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The asymmetric unit of the title compound, C14H16N42+·2C7H4NO4·2C7H5NO4, comprises one-half of the 3,3′-(p-phenyl­enedimethyl­ene)di-1H-imidazol-1-ium dication, which lies on an inversion centre, one 4-nitro­benzoate anion and one 4-nitro­benzoic acid mol­ecule. In the crystal, the components are linked into a two-dimensional network parallel to (110) by O—H...O, N—H...O and C—H...O hydrogen bonds.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S160053681001929X/ci5093sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S160053681001929X/ci5093Isup2.hkl
Contains datablock I

CCDC reference: 781441

Key indicators

  • Single-crystal X-ray study
  • T = 295 K
  • Mean [sigma](C-C) = 0.007 Å
  • R factor = 0.081
  • wR factor = 0.191
  • Data-to-parameter ratio = 12.0

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for N2 PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for N1 PLAT250_ALERT_2_C Large U3/U1 Ratio for Average U(i,j) Tensor .... 2.02 PLAT340_ALERT_3_C Low Bond Precision on C-C Bonds (x 1000) Ang .. 7 PLAT910_ALERT_3_C Missing # of FCF Reflections Below Th(Min) ..... 4 PLAT911_ALERT_3_C Missing # FCF Refl Between THmin & STh/L= 0.594 2 PLAT042_ALERT_1_C Calc. and Reported MoietyFormula Strings Differ ?
Alert level G PLAT154_ALERT_1_G The su's on the Cell Angles are Equal (x 10000) 3000 Deg.
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 7 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 2 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 3 ALERT type 2 Indicator that the structure model may be wrong or deficient 3 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

Over the past few years, efforts have been focused on the investigation of coordination polymers with flexible ligands. Di-imidazole flexbile ligands such as 1,4-bis(1H-imidazol-1-yl)methylbenzene (bix) find numerous applications in constructing metal-organic coordination polymers as they can rotate freely about methylene carbon atoms to adjust to the coordination environment. We report here the crystal structure of the title compound.

The asymmetric unit comprises one-half of a bix2+ dication lying on an inversion centre, one 4-nitrobenzoate anion and one neutral 4-nitrobenzoic acid molecule (Fig. 1). Bond distances and angles are normal (Chen et al., 2010).

In the crystal structure, the dications, anions and neutral 4-nitrobenzoic acid molecule are interlinked by O—H···O, N—H···O and C—H···O hydrogen bonds (Table 1), forming a two-dimensional hydrogen-bonded network parallel to the (110).

Related literature top

For the synthesis of 1,4-bis(imidazol-1-ylmethyl)benzene, see: Hoskins et al. (1997). For a related structure, see: Chen et al. (2010).

Experimental top

1,4-Bis(imidazol-1-ylmethyl)benzene (bix) was prepared according to a literature method (Hoskins et al., 1997). 1:4 molar amounts of bix (23.8 mg, 0.1 mmol) and 4-nitrobenzoic acid (66.9 mg , 0.4 mmol) were dissolved in 95% ethanol (30 ml). The mixture was stirred and refluxed for 1 h and then filtered. The resulting colourless solution was allowed to stand in air for two weeks. Colourless crystals of the title compound suitable for X-ray diffraction analysis were obtained by slow evaporation of the solution.

Refinement top

H atoms were positioned geometrically [O–H = 0.85 Å, N–H = 0.86 Å and C–H = 0.93 or 0.97 Å] and refined using a riding model, with Uiso(H) = 1.5Ueq(O) and 1.2Ueq(C,N).

Structure description top

Over the past few years, efforts have been focused on the investigation of coordination polymers with flexible ligands. Di-imidazole flexbile ligands such as 1,4-bis(1H-imidazol-1-yl)methylbenzene (bix) find numerous applications in constructing metal-organic coordination polymers as they can rotate freely about methylene carbon atoms to adjust to the coordination environment. We report here the crystal structure of the title compound.

The asymmetric unit comprises one-half of a bix2+ dication lying on an inversion centre, one 4-nitrobenzoate anion and one neutral 4-nitrobenzoic acid molecule (Fig. 1). Bond distances and angles are normal (Chen et al., 2010).

In the crystal structure, the dications, anions and neutral 4-nitrobenzoic acid molecule are interlinked by O—H···O, N—H···O and C—H···O hydrogen bonds (Table 1), forming a two-dimensional hydrogen-bonded network parallel to the (110).

For the synthesis of 1,4-bis(imidazol-1-ylmethyl)benzene, see: Hoskins et al. (1997). For a related structure, see: Chen et al. (2010).

Computing details top

Data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 1999); data reduction: SAINT (Bruker, 1999); 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. The asymmetric unit of the title compound, showing the atomic numbering and 30% probability displacement ellipsoids. Atoms labelled with the suffix A are generated by the symmetry operation (-x, 1-y, -z).
3,3'-(p-Phenylenedimethylene)di-1H-imidazol-1-ium bis(4-nitrobenzoate)–4-nitrobenzoic acid (1/2) top
Crystal data top
C14H16N42+·2C7H4NO4·2C7H5NO4Z = 1
Mr = 906.77F(000) = 470
Triclinic, P1Dx = 1.474 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 7.2659 (15) ÅCell parameters from 3889 reflections
b = 12.689 (3) Åθ = 4.6–22.7°
c = 13.028 (3) ŵ = 0.12 mm1
α = 112.94 (3)°T = 295 K
β = 102.49 (3)°Prism, colourless
γ = 101.94 (3)°0.20 × 0.20 × 0.20 mm
V = 1021.8 (6) Å3
Data collection top
Bruker SMART CCD area-detector
diffractometer
3590 independent reflections
Radiation source: fine–focus sealed tube2019 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.066
φ and ω scansθmax = 25.0°, θmin = 3.0°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 88
Tmin = 0.968, Tmax = 0.971k = 1515
8835 measured reflectionsl = 1515
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)] = 0.081Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.191H-atom parameters constrained
S = 1.19 w = 1/[σ2(Fo2) + (0.0648P)2 + 0.2399P]
where P = (Fo2 + 2Fc2)/3
3590 reflections(Δ/σ)max = 0.001
298 parametersΔρmax = 0.42 e Å3
0 restraintsΔρmin = 0.24 e Å3
Crystal data top
C14H16N42+·2C7H4NO4·2C7H5NO4γ = 101.94 (3)°
Mr = 906.77V = 1021.8 (6) Å3
Triclinic, P1Z = 1
a = 7.2659 (15) ÅMo Kα radiation
b = 12.689 (3) ŵ = 0.12 mm1
c = 13.028 (3) ÅT = 295 K
α = 112.94 (3)°0.20 × 0.20 × 0.20 mm
β = 102.49 (3)°
Data collection top
Bruker SMART CCD area-detector
diffractometer
3590 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
2019 reflections with I > 2σ(I)
Tmin = 0.968, Tmax = 0.971Rint = 0.066
8835 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0810 restraints
wR(F2) = 0.191H-atom parameters constrained
S = 1.19Δρmax = 0.42 e Å3
3590 reflectionsΔρmin = 0.24 e Å3
298 parameters
Special details top

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*/Ueq
O70.1748 (5)0.3773 (3)0.6201 (3)0.0628 (9)
O80.2413 (5)0.4626 (3)0.5069 (3)0.0636 (9)
N40.2722 (5)0.3310 (3)0.2960 (3)0.0468 (9)
H4A0.25960.33280.36070.056*
N30.3203 (4)0.3884 (3)0.1672 (3)0.0341 (8)
C110.2099 (5)0.5846 (3)0.6892 (3)0.0346 (10)
C120.1960 (6)0.5971 (4)0.7973 (3)0.0378 (10)
H120.17870.53050.81240.045*
C200.0546 (6)0.4031 (4)0.0614 (3)0.0417 (11)
H200.09100.33710.10310.050*
C100.2349 (6)0.6835 (4)0.6673 (4)0.0454 (11)
H100.24470.67530.59470.054*
C210.1173 (6)0.4176 (4)0.1146 (4)0.0417 (11)
H210.19520.36210.19180.050*
C130.2074 (6)0.7074 (4)0.8830 (4)0.0426 (11)
H130.19810.71600.95580.051*
C170.2842 (6)0.2657 (4)0.1182 (4)0.0397 (10)
H170.28080.21610.04270.048*
C80.2328 (6)0.8040 (4)0.8581 (4)0.0423 (11)
C140.2070 (6)0.4663 (4)0.5962 (4)0.0417 (11)
C190.1743 (6)0.4850 (4)0.0531 (3)0.0359 (10)
C90.2457 (6)0.7939 (4)0.7505 (4)0.0510 (12)
H90.26120.86030.73510.061*
N20.2409 (6)0.9230 (4)0.9474 (4)0.0642 (12)
C150.3111 (6)0.4252 (4)0.2754 (4)0.0405 (10)
H150.32910.50440.32790.049*
O60.2194 (6)0.9302 (3)1.0400 (3)0.0946 (14)
C160.2548 (6)0.2308 (4)0.1995 (4)0.0445 (11)
H160.22770.15250.19130.053*
O50.2639 (7)1.0065 (3)0.9231 (4)0.1088 (16)
C180.3622 (6)0.4672 (4)0.1113 (4)0.0472 (11)
H18A0.42260.43180.05250.057*
H18B0.45670.54520.17060.057*
C40.4933 (6)0.8837 (3)0.5529 (3)0.0360 (10)
O30.4409 (5)0.7026 (3)0.3853 (3)0.0731 (11)
O20.4178 (6)1.2399 (3)0.8522 (3)0.0791 (11)
O40.7429 (5)0.7925 (3)0.5183 (3)0.0700 (10)
C10.3648 (7)1.0618 (4)0.6869 (4)0.0423 (11)
N10.2961 (7)1.1562 (4)0.7606 (4)0.0616 (11)
C50.6275 (6)0.9830 (3)0.6549 (3)0.0417 (11)
H50.76100.98870.67790.050*
C30.2940 (6)0.8758 (4)0.5190 (3)0.0432 (11)
H30.20410.80990.45030.052*
C20.2281 (7)0.9650 (4)0.5863 (4)0.0473 (11)
H20.09470.95960.56420.057*
C60.5638 (7)1.0733 (4)0.7224 (4)0.0451 (11)
H60.65331.14030.79030.054*
C70.5608 (8)0.7845 (4)0.4785 (4)0.0470 (11)
O10.1202 (7)1.1467 (4)0.7276 (4)0.1083 (15)
H2A0.21070.32060.57730.162*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O70.086 (3)0.0432 (19)0.072 (2)0.0297 (18)0.0469 (19)0.0238 (18)
O80.086 (3)0.065 (2)0.0381 (19)0.0274 (19)0.0290 (18)0.0162 (17)
N40.048 (2)0.062 (3)0.035 (2)0.0202 (19)0.0143 (17)0.025 (2)
N30.035 (2)0.038 (2)0.032 (2)0.0177 (16)0.0105 (15)0.0157 (17)
C110.028 (2)0.039 (2)0.032 (2)0.0081 (18)0.0080 (18)0.013 (2)
C120.039 (3)0.042 (3)0.041 (3)0.016 (2)0.019 (2)0.023 (2)
C200.049 (3)0.041 (3)0.043 (3)0.023 (2)0.018 (2)0.021 (2)
C100.058 (3)0.047 (3)0.034 (3)0.017 (2)0.017 (2)0.019 (2)
C210.049 (3)0.038 (3)0.032 (2)0.013 (2)0.008 (2)0.013 (2)
C130.041 (3)0.053 (3)0.034 (2)0.017 (2)0.016 (2)0.016 (2)
C170.045 (3)0.034 (2)0.037 (3)0.020 (2)0.012 (2)0.011 (2)
C80.038 (3)0.036 (2)0.041 (3)0.013 (2)0.009 (2)0.007 (2)
C140.029 (2)0.045 (3)0.042 (3)0.009 (2)0.008 (2)0.013 (2)
C190.036 (3)0.040 (2)0.037 (3)0.008 (2)0.011 (2)0.025 (2)
C90.064 (3)0.043 (3)0.053 (3)0.019 (2)0.020 (2)0.026 (3)
N20.065 (3)0.050 (3)0.059 (3)0.022 (2)0.013 (2)0.008 (3)
C150.033 (3)0.040 (3)0.035 (3)0.015 (2)0.0044 (19)0.006 (2)
O60.138 (4)0.083 (3)0.046 (2)0.055 (3)0.026 (2)0.006 (2)
C160.046 (3)0.034 (3)0.050 (3)0.014 (2)0.010 (2)0.018 (2)
O50.177 (5)0.046 (2)0.115 (4)0.046 (3)0.072 (3)0.029 (2)
C180.041 (3)0.054 (3)0.053 (3)0.015 (2)0.014 (2)0.032 (2)
C40.053 (3)0.025 (2)0.032 (2)0.012 (2)0.015 (2)0.0134 (19)
O30.082 (3)0.047 (2)0.051 (2)0.0251 (18)0.0019 (19)0.0063 (17)
O20.091 (3)0.054 (2)0.066 (2)0.023 (2)0.032 (2)0.001 (2)
O40.057 (2)0.047 (2)0.076 (2)0.0193 (17)0.0156 (19)0.0005 (18)
C10.056 (3)0.036 (2)0.046 (3)0.021 (2)0.025 (2)0.021 (2)
N10.067 (3)0.049 (3)0.065 (3)0.023 (2)0.035 (3)0.015 (2)
C50.044 (3)0.033 (2)0.042 (3)0.010 (2)0.010 (2)0.014 (2)
C30.050 (3)0.036 (3)0.033 (2)0.009 (2)0.004 (2)0.013 (2)
C20.047 (3)0.044 (3)0.043 (3)0.013 (2)0.011 (2)0.016 (2)
C60.059 (3)0.033 (2)0.034 (2)0.012 (2)0.014 (2)0.009 (2)
C70.066 (4)0.028 (2)0.042 (3)0.012 (2)0.015 (3)0.014 (2)
O10.072 (3)0.086 (3)0.129 (4)0.040 (2)0.037 (3)0.003 (3)
Geometric parameters (Å, º) top
O7—C141.274 (5)C8—N21.484 (5)
O7—H2A0.85C19—C21i1.387 (5)
O8—C141.227 (5)C19—C181.519 (5)
N4—C151.313 (5)C9—H90.93
N4—C161.354 (5)N2—O51.210 (5)
N4—H4A0.86N2—O61.220 (5)
N3—C151.324 (5)C15—H150.93
N3—C171.373 (5)C16—H160.93
N3—C181.469 (5)C18—H18A0.97
C11—C101.378 (5)C18—H18B0.97
C11—C121.383 (5)C4—C51.389 (5)
C11—C141.510 (5)C4—C31.389 (5)
C12—C131.380 (5)C4—C71.509 (6)
C12—H120.93O3—C71.224 (5)
C20—C211.376 (5)O2—N11.225 (5)
C20—C191.385 (5)O4—C71.279 (5)
C20—H200.93C1—C21.374 (6)
C10—C91.370 (6)C1—C61.377 (6)
C10—H100.93C1—N11.472 (5)
C21—C19i1.387 (5)N1—O11.221 (5)
C21—H210.93C5—C61.382 (5)
C13—C81.373 (5)C5—H50.93
C13—H130.93C3—C21.382 (5)
C17—C161.336 (5)C3—H30.93
C17—H170.93C2—H20.93
C8—C91.382 (6)C6—H60.93
C14—O7—H2A111.6O5—N2—O6123.9 (4)
C15—N4—C16109.4 (3)O5—N2—C8118.0 (5)
C15—N4—H4A125.3O6—N2—C8118.1 (5)
C16—N4—H4A125.3N4—C15—N3108.4 (4)
C15—N3—C17108.0 (3)N4—C15—H15125.8
C15—N3—C18125.0 (3)N3—C15—H15125.8
C17—N3—C18127.0 (3)C17—C16—N4107.0 (4)
C10—C11—C12119.4 (4)C17—C16—H16126.5
C10—C11—C14119.0 (4)N4—C16—H16126.5
C12—C11—C14121.6 (4)N3—C18—C19111.7 (3)
C13—C12—C11120.7 (4)N3—C18—H18A109.3
C13—C12—H12119.7C19—C18—H18A109.3
C11—C12—H12119.7N3—C18—H18B109.3
C21—C20—C19121.1 (4)C19—C18—H18B109.3
C21—C20—H20119.4H18A—C18—H18B107.9
C19—C20—H20119.4C5—C4—C3119.5 (4)
C9—C10—C11121.2 (4)C5—C4—C7121.0 (4)
C9—C10—H10119.4C3—C4—C7119.6 (4)
C11—C10—H10119.4C2—C1—C6122.6 (4)
C20—C21—C19i120.0 (4)C2—C1—N1118.9 (4)
C20—C21—H21120.0C6—C1—N1118.5 (4)
C19i—C21—H21120.0O1—N1—O2123.3 (4)
C8—C13—C12118.3 (4)O1—N1—C1118.3 (4)
C8—C13—H13120.8O2—N1—C1118.4 (5)
C12—C13—H13120.8C6—C5—C4120.4 (4)
C16—C17—N3107.1 (4)C6—C5—H5119.8
C16—C17—H17126.4C4—C5—H5119.8
N3—C17—H17126.4C2—C3—C4120.7 (4)
C13—C8—C9122.2 (4)C2—C3—H3119.7
C13—C8—N2119.5 (4)C4—C3—H3119.7
C9—C8—N2118.2 (4)C1—C2—C3118.4 (4)
O8—C14—O7124.9 (4)C1—C2—H2120.8
O8—C14—C11119.4 (4)C3—C2—H2120.8
O7—C14—C11115.7 (4)C1—C6—C5118.5 (4)
C20—C19—C21i118.8 (4)C1—C6—H6120.7
C20—C19—C18120.6 (4)C5—C6—H6120.7
C21i—C19—C18120.5 (4)O3—C7—O4124.3 (4)
C10—C9—C8118.2 (4)O3—C7—C4119.0 (5)
C10—C9—H9120.9O4—C7—C4116.7 (4)
C8—C9—H9120.9
Symmetry code: (i) x, y+1, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O7—H2A···O3ii0.852.573.167 (5)128
O7—H2A···O4ii0.851.652.494 (5)173
N4—H4A···O80.862.032.690 (5)133
C15—H15···O30.932.233.073 (7)150
C17—H17···O5iii0.932.463.228 (7)140
C21—H21···O3i0.932.463.321 (6)154
Symmetry codes: (i) x, y+1, z; (ii) x+1, y+1, z+1; (iii) x, y1, z1.

Experimental details

Crystal data
Chemical formulaC14H16N42+·2C7H4NO4·2C7H5NO4
Mr906.77
Crystal system, space groupTriclinic, P1
Temperature (K)295
a, b, c (Å)7.2659 (15), 12.689 (3), 13.028 (3)
α, β, γ (°)112.94 (3), 102.49 (3), 101.94 (3)
V3)1021.8 (6)
Z1
Radiation typeMo Kα
µ (mm1)0.12
Crystal size (mm)0.20 × 0.20 × 0.20
Data collection
DiffractometerBruker SMART CCD area-detector
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.968, 0.971
No. of measured, independent and
observed [I > 2σ(I)] reflections
8835, 3590, 2019
Rint0.066
(sin θ/λ)max1)0.594
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.081, 0.191, 1.19
No. of reflections3590
No. of parameters298
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.42, 0.24

Computer programs: SMART (Bruker, 1998), SAINT (Bruker, 1999), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O7—H2A···O3i0.852.573.167 (5)128
O7—H2A···O4i0.851.652.494 (5)173
N4—H4A···O80.862.032.690 (5)133
C15—H15···O30.932.233.073 (7)150
C17—H17···O5ii0.932.463.228 (7)140
C21—H21···O3iii0.932.463.321 (6)154
Symmetry codes: (i) x+1, y+1, z+1; (ii) x, y1, z1; (iii) x, y+1, z.
 

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