organic compounds
4-(Dimethylamino)pyridinium tribromide: whole molecule disorder of cation and anion
aDepartment of Chemistry, University of Malaya, 50603 Kuala Lumpur, Malaysia
*Correspondence e-mail: seikweng@um.edu.my
In the title salt, C7H11N2+·Br3−, the cation and the near-linear anion [Br—Br—Br = 179.41 (8)°] both show whole-molecule disorder about crystallographic twofold rotation axes. The cation is weakly hydrogen-bonded to the anion by an N—H⋯Br interaction. The crystal studied was found to be a racemic twin, with a twin component of nearly 50%.
Related literature
The compound is known commercially as 4-(dimethylamino)pyridine hydrobromide perbromide, [C7H10N2]·[HBr]·[Br2]. The 4-dimethylaminopyridinium cation furnishes a number of salts with organic and inorganic acids. For 4-dimethylaminopyridinium bromide, see: Mayr-Stein & Bolte (2000). For dimethylaminopyridinium chloride and its dihydrate, see: Bryant & King (1992); Chao et al. (1977).
Experimental
Crystal data
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Data collection: APEX2 (Bruker, 2008); cell SAINT (Bruker, 2008); 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: publCIF (Westrip, 2009).
Supporting information
10.1107/S1600536809017048/hb2966sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536809017048/hb2966Isup2.hkl
Commercially-available 4-dimethylaminopyridine hydrobromide perbromide was recrystallized from ethanol to give colourless blocks of (I).
The Br3 anion lies on a twofold rotation axis, but it was allowed to refine off this
as a three-atom species.The cation is disordered about another twofold rotation axis; this was refined as a cation with its atoms of half occupancies. The pyridyl portion was refined as a rigid hexagon of 1.39 Å sides; the pair of N–Cmethyl distances were restrained to within 0.01 Å of each other. The cation was restrained to be nearly planar, and the anisotropic displacement factors were restrained to be nearly isotropic.
The hydrogen atoms were placed at calculated positions (C–H 0.95, N–H 0.88 Å) and refined as riding with Uiso(H) = 1.2Ueq(C,N).
Data collection: APEX2 (Bruker, 2008); cell
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: pubCIF (Westrip, 2009).Fig. 1. Thermal ellipsoid plot (Barbour, 2001) of [C7H11N2][Br3] at the 70% probability level. Hydrogen atoms are drawn as spheres of arbitrary radius. |
C7H11N2+·Br3− | F(000) = 344 |
Mr = 362.91 | Dx = 2.222 Mg m−3 |
Orthorhombic, P2221 | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: P 2c 2 | Cell parameters from 2094 reflections |
a = 4.1688 (1) Å | θ = 2.7–28.3° |
b = 8.8349 (2) Å | µ = 11.11 mm−1 |
c = 14.7255 (4) Å | T = 100 K |
V = 542.35 (2) Å3 | Block, colorless |
Z = 2 | 0.20 × 0.15 × 0.10 mm |
Bruker SMART APEX CCD diffractometer | 1256 independent reflections |
Radiation source: fine-focus sealed tube | 1114 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.025 |
ω scans | θmax = 27.5°, θmin = 2.3° |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −5→5 |
Tmin = 0.656, Tmax = 1.000 | k = −11→11 |
5156 measured reflections | l = −19→19 |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.021 | H-atom parameters constrained |
wR(F2) = 0.051 | w = 1/[σ2(Fo2) + (0.0322P)2] where P = (Fo2 + 2Fc2)/3 |
S = 0.98 | (Δ/σ)max = 0.001 |
1256 reflections | Δρmax = 0.42 e Å−3 |
100 parameters | Δρmin = −0.34 e Å−3 |
60 restraints | Absolute structure: Flack (1983), 480 Friedel pairs |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: 0.47 (4) |
C7H11N2+·Br3− | V = 542.35 (2) Å3 |
Mr = 362.91 | Z = 2 |
Orthorhombic, P2221 | Mo Kα radiation |
a = 4.1688 (1) Å | µ = 11.11 mm−1 |
b = 8.8349 (2) Å | T = 100 K |
c = 14.7255 (4) Å | 0.20 × 0.15 × 0.10 mm |
Bruker SMART APEX CCD diffractometer | 1256 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | 1114 reflections with I > 2σ(I) |
Tmin = 0.656, Tmax = 1.000 | Rint = 0.025 |
5156 measured reflections |
R[F2 > 2σ(F2)] = 0.021 | H-atom parameters constrained |
wR(F2) = 0.051 | Δρmax = 0.42 e Å−3 |
S = 0.98 | Δρmin = −0.34 e Å−3 |
1256 reflections | Absolute structure: Flack (1983), 480 Friedel pairs |
100 parameters | Absolute structure parameter: 0.47 (4) |
60 restraints |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
Br1 | 0.5290 (6) | 0.25953 (5) | 0.23869 (12) | 0.0155 (3) | 0.50 |
Br2 | 0.2738 (3) | 0.27497 (11) | 0.07779 (5) | 0.0196 (2) | 0.50 |
Br3 | 0.7682 (3) | 0.24565 (11) | 0.39355 (5) | 0.01777 (18) | 0.50 |
N2 | 1.1882 (7) | 0.2417 (5) | −0.3550 (3) | 0.0144 (9) | 0.50 |
N1 | 0.7232 (7) | 0.2399 (4) | −0.10428 (15) | 0.0209 (11) | 0.50 |
H1 | 0.6250 | 0.2392 | −0.0514 | 0.025* | 0.50 |
C1 | 0.7724 (9) | 0.1050 (3) | −0.1509 (2) | 0.0190 (11) | 0.50 |
H1A | 0.7000 | 0.0122 | −0.1257 | 0.023* | 0.50 |
C2 | 0.9276 (8) | 0.1061 (3) | −0.23446 (19) | 0.0196 (13) | 0.50 |
H2 | 0.9612 | 0.0140 | −0.2663 | 0.024* | 0.50 |
C3 | 1.0335 (5) | 0.2420 (3) | −0.27138 (13) | 0.0147 (11) | 0.50 |
C4 | 0.9844 (9) | 0.3768 (3) | −0.2248 (2) | 0.0195 (12) | 0.50 |
H4 | 1.0568 | 0.4697 | −0.2500 | 0.023* | 0.50 |
C5 | 0.8292 (9) | 0.3757 (3) | −0.1412 (2) | 0.0208 (14) | 0.50 |
H5 | 0.7956 | 0.4679 | −0.1093 | 0.025* | 0.50 |
C6 | 1.2376 (13) | 0.1015 (6) | −0.4024 (3) | 0.0226 (13) | 0.50 |
H6A | 1.0314 | 0.0498 | −0.4102 | 0.034* | 0.50 |
H6B | 1.3829 | 0.0370 | −0.3672 | 0.034* | 0.50 |
H6C | 1.3321 | 0.1220 | −0.4620 | 0.034* | 0.50 |
C7 | 1.2983 (11) | 0.3839 (6) | −0.3936 (4) | 0.0223 (14) | 0.50 |
H7A | 1.1130 | 0.4479 | −0.4077 | 0.033* | 0.50 |
H7B | 1.4196 | 0.3638 | −0.4493 | 0.033* | 0.50 |
H7C | 1.4366 | 0.4359 | −0.3497 | 0.033* | 0.50 |
U11 | U22 | U33 | U12 | U13 | U23 | |
Br1 | 0.0195 (8) | 0.01421 (16) | 0.0128 (8) | −0.0005 (3) | 0.0021 (5) | −0.0007 (2) |
Br2 | 0.0201 (4) | 0.0274 (5) | 0.0112 (4) | 0.0019 (3) | 0.0015 (3) | −0.0010 (3) |
Br3 | 0.0210 (4) | 0.0207 (4) | 0.0116 (4) | −0.0011 (3) | 0.0007 (3) | 0.0001 (3) |
N2 | 0.021 (2) | 0.0110 (19) | 0.011 (2) | −0.001 (2) | −0.0034 (17) | 0.005 (2) |
N1 | 0.023 (3) | 0.032 (3) | 0.008 (2) | 0.007 (3) | 0.0025 (19) | −0.001 (2) |
C1 | 0.019 (3) | 0.021 (3) | 0.017 (3) | −0.001 (2) | −0.003 (3) | 0.002 (2) |
C2 | 0.012 (3) | 0.0175 (19) | 0.029 (4) | −0.0005 (16) | 0.004 (3) | 0.003 (2) |
C3 | 0.019 (2) | 0.0179 (18) | 0.008 (3) | −0.001 (3) | −0.002 (2) | 0.0001 (17) |
C4 | 0.020 (2) | 0.022 (2) | 0.016 (3) | −0.004 (3) | −0.005 (4) | 0.0004 (16) |
C5 | 0.019 (3) | 0.023 (3) | 0.020 (3) | 0.001 (2) | −0.001 (3) | 0.001 (3) |
C6 | 0.032 (3) | 0.019 (2) | 0.017 (3) | 0.000 (3) | −0.001 (4) | 0.004 (2) |
C7 | 0.023 (4) | 0.023 (3) | 0.020 (3) | 0.005 (2) | 0.008 (3) | −0.005 (2) |
Br1—Br3 | 2.492 (3) | C2—H2 | 0.9500 |
Br1—Br2 | 2.601 (3) | C3—C4 | 1.3900 |
N2—C3 | 1.390 (5) | C4—C5 | 1.3900 |
N2—C6 | 1.436 (7) | C4—H4 | 0.9500 |
N2—C7 | 1.454 (7) | C5—H5 | 0.9500 |
N1—C1 | 1.3900 | C6—H6A | 0.9800 |
N1—C5 | 1.3900 | C6—H6B | 0.9800 |
N1—H1 | 0.8800 | C6—H6C | 0.9800 |
C1—C2 | 1.3900 | C7—H7A | 0.9800 |
C1—H1A | 0.9500 | C7—H7B | 0.9800 |
C2—C3 | 1.3900 | C7—H7C | 0.9800 |
Br3—Br1—Br2 | 179.41 (8) | C5—C4—H4 | 120.0 |
C3—N2—C6 | 119.9 (4) | C3—C4—H4 | 120.0 |
C3—N2—C7 | 119.4 (4) | C4—C5—N1 | 120.0 |
C6—N2—C7 | 120.7 (4) | C4—C5—H5 | 120.0 |
C1—N1—C5 | 120.0 | N1—C5—H5 | 120.0 |
C1—N1—H1 | 120.0 | N2—C6—H6A | 109.5 |
C5—N1—H1 | 120.0 | N2—C6—H6B | 109.5 |
N1—C1—C2 | 120.0 | H6A—C6—H6B | 109.5 |
N1—C1—H1A | 120.0 | N2—C6—H6C | 109.5 |
C2—C1—H1A | 120.0 | H6A—C6—H6C | 109.5 |
C1—C2—C3 | 120.0 | H6B—C6—H6C | 109.5 |
C1—C2—H2 | 120.0 | N2—C7—H7A | 109.5 |
C3—C2—H2 | 120.0 | N2—C7—H7B | 109.5 |
N2—C3—C4 | 120.5 (3) | H7A—C7—H7B | 109.5 |
N2—C3—C2 | 119.5 (3) | N2—C7—H7C | 109.5 |
C4—C3—C2 | 120.0 | H7A—C7—H7C | 109.5 |
C5—C4—C3 | 120.0 | H7B—C7—H7C | 109.5 |
C5—N1—C1—C2 | 0.0 | C1—C2—C3—N2 | −179.96 (9) |
N1—C1—C2—C3 | 0.0 | C1—C2—C3—C4 | 0.0 |
C6—N2—C3—C4 | 179.95 (9) | N2—C3—C4—C5 | 179.96 (9) |
C7—N2—C3—C4 | −0.07 (11) | C2—C3—C4—C5 | 0.0 |
C6—N2—C3—C2 | −0.08 (13) | C3—C4—C5—N1 | 0.0 |
C7—N2—C3—C2 | 179.90 (9) | C1—N1—C5—C4 | 0.0 |
Experimental details
Crystal data | |
Chemical formula | C7H11N2+·Br3− |
Mr | 362.91 |
Crystal system, space group | Orthorhombic, P2221 |
Temperature (K) | 100 |
a, b, c (Å) | 4.1688 (1), 8.8349 (2), 14.7255 (4) |
V (Å3) | 542.35 (2) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 11.11 |
Crystal size (mm) | 0.20 × 0.15 × 0.10 |
Data collection | |
Diffractometer | Bruker SMART APEX CCD diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 1996) |
Tmin, Tmax | 0.656, 1.000 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 5156, 1256, 1114 |
Rint | 0.025 |
(sin θ/λ)max (Å−1) | 0.649 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.021, 0.051, 0.98 |
No. of reflections | 1256 |
No. of parameters | 100 |
No. of restraints | 60 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.42, −0.34 |
Absolute structure | Flack (1983), 480 Friedel pairs |
Absolute structure parameter | 0.47 (4) |
Computer programs: APEX2 (Bruker, 2008), SAINT (Bruker, 2008), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), X-SEED (Barbour, 2001), pubCIF (Westrip, 2009).
Acknowledgements
I thank the University of Malaya for supporting this study.
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