Abstract
In the title compound, C16H21N2O+·Cl−, the amide group makes a dihedral angle of 25.9 (1)° with respect to the pyridine ring. In the crystal, intermolecular N—H⋯Cl bonds and weak C—H⋯Cl and C—H⋯O contacts link the cations and the anions into layers parallel to the ac plane. The layers are packed along [010] by hydrophobic interactions between adamantane units.
Related literature
For biomedical properties of adamantane-1-amine derivatives, see: Lees (2005 ▶); Nayyar et al. (2007 ▶). For ferroelectric properties of pyridinium salts, see: Ye et al. (2010 ▶); Zhang et al. (2010 ▶).
Experimental
Crystal data
C16H21N2O+·Cl−
M r = 292.80
Monoclinic,
a = 7.117 (4) Å
b = 23.093 (13) Å
c = 11.241 (5) Å
β = 127.56 (2)°
V = 1464.5 (13) Å3
Z = 4
Mo Kα radiation
μ = 0.26 mm−1
T = 293 K
0.20 × 0.20 × 0.20 mm
Data collection
Rigaku SCXmini diffractometer
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005 ▶) T min = 0.950, T max = 0.950
14193 measured reflections
3377 independent reflections
2910 reflections with I > 2σ(I)
R int = 0.042
Refinement
R[F 2 > 2σ(F 2)] = 0.056
wR(F 2) = 0.139
S = 1.11
3377 reflections
202 parameters
H-atom parameters constrained
Δρmax = 0.23 e Å−3
Δρmin = −0.22 e Å−3
Data collection: CrystalClear (Rigaku, 2005 ▶); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL/PC (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXTL/PC.
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810052499/si2302sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810052499/si2302Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N1—H1A⋯Cl1i | 0.90 | 2.16 | 3.017 (2) | 160 |
| N2—H2A⋯Cl1ii | 0.90 | 2.50 | 3.293 (2) | 147 |
| C2—H2B⋯Cl1iii | 0.96 | 2.79 | 3.535 (3) | 136 |
| C3—H3A⋯Cl1iv | 0.96 | 2.78 | 3.536 (3) | 136 |
| C4—H4A⋯O1ii | 0.96 | 2.35 | 3.203 (3) | 147 |
Symmetry codes: (i)
; (ii)
; (iii)
; (iv)
.
Acknowledgments
The author is grateful to the starter fund of Southeast University for financial support to buy the X-ray diffractometer.
supplementary crystallographic information
Comment
The study of amantadine and its derivatives has attracted much attention owing to their multifunction and technological applications in many areas, such as biomedicine (Lees 2005; Nayyar et al.2007). Amantadine can crystallize in different space groups owing to its randomness. As one part of our systematic research on dielectric, ferroelectric, and phase-transition materials (Ye et al. 2010; Zhang et al. 2010), we synthesize the title compound and investigated its dielectric property. In the range of 110 K to its melting point (428–432 K), the dielectric constant increases smoothly as a function of temperature. It means that this compound might not undergo a distinct structural phase transition in the measured temperature range.
The asymmetric unit of the title compound contains one protonated N- (1-adamantyl)isonicotinamide basic ion and one negative chlorine ion (Fig. 1). The torsion angles of C2—C1—C6—O1 and C2—C1—C6—N2 are 24.5 (3) ånd -157.5 (2) °, C5—C1—C6—O1 and C5—C1—C6—N2 are -151.3 (2) ° and 26.7 (3) °. Intermolecular N—H···Cl bonds and weak C—H···Cl and C—H···O contacts link cationic molecules parallel to (1 0 1) (Table 1). The layers are packed by hydrophobic interactions between adamantane units along the b-axis (Fig 2).
Experimental
Isonicotinic acid 5 g was added in thionyl chloride (50 ml), and the mixture reacted at 353 K for 5 h. Then the solvate was removed under reduced pressure, the isonicotinoyl chloride was obtained. The l-aminodiamantane hydrochloride (10 mmol) and triethylamine 2.02 g (20 mmol) dissolved in chloroform (40 ml) at 273 K, then the isonicotinoyl chloride 1.51 g (10 mmol) was added. Then the reactant mixture was stired for 7 h at room temperature and some flaxen solid appeared. After filtering the mixture, the solid was dissolved in water and was neutralized with sodium carbonate, The mixed solution was extracted by dichloromethane. The N-(1-adamantyl)isonicotinamide was obtained when the dichloromethane was evaporated under reduced pressure.
The N(1-adamantyl)isonicotinamide 2.56 g (10 mmol) was dissolved in methanol and the chlorhydric acid 1 ml (12 mmol/ml) was added. The crystals suitable for structure determination were grown by slow evaporation of the filter solution at room temperature.
Refinement
Positional parameters of all H atoms were calculated geometrically and were allowed to ride on the C and N atoms to which they are bonded, with N–H and C–H distances 0.90 Å and 0.96 Å, respectively. The isotropic displace ment parameters of the H atoms were refined freely with Uiso(H) = 1.7Ueq(N), and the Uiso(H) at carbon atoms range between 1.1 and 1.6Ueq(C).
Figures
Fig. 1.
The molecular structure of the title compound, with the atomic numbering scheme. Displacement ellipsoids are drawn at the 30% probability level.
Fig. 2.
A view of a packing section of the title compound, stacking along the b axis. Dashed lines indicate hydrogen bonds.
Crystal data
| C16H21N2O+·Cl− | F(000) = 624 |
| Mr = 292.80 | Dx = 1.328 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 3642 reflections |
| a = 7.117 (4) Å | θ = 2.9–27.6° |
| b = 23.093 (13) Å | µ = 0.26 mm−1 |
| c = 11.241 (5) Å | T = 293 K |
| β = 127.56 (2)° | Prism, colourless |
| V = 1464.5 (13) Å3 | 0.20 × 0.20 × 0.20 mm |
| Z = 4 |
Data collection
| Rigaku SCXmini diffractometer | 3377 independent reflections |
| Radiation source: fine-focus sealed tube | 2910 reflections with I > 2σ(I) |
| graphite | Rint = 0.042 |
| Detector resolution: 13.6612 pixels mm-1 | θmax = 27.6°, θmin = 2.9° |
| ω scans | h = −9→9 |
| Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | k = −30→30 |
| Tmin = 0.950, Tmax = 0.950 | l = −14→14 |
| 14193 measured reflections |
Refinement
| 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)] = 0.056 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.139 | H-atom parameters constrained |
| S = 1.11 | w = 1/[σ2(Fo2) + (0.0598P)2 + 0.5955P] where P = (Fo2 + 2Fc2)/3 |
| 3377 reflections | (Δ/σ)max = 0.041 |
| 202 parameters | Δρmax = 0.23 e Å−3 |
| 0 restraints | Δρmin = −0.22 e Å−3 |
Special details
| 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)
| x | y | z | Uiso*/Ueq | ||
| Cl1 | 0.13642 (10) | −0.01867 (2) | 0.85883 (6) | 0.03808 (17) | |
| O1 | 0.3301 (3) | −0.12489 (9) | 0.51605 (18) | 0.0531 (5) | |
| N1 | 0.6627 (4) | −0.03832 (8) | 0.2831 (2) | 0.0406 (5) | |
| H1A | 0.6865 | −0.0228 | 0.2198 | 0.070 (9)* | |
| N2 | 0.7203 (3) | −0.11813 (8) | 0.71977 (19) | 0.0345 (4) | |
| H2A | 0.8612 | −0.1036 | 0.7512 | 0.059 (8)* | |
| C1 | 0.5926 (4) | −0.08374 (9) | 0.4772 (2) | 0.0307 (4) | |
| C2 | 0.4096 (4) | −0.05633 (10) | 0.3459 (2) | 0.0375 (5) | |
| H2B | 0.2555 | −0.0532 | 0.3221 | 0.050 (7)* | |
| C3 | 0.4491 (4) | −0.03368 (10) | 0.2503 (3) | 0.0412 (5) | |
| H3A | 0.3237 | −0.0144 | 0.1599 | 0.053 (8)* | |
| C4 | 0.8423 (4) | −0.06503 (10) | 0.4063 (3) | 0.0426 (5) | |
| H4A | 0.9931 | −0.0680 | 0.4254 | 0.053 (8)* | |
| C5 | 0.8118 (4) | −0.08820 (10) | 0.5065 (3) | 0.0384 (5) | |
| H5A | 0.9410 | −0.1072 | 0.5959 | 0.050 (7)* | |
| C6 | 0.5359 (4) | −0.11061 (10) | 0.5753 (2) | 0.0349 (5) | |
| C7 | 0.7100 (3) | −0.14894 (8) | 0.8312 (2) | 0.0286 (4) | |
| C8 | 0.6137 (4) | −0.21041 (9) | 0.7764 (2) | 0.0381 (5) | |
| H8A | 0.4549 | −0.2086 | 0.6847 | 0.043 (7)* | |
| H8B | 0.7099 | −0.2307 | 0.7568 | 0.059 (8)* | |
| C9 | 0.9648 (4) | −0.15297 (10) | 0.9762 (2) | 0.0404 (5) | |
| H9A | 1.0617 | −0.1731 | 0.9569 | 0.057 (8)* | |
| H9B | 1.0284 | −0.1147 | 1.0111 | 0.044 (7)* | |
| C10 | 0.5588 (4) | −0.11689 (9) | 0.8641 (3) | 0.0376 (5) | |
| H10A | 0.6192 | −0.0784 | 0.8989 | 0.050 (7)* | |
| H10B | 0.3989 | −0.1139 | 0.7738 | 0.046 (7)* | |
| C11 | 0.6166 (4) | −0.24278 (9) | 0.8968 (3) | 0.0415 (5) | |
| H11A | 0.5551 | −0.2811 | 0.8615 | 0.057 (8)* | |
| C12 | 0.4621 (4) | −0.21057 (10) | 0.9256 (3) | 0.0427 (5) | |
| H12A | 0.3033 | −0.2080 | 0.8341 | 0.060 (8)* | |
| H12B | 0.4575 | −0.2313 | 0.9978 | 0.060 (8)* | |
| C13 | 0.5605 (4) | −0.15005 (10) | 0.9832 (3) | 0.0403 (5) | |
| H13A | 0.4650 | −0.1300 | 1.0037 | 0.064 (8)* | |
| C14 | 0.8703 (5) | −0.24643 (10) | 1.0405 (3) | 0.0463 (6) | |
| H14A | 0.8734 | −0.2675 | 1.1153 | 0.056 (8)* | |
| H14B | 0.9668 | −0.2668 | 1.0211 | 0.067 (9)* | |
| C15 | 0.9674 (4) | −0.18568 (11) | 1.0960 (2) | 0.0419 (5) | |
| H15A | 1.1271 | −0.1879 | 1.1867 | 0.053 (7)* | |
| C16 | 0.8150 (5) | −0.15348 (11) | 1.1268 (3) | 0.0450 (6) | |
| H16A | 0.8771 | −0.1152 | 1.1629 | 0.050 (7)* | |
| H16B | 0.8180 | −0.1735 | 1.2028 | 0.059 (8)* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cl1 | 0.0399 (3) | 0.0436 (3) | 0.0357 (3) | −0.0034 (2) | 0.0256 (3) | 0.0040 (2) |
| O1 | 0.0297 (9) | 0.0891 (13) | 0.0340 (9) | −0.0059 (8) | 0.0160 (7) | 0.0178 (8) |
| N1 | 0.0554 (12) | 0.0444 (10) | 0.0346 (10) | −0.0066 (9) | 0.0340 (10) | 0.0014 (8) |
| N2 | 0.0293 (9) | 0.0497 (10) | 0.0246 (8) | −0.0055 (7) | 0.0166 (8) | 0.0054 (7) |
| C1 | 0.0320 (10) | 0.0365 (10) | 0.0262 (10) | −0.0031 (8) | 0.0189 (9) | 0.0004 (8) |
| C2 | 0.0336 (11) | 0.0460 (12) | 0.0328 (11) | 0.0025 (9) | 0.0203 (10) | 0.0092 (9) |
| C3 | 0.0462 (13) | 0.0443 (12) | 0.0306 (11) | −0.0007 (10) | 0.0220 (11) | 0.0076 (9) |
| C4 | 0.0419 (13) | 0.0553 (14) | 0.0440 (13) | −0.0019 (10) | 0.0331 (12) | −0.0004 (10) |
| C5 | 0.0339 (11) | 0.0497 (13) | 0.0333 (11) | 0.0041 (9) | 0.0213 (10) | 0.0064 (9) |
| C6 | 0.0307 (11) | 0.0459 (12) | 0.0296 (11) | −0.0006 (8) | 0.0191 (9) | 0.0068 (8) |
| C7 | 0.0291 (10) | 0.0354 (10) | 0.0229 (9) | −0.0015 (8) | 0.0166 (8) | 0.0036 (7) |
| C8 | 0.0458 (13) | 0.0383 (12) | 0.0332 (11) | −0.0039 (9) | 0.0257 (11) | −0.0036 (9) |
| C9 | 0.0295 (11) | 0.0546 (14) | 0.0319 (11) | −0.0049 (9) | 0.0160 (10) | 0.0079 (10) |
| C10 | 0.0453 (13) | 0.0372 (11) | 0.0369 (12) | 0.0088 (9) | 0.0286 (11) | 0.0078 (9) |
| C11 | 0.0527 (14) | 0.0303 (11) | 0.0400 (12) | −0.0070 (9) | 0.0274 (11) | 0.0006 (9) |
| C12 | 0.0372 (12) | 0.0569 (14) | 0.0361 (12) | −0.0047 (10) | 0.0233 (11) | 0.0091 (10) |
| C13 | 0.0492 (14) | 0.0478 (13) | 0.0382 (12) | 0.0093 (10) | 0.0340 (12) | 0.0066 (9) |
| C14 | 0.0523 (15) | 0.0427 (13) | 0.0482 (14) | 0.0117 (10) | 0.0328 (13) | 0.0168 (10) |
| C15 | 0.0294 (11) | 0.0583 (14) | 0.0267 (11) | −0.0015 (9) | 0.0112 (9) | 0.0122 (9) |
| C16 | 0.0571 (15) | 0.0491 (14) | 0.0297 (12) | −0.0087 (11) | 0.0270 (12) | −0.0011 (9) |
Geometric parameters (Å, °)
| O1—C6 | 1.228 (3) | C9—C15 | 1.535 (3) |
| N1—C3 | 1.332 (3) | C9—H9A | 0.9600 |
| N1—C4 | 1.332 (3) | C9—H9B | 0.9601 |
| N1—H1A | 0.9000 | C10—C13 | 1.536 (3) |
| N2—C6 | 1.339 (3) | C10—H10A | 0.9602 |
| N2—C7 | 1.480 (2) | C10—H10B | 0.9599 |
| N2—H2A | 0.9000 | C11—C12 | 1.517 (3) |
| C1—C5 | 1.388 (3) | C11—C14 | 1.523 (4) |
| C1—C2 | 1.390 (3) | C11—H11A | 0.9599 |
| C1—C6 | 1.519 (3) | C12—C13 | 1.520 (3) |
| C2—C3 | 1.369 (3) | C12—H12A | 0.9599 |
| C2—H2B | 0.9601 | C12—H12B | 0.9600 |
| C3—H3A | 0.9599 | C13—C16 | 1.526 (3) |
| C4—C5 | 1.379 (3) | C13—H13A | 0.9601 |
| C4—H4A | 0.9601 | C14—C15 | 1.520 (4) |
| C5—H5A | 0.9599 | C14—H14A | 0.9601 |
| C7—C10 | 1.526 (3) | C14—H14B | 0.9600 |
| C7—C8 | 1.533 (3) | C15—C16 | 1.518 (3) |
| C7—C9 | 1.533 (3) | C15—H15A | 0.9600 |
| C8—C11 | 1.535 (3) | C16—H16A | 0.9599 |
| C8—H8A | 0.9600 | C16—H16B | 0.9599 |
| C8—H8B | 0.9600 | ||
| C3—N1—C4 | 122.33 (19) | C7—C10—C13 | 109.73 (17) |
| C3—N1—H1A | 118.9 | C7—C10—H10A | 109.9 |
| C4—N1—H1A | 118.8 | C13—C10—H10A | 110.0 |
| C6—N2—C7 | 124.82 (18) | C7—C10—H10B | 109.6 |
| C6—N2—H2A | 117.5 | C13—C10—H10B | 109.4 |
| C7—N2—H2A | 117.7 | H10A—C10—H10B | 108.2 |
| C5—C1—C2 | 118.42 (19) | C12—C11—C14 | 110.2 (2) |
| C5—C1—C6 | 123.72 (18) | C12—C11—C8 | 109.11 (19) |
| C2—C1—C6 | 117.73 (19) | C14—C11—C8 | 109.4 (2) |
| C3—C2—C1 | 120.0 (2) | C12—C11—H11A | 109.5 |
| C3—C2—H2B | 119.9 | C14—C11—H11A | 109.5 |
| C1—C2—H2B | 120.1 | C8—C11—H11A | 109.1 |
| N1—C3—C2 | 119.8 (2) | C11—C12—C13 | 109.63 (18) |
| N1—C3—H3A | 119.8 | C11—C12—H12A | 109.6 |
| C2—C3—H3A | 120.3 | C13—C12—H12A | 109.5 |
| N1—C4—C5 | 120.0 (2) | C11—C12—H12B | 109.8 |
| N1—C4—H4A | 119.9 | C13—C12—H12B | 110.1 |
| C5—C4—H4A | 120.1 | H12A—C12—H12B | 108.2 |
| C4—C5—C1 | 119.4 (2) | C12—C13—C16 | 110.15 (19) |
| C4—C5—H5A | 120.3 | C12—C13—C10 | 109.30 (19) |
| C1—C5—H5A | 120.2 | C16—C13—C10 | 108.74 (19) |
| O1—C6—N2 | 125.90 (19) | C12—C13—H13A | 109.7 |
| O1—C6—C1 | 118.23 (19) | C16—C13—H13A | 109.2 |
| N2—C6—C1 | 115.83 (18) | C10—C13—H13A | 109.8 |
| N2—C7—C10 | 112.20 (17) | C15—C14—C11 | 109.43 (18) |
| N2—C7—C8 | 110.26 (16) | C15—C14—H14A | 110.2 |
| C10—C7—C8 | 109.73 (17) | C11—C14—H14A | 109.7 |
| N2—C7—C9 | 107.00 (16) | C15—C14—H14B | 109.6 |
| C10—C7—C9 | 108.87 (18) | C11—C14—H14B | 109.7 |
| C8—C7—C9 | 108.68 (17) | H14A—C14—H14B | 108.2 |
| C11—C8—C7 | 109.54 (17) | C16—C15—C14 | 109.7 (2) |
| C11—C8—H8A | 110.0 | C16—C15—C9 | 109.31 (19) |
| C7—C8—H8A | 109.7 | C14—C15—C9 | 109.5 (2) |
| C11—C8—H8B | 109.7 | C16—C15—H15A | 109.4 |
| C7—C8—H8B | 109.7 | C14—C15—H15A | 109.5 |
| H8A—C8—H8B | 108.2 | C9—C15—H15A | 109.4 |
| C15—C9—C7 | 109.69 (17) | C15—C16—C13 | 109.68 (19) |
| C15—C9—H9A | 109.6 | C15—C16—H16A | 109.8 |
| C7—C9—H9A | 109.6 | C13—C16—H16A | 110.1 |
| C15—C9—H9B | 110.1 | C15—C16—H16B | 109.6 |
| C7—C9—H9B | 109.6 | C13—C16—H16B | 109.5 |
| H9A—C9—H9B | 108.2 | H16A—C16—H16B | 108.1 |
| C5—C1—C2—C3 | −1.1 (3) | C8—C7—C9—C15 | −59.8 (2) |
| C6—C1—C2—C3 | −177.1 (2) | N2—C7—C10—C13 | −178.48 (17) |
| C4—N1—C3—C2 | 0.7 (3) | C8—C7—C10—C13 | 58.6 (2) |
| C1—C2—C3—N1 | 0.4 (3) | C9—C7—C10—C13 | −60.2 (2) |
| C3—N1—C4—C5 | −1.1 (4) | C7—C8—C11—C12 | 60.1 (2) |
| N1—C4—C5—C1 | 0.4 (4) | C7—C8—C11—C14 | −60.6 (2) |
| C2—C1—C5—C4 | 0.6 (3) | C14—C11—C12—C13 | 58.8 (2) |
| C6—C1—C5—C4 | 176.4 (2) | C8—C11—C12—C13 | −61.3 (2) |
| C7—N2—C6—O1 | 4.6 (4) | C11—C12—C13—C16 | −58.4 (2) |
| C7—N2—C6—C1 | −173.26 (18) | C11—C12—C13—C10 | 61.0 (2) |
| C5—C1—C6—O1 | −151.3 (2) | C7—C10—C13—C12 | −59.5 (2) |
| C2—C1—C6—O1 | 24.5 (3) | C7—C10—C13—C16 | 60.8 (2) |
| C5—C1—C6—N2 | 26.7 (3) | C12—C11—C14—C15 | −59.6 (2) |
| C2—C1—C6—N2 | −157.5 (2) | C8—C11—C14—C15 | 60.4 (3) |
| C6—N2—C7—C10 | −66.8 (3) | C11—C14—C15—C16 | 59.8 (2) |
| C6—N2—C7—C8 | 55.8 (3) | C11—C14—C15—C9 | −60.2 (3) |
| C6—N2—C7—C9 | 173.9 (2) | C7—C9—C15—C16 | −59.9 (2) |
| N2—C7—C8—C11 | 177.02 (18) | C7—C9—C15—C14 | 60.2 (3) |
| C10—C7—C8—C11 | −58.9 (2) | C14—C15—C16—C13 | −59.6 (2) |
| C9—C7—C8—C11 | 60.0 (2) | C9—C15—C16—C13 | 60.6 (2) |
| N2—C7—C9—C15 | −178.89 (18) | C12—C13—C16—C15 | 59.0 (2) |
| C10—C7—C9—C15 | 59.6 (2) | C10—C13—C16—C15 | −60.8 (2) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1A···Cl1i | 0.90 | 2.16 | 3.017 (2) | 160. |
| N2—H2A···Cl1ii | 0.90 | 2.50 | 3.293 (2) | 147. |
| C2—H2B···Cl1iii | 0.96 | 2.79 | 3.535 (3) | 136. |
| C3—H3A···Cl1iv | 0.96 | 2.78 | 3.536 (3) | 136. |
| C4—H4A···O1ii | 0.96 | 2.35 | 3.203 (3) | 147. |
Symmetry codes: (i) −x+1, −y, −z+1; (ii) x+1, y, z; (iii) −x, −y, −z+1; (iv) x, y, z−1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SI2302).
References
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810052499/si2302sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810052499/si2302Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


