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

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1,1′,2,2′-Tetra­methyl-3,3′-(p-phenyl­enedi­methyl­ene)diimidazol-1-ium dibromide

aDepartment of Chemistry, University of Malaya, 50603 Kuala Lumpur, Malaysia
*Correspondence e-mail: seikweng@um.edu.my

(Received 4 July 2009; accepted 6 July 2009; online 11 July 2009)

The title imidazolium-based ionic-liquid salt, C18H24N42+·2Br, has the cation lying about a center of inversion. The five-membered imidazole ring is disordered over two positions with the major component having a site occupancy of 0.712 (4); the N-bound methyl substituents are ordered. The imidazole ring is approximately perpendicular to the six-membered phenyl­ene ring [dihedral angle = 80.7 (5)° for the major disorder component and 89.8 (3)° for the other; the two components are off-set by 10.1 (6)°].

Related literature

For background to imidazolium-based ionic liquid salts, see: Ganesan et al. (2008[Ganesan, K., Alias, Y. & Ng, S. W. (2008). Acta Cryst. C64, o478-o480.]). For 2,2′-dimethyl-3,3′-(p-phenyl­enedimethyl­ene)diimidazol-1-ium dibromide, see: Dobrzańska (2005[Dobrzańska, L. (2005). Acta Cryst. E61, o4113-o4115.]).

[Scheme 1]

Experimental

Crystal data
  • C18H24N42+·2Br

  • Mr = 456.23

  • Monoclinic, P 21 /n

  • a = 8.5689 (4) Å

  • b = 9.8617 (5) Å

  • c = 11.0272 (4) Å

  • β = 93.222 (3)°

  • V = 930.37 (7) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 4.36 mm−1

  • T = 140 K

  • 0.40 × 0.08 × 0.04 mm

Data collection
  • Bruker SMART APEX diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996[Sheldrick, G. M. (1996). SADABS. University of Göttingen, Germany.]) Tmin = 0.274, Tmax = 0.845

  • 5882 measured reflections

  • 2131 independent reflections

  • 1575 reflections with I > 2σ(I)

  • Rint = 0.051

Refinement
  • R[F2 > 2σ(F2)] = 0.039

  • wR(F2) = 0.096

  • S = 1.04

  • 2131 reflections

  • 112 parameters

  • 36 restraints

  • H-atom parameters constrained

  • Δρmax = 0.54 e Å−3

  • Δρmin = −0.99 e Å−3

Data collection: APEX2 (Bruker, 2008[Bruker (2008). APEX2 and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.]); cell refinement: SAINT (Bruker, 2008[Bruker (2008). APEX2 and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.]); data reduction: SAINT; 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: X-SEED (Barbour, 2001[Barbour, L. J. (2001). J. Supramol. Chem. 1, 189-191.]); software used to prepare material for publication: publCIF (Westrip, 2009[Westrip, S. P. (2009). publCIF. In preparation.]).

Supporting information


Related literature top

For background to imidazolium-based ionic liquid salts, see: Ganesan et al. (2008). For 2,2'-dimethyl-3,3'-(p-phenylenedimethylene)diimidazol-1-ium dibromide, see: Dobrzańska (2005).

Experimental top

α,α-Dibromo-p-xylene (0.78 g, 3 mmol) and 1,2-dimethylimidazole (0.58 g, 6 mmol) were refluxed in DMF (50 ml) for 3 h. The product that separated from solution was collected and washed with ether. Crystals were grown from its solution in water.

Refinement top

The imidazolyl ring is disordered over two positions (the two N-bound methyl groups are ordered); the major component had a site occupancy = 0.712 (4). The ring was refined as a regular pentagon of 1.35 Å sides. The anisotropic displacement parameters of the primed atoms were restrained to those of the unprimed ones; these were further restrained to be nearly isotropic.

Carbon-bound H-atoms were placed in calculated positions (C—H 0.95 to 0.99 Å) and were included in the refinement in the riding model approximation, with U(H) set to 1.2 to 1.5Ueq(C).

Computing details top

Data collection: APEX2 (Bruker, 2008); cell refinement: SAINT (Bruker, 2008); data reduction: SAINT (Bruker, 2008); 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: publCIF (Westrip, 2009).

Figures top
[Figure 1] Fig. 1. Thermal ellipsoid plot (Barbour, 2001) of [C18H24N4]2+ 2Br- at the 70% probability level; hydrogen atoms are drawn as spheres of arbitrary radius. The imidazolyl ring is disordered; the minor component of the disorder is not shown. The non-H atoms comprising the asymmetric unit are labelled and the unlabelled atoms are related by 1-x, -y, -z.
1,1',2,2'-Tetramethyl-3,3'-(p-phenylenedimethylene)diimidazol-1-ium dibromide top
Crystal data top
C18H24N42+·2BrF(000) = 460
Mr = 456.23Dx = 1.629 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 1543 reflections
a = 8.5689 (4) Åθ = 2.8–25.5°
b = 9.8617 (5) ŵ = 4.36 mm1
c = 11.0272 (4) ÅT = 140 K
β = 93.222 (3)°Prism, colorless
V = 930.37 (7) Å30.40 × 0.08 × 0.04 mm
Z = 2
Data collection top
Bruker SMART APEX
diffractometer
2131 independent reflections
Radiation source: fine-focus sealed tube1575 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.051
ω scansθmax = 27.5°, θmin = 2.8°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 1110
Tmin = 0.274, Tmax = 0.845k = 1212
5882 measured reflectionsl = 1414
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.039Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.096H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0403P)2 + 0.5004P]
where P = (Fo2 + 2Fc2)/3
2131 reflections(Δ/σ)max = 0.001
112 parametersΔρmax = 0.54 e Å3
36 restraintsΔρmin = 0.99 e Å3
Crystal data top
C18H24N42+·2BrV = 930.37 (7) Å3
Mr = 456.23Z = 2
Monoclinic, P21/nMo Kα radiation
a = 8.5689 (4) ŵ = 4.36 mm1
b = 9.8617 (5) ÅT = 140 K
c = 11.0272 (4) Å0.40 × 0.08 × 0.04 mm
β = 93.222 (3)°
Data collection top
Bruker SMART APEX
diffractometer
2131 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
1575 reflections with I > 2σ(I)
Tmin = 0.274, Tmax = 0.845Rint = 0.051
5882 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.03936 restraints
wR(F2) = 0.096H-atom parameters constrained
S = 1.04Δρmax = 0.54 e Å3
2131 reflectionsΔρmin = 0.99 e Å3
112 parameters
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Br10.46792 (4)0.59691 (4)0.76873 (3)0.02742 (14)
C10.6432 (4)0.0488 (4)0.4669 (3)0.0194 (7)
H10.74140.08230.44450.023*
C20.6148 (4)0.0331 (3)0.5895 (3)0.0194 (7)
H20.69360.05580.65010.023*
C30.4712 (4)0.0158 (3)0.6230 (3)0.0188 (7)
C40.4343 (4)0.0353 (4)0.7539 (3)0.0201 (7)
H4A0.32040.02460.76150.024*0.712 (4)
H4B0.46310.12870.77940.024*0.712 (4)
H4C0.40030.13030.76490.024*0.288 (4)
H4D0.34520.02410.77140.024*0.288 (4)
N10.5158 (3)0.0594 (3)0.8328 (3)0.0199 (10)0.712 (4)
C50.4760 (4)0.1910 (3)0.8444 (3)0.0259 (11)0.712 (4)
H50.38620.23360.80720.031*0.712 (4)
C60.5862 (4)0.2513 (2)0.9182 (3)0.0270 (13)0.712 (4)
H60.58750.34390.94210.032*0.712 (4)
N20.6941 (3)0.1570 (3)0.9523 (3)0.0207 (9)0.712 (4)
C70.6507 (4)0.0384 (2)0.8994 (3)0.0203 (11)0.712 (4)
C80.7408 (7)0.0908 (5)0.9105 (5)0.0256 (12)0.712 (4)
H8A0.82620.08890.85490.038*0.712 (4)
H8B0.67140.16730.88960.038*0.712 (4)
H8C0.78420.10120.99410.038*0.712 (4)
N1'0.5677 (9)0.0057 (8)0.8456 (6)0.0199 (10)0.288
C5'0.6581 (11)0.1058 (6)0.8950 (8)0.0259 (11)0.288
H5'0.64800.19980.87750.031*0.288 (4)
C6'0.7654 (9)0.0488 (8)0.9736 (8)0.0270 (13)0.288
H6'0.84400.09561.02110.032*0.288 (4)
N2'0.7413 (9)0.0865 (7)0.9728 (7)0.0207 (9)0.288
C7'0.6192 (10)0.1132 (6)0.8937 (7)0.0203 (11)0.288
C8'0.5509 (19)0.2515 (14)0.8644 (14)0.0256 (12)0.288
H8'10.54730.30480.93920.038*0.288 (4)
H8'20.44480.24120.82750.038*0.288 (4)
H8'30.61620.29830.80740.038*0.288 (4)
C90.8342 (5)0.1840 (4)1.0313 (3)0.0293 (9)
H9A0.82780.27551.06540.044*0.712 (4)
H9B0.92720.17700.98400.044*0.712 (4)
H9C0.84100.11751.09750.044*0.712 (4)
H9D0.77980.27151.02790.044*0.288 (4)
H9E0.93300.19190.99120.044*0.288 (4)
H9F0.85550.15771.11640.044*0.288 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.0221 (2)0.0266 (2)0.0336 (2)0.00039 (17)0.00258 (14)0.00512 (16)
C10.0122 (19)0.0253 (17)0.0208 (17)0.0017 (14)0.0021 (13)0.0009 (13)
C20.016 (2)0.0235 (18)0.0183 (17)0.0002 (14)0.0025 (13)0.0002 (13)
C30.019 (2)0.0188 (17)0.0192 (17)0.0022 (14)0.0025 (13)0.0007 (13)
C40.013 (2)0.0275 (18)0.0194 (17)0.0009 (14)0.0008 (13)0.0010 (13)
N10.018 (2)0.025 (2)0.0168 (18)0.0023 (17)0.0016 (16)0.0014 (17)
C50.025 (3)0.030 (3)0.022 (2)0.008 (2)0.000 (2)0.000 (2)
C60.027 (3)0.026 (3)0.028 (3)0.006 (2)0.000 (2)0.002 (2)
N20.020 (3)0.025 (2)0.0164 (19)0.0032 (18)0.0019 (16)0.0007 (17)
C70.018 (3)0.023 (3)0.021 (2)0.000 (2)0.0055 (18)0.005 (2)
C80.021 (3)0.021 (2)0.034 (3)0.009 (2)0.000 (2)0.012 (2)
N1'0.018 (2)0.025 (2)0.0168 (18)0.0023 (17)0.0016 (16)0.0014 (17)
C5'0.025 (3)0.030 (3)0.022 (2)0.008 (2)0.000 (2)0.000 (2)
C6'0.027 (3)0.026 (3)0.028 (3)0.006 (2)0.000 (2)0.002 (2)
N2'0.020 (3)0.025 (2)0.0164 (19)0.0032 (18)0.0019 (16)0.0007 (17)
C7'0.018 (3)0.023 (3)0.021 (2)0.000 (2)0.0055 (18)0.005 (2)
C8'0.021 (3)0.021 (2)0.034 (3)0.009 (2)0.000 (2)0.012 (2)
C90.025 (2)0.034 (2)0.027 (2)0.0067 (17)0.0061 (16)0.0026 (16)
Geometric parameters (Å, º) top
C1—C3i1.392 (5)C8—H8A0.9800
C1—C21.396 (4)C8—H8B0.9800
C1—H10.9500C8—H8C0.9800
C2—C31.391 (5)N1'—C5'1.3500
C2—H20.9500N1'—C7'1.3500
C3—C1i1.392 (5)C5'—C6'1.3500
C3—C41.507 (4)C5'—H5'0.9500
C4—N11.432 (4)C6'—N2'1.3500
C4—N1'1.512 (7)C6'—H6'0.9500
C4—H4A0.9900N2'—C7'1.3500
C4—H4B0.9900N2'—C91.384 (7)
C4—H4C0.9900C7'—C8'1.513 (15)
C4—H4D0.9900C8'—H8'10.9800
N1—C51.3500C8'—H8'20.9800
N1—C71.3500C8'—H8'30.9800
C5—C61.3500C9—H9A0.9800
C5—H50.9500C9—H9B0.9800
C6—N21.3500C9—H9C0.9800
C6—H60.9500C9—H9D0.9800
N2—C71.3500C9—H9E0.9800
N2—C91.468 (4)C9—H9F0.9800
C7—C81.492 (5)
C3i—C1—C2120.6 (3)N2—C7—C8125.2 (3)
C3i—C1—H1119.7N1—C7—C8126.8 (3)
C2—C1—H1119.7C5'—N1'—C7'108.0
C3—C2—C1120.1 (3)C5'—N1'—C4121.6 (6)
C3—C2—H2120.0C7'—N1'—C4130.4 (6)
C1—C2—H2120.0C6'—C5'—N1'108.0
C2—C3—C1i119.3 (3)C6'—C5'—H5'126.0
C2—C3—C4122.4 (3)N1'—C5'—H5'126.0
C1i—C3—C4118.3 (3)C5'—C6'—N2'108.0
N1—C4—C3112.1 (3)C5'—C6'—H6'126.0
C3—C4—N1'115.1 (4)N2'—C6'—H6'126.0
N1—C4—H4A109.2C7'—N2'—C6'108.0
C3—C4—H4A109.2C7'—N2'—C9124.8 (6)
N1'—C4—H4A129.4C6'—N2'—C9126.8 (6)
N1—C4—H4B109.2N2'—C7'—N1'108.0
C3—C4—H4B109.2N2'—C7'—C8'126.2 (8)
H4A—C4—H4B107.9N1'—C7'—C8'125.8 (8)
C3—C4—H4C108.5C7'—C8'—H8'1109.5
N1'—C4—H4C108.5C7'—C8'—H8'2109.5
C3—C4—H4D108.5H8'1—C8'—H8'2109.5
N1'—C4—H4D108.5C7'—C8'—H8'3109.5
H4C—C4—H4D107.5H8'1—C8'—H8'3109.5
C5—N1—C7108.0H8'2—C8'—H8'3109.5
C5—N1—C4124.6 (3)N2—C9—H9A109.5
C7—N1—C4127.2 (3)N2—C9—H9B109.5
N1—C5—C6108.0H9A—C9—H9B109.5
N1—C5—H5126.0N2—C9—H9C109.5
C6—C5—H5126.0H9A—C9—H9C109.5
N2—C6—C5108.0H9B—C9—H9C109.5
N2—C6—H6126.0N2'—C9—H9D109.5
C5—C6—H6126.0N2'—C9—H9E109.5
C6—N2—C7108.0H9D—C9—H9E109.5
C6—N2—C9124.4 (3)N2'—C9—H9F109.5
C7—N2—C9127.6 (3)H9D—C9—H9F109.5
N2—C7—N1108.0H9E—C9—H9F109.5
C3i—C1—C2—C30.1 (6)C4—N1—C7—C83.3 (5)
C1—C2—C3—C1i0.1 (6)N1—C4—N1'—C5'170.1 (11)
C1—C2—C3—C4179.8 (3)C3—C4—N1'—C5'98.3 (6)
C2—C3—C4—N130.3 (5)N1—C4—N1'—C7'9.2 (5)
C1i—C3—C4—N1150.0 (3)C3—C4—N1'—C7'82.4 (8)
C2—C3—C4—N1'3.4 (6)C7'—N1'—C5'—C6'0.0
C1i—C3—C4—N1'176.3 (4)C4—N1'—C5'—C6'179.5 (8)
C3—C4—N1—C576.5 (4)N1'—C5'—C6'—N2'0.0
N1'—C4—N1—C5178.8 (8)C5'—C6'—N2'—C7'0.0
C3—C4—N1—C797.3 (3)C5'—C6'—N2'—C9173.4 (8)
N1'—C4—N1—C74.9 (7)C6'—N2'—C7'—N1'0.0
C7—N1—C5—C60.0C9—N2'—C7'—N1'173.5 (8)
C4—N1—C5—C6174.8 (3)C6'—N2'—C7'—C8'179.7 (11)
N1—C5—C6—N20.0C9—N2'—C7'—C8'6.8 (12)
C5—C6—N2—C70.0C5'—N1'—C7'—N2'0.0
C5—C6—N2—C9179.0 (3)C4—N1'—C7'—N2'179.4 (8)
C6—N2—C7—N10.0C5'—N1'—C7'—C8'179.7 (11)
C9—N2—C7—N1179.0 (4)C4—N1'—C7'—C8'0.3 (12)
C6—N2—C7—C8178.0 (4)C7'—N2'—C9—N26.6 (5)
C9—N2—C7—C81.0 (5)C6'—N2'—C9—N2179.0 (11)
C5—N1—C7—N20.0C6—N2—C9—N2'171.4 (8)
C4—N1—C7—N2174.7 (3)C7—N2—C9—N2'9.8 (7)
C5—N1—C7—C8177.9 (4)
Symmetry code: (i) x+1, y, z+1.

Experimental details

Crystal data
Chemical formulaC18H24N42+·2Br
Mr456.23
Crystal system, space groupMonoclinic, P21/n
Temperature (K)140
a, b, c (Å)8.5689 (4), 9.8617 (5), 11.0272 (4)
β (°) 93.222 (3)
V3)930.37 (7)
Z2
Radiation typeMo Kα
µ (mm1)4.36
Crystal size (mm)0.40 × 0.08 × 0.04
Data collection
DiffractometerBruker SMART APEX
diffractometer
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.274, 0.845
No. of measured, independent and
observed [I > 2σ(I)] reflections
5882, 2131, 1575
Rint0.051
(sin θ/λ)max1)0.650
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.039, 0.096, 1.04
No. of reflections2131
No. of parameters112
No. of restraints36
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.54, 0.99

Computer programs: APEX2 (Bruker, 2008), SAINT (Bruker, 2008), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), X-SEED (Barbour, 2001), publCIF (Westrip, 2009).

 

Acknowledgements

We thank the University of Malaya (grant Nos. TA 0009/2008 A and FS343/2008 A) for supporting this study.

References

First citationBarbour, L. J. (2001). J. Supramol. Chem. 1, 189–191.  CrossRef CAS Google Scholar
First citationBruker (2008). APEX2 and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.  Google Scholar
First citationDobrzańska, L. (2005). Acta Cryst. E61, o4113–o4115.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationGanesan, K., Alias, Y. & Ng, S. W. (2008). Acta Cryst. C64, o478–o480.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationSheldrick, G. M. (1996). SADABS. University of Göttingen, Germany.  Google Scholar
First citationSheldrick, G. M. (2008). Acta Cryst. A64, 112–122.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationWestrip, S. P. (2009). publCIF. In preparation.  Google Scholar

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