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The asymmetric unit of the title compound, C16H31N2+·Br-·H2O, contains one crystallographically independent 1-do­decyl-3-methyl­imidazolium cation, one bromide anion, to counterbalance the charge, and one solvent water mol­ecule. The halide anion forms hydrogen bonds with the H atoms of the imidazole ring and with the water H atoms.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805025717/bt6712sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536805025717/bt6712Isup2.hkl
Contains datablock I

CCDC reference: 283758

Key indicators

  • Single-crystal X-ray study
  • T = 263 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.026
  • wR factor = 0.069
  • Data-to-parameter ratio = 21.9

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT029_ALERT_3_C _diffrn_measured_fraction_theta_full Low ....... 0.98 PLAT042_ALERT_1_C Calc. and Rep. MoietyFormula Strings Differ .... ?
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 2 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 1 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion

Computing details top

Data collection: X-AREA (Stoe & Cie, 2002); cell refinement: X-AREA; data reduction: X-AREA; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: DIAMOND (Brandenburg, 1996); software used to prepare material for publication: SHELXL97.

1-Dodecyl-3-methylimidazolium bromide monohydrate top
Crystal data top
C16H31N2+·Br·H2OZ = 2
Mr = 349.34F(000) = 372
Triclinic, P1Dx = 1.221 Mg m3
Hall symbol: -P 1Melting point: unknown K
a = 5.500 (5) ÅMo Kα radiation, λ = 0.71073 Å
b = 7.794 (5) ÅCell parameters from 4273 reflections
c = 22.961 (5) Åθ = 2.8–28.3°
α = 81.893 (5)°µ = 2.16 mm1
β = 83.761 (5)°T = 263 K
γ = 78.102 (5)°Needle, white
V = 950.3 (11) Å30.3 × 0.2 × 0.1 mm
Data collection top
Stoe IPDS-I
diffractometer
4167 independent reflections
Radiation source: fine-focus sealed tube3523 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.034
φ scansθmax = 27.3°, θmin = 1.8°
Absorption correction: numerical
[X-RED32 (Stoe & Cie, 2002) and X-SHAPE (Stoe & Cie, 2001)]
h = 67
Tmin = 0.585, Tmax = 0.794k = 99
14912 measured reflectionsl = 2929
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)] = 0.026Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.069H atoms treated by a mixture of independent and constrained refinement
S = 1.04 w = 1/[σ2(Fo2) + (0.0397P)2 + 0.1463P]
where P = (Fo2 + 2Fc2)/3
4167 reflections(Δ/σ)max = 0.001
190 parametersΔρmax = 0.24 e Å3
2 restraintsΔρmin = 0.29 e Å3
Special details top

Experimental. A suitable single-crystal was carefully selected under a polarizing microscope and mounted in a glass capillary. The scattering intensities were collected with an imaging plate diffractometer (Stoe IPDS-I) equipped with a fine focus sealed tube X-ray source (Mo Kα, λ = 0.71073 Å) operating at 50 kV and 30 mA. Intensity data were collected at 263 K by φ scans in 360 frames (0 < φ < 180° exposure time of 10 min) in the 2Θ range 1.91 - 54.78 °·Structure solution and refinement were carried out using the program SHELXL97 (Sheldrick, 1997). A numerical absorption correction (X-RED (Stoe & Cie, 2001) was applied after optimization of the crystal shape (X-SHAPE (Stoe & Cie, 2001)). The final difference maps were free of any chemically significant features. The refinement was based on F2 for ALL reflections.

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. Carbon-bound H atoms were positioned with idealized geometry (methine d(C—H) = 93 pm, methylene: d(C—H) = 99 pm; methyl: d(C—H) = 98 pm) and refined with fixed isotropic displacement parameters [Uiso(H)=1.5Ueq (for methyl C) and Uiso(H)=1.2Ueq (for methylene C)] using a riding atom model. The methyl groups were idealized, then refined as a rigid group allowed to rotate but not tip. The water H atoms were located in a difference map and their bond length restrained.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Br0.73175 (3)0.32730 (3)0.383956 (8)0.05446 (8)
N10.4615 (3)0.05054 (19)0.36555 (6)0.0442 (3)
N20.6005 (3)0.21059 (19)0.44379 (6)0.0463 (3)
O0.1671 (4)0.5835 (3)0.34933 (13)0.1026 (7)
H1O0.315 (4)0.528 (4)0.3517 (16)0.128 (13)*
H2O0.084 (5)0.500 (3)0.3521 (15)0.110 (11)*
C10.6543 (3)0.1654 (2)0.38675 (8)0.0472 (4)
H10.80250.20720.36520.057*
C20.3659 (3)0.1219 (2)0.45970 (8)0.0506 (4)
H20.28220.12960.49710.061*
C30.2797 (3)0.0214 (3)0.41077 (8)0.0505 (4)
H30.12520.05380.40820.061*
C40.4544 (4)0.0394 (3)0.30472 (8)0.0525 (4)
H4A0.60500.00890.28170.063*
H4B0.45220.16390.30530.063*
C50.2312 (3)0.0207 (2)0.27513 (7)0.0469 (4)
H5A0.07960.07540.29650.056*
H5B0.22780.10350.27580.056*
C60.2431 (4)0.1079 (3)0.21164 (8)0.0505 (4)
H6A0.25050.23120.21160.061*
H6B0.39590.05240.19090.061*
C70.0246 (3)0.0978 (3)0.17806 (7)0.0498 (4)
H7A0.12810.15630.19800.060*
H7B0.01430.02530.17880.060*
C80.0437 (3)0.1816 (3)0.11422 (8)0.0502 (4)
H8A0.05240.30490.11370.060*
H8B0.19810.12420.09460.060*
C90.1699 (4)0.1712 (3)0.07940 (8)0.0502 (4)
H9A0.32460.22840.09900.060*
H9B0.17830.04800.07960.060*
C100.1486 (3)0.2563 (3)0.01589 (8)0.0503 (4)
H10A0.00620.19910.00360.060*
H10B0.14010.37940.01570.060*
C110.3622 (4)0.2466 (3)0.01946 (8)0.0507 (4)
H11A0.51720.30380.00000.061*
H11B0.37080.12350.01940.061*
C120.3394 (4)0.3321 (3)0.08305 (8)0.0506 (4)
H12A0.33120.45520.08310.061*
H12B0.18400.27510.10230.061*
C130.5513 (4)0.3224 (3)0.11872 (8)0.0513 (4)
H13A0.55840.19920.11900.062*
H13B0.70690.37820.09910.062*
C140.5312 (4)0.4089 (3)0.18186 (8)0.0579 (5)
H14A0.52540.53230.18170.070*
H14B0.37550.35350.20150.070*
C150.7430 (5)0.3974 (3)0.21700 (10)0.0725 (6)
H15A0.71830.45510.25640.109*
H15B0.89780.45430.19850.109*
H15C0.74730.27560.21850.109*
C160.7654 (4)0.3362 (3)0.48298 (9)0.0606 (5)
H16A0.66800.38080.51680.091*0.50
H16B0.88420.27750.49560.091*0.50
H16C0.85180.43250.46220.091*0.50
H16D0.93470.34640.46620.091*0.50
H16E0.71840.44960.48750.091*0.50
H16F0.75090.29470.52090.091*0.50
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br0.05039 (11)0.05782 (12)0.05377 (11)0.00501 (8)0.01003 (8)0.00571 (8)
N10.0451 (7)0.0469 (7)0.0403 (7)0.0070 (6)0.0101 (6)0.0025 (6)
N20.0477 (8)0.0453 (7)0.0441 (7)0.0008 (6)0.0135 (6)0.0043 (6)
O0.0575 (10)0.0631 (11)0.175 (2)0.0021 (9)0.0001 (12)0.0037 (12)
C10.0429 (8)0.0494 (9)0.0477 (9)0.0024 (7)0.0071 (7)0.0084 (7)
C20.0489 (9)0.0588 (10)0.0413 (9)0.0022 (8)0.0060 (7)0.0069 (8)
C30.0438 (9)0.0561 (10)0.0476 (9)0.0023 (8)0.0089 (7)0.0065 (8)
C40.0568 (11)0.0591 (11)0.0434 (9)0.0174 (9)0.0123 (8)0.0027 (8)
C50.0492 (9)0.0526 (9)0.0396 (8)0.0115 (8)0.0081 (7)0.0026 (7)
C60.0525 (10)0.0569 (10)0.0432 (9)0.0158 (8)0.0099 (8)0.0021 (8)
C70.0517 (10)0.0584 (10)0.0406 (9)0.0176 (8)0.0089 (7)0.0036 (7)
C80.0508 (10)0.0597 (10)0.0412 (9)0.0165 (8)0.0083 (7)0.0024 (7)
C90.0521 (10)0.0577 (10)0.0420 (9)0.0164 (8)0.0094 (8)0.0020 (8)
C100.0511 (10)0.0584 (10)0.0428 (9)0.0160 (8)0.0084 (8)0.0009 (8)
C110.0537 (10)0.0579 (10)0.0421 (9)0.0168 (8)0.0092 (8)0.0008 (8)
C120.0527 (10)0.0574 (10)0.0432 (9)0.0165 (8)0.0088 (8)0.0006 (8)
C130.0548 (10)0.0564 (10)0.0439 (9)0.0148 (8)0.0094 (8)0.0002 (8)
C140.0631 (12)0.0675 (12)0.0443 (9)0.0183 (10)0.0104 (9)0.0023 (8)
C150.0807 (15)0.0894 (16)0.0504 (11)0.0223 (13)0.0224 (11)0.0028 (11)
C160.0626 (12)0.0563 (11)0.0569 (11)0.0072 (9)0.0230 (9)0.0005 (9)
Geometric parameters (Å, º) top
N1—C11.327 (2)C9—C101.517 (2)
N1—C31.370 (2)C9—H9A0.9700
N1—C41.472 (2)C9—H9B0.9700
N2—C11.325 (2)C10—C111.518 (3)
N2—C21.370 (2)C10—H10A0.9700
N2—C161.467 (2)C10—H10B0.9700
O—H1O0.842 (18)C11—C121.521 (2)
O—H2O0.859 (18)C11—H11A0.9700
C1—H10.9300C11—H11B0.9700
C2—C31.347 (2)C12—C131.515 (3)
C2—H20.9300C12—H12A0.9700
C3—H30.9300C12—H12B0.9700
C4—C51.508 (3)C13—C141.513 (2)
C4—H4A0.9700C13—H13A0.9700
C4—H4B0.9700C13—H13B0.9700
C5—C61.520 (2)C14—C151.511 (3)
C5—H5A0.9700C14—H14A0.9700
C5—H5B0.9700C14—H14B0.9700
C6—C71.517 (3)C15—H15A0.9600
C6—H6A0.9700C15—H15B0.9600
C6—H6B0.9700C15—H15C0.9600
C7—C81.520 (2)C16—H16A0.9600
C7—H7A0.9700C16—H16B0.9600
C7—H7B0.9700C16—H16C0.9600
C8—C91.513 (3)C16—H16D0.9600
C8—H8A0.9700C16—H16E0.9600
C8—H8B0.9700C16—H16F0.9600
C1—N1—C3108.37 (15)C9—C10—H10B108.7
C1—N1—C4125.22 (15)C11—C10—H10B108.7
C3—N1—C4126.26 (15)H10A—C10—H10B107.6
C1—N2—C2108.71 (14)C10—C11—C12114.00 (16)
C1—N2—C16125.31 (16)C10—C11—H11A108.8
C2—N2—C16125.98 (16)C12—C11—H11A108.8
H1O—O—H2O103 (3)C10—C11—H11B108.8
N2—C1—N1108.66 (15)C12—C11—H11B108.8
N2—C1—H1125.7H11A—C11—H11B107.6
N1—C1—H1125.7C13—C12—C11114.36 (16)
C3—C2—N2106.90 (16)C13—C12—H12A108.7
C3—C2—H2126.5C11—C12—H12A108.7
N2—C2—H2126.5C13—C12—H12B108.7
C2—C3—N1107.36 (16)C11—C12—H12B108.7
C2—C3—H3126.3H12A—C12—H12B107.6
N1—C3—H3126.3C14—C13—C12114.63 (16)
N1—C4—C5113.05 (15)C14—C13—H13A108.6
N1—C4—H4A109.0C12—C13—H13A108.6
C5—C4—H4A109.0C14—C13—H13B108.6
N1—C4—H4B109.0C12—C13—H13B108.6
C5—C4—H4B109.0H13A—C13—H13B107.6
H4A—C4—H4B107.8C15—C14—C13114.08 (18)
C4—C5—C6110.22 (15)C15—C14—H14A108.7
C4—C5—H5A109.6C13—C14—H14A108.7
C6—C5—H5A109.6C15—C14—H14B108.7
C4—C5—H5B109.6C13—C14—H14B108.7
C6—C5—H5B109.6H14A—C14—H14B107.6
H5A—C5—H5B108.1C14—C15—H15A109.5
C7—C6—C5114.32 (16)C14—C15—H15B109.5
C7—C6—H6A108.7H15A—C15—H15B109.5
C5—C6—H6A108.7C14—C15—H15C109.5
C7—C6—H6B108.7H15A—C15—H15C109.5
C5—C6—H6B108.7H15B—C15—H15C109.5
H6A—C6—H6B107.6N2—C16—H16A109.5
C6—C7—C8113.41 (16)N2—C16—H16B109.5
C6—C7—H7A108.9H16A—C16—H16B109.5
C8—C7—H7A108.9N2—C16—H16C109.5
C6—C7—H7B108.9H16A—C16—H16C109.5
C8—C7—H7B108.9H16B—C16—H16C109.5
H7A—C7—H7B107.7N2—C16—H16D109.5
C9—C8—C7114.58 (16)H16A—C16—H16D141.1
C9—C8—H8A108.6H16B—C16—H16D56.3
C7—C8—H8A108.6H16C—C16—H16D56.3
C9—C8—H8B108.6N2—C16—H16E109.5
C7—C8—H8B108.6H16A—C16—H16E56.3
H8A—C8—H8B107.6H16B—C16—H16E141.1
C8—C9—C10113.90 (16)H16C—C16—H16E56.3
C8—C9—H9A108.8H16D—C16—H16E109.5
C10—C9—H9A108.8N2—C16—H16F109.5
C8—C9—H9B108.8H16A—C16—H16F56.3
C10—C9—H9B108.8H16B—C16—H16F56.3
H9A—C9—H9B107.7H16C—C16—H16F141.1
C9—C10—C11114.33 (16)H16D—C16—H16F109.5
C9—C10—H10A108.7H16E—C16—H16F109.5
C11—C10—H10A108.7
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O—H2O···Bri0.86 (2)2.57 (2)3.386 (3)159 (3)
O—H1O···Br0.84 (2)2.61 (2)3.435 (3)166 (3)
C3—H3···Bri0.932.753.661 (3)167
C1—H1···Oii0.932.343.193 (4)152
Symmetry codes: (i) x1, y, z; (ii) x+1, y1, z.
 

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