Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805035324/hg6248sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536805035324/hg6248Isup2.hkl |
CCDC reference: 293907
Data collection: APEXII (Bruker 2004); cell refinement: APEXII; data reduction: SAINT (Bruker 2004); program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker 2004); software used to prepare material for publication: SHELXTL.
C6H14N+·C2HCl2O2− | F(000) = 480 |
Mr = 228.10 | Dx = 1.380 Mg m−3 |
Orthorhombic, P212121 | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: P 2ac 2ab | Cell parameters from 5012 reflections |
a = 6.6435 (8) Å | θ = 2.6–28.6° |
b = 8.596 (1) Å | µ = 0.56 mm−1 |
c = 19.135 (2) Å | T = 293 K |
V = 1092.8 (2) Å3 | Block, colourless |
Z = 4 | 0.36 × 0.18 × 0.16 mm |
CCD area detector diffractometer | 2308 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.021 |
Graphite monochromator | θmax = 27.5°, θmin = 2.6° |
phi and ω scans | h = −8→8 |
9724 measured reflections | k = −11→11 |
2497 independent reflections | l = −23→24 |
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)] = 0.030 | H-atom parameters constrained |
wR(F2) = 0.078 | w = 1/[σ2(Fo2) + (0.0362P)2 + 0.2076P] where P = (Fo2 + 2Fc2)/3 |
S = 1.08 | (Δ/σ)max < 0.001 |
2497 reflections | Δρmax = 0.28 e Å−3 |
119 parameters | Δρmin = −0.30 e Å−3 |
0 restraints | Absolute structure: Flack (1983) |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: 0.02 (7) |
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. |
x | y | z | Uiso*/Ueq | ||
Cl1 | 0.79188 (9) | 0.84051 (6) | 0.09568 (4) | 0.06923 (18) | |
Cl2 | 0.40787 (7) | 0.68190 (5) | 0.10149 (3) | 0.05118 (14) | |
O1 | 0.6319 (2) | 0.43221 (14) | 0.02881 (8) | 0.0489 (3) | |
O2 | 0.9293 (2) | 0.54366 (16) | 0.04601 (10) | 0.0623 (4) | |
N1 | 0.2368 (2) | 0.32573 (16) | 0.05461 (8) | 0.0400 (3) | |
H1A | 0.3514 | 0.3734 | 0.0436 | 0.060* | |
H1B | 0.1346 | 0.3918 | 0.0497 | 0.060* | |
H1C | 0.2186 | 0.2446 | 0.0264 | 0.060* | |
C1 | 0.7440 (3) | 0.54286 (18) | 0.04346 (9) | 0.0361 (3) | |
C2 | 0.6372 (2) | 0.70105 (18) | 0.05455 (10) | 0.0373 (3) | |
H2 | 0.6034 | 0.7418 | 0.0082 | 0.045* | |
C3 | 0.2462 (3) | 0.2710 (2) | 0.12862 (10) | 0.0419 (4) | |
H3 | 0.2684 | 0.3613 | 0.1589 | 0.050* | |
C4 | 0.4200 (3) | 0.1595 (3) | 0.13795 (12) | 0.0576 (5) | |
H4A | 0.5452 | 0.2116 | 0.1264 | 0.069* | |
H4B | 0.4040 | 0.0719 | 0.1065 | 0.069* | |
C5 | 0.4285 (4) | 0.1012 (3) | 0.21307 (14) | 0.0737 (7) | |
H5A | 0.5355 | 0.0251 | 0.2175 | 0.088* | |
H5B | 0.4593 | 0.1875 | 0.2439 | 0.088* | |
C6 | 0.2320 (5) | 0.0283 (3) | 0.23508 (14) | 0.0756 (7) | |
H6A | 0.2104 | −0.0663 | 0.2085 | 0.091* | |
H6B | 0.2392 | 0.0005 | 0.2841 | 0.091* | |
C7 | 0.0571 (5) | 0.1366 (4) | 0.22380 (14) | 0.0770 (8) | |
H7A | 0.0690 | 0.2244 | 0.2554 | 0.092* | |
H7B | −0.0671 | 0.0825 | 0.2347 | 0.092* | |
C8 | 0.0481 (3) | 0.1958 (3) | 0.14873 (13) | 0.0590 (5) | |
H8A | 0.0200 | 0.1098 | 0.1174 | 0.071* | |
H8B | −0.0598 | 0.2711 | 0.1442 | 0.071* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cl1 | 0.0589 (3) | 0.0484 (3) | 0.1004 (4) | −0.0151 (2) | 0.0005 (3) | −0.0276 (3) |
Cl2 | 0.0435 (2) | 0.0401 (2) | 0.0699 (3) | 0.00055 (19) | 0.0143 (2) | −0.0091 (2) |
O1 | 0.0407 (7) | 0.0286 (6) | 0.0773 (9) | −0.0040 (5) | 0.0109 (6) | −0.0133 (6) |
O2 | 0.0338 (7) | 0.0378 (7) | 0.1151 (13) | 0.0066 (6) | −0.0001 (8) | 0.0053 (8) |
N1 | 0.0322 (7) | 0.0276 (6) | 0.0600 (8) | 0.0001 (6) | −0.0024 (7) | −0.0054 (6) |
C1 | 0.0351 (8) | 0.0262 (7) | 0.0470 (9) | 0.0029 (7) | 0.0030 (7) | 0.0033 (6) |
C2 | 0.0338 (8) | 0.0268 (7) | 0.0513 (9) | −0.0018 (6) | 0.0008 (7) | −0.0039 (7) |
C3 | 0.0398 (9) | 0.0304 (8) | 0.0554 (10) | −0.0028 (7) | −0.0002 (8) | −0.0084 (7) |
C4 | 0.0439 (10) | 0.0606 (13) | 0.0684 (13) | 0.0056 (10) | 0.0020 (10) | 0.0127 (10) |
C5 | 0.0708 (16) | 0.0781 (17) | 0.0723 (15) | 0.0058 (14) | −0.0059 (13) | 0.0191 (13) |
C6 | 0.098 (2) | 0.0617 (14) | 0.0668 (14) | −0.0034 (16) | 0.0133 (15) | 0.0121 (11) |
C7 | 0.0717 (16) | 0.0764 (17) | 0.0828 (17) | −0.0062 (14) | 0.0281 (14) | 0.0054 (14) |
C8 | 0.0411 (10) | 0.0575 (13) | 0.0784 (14) | −0.0041 (10) | 0.0105 (10) | −0.0024 (12) |
Cl1—C2 | 1.7641 (17) | C4—H4A | 0.9700 |
Cl2—C2 | 1.7763 (17) | C4—H4B | 0.9700 |
O1—C1 | 1.240 (2) | C5—C6 | 1.508 (4) |
O2—C1 | 1.232 (2) | C5—H5A | 0.9700 |
N1—C3 | 1.494 (2) | C5—H5B | 0.9700 |
N1—H1A | 0.8900 | C6—C7 | 1.504 (4) |
N1—H1B | 0.8900 | C6—H6A | 0.9700 |
N1—H1C | 0.8900 | C6—H6B | 0.9700 |
C1—C2 | 1.548 (2) | C7—C8 | 1.525 (4) |
C2—H2 | 0.9800 | C7—H7A | 0.9700 |
C3—C4 | 1.511 (3) | C7—H7B | 0.9700 |
C3—C8 | 1.516 (3) | C8—H8A | 0.9700 |
C3—H3 | 0.9800 | C8—H8B | 0.9700 |
C4—C5 | 1.523 (3) | ||
C3—N1—H1A | 109.5 | H4A—C4—H4B | 108.1 |
C3—N1—H1B | 109.5 | C6—C5—C4 | 111.6 (2) |
H1A—N1—H1B | 109.5 | C6—C5—H5A | 109.3 |
C3—N1—H1C | 109.5 | C4—C5—H5A | 109.3 |
H1A—N1—H1C | 109.5 | C6—C5—H5B | 109.3 |
H1B—N1—H1C | 109.5 | C4—C5—H5B | 109.3 |
O2—C1—O1 | 127.83 (16) | H5A—C5—H5B | 108.0 |
O2—C1—C2 | 116.59 (15) | C7—C6—C5 | 111.8 (2) |
O1—C1—C2 | 115.42 (15) | C7—C6—H6A | 109.3 |
C1—C2—Cl1 | 113.02 (12) | C5—C6—H6A | 109.3 |
C1—C2—Cl2 | 112.39 (11) | C7—C6—H6B | 109.3 |
Cl1—C2—Cl2 | 109.70 (10) | C5—C6—H6B | 109.3 |
C1—C2—H2 | 107.1 | H6A—C6—H6B | 107.9 |
Cl1—C2—H2 | 107.1 | C6—C7—C8 | 111.8 (2) |
Cl2—C2—H2 | 107.1 | C6—C7—H7A | 109.2 |
N1—C3—C4 | 110.13 (16) | C8—C7—H7A | 109.2 |
N1—C3—C8 | 109.78 (16) | C6—C7—H7B | 109.2 |
C4—C3—C8 | 111.28 (16) | C8—C7—H7B | 109.2 |
N1—C3—H3 | 108.5 | H7A—C7—H7B | 107.9 |
C4—C3—H3 | 108.5 | C3—C8—C7 | 110.3 (2) |
C8—C3—H3 | 108.5 | C3—C8—H8A | 109.6 |
C3—C4—C5 | 110.38 (19) | C7—C8—H8A | 109.6 |
C3—C4—H4A | 109.6 | C3—C8—H8B | 109.6 |
C5—C4—H4A | 109.6 | C7—C8—H8B | 109.6 |
C3—C4—H4B | 109.6 | H8A—C8—H8B | 108.1 |
C5—C4—H4B | 109.6 | ||
O2—C1—C2—Cl1 | −19.0 (2) | C3—C4—C5—C6 | 55.5 (3) |
O1—C1—C2—Cl1 | 165.27 (14) | C4—C5—C6—C7 | −54.3 (3) |
O2—C1—C2—Cl2 | −143.78 (16) | C5—C6—C7—C8 | 54.0 (3) |
O1—C1—C2—Cl2 | 40.4 (2) | N1—C3—C8—C7 | 178.94 (18) |
N1—C3—C4—C5 | −179.11 (18) | C4—C3—C8—C7 | 56.8 (3) |
C8—C3—C4—C5 | −57.1 (3) | C6—C7—C8—C3 | −55.0 (3) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1C···O1i | 0.89 | 1.94 | 2.8194 (19) | 170 |
N1—H1B···O2ii | 0.89 | 1.89 | 2.7765 (19) | 175 |
N1—H1A···Cl2 | 0.89 | 2.90 | 3.3868 (15) | 116 |
N1—H1A···O1 | 0.89 | 1.95 | 2.8237 (19) | 166 |
Symmetry codes: (i) x−1/2, −y+1/2, −z; (ii) x−1, y, z. |