010 (16)
C3 0.0160 (18) 0.0128 (19) 0.0144 (18) −0.0016 (17) 0.0004 (14) −0.0021 (17)
C4 0.0145 (19) 0.025 (2) 0.018 (2) −0.0043 (18) 0.0032 (16) −0.0028 (18)
C5 0.0131 (18) 0.026 (2) 0.018 (2) 0.0021 (19) 0.0008 (15) −0.0008 (19)
C6 0.021 (2) 0.010 (2) 0.019 (2) −0.0004 (17) −0.0022 (16) 0.0039 (16)
C7 0.0177 (19) 0.016 (2) 0.0150 (19) 0.0011 (17) 0.0002 (15) 0.0010 (16)
C8 0.0175 (19) 0.015 (2) 0.019 (2) 0.0016 (17) 0.0007 (16) 0.0014 (17)
C9 0.0159 (19) 0.015 (2) 0.0166 (19) 0.0021 (16) −0.0006 (15) 0.0014 (16)
C10 0.020 (2) 0.020 (2) 0.019 (2) 0.0037 (18) 0.0011 (16) −0.0003 (18)
C11 0.0158 (19) 0.014 (2) 0.019 (2) 0.0012 (16) 0.0013 (16) 0.0010 (17)
C12 0.021 (2) 0.021 (2) 0.017 (2) 0.0009 (18) 0.0031 (16) 0.0011 (18)
C13 0.025 (2) 0.024 (3) 0.016 (2) 0.0012 (19) 0.0033 (16) −0.0001 (18)

Geometric parameters (Å, °)

O1—C1 1.332 (5) C7—H7A 0.9900
O1—H1 0.837 (19) C7—H7B 0.9900
O2—C1 1.200 (5) C8—C9 1.524 (5)
N1—C3 1.331 (5) C8—H8A 0.9900
N1—C4 1.381 (5) C8—H8B 0.9900
N1—C2 1.457 (5) C9—C10 1.521 (6)
N2—C3 1.331 (5) C9—H9A 0.9900
N2—C5 1.382 (5) C9—H9B 0.9900
N2—C6 1.462 (5) C10—C11 1.528 (6)
C1—C2 1.517 (5) C10—H10A 0.9900
C2—H2A 0.9900 C10—H10B 0.9900
C2—H2B 0.9900 C11—C12 1.524 (6)
C3—H3 0.9500 C11—H11A 0.9900
C4—C5 1.344 (6) C11—H11B 0.9900
C4—H4 0.9500 C12—C13 1.527 (6)
C5—H5 0.9500 C12—H12A 0.9900
C6—C7 1.515 (6) C12—H12B 0.9900
C6—H6A 0.9900 C13—H13A 0.9800
C6—H6B 0.9900 C13—H13B 0.9800
C7—C8 1.523 (5) C13—H13C 0.9800
C1—O1—H1 107 (3) C7—C8—C9 113.0 (3)
C3—N1—C4 109.0 (3) C7—C8—H8A 109.0
C3—N1—C2 125.1 (3) C9—C8—H8A 109.0
C4—N1—C2 125.7 (3) C7—C8—H8B 109.0
C3—N2—C5 108.6 (3) C9—C8—H8B 109.0
C3—N2—C6 125.5 (3) H8A—C8—H8B 107.8
C5—N2—C6 125.5 (3) C10—C9—C8 113.6 (3)
O2—C1—O1 126.0 (4) C10—C9—H9A 108.9
O2—C1—C2 123.9 (4) C8—C9—H9A 108.9
O1—C1—C2 110.0 (3) C10—C9—H9B 108.9
N1—C2—C1 110.7 (3) C8—C9—H9B 108.9
N1—C2—H2A 109.5 H9A—C9—H9B 107.7
C1—C2—H2A 109.5 C9—C10—C11 113.6 (4)
N1—C2—H2B 109.5 C9—C10—H10A 108.8
C1—C2—H2B 109.5 C11—C10—H10A 108.8
H2A—C2—H2B 108.1 C9—C10—H10B 108.8
N2—C3—N1 108.2 (3) C11—C10—H10B 108.8
N2—C3—H3 125.9 H10A—C10—H10B 107.7
N1—C3—H3 125.9 C12—C11—C10 113.9 (3)
C5—C4—N1 106.9 (4) C12—C11—H11A 108.8
C5—C4—H4 126.6 C10—C11—H11A 108.8
N1—C4—H4 126.6 C12—C11—H11B 108.8
C4—C5—N2 107.3 (3) C10—C11—H11B 108.8
C4—C5—H5 126.3 H11A—C11—H11B 107.7
N2—C5—H5 126.3 C11—C12—C13 113.1 (4)
N2—C6—C7 111.5 (3) C11—C12—H12A 109.0
N2—C6—H6A 109.3 C13—C12—H12A 109.0
C7—C6—H6A 109.3 C11—C12—H12B 109.0
N2—C6—H6B 109.3 C13—C12—H12B 109.0
C7—C6—H6B 109.3 H12A—C12—H12B 107.8
H6A—C6—H6B 108.0 C12—C13—H13A 109.5
C6—C7—C8 112.2 (3) C12—C13—H13B 109.5
C6—C7—H7A 109.2 H13A—C13—H13B 109.5
C8—C7—H7A 109.2 C12—C13—H13C 109.5
C6—C7—H7B 109.2 H13A—C13—H13C 109.5
C8—C7—H7B 109.2 H13B—C13—H13C 109.5
H7A—C7—H7B 107.9

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C6—H6B···Br1i 0.99 2.89 3.772 (4) 148
C5—H5···Br1ii 0.95 2.91 3.681 (4) 139
C4—H4···O2iii 0.95 2.25 3.151 (5) 158
C3—H3···Br1i 0.95 2.82 3.593 (4) 139
C2—H2B···Br1iv 0.99 2.90 3.676 (4) 136
C2—H2A···O2v 0.99 2.44 3.328 (5) 150
O1—H1···Br1 0.84 (2) 2.33 (2) 3.153 (3) 168 (4)

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: IS2721).

References

  1. Barbour, L. J. (2001). J. Supramol. Chem 1, 189–191.
  2. Bruker (2007). APEX2 and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  3. Chen, Y., Song, W., Xu, J., Yang, X.-R. & Tian, D.-B. (2009). Acta Cryst. E65, o2617. [DOI] [PMC free article] [PubMed]
  4. Sheldrick, G. M. (1996). SADABS University of Göttingen, Germany.
  5. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  6. Wei, Z., Wei, X., Fu, S., Liu, J. & Zhang, D. (2009). Acta Cryst. E65, o1159. [DOI] [PMC free article] [PubMed]
  7. Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.

Associated Data

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

Supplementary Materials

Crystal structure: contains datablock(s) I, New_Global_Publ_Block. DOI: 10.1107/S1600536811022094/is2721sup1.cif

e-67-o1701-sup1.cif (16.8KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811022094/is2721Isup2.hkl

e-67-o1701-Isup2.hkl (135.6KB, hkl)

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


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