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In the crystal of the title mol­ecular salt, C8H6F3N2+·HSO4, cation-to-anion N—H...O hydrogen bonds generate [100] chains. Anion-to-anion O—H...O hydrogen bonds generate [001] helices and cross-link the chains into a three-dimensional network.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536811048811/hb6491sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536811048811/hb6491Isup2.hkl
Contains datablock I

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S1600536811048811/hb6491Isup3.cml
Supplementary material

CCDC reference: 858529

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.009 Å
  • R factor = 0.052
  • wR factor = 0.134
  • Data-to-parameter ratio = 11.8

checkCIF/PLATON results

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Alert level C PLAT094_ALERT_2_C Ratio of Maximum / Minimum Residual Density .... 2.08 PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for C1 PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for S1 PLAT340_ALERT_3_C Low Bond Precision on C-C Bonds ............... 0.0087 Ang PLAT910_ALERT_3_C Missing # of FCF Reflections Below Th(Min) ..... 2 PLAT913_ALERT_3_C Missing # of Very Strong Reflections in FCF .... 1
Alert level G REFLT03_ALERT_4_G Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF. From the CIF: _diffrn_reflns_theta_max 24.99 From the CIF: _reflns_number_total 1977 Count of symmetry unique reflns 1020 Completeness (_total/calc) 193.82% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 957 Fraction of Friedel pairs measured 0.938 Are heavy atom types Z>Si present yes PLAT002_ALERT_2_G Number of Distance or Angle Restraints on AtSite 2 PLAT003_ALERT_2_G Number of Uiso or Uij Restrained Atom Sites .... 2 PLAT005_ALERT_5_G No _iucr_refine_instructions_details in CIF .... ? PLAT194_ALERT_1_G Missing _cell_measurement_reflns_used datum .... ? PLAT199_ALERT_1_G Check the Reported _cell_measurement_temperature 293 K PLAT200_ALERT_1_G Check the Reported _diffrn_ambient_temperature 293 K PLAT860_ALERT_3_G Note: Number of Least-Squares Restraints ....... 8 PLAT909_ALERT_3_G Percentage of Observed Data at Theta(Max) still 90 Perc. PLAT961_ALERT_5_G Dataset Contains no Negative Intensities ....... !
0 ALERT level A = Most likely a serious problem - resolve or explain 0 ALERT level B = A potentially serious problem, consider carefully 6 ALERT level C = Check. Ensure it is not caused by an omission or oversight 10 ALERT level G = General information/check it is not something unexpected 3 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 5 ALERT type 2 Indicator that the structure model may be wrong or deficient 5 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 2 ALERT type 5 Informative message, check
checkCIF publication errors
Alert level G PUBL013_ALERT_1_G The _publ_section_comment (discussion of study) is missing. This is required for a full paper submission (but is optional for an electronic paper).
0 ALERT level A = Data missing that is essential or data in wrong format 1 ALERT level G = General alerts. Data that may be required is missing

Related literature top

For a related structure and background to molecular salts, see: Liu (2011).

Experimental top

0.144 g(1 mmol) of 2-Trifluoromethl-1H-benzimidazole was firstly dissolved in 30 ml me thanol, to which 0.1 g (1 mmol) of sulfuric acid was then added to afford the solution without any precipitation under stirring at the ambient temperature. Colourless blocks of the title compound were obtained by the slow evaporation of the above solution after 2 days in air.

The dielectric constant of the compound as a function of temperature indicates that the permittivity is basically temperature-independent (ε = C/(T–T0)), suggesting that this compound is not ferroelectric or there may be no distinct phase transition occurring within the measured temperature within the measured temperature (below the melting point).

Refinement top

H atoms were placed in calculated positions (N—H = 0.89 Å; C—H = 0.93Å for Csp2 atoms and C—H = 0.96Å and 0.97Å for Csp3 atoms), assigned fixed Uiso values [Uiso = 1.2Ueq(Csp2) and 1.5Ueq(Csp3,N)] and allowed to ride.The H atom bonding with N was found with O—H bond distance of 0.8600Åin the difference electron density map.

Structure description top

For a related structure and background to molecular salts, see: Liu (2011).

Computing details top

Data collection: CrystalClear (Rigaku, 2005); cell refinement: CrystalClear (Rigaku, 2005); data reduction: CrystalClear (Rigaku, 2005); 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 molecular structure of the title compound, showing 30% probability displacement ellipsoids.
[Figure 2] Fig. 2. A view of the packing of the title compound, stacking along the a axis. Dashed lines indicate hydrogen bonds.
2-Trifluoromethyl-1H-benzimidazol-3-ium hydrogen sulfate top
Crystal data top
C8H6F3N2+·HSO4F(000) = 864
Mr = 284.22Dx = 1.681 Mg m3
Hexagonal, P65Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 65θ = 3.1–27.6°
a = 9.4119 (13) ŵ = 0.34 mm1
c = 21.960 (4) ÅT = 293 K
V = 1684.7 (5) Å3Block, colorless
Z = 60.20 × 0.20 × 0.20 mm
Data collection top
Rigaku Mercury2 CCD
diffractometer
1977 independent reflections
Radiation source: fine-focus sealed tube1941 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.038
CCD_Profile_fitting scansθmax = 25.0°, θmin = 3.1°
Absorption correction: multi-scan
(CrystalClear; Rigaku, 2005)
h = 1111
Tmin = 0.935, Tmax = 0.935k = 1111
14287 measured reflectionsl = 2626
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.052H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.134 w = 1/[σ2(Fo2) + (0.0593P)2 + 1.9666P]
where P = (Fo2 + 2Fc2)/3
S = 1.11(Δ/σ)max < 0.001
1977 reflectionsΔρmax = 0.53 e Å3
167 parametersΔρmin = 0.25 e Å3
8 restraintsAbsolute structure: Flack (1983), 957 Friedel pairs
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.03 (16)
Crystal data top
C8H6F3N2+·HSO4Z = 6
Mr = 284.22Mo Kα radiation
Hexagonal, P65µ = 0.34 mm1
a = 9.4119 (13) ÅT = 293 K
c = 21.960 (4) Å0.20 × 0.20 × 0.20 mm
V = 1684.7 (5) Å3
Data collection top
Rigaku Mercury2 CCD
diffractometer
1977 independent reflections
Absorption correction: multi-scan
(CrystalClear; Rigaku, 2005)
1941 reflections with I > 2σ(I)
Tmin = 0.935, Tmax = 0.935Rint = 0.038
14287 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.052H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.134Δρmax = 0.53 e Å3
S = 1.11Δρmin = 0.25 e Å3
1977 reflectionsAbsolute structure: Flack (1983), 957 Friedel pairs
167 parametersAbsolute structure parameter: 0.03 (16)
8 restraints
Special details top

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) top
xyzUiso*/Ueq
S10.09970 (14)0.72553 (17)0.16867 (6)0.0442 (3)
N10.4873 (5)0.7391 (5)0.1735 (2)0.0418 (9)
H1A0.38430.70580.17700.050*
N20.7169 (4)0.7349 (5)0.16388 (17)0.0348 (8)
H2A0.78350.69810.15960.042*
C30.6124 (6)0.9017 (6)0.1722 (2)0.0418 (11)
C80.7613 (5)0.9011 (6)0.1675 (2)0.0371 (10)
C40.6126 (7)1.0512 (7)0.1762 (3)0.0508 (13)
H40.51521.05350.17920.061*
O30.0637 (4)0.6347 (5)0.14218 (18)0.0558 (11)
F30.5450 (5)0.4034 (5)0.1391 (3)0.0928 (15)
C60.9082 (7)1.1891 (7)0.1712 (3)0.0527 (13)
H61.00661.28830.17100.063*
O10.0866 (5)0.8248 (5)0.2230 (2)0.0627 (11)
C50.7592 (8)1.1907 (7)0.1755 (3)0.0589 (15)
H50.76231.29090.17800.071*
F10.3262 (5)0.4077 (6)0.1346 (3)0.116 (2)
F20.4211 (10)0.3991 (6)0.2195 (2)0.157 (3)
O40.1589 (5)0.6207 (5)0.19150 (19)0.0571 (11)
C70.9120 (6)1.0455 (7)0.1670 (3)0.0456 (11)
H71.01031.04480.16410.055*
C10.4609 (6)0.4596 (7)0.1670 (3)0.0520 (13)
O20.2184 (6)0.8507 (9)0.1300 (3)0.110 (2)
C20.5531 (5)0.6434 (6)0.1683 (2)0.0373 (9)
H10.041 (10)0.754 (9)0.251 (3)0.10 (3)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0252 (5)0.0626 (9)0.0458 (6)0.0227 (5)0.0080 (5)0.0144 (6)
N10.0295 (19)0.051 (2)0.051 (2)0.0252 (19)0.0012 (18)0.0049 (19)
N20.0243 (17)0.044 (2)0.040 (2)0.0205 (16)0.0009 (16)0.0062 (18)
C30.037 (2)0.050 (3)0.043 (3)0.025 (2)0.001 (2)0.002 (2)
C80.037 (2)0.043 (3)0.037 (2)0.024 (2)0.006 (2)0.005 (2)
C40.057 (3)0.058 (3)0.059 (3)0.044 (3)0.002 (3)0.003 (3)
O30.0362 (19)0.087 (3)0.059 (2)0.042 (2)0.0057 (16)0.015 (2)
F30.070 (2)0.058 (2)0.158 (4)0.038 (2)0.018 (3)0.012 (3)
C60.044 (3)0.045 (3)0.062 (3)0.017 (2)0.006 (3)0.009 (3)
O10.056 (3)0.048 (2)0.079 (3)0.022 (2)0.009 (2)0.012 (2)
C50.073 (4)0.052 (3)0.070 (4)0.045 (3)0.005 (3)0.005 (3)
F10.047 (2)0.070 (3)0.213 (6)0.0161 (19)0.039 (3)0.044 (3)
F20.246 (6)0.055 (3)0.072 (3)0.002 (3)0.038 (4)0.009 (2)
O40.0403 (19)0.074 (3)0.072 (3)0.039 (2)0.0007 (17)0.007 (2)
C70.030 (2)0.055 (3)0.050 (3)0.020 (2)0.002 (2)0.003 (2)
C10.036 (3)0.043 (3)0.067 (3)0.012 (2)0.014 (3)0.001 (3)
O20.057 (3)0.155 (5)0.108 (4)0.045 (3)0.032 (3)0.093 (4)
C20.030 (2)0.040 (2)0.042 (2)0.0176 (19)0.0001 (19)0.010 (2)
Geometric parameters (Å, º) top
S1—O21.429 (5)C4—C51.348 (9)
S1—O41.444 (4)C4—H40.9300
S1—O31.456 (4)F3—C11.304 (6)
S1—O11.558 (5)C6—C71.373 (8)
N1—C21.329 (6)C6—C51.414 (8)
N1—C31.388 (6)C6—H60.9300
N1—H1A0.8600O1—H10.86 (2)
N2—C21.341 (6)C5—H50.9300
N2—C81.405 (6)F1—C11.317 (8)
N2—H2A0.8600F2—C11.258 (8)
C3—C81.407 (6)C7—H70.9300
C3—C41.409 (7)C1—C21.499 (7)
C8—C71.390 (7)
O2—S1—O4111.1 (3)C3—C4—H4121.2
O2—S1—O3114.0 (3)C7—C6—C5122.0 (5)
O4—S1—O3113.1 (3)C7—C6—H6119.0
O2—S1—O1103.0 (4)C5—C6—H6119.0
O4—S1—O1108.5 (3)S1—O1—H1104 (7)
O3—S1—O1106.3 (2)C4—C5—C6121.9 (5)
C2—N1—C3108.6 (4)C4—C5—H5119.1
C2—N1—H1A125.7C6—C5—H5119.1
C3—N1—H1A125.7C6—C7—C8116.5 (4)
C2—N2—C8108.5 (3)C6—C7—H7121.8
C2—N2—H2A125.8C8—C7—H7121.8
C8—N2—H2A125.8F2—C1—F3110.5 (7)
N1—C3—C8107.2 (4)F2—C1—F1108.3 (6)
N1—C3—C4132.5 (4)F3—C1—F1105.2 (5)
C8—C3—C4120.3 (5)F2—C1—C2112.0 (5)
C7—C8—N2132.7 (4)F3—C1—C2111.0 (4)
C7—C8—C3121.9 (4)F1—C1—C2109.5 (5)
N2—C8—C3105.4 (4)N1—C2—N2110.3 (4)
C5—C4—C3117.5 (5)N1—C2—C1125.9 (4)
C5—C4—H4121.2N2—C2—C1123.8 (4)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2A···O3i0.861.852.707 (5)173
N1—H1A···O40.861.882.740 (7)174
O1—H1···O2ii0.86 (2)1.86 (6)2.608 (7)145 (9)
Symmetry codes: (i) x+1, y, z; (ii) y1, x+y, z+1/6.

Experimental details

Crystal data
Chemical formulaC8H6F3N2+·HSO4
Mr284.22
Crystal system, space groupHexagonal, P65
Temperature (K)293
a, c (Å)9.4119 (13), 21.960 (4)
V3)1684.7 (5)
Z6
Radiation typeMo Kα
µ (mm1)0.34
Crystal size (mm)0.20 × 0.20 × 0.20
Data collection
DiffractometerRigaku Mercury2 CCD
Absorption correctionMulti-scan
(CrystalClear; Rigaku, 2005)
Tmin, Tmax0.935, 0.935
No. of measured, independent and
observed [I > 2σ(I)] reflections
14287, 1977, 1941
Rint0.038
(sin θ/λ)max1)0.594
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.052, 0.134, 1.11
No. of reflections1977
No. of parameters167
No. of restraints8
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.53, 0.25
Absolute structureFlack (1983), 957 Friedel pairs
Absolute structure parameter0.03 (16)

Computer programs: CrystalClear (Rigaku, 2005), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2A···O3i0.861.852.707 (5)173
N1—H1A···O40.861.882.740 (7)174
O1—H1···O2ii0.86 (2)1.86 (6)2.608 (7)145 (9)
Symmetry codes: (i) x+1, y, z; (ii) y1, x+y, z+1/6.
 

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