organic compounds
1-(2-Bromoethyl)-1,4-diazoniabicyclo[2.2.2]octane bromide tetrafluoroborate
aOrdered Matter Science Research Center, College of Chemistry and Chemical Engineering, Southeast University, Nanjing 211189, People's Republic of China
*Correspondence e-mail: xjm_cool@163.com
In the crystal of the title compound, C8H17BrN22+·Br−·BF4−, a weak intermolecular N—H⋯Br hydrogen bond is observed between the cation and the bromide anion. A two-part disorder model was applied to the BF4− anion with a refined major–minor occupancy ratio of 0.837 (14):0.163 (14).
Related literature
For the crystal structures and properties of related compounds, see: Chen et al.(2009); Fu et al. (2009); Zhao et al. (2008).
Experimental
Crystal data
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Refinement
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Data collection: CrystalClear (Rigaku, 2005); cell CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.
Supporting information
https://doi.org/10.1107/S1600536810017204/nk2032sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536810017204/nk2032Isup2.hkl
1,4-Diazabicyclo [2.2.2]octane (5.6 g, 0.05 mol) was dissolved in 20 ml of chloroform. To this solution 0.048 mol of 1,2-dibromoethane was added at once and the mixture was refluxed for 8 hours. On standing for 16 hours at room temperature, colorless crystals were obtained in large quantity. The crude product was collected and dissolved in 20 ml methanol, and 10ml HBF4 (1 mol/L) in methanol was added slowly with stirring, while white precipitate formed at once.The suspension was filtered, and dissolved in H2O, After a few weeks, colorless crystals were obtained by slow evaporation.
Positional parameters of all the H atoms except for H2 were calculated geometrically and the H atoms were set to ride on the C atoms to which they are bonded, with Uiso(H) = 1.2Ueq(C). The H2 on the N2 was freely refined. The BF4- anion was refined using a two-part disorder model with a major:minor occupancy ratio of 84:16%. Distance similarity and mild displacement parameter restraints were applied to the minor component.
The variable-temperature dielectric response, especially in relatively high frequency range, is very useful for searching phase transitions, in which there is a dielectric anomaly at the transition temperature. Unluckily, the title compound has no dielectric disuniform from 93 K to 453 K( m.p. > 473 K ) and report here.
In this report we have established unambiguously the structure at 293 K of the title compound in the solid state by X-ray
As shown in Fig. 1. Single crystal X-ray analysis reveals that there are weak hydrogen bonds between 1-(2-bromoethyl)-1,4-diazabicyclo[2.2.2]octane-1,4-diium cation and bromide anion.For the crystal structures and properties of related compounds, see: Chen et al. (2009); Fu et al. (2009); Zhao et al. (2008).
For the crystal structures and properties of related compounds, see: Chen et al.(2009); Fu et al. (2009); Zhao et al. (2008).
Data collection: CrystalClear (Rigaku, 2005); cell
CrystalClear (Rigaku, 2005); data reduction: CrystalClear (Rigaku, 2005); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).Fig. 1. The asymmetric unit of the title compound, showing the atomic numbering scheme. Displacement ellipsoids are drawn at the 30% probability level and the minor disorder component is omitted. |
C8H17BrN22+·BF4−·Br− | F(000) = 1520 |
Mr = 387.87 | Dx = 1.886 Mg m−3 |
Orthorhombic, Pbca | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ac 2ab | Cell parameters from 5732 reflections |
a = 11.972 (2) Å | θ = 3.7–27.5° |
b = 10.782 (2) Å | µ = 5.96 mm−1 |
c = 21.165 (4) Å | T = 293 K |
V = 2732.0 (10) Å3 | Prism, colourless |
Z = 8 | 0.3 × 0.25 × 0.2 mm |
Rigaku Mercury2 diffractometer | 3124 independent reflections |
Radiation source: fine-focus sealed tube | 1881 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.109 |
CCD_Profile_fitting scans | θmax = 27.5°, θmin = 3.2° |
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | h = −15→15 |
Tmin = 0.191, Tmax = 0.303 | k = −14→14 |
26313 measured reflections | l = −27→27 |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.058 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.108 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.04 | w = 1/[σ2(Fo2) + (0.0229P)2 + 7.8245P] where P = (Fo2 + 2Fc2)/3 |
3124 reflections | (Δ/σ)max < 0.001 |
198 parameters | Δρmax = 0.47 e Å−3 |
34 restraints | Δρmin = −0.47 e Å−3 |
C8H17BrN22+·BF4−·Br− | V = 2732.0 (10) Å3 |
Mr = 387.87 | Z = 8 |
Orthorhombic, Pbca | Mo Kα radiation |
a = 11.972 (2) Å | µ = 5.96 mm−1 |
b = 10.782 (2) Å | T = 293 K |
c = 21.165 (4) Å | 0.3 × 0.25 × 0.2 mm |
Rigaku Mercury2 diffractometer | 3124 independent reflections |
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | 1881 reflections with I > 2σ(I) |
Tmin = 0.191, Tmax = 0.303 | Rint = 0.109 |
26313 measured reflections |
R[F2 > 2σ(F2)] = 0.058 | 34 restraints |
wR(F2) = 0.108 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.04 | Δρmax = 0.47 e Å−3 |
3124 reflections | Δρmin = −0.47 e Å−3 |
198 parameters |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
Br1 | 0.71717 (5) | 0.02659 (6) | 0.01789 (3) | 0.0522 (2) | |
Br2 | 1.27841 (5) | 0.46079 (6) | 0.27319 (3) | 0.0510 (2) | |
C1 | 0.7924 (4) | 0.1425 (6) | 0.0745 (3) | 0.0471 (15) | |
H1A | 0.7844 | 0.2268 | 0.0592 | 0.057* | |
H1B | 0.7609 | 0.1375 | 0.1167 | 0.057* | |
C2 | 0.9138 (4) | 0.1047 (5) | 0.0752 (3) | 0.0411 (14) | |
H2A | 0.9423 | 0.1082 | 0.0324 | 0.049* | |
H2B | 0.9189 | 0.0193 | 0.0893 | 0.049* | |
C3 | 0.9635 (5) | 0.1612 (6) | 0.1856 (2) | 0.0523 (17) | |
H3A | 0.9787 | 0.0751 | 0.1957 | 0.063* | |
H3B | 0.8853 | 0.1774 | 0.1942 | 0.063* | |
C4 | 1.0354 (5) | 0.2443 (6) | 0.2262 (2) | 0.0464 (15) | |
H4A | 0.9891 | 0.3048 | 0.2478 | 0.056* | |
H4B | 1.0741 | 0.1953 | 0.2578 | 0.056* | |
C5 | 0.9738 (5) | 0.3202 (5) | 0.1038 (3) | 0.0402 (14) | |
H5A | 0.9839 | 0.3358 | 0.0590 | 0.048* | |
H5B | 0.8991 | 0.3465 | 0.1154 | 0.048* | |
C6 | 1.0584 (5) | 0.3924 (5) | 0.1409 (3) | 0.0466 (15) | |
H6A | 1.1116 | 0.4305 | 0.1124 | 0.056* | |
H6B | 1.0213 | 0.4578 | 0.1644 | 0.056* | |
C7 | 1.1075 (4) | 0.1500 (6) | 0.1040 (3) | 0.0512 (16) | |
H7A | 1.1266 | 0.1717 | 0.0609 | 0.061* | |
H7B | 1.1174 | 0.0612 | 0.1090 | 0.061* | |
C8 | 1.1838 (4) | 0.2187 (6) | 0.1496 (3) | 0.0491 (16) | |
H8A | 1.2188 | 0.1603 | 0.1783 | 0.059* | |
H8B | 1.2422 | 0.2612 | 0.1263 | 0.059* | |
N1 | 0.9874 (3) | 0.1842 (4) | 0.11705 (17) | 0.0266 (10) | |
N2 | 1.1176 (4) | 0.3085 (5) | 0.1852 (2) | 0.0397 (12) | |
H2 | 1.165 (6) | 0.349 (6) | 0.212 (3) | 0.09 (2)* | |
B1 | 0.4770 (8) | 0.2507 (9) | 0.0910 (4) | 0.0421 (19) | 0.837 (14) |
F1 | 0.5239 (8) | 0.1669 (6) | 0.1311 (3) | 0.086 (2) | 0.837 (14) |
F2 | 0.4322 (7) | 0.3475 (6) | 0.1246 (4) | 0.074 (2) | 0.837 (14) |
F3 | 0.3930 (7) | 0.1935 (9) | 0.0574 (5) | 0.090 (3) | 0.837 (14) |
F4 | 0.5562 (5) | 0.2945 (7) | 0.0483 (3) | 0.0681 (19) | 0.837 (14) |
B1' | 0.460 (3) | 0.244 (3) | 0.0923 (13) | 0.0421 (19) | 0.163 (14) |
F1' | 0.454 (3) | 0.186 (2) | 0.1488 (12) | 0.067 (7) | 0.163 (14) |
F2' | 0.401 (3) | 0.353 (3) | 0.0918 (18) | 0.065 (8) | 0.163 (14) |
F3' | 0.419 (4) | 0.168 (5) | 0.0460 (19) | 0.082 (9) | 0.163 (14) |
F4' | 0.569 (2) | 0.276 (4) | 0.078 (2) | 0.084 (9) | 0.163 (14) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Br1 | 0.0483 (4) | 0.0598 (4) | 0.0485 (4) | −0.0138 (3) | −0.0101 (3) | −0.0049 (3) |
Br2 | 0.0442 (4) | 0.0533 (4) | 0.0555 (4) | 0.0022 (3) | −0.0125 (3) | −0.0125 (3) |
C1 | 0.039 (3) | 0.056 (4) | 0.046 (4) | −0.010 (3) | −0.010 (3) | −0.010 (3) |
C2 | 0.036 (3) | 0.039 (3) | 0.048 (4) | −0.005 (3) | −0.004 (3) | −0.006 (3) |
C3 | 0.051 (4) | 0.072 (4) | 0.033 (3) | −0.020 (3) | 0.002 (3) | 0.015 (3) |
C4 | 0.047 (3) | 0.067 (4) | 0.025 (3) | 0.003 (3) | 0.000 (3) | 0.001 (3) |
C5 | 0.048 (3) | 0.027 (3) | 0.045 (3) | 0.006 (3) | −0.016 (3) | −0.003 (3) |
C6 | 0.064 (4) | 0.029 (3) | 0.047 (4) | −0.006 (3) | −0.007 (3) | 0.002 (3) |
C7 | 0.034 (3) | 0.052 (4) | 0.067 (4) | 0.009 (3) | 0.008 (3) | −0.017 (3) |
C8 | 0.028 (3) | 0.062 (4) | 0.057 (4) | 0.001 (3) | 0.002 (3) | −0.006 (3) |
N1 | 0.026 (2) | 0.026 (2) | 0.028 (2) | −0.0026 (19) | 0.0001 (18) | −0.0006 (18) |
N2 | 0.036 (3) | 0.049 (3) | 0.034 (3) | −0.011 (2) | −0.004 (2) | −0.002 (2) |
B1 | 0.043 (5) | 0.041 (4) | 0.043 (5) | −0.004 (4) | −0.009 (4) | 0.000 (3) |
F1 | 0.125 (7) | 0.079 (4) | 0.055 (4) | 0.022 (4) | −0.005 (4) | 0.019 (3) |
F2 | 0.087 (5) | 0.054 (3) | 0.080 (5) | 0.002 (3) | 0.021 (4) | −0.022 (4) |
F3 | 0.079 (5) | 0.118 (6) | 0.073 (5) | −0.021 (4) | −0.002 (4) | −0.040 (4) |
F4 | 0.063 (3) | 0.090 (4) | 0.051 (4) | 0.003 (3) | 0.012 (3) | 0.017 (3) |
B1' | 0.043 (5) | 0.041 (4) | 0.043 (5) | −0.004 (4) | −0.009 (4) | 0.000 (3) |
F1' | 0.092 (17) | 0.063 (13) | 0.047 (13) | 0.037 (13) | 0.009 (12) | −0.001 (11) |
F2' | 0.064 (15) | 0.048 (12) | 0.082 (18) | −0.007 (12) | 0.028 (14) | 0.004 (14) |
F3' | 0.096 (18) | 0.097 (17) | 0.052 (15) | −0.041 (16) | 0.000 (15) | −0.040 (13) |
F4' | 0.053 (14) | 0.099 (16) | 0.101 (19) | −0.009 (13) | 0.001 (15) | 0.015 (17) |
Br1—C1 | 1.952 (5) | C6—H6A | 0.9700 |
C1—C2 | 1.509 (7) | C6—H6B | 0.9700 |
C1—H1A | 0.9700 | C7—N1 | 1.510 (6) |
C1—H1B | 0.9700 | C7—C8 | 1.521 (8) |
C2—N1 | 1.515 (6) | C7—H7A | 0.9700 |
C2—H2A | 0.9700 | C7—H7B | 0.9700 |
C2—H2B | 0.9700 | C8—N2 | 1.461 (7) |
C3—N1 | 1.499 (6) | C8—H8A | 0.9700 |
C3—C4 | 1.511 (7) | C8—H8B | 0.9700 |
C3—H3A | 0.9700 | N2—H2 | 0.91 (7) |
C3—H3B | 0.9700 | B1—F1 | 1.361 (9) |
C4—N2 | 1.483 (7) | B1—F2 | 1.371 (9) |
C4—H4A | 0.9700 | B1—F3 | 1.377 (9) |
C4—H4B | 0.9700 | B1—F4 | 1.393 (9) |
C5—C6 | 1.500 (7) | B1'—F1' | 1.354 (19) |
C5—N1 | 1.502 (6) | B1'—F2' | 1.364 (19) |
C5—H5A | 0.9700 | B1'—F3' | 1.370 (19) |
C5—H5B | 0.9700 | B1'—F4' | 1.388 (19) |
C6—N2 | 1.484 (7) | ||
C2—C1—Br1 | 106.1 (4) | N1—C7—C8 | 109.7 (4) |
C2—C1—H1A | 110.5 | N1—C7—H7A | 109.7 |
Br1—C1—H1A | 110.5 | C8—C7—H7A | 109.7 |
C2—C1—H1B | 110.5 | N1—C7—H7B | 109.7 |
Br1—C1—H1B | 110.5 | C8—C7—H7B | 109.7 |
H1A—C1—H1B | 108.7 | H7A—C7—H7B | 108.2 |
C1—C2—N1 | 114.4 (4) | N2—C8—C7 | 108.9 (4) |
C1—C2—H2A | 108.7 | N2—C8—H8A | 109.9 |
N1—C2—H2A | 108.7 | C7—C8—H8A | 109.9 |
C1—C2—H2B | 108.7 | N2—C8—H8B | 109.9 |
N1—C2—H2B | 108.7 | C7—C8—H8B | 109.9 |
H2A—C2—H2B | 107.6 | H8A—C8—H8B | 108.3 |
N1—C3—C4 | 110.1 (4) | C3—N1—C5 | 108.8 (4) |
N1—C3—H3A | 109.6 | C3—N1—C7 | 108.5 (4) |
C4—C3—H3A | 109.6 | C5—N1—C7 | 107.9 (4) |
N1—C3—H3B | 109.6 | C3—N1—C2 | 111.2 (4) |
C4—C3—H3B | 109.6 | C5—N1—C2 | 112.3 (4) |
H3A—C3—H3B | 108.2 | C7—N1—C2 | 108.0 (4) |
N2—C4—C3 | 108.8 (4) | C8—N2—C4 | 110.7 (5) |
N2—C4—H4A | 109.9 | C8—N2—C6 | 109.7 (5) |
C3—C4—H4A | 109.9 | C4—N2—C6 | 109.7 (4) |
N2—C4—H4B | 109.9 | C8—N2—H2 | 108 (4) |
C3—C4—H4B | 109.9 | C4—N2—H2 | 106 (4) |
H4A—C4—H4B | 108.3 | C6—N2—H2 | 113 (4) |
C6—C5—N1 | 109.6 (4) | F1—B1—F2 | 110.1 (7) |
C6—C5—H5A | 109.8 | F1—B1—F3 | 109.0 (7) |
N1—C5—H5A | 109.8 | F2—B1—F3 | 108.8 (7) |
C6—C5—H5B | 109.8 | F1—B1—F4 | 110.4 (7) |
N1—C5—H5B | 109.8 | F2—B1—F4 | 110.1 (7) |
H5A—C5—H5B | 108.2 | F3—B1—F4 | 108.3 (7) |
N2—C6—C5 | 109.7 (4) | F1'—B1'—F2' | 112 (2) |
N2—C6—H6A | 109.7 | F1'—B1'—F3' | 109 (2) |
C5—C6—H6A | 109.7 | F2'—B1'—F3' | 109 (2) |
N2—C6—H6B | 109.7 | F1'—B1'—F4' | 111 (2) |
C5—C6—H6B | 109.7 | F2'—B1'—F4' | 106 (2) |
H6A—C6—H6B | 108.2 | F3'—B1'—F4' | 109 (2) |
Br1—C1—C2—N1 | −179.9 (4) | C8—C7—N1—C5 | 63.8 (6) |
N1—C3—C4—N2 | −8.1 (7) | C8—C7—N1—C2 | −174.6 (5) |
N1—C5—C6—N2 | −7.7 (6) | C1—C2—N1—C3 | 70.8 (6) |
N1—C7—C8—N2 | −7.9 (7) | C1—C2—N1—C5 | −51.3 (6) |
C4—C3—N1—C5 | −54.1 (6) | C1—C2—N1—C7 | −170.2 (5) |
C4—C3—N1—C7 | 63.1 (6) | C7—C8—N2—C4 | 65.3 (6) |
C4—C3—N1—C2 | −178.3 (5) | C7—C8—N2—C6 | −55.8 (6) |
C6—C5—N1—C3 | 63.3 (6) | C3—C4—N2—C8 | −56.3 (6) |
C6—C5—N1—C7 | −54.3 (6) | C3—C4—N2—C6 | 64.9 (6) |
C6—C5—N1—C2 | −173.2 (4) | C5—C6—N2—C8 | 65.9 (6) |
C8—C7—N1—C3 | −53.9 (6) | C5—C6—N2—C4 | −55.9 (6) |
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H2···Br2 | 0.91 (7) | 2.23 (7) | 3.141 (5) | 176 (6) |
Experimental details
Crystal data | |
Chemical formula | C8H17BrN22+·BF4−·Br− |
Mr | 387.87 |
Crystal system, space group | Orthorhombic, Pbca |
Temperature (K) | 293 |
a, b, c (Å) | 11.972 (2), 10.782 (2), 21.165 (4) |
V (Å3) | 2732.0 (10) |
Z | 8 |
Radiation type | Mo Kα |
µ (mm−1) | 5.96 |
Crystal size (mm) | 0.3 × 0.25 × 0.2 |
Data collection | |
Diffractometer | Rigaku Mercury2 |
Absorption correction | Multi-scan (CrystalClear; Rigaku, 2005) |
Tmin, Tmax | 0.191, 0.303 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 26313, 3124, 1881 |
Rint | 0.109 |
(sin θ/λ)max (Å−1) | 0.649 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.058, 0.108, 1.04 |
No. of reflections | 3124 |
No. of parameters | 198 |
No. of restraints | 34 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.47, −0.47 |
Computer programs: CrystalClear (Rigaku, 2005), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H2···Br2 | 0.91 (7) | 2.23 (7) | 3.141 (5) | 176 (6) |
Acknowledgements
This work was supported by a start-up grant from Southeast University.
References
Chen, L.-Z., Zhao, H., Ge, J.-Z., Wu, D.-H. & Xiong, R.-G. (2009). Cryst. Growth Des. 9, 3828–3831. Web of Science CSD CrossRef CAS Google Scholar
Fu, D.-W., Ge, J.-Z., Dai, J., Ye, H.-Y. & Qu, Z.-R. (2009). Inorg. Chem. Commun. 12, 994–997. Web of Science CSD CrossRef CAS Google Scholar
Rigaku (2005). CrystalClear. Rigaku Corporation, Tokyo, Japan. Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Zhao, H., Qu, Z.-R., Ye, H.-Y. & Xiong, R.-G. (2008). Chem. Soc. Rev. 37, 84–100. Web of Science CrossRef PubMed Google Scholar
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The variable-temperature dielectric response, especially in relatively high frequency range, is very useful for searching phase transitions, in which there is a dielectric anomaly at the transition temperature. Unluckily, the title compound has no dielectric disuniform from 93 K to 453 K( m.p. > 473 K ) and report here.
In this report we have established unambiguously the structure at 293 K of the title compound in the solid state by X-ray diffraction analysis. As shown in Fig. 1. Single crystal X-ray analysis reveals that there are weak hydrogen bonds between 1-(2-bromoethyl)-1,4-diazabicyclo[2.2.2]octane-1,4-diium cation and bromide anion.
For the crystal structures and properties of related compounds, see: Chen et al. (2009); Fu et al. (2009); Zhao et al. (2008).