Abstract
In the title compound, C14H20N2O3·H2O, the geometry about the morpholine N atom implies sp 3 hybridization. In the crystal, symmetry-related molecules are linked by intermolecular N—H⋯O, O—H⋯O and O—H⋯N hydrogen bonds, forming infinite chains along the b axis. The chain structure is further stabilized by intramolecular C—H⋯O interactions.
Related literature
For related structures, see: Ahmad et al. (2009 ▶); Fun et al. (2010 ▶); Gowda et al. (2009a
▶,b
▶); Ma et al. (2009 ▶).
Experimental
Crystal data
C14H20N2O3·H2O
M r = 282.34
Triclinic,
a = 7.0560 (3) Å
b = 10.2859 (6) Å
c = 10.7234 (6) Å
α = 87.572 (3)°
β = 73.326 (3)°
γ = 79.876 (3)°
V = 733.92 (7) Å3
Z = 2
Mo Kα radiation
μ = 0.09 mm−1
T = 293 K
0.30 × 0.25 × 0.20 mm
Data collection
Bruker SMART CCD area-detector diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2001 ▶) T min = 0.603, T max = 0.705
17239 measured reflections
3723 independent reflections
2697 reflections with I > 2σ(I)
R int = 0.028
Refinement
R[F 2 > 2σ(F 2)] = 0.044
wR(F 2) = 0.138
S = 1.05
3723 reflections
194 parameters
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.20 e Å−3
Δρmin = −0.19 e Å−3
Data collection: SMART (Bruker, 2001 ▶); cell refinement: SAINT (Bruker, 2001 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: PLATON (Spek, 2009 ▶) and ZORTEP (Zsolnai, 1997 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶).
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810053675/jh2248sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810053675/jh2248Isup2.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—H1⋯O6i | 0.860 (18) | 2.157 (18) | 3.0148 (17) | 174.8 (14) |
| O6—H6A⋯O5 | 0.82 (2) | 2.06 (3) | 2.8640 (18) | 165 (2) |
| O6—H6B⋯N2 | 0.86 (3) | 2.11 (2) | 2.9586 (17) | 171 (2) |
| C4—H4⋯O1 | 0.93 (3) | 2.32 | 2.890 (2) | 120 |
Symmetry code: (i)
.
Acknowledgments
VG thanks the UGC, India, for financial assistance under Minor Research Project (2010–2011) and also thanks the Sophisticated Analytical Instrument Facility, IIT-Madras, Chennai, for the data collection. PP thanks the Research Fund of the University Institute of Pharmaceutical Sciences for its support to this work.
supplementary crystallographic information
Comment
Acetamide is important in the field of medicine as many biologically active compounds are synthesized by using acetamide. Benzanilides and benzamides exhibit wide range of biological activity and are extensively used in organic synthesis. Various N–substituted benzamides exhibit potent antiemetic activity (Ma et al., 2009). As a part of studying the ring and side-chain substitutions on the crystal structures of chemically and biologically important class of compounds such as acetanilides, we report herein the crystal structure of the title compound(I). The conformation of the N—H bond in the structure of the title compound(I), is anti to the C═O bond and to the phenyl ring as it has been observed in the related structures containing acetamide derivatives (Gowda et al.,2009a; Gowda et al.,2009b; Ahmad et al., 2009; Ma et al., 2009; Fun et al., 2010). Atom N1 has a trigonal configuration, the sum of three bond angles around them being 360°, whereas N2 atom is sp3 hybridized. The mean plane through the acetamide unit is inclined at a dihedral angle of 13.01 (11)° with respect to phenyl ring and 42.46 (8)° with respect to morpholine ring. The torsion angles and the least squares plane confirm that the morpholino ring is planar with the largest out-of-plane displacement of N2 (0.2458 (9) Å) and the phenyl ring is also planar with the root mean square deviation of 0.0034 Å.The morpholinoethoxy substitution at C6 [C4—C5—C6—O3=179.86 (13)°] is in anti-periplanar position. The exocyclic angle C2—N1—C3 [128.45 (11)°] deviates significantly from the normal value of 120°. This may be due to the intramolecular non-bonded interactions between atom O1 and H4 at C4 (O1······.H4 = 2.3159 Å). The widening of the exocyclic angle C5—C6—O3 [125.00 (12)°] deviate significantly from the normal value of 120° might be due to the consequence of repulsion between H5 and H9B at C9 (H5···H9B=2.3233 Å). The exocyclic angle O3—C9—C10 [103.45 (11)°] deviates by ca 6° from the tetrahedral value because of the intramolecular non-bonded interaction between O3 and H10A at C10 (O3···H10A = 2.3848 Å). The widening of the exocyclic angle C9—C10—N2[113.88 (11)°] from the normal value of 109° may be due to the repulsion between H9B and H11A [H9B···H11A = 2.3257 Å]. In the crystal structure, symmetry related molecules are linked by linear intermolecular N—H···O, O—H···O and O—H···N hydrogen bonds to form an infinite one-dimensional chain along the b axis.
Experimental
N-[4-Hydroxyphenyl]acetamide (1.0 g, 6.62 mmol) was dissolved in ethyl methyl ketone (100 ml) and anhydrous potassium carbonate (3.0–4.0 g) was added. The reaction mixture was refluxed for 2 hrs. To it 4-(2-chloroethyl) morpholine hydrochloride (1.0 g, 6.68 mmol) was added and the reaction mixture was further refluxed with continuous stirring for 7 h. Reaction was monitored with the help of TLC. The slurry obtained was filtered, the solvent was removed under reduced pressure and the solid obtained was crystallized from a mixture of ethyl acetate and ether to afford the title compound(I) (1.43 g, 81.81%), mp 100–102°C.
Refinement
Water H atoms were located in a difference Fourier maps and were included in the structure-factor calculations and isotropically refined. All the other H atoms were positioned geometrically and treated as riding on their parent atoms, with C—H = 0.93(aromatic),0.96(methyl) and 0.97Å (methylene),N—H = 0.86Å and refined using a riding model with Uiso(H) = 1.2Ueq or 1.5Ueq (parent atom).In the absence of significant anomalous scattering effects,Friedel pairs were merged.
Figures
Fig. 1.
The molecular structure of the title compound.Displacement ellipsoids are drawn at the 50% probability level.
Fig. 2.
Crystal packing of the title compound with intermolecular N—H···O, O—H···O and O—H···N hydrogen bonds shown as dashed lines.
Fig. 3.
Crystal Packing of the title compound viewed along the b axis.
Crystal data
| C14H20N2O3·H2O | V = 733.92 (7) Å3 |
| Mr = 282.34 | Z = 2 |
| Triclinic, P1 | F(000) = 304 |
| a = 7.0560 (3) Å | Dx = 1.278 Mg m−3 |
| b = 10.2859 (6) Å | Mo Kα radiation, λ = 0.71073 Å |
| c = 10.7234 (6) Å | µ = 0.09 mm−1 |
| α = 87.572 (3)° | T = 293 K |
| β = 73.326 (3)° | Block, colourless |
| γ = 79.876 (3)° | 0.30 × 0.25 × 0.20 mm |
Data collection
| Bruker SMART CCD area-detector diffractometer | 3723 independent reflections |
| Radiation source: fine-focus sealed tube | 2697 reflections with I > 2σ(I) |
| graphite | Rint = 0.028 |
| multi–scan | θmax = 28.5°, θmin = 2.0° |
| Absorption correction: multi-scan (SADABS; Bruker, 2001) | h = −6→9 |
| Tmin = 0.603, Tmax = 0.705 | k = −13→13 |
| 17239 measured reflections | l = −14→14 |
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)] = 0.044 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.138 | H atoms treated by a mixture of independent and constrained refinement |
| S = 1.05 | w = 1/[σ2(Fo2) + (0.0701P)2 + 0.1005P] where P = (Fo2 + 2Fc2)/3 |
| 3723 reflections | (Δ/σ)max < 0.001 |
| 194 parameters | Δρmax = 0.20 e Å−3 |
| 0 restraints | Δρmin = −0.19 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 | ||
| C1 | −1.0978 (2) | 0.87498 (15) | 0.43055 (17) | 0.0553 (4) | |
| H1A | −1.1906 | 0.8271 | 0.4103 | 0.083* | |
| H1B | −1.0726 | 0.9451 | 0.3692 | 0.083* | |
| H1C | −1.1540 | 0.9115 | 0.5169 | 0.083* | |
| C2 | −0.9045 (2) | 0.78313 (14) | 0.42318 (14) | 0.0469 (3) | |
| C3 | −0.54229 (18) | 0.74747 (11) | 0.30094 (12) | 0.0375 (3) | |
| C4 | −0.47022 (19) | 0.64413 (12) | 0.37122 (13) | 0.0424 (3) | |
| H4 | −0.5557 | 0.6167 | 0.4472 | 0.051* | |
| C5 | −0.27177 (19) | 0.58104 (12) | 0.32949 (13) | 0.0429 (3) | |
| H5 | −0.2246 | 0.5123 | 0.3778 | 0.051* | |
| C6 | −0.14488 (19) | 0.62023 (13) | 0.21659 (14) | 0.0455 (3) | |
| C7 | −0.2163 (2) | 0.72379 (15) | 0.14592 (15) | 0.0541 (4) | |
| H7 | −0.1311 | 0.7506 | 0.0696 | 0.065* | |
| C8 | −0.4117 (2) | 0.78676 (13) | 0.18802 (14) | 0.0465 (3) | |
| H8 | −0.4575 | 0.8567 | 0.1403 | 0.056* | |
| C9 | 0.1304 (2) | 0.45012 (14) | 0.22585 (16) | 0.0514 (4) | |
| H9A | 0.0572 | 0.3790 | 0.2243 | 0.062* | |
| H9B | 0.1241 | 0.4676 | 0.3152 | 0.062* | |
| C10 | 0.3450 (2) | 0.41666 (14) | 0.14270 (15) | 0.0492 (3) | |
| H10A | 0.3467 | 0.4195 | 0.0519 | 0.059* | |
| H10B | 0.4183 | 0.4836 | 0.1564 | 0.059* | |
| C11 | 0.4840 (2) | 0.28395 (14) | 0.29775 (15) | 0.0494 (3) | |
| H11A | 0.3564 | 0.2987 | 0.3649 | 0.059* | |
| H11B | 0.5564 | 0.3542 | 0.3040 | 0.059* | |
| C12 | 0.6040 (2) | 0.15244 (16) | 0.31893 (16) | 0.0588 (4) | |
| H12A | 0.6279 | 0.1526 | 0.4036 | 0.071* | |
| H12B | 0.5276 | 0.0829 | 0.3180 | 0.071* | |
| C13 | 0.7573 (2) | 0.12794 (15) | 0.09625 (16) | 0.0567 (4) | |
| H13A | 0.6811 | 0.0594 | 0.0917 | 0.068* | |
| H13B | 0.8851 | 0.1096 | 0.0296 | 0.068* | |
| C14 | 0.6448 (2) | 0.25923 (15) | 0.07117 (15) | 0.0516 (4) | |
| H14A | 0.7218 | 0.3279 | 0.0741 | 0.062* | |
| H14B | 0.6257 | 0.2590 | −0.0149 | 0.062* | |
| N1 | −0.74111 (16) | 0.81708 (11) | 0.33615 (12) | 0.0437 (3) | |
| N2 | 0.44861 (14) | 0.28678 (10) | 0.16958 (11) | 0.0406 (3) | |
| O1 | −0.89898 (17) | 0.68586 (13) | 0.49128 (14) | 0.0801 (4) | |
| O3 | 0.05217 (15) | 0.56571 (11) | 0.16672 (11) | 0.0655 (3) | |
| O5 | 0.79129 (15) | 0.12632 (12) | 0.22060 (12) | 0.0651 (3) | |
| O6 | 1.21505 (19) | 0.07084 (12) | 0.18771 (14) | 0.0651 (3) | |
| H1 | −0.757 (2) | 0.8870 (18) | 0.2907 (16) | 0.055 (4)* | |
| H6A | 1.095 (4) | 0.100 (2) | 0.202 (2) | 0.081 (6)* | |
| H6B | 1.275 (4) | 0.138 (2) | 0.177 (2) | 0.092 (7)* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0363 (7) | 0.0512 (8) | 0.0731 (10) | −0.0017 (6) | −0.0114 (6) | 0.0060 (7) |
| C2 | 0.0388 (7) | 0.0432 (7) | 0.0555 (8) | −0.0029 (5) | −0.0119 (6) | 0.0080 (6) |
| C3 | 0.0352 (6) | 0.0306 (6) | 0.0449 (7) | −0.0010 (5) | −0.0115 (5) | 0.0012 (5) |
| C4 | 0.0393 (6) | 0.0372 (6) | 0.0455 (7) | −0.0012 (5) | −0.0082 (5) | 0.0086 (5) |
| C5 | 0.0402 (6) | 0.0348 (6) | 0.0498 (7) | 0.0009 (5) | −0.0123 (5) | 0.0101 (5) |
| C6 | 0.0352 (6) | 0.0399 (7) | 0.0545 (8) | 0.0027 (5) | −0.0085 (5) | 0.0079 (6) |
| C7 | 0.0410 (7) | 0.0529 (8) | 0.0569 (9) | 0.0004 (6) | −0.0037 (6) | 0.0215 (7) |
| C8 | 0.0418 (7) | 0.0398 (7) | 0.0541 (8) | −0.0004 (5) | −0.0136 (6) | 0.0156 (6) |
| C9 | 0.0386 (7) | 0.0436 (7) | 0.0610 (9) | 0.0055 (5) | −0.0063 (6) | 0.0141 (6) |
| C10 | 0.0376 (7) | 0.0450 (7) | 0.0563 (8) | 0.0026 (5) | −0.0073 (6) | 0.0121 (6) |
| C11 | 0.0454 (7) | 0.0464 (7) | 0.0543 (8) | 0.0016 (6) | −0.0163 (6) | 0.0011 (6) |
| C12 | 0.0510 (8) | 0.0591 (9) | 0.0628 (9) | 0.0069 (7) | −0.0214 (7) | 0.0086 (7) |
| C13 | 0.0365 (7) | 0.0506 (8) | 0.0714 (10) | 0.0036 (6) | −0.0033 (6) | −0.0010 (7) |
| C14 | 0.0355 (7) | 0.0531 (8) | 0.0559 (8) | 0.0011 (6) | −0.0027 (6) | 0.0044 (6) |
| N1 | 0.0365 (5) | 0.0343 (6) | 0.0546 (7) | 0.0021 (4) | −0.0099 (5) | 0.0088 (5) |
| N2 | 0.0289 (5) | 0.0398 (6) | 0.0479 (6) | 0.0017 (4) | −0.0076 (4) | 0.0042 (4) |
| O1 | 0.0478 (6) | 0.0771 (8) | 0.0989 (10) | −0.0024 (6) | −0.0066 (6) | 0.0474 (7) |
| O3 | 0.0381 (5) | 0.0613 (7) | 0.0755 (7) | 0.0121 (5) | 0.0012 (5) | 0.0308 (6) |
| O5 | 0.0370 (5) | 0.0686 (7) | 0.0857 (8) | 0.0073 (5) | −0.0218 (5) | 0.0077 (6) |
| O6 | 0.0418 (6) | 0.0487 (6) | 0.1051 (10) | −0.0033 (5) | −0.0256 (6) | 0.0132 (6) |
Geometric parameters (Å, °)
| C1—C2 | 1.5007 (19) | C9—H9B | 0.9700 |
| C1—H1A | 0.9600 | C10—N2 | 1.4655 (16) |
| C1—H1B | 0.9600 | C10—H10A | 0.9700 |
| C1—H1C | 0.9600 | C10—H10B | 0.9700 |
| C2—O1 | 1.2151 (17) | C11—N2 | 1.4638 (18) |
| C2—N1 | 1.3483 (17) | C11—C12 | 1.510 (2) |
| C3—C4 | 1.3851 (17) | C11—H11A | 0.9700 |
| C3—C8 | 1.3883 (18) | C11—H11B | 0.9700 |
| C3—N1 | 1.4103 (15) | C12—O5 | 1.4250 (19) |
| C4—C5 | 1.3884 (17) | C12—H12A | 0.9700 |
| C4—H4 | 0.9300 | C12—H12B | 0.9700 |
| C5—C6 | 1.3760 (19) | C13—O5 | 1.420 (2) |
| C5—H5 | 0.9300 | C13—C14 | 1.497 (2) |
| C6—O3 | 1.3632 (15) | C13—H13A | 0.9700 |
| C6—C7 | 1.3873 (18) | C13—H13B | 0.9700 |
| C7—C8 | 1.3707 (18) | C14—N2 | 1.4695 (16) |
| C7—H7 | 0.9300 | C14—H14A | 0.9700 |
| C8—H8 | 0.9300 | C14—H14B | 0.9700 |
| C9—O3 | 1.4236 (16) | N1—H1 | 0.860 (18) |
| C9—C10 | 1.5079 (18) | O6—H6A | 0.82 (2) |
| C9—H9A | 0.9700 | O6—H6B | 0.86 (3) |
| C2—C1—H1A | 109.5 | N2—C10—H10B | 108.8 |
| C2—C1—H1B | 109.5 | C9—C10—H10B | 108.8 |
| H1A—C1—H1B | 109.5 | H10A—C10—H10B | 107.7 |
| C2—C1—H1C | 109.5 | N2—C11—C12 | 110.39 (12) |
| H1A—C1—H1C | 109.5 | N2—C11—H11A | 109.6 |
| H1B—C1—H1C | 109.5 | C12—C11—H11A | 109.6 |
| O1—C2—N1 | 123.54 (13) | N2—C11—H11B | 109.6 |
| O1—C2—C1 | 121.51 (13) | C12—C11—H11B | 109.6 |
| N1—C2—C1 | 114.95 (12) | H11A—C11—H11B | 108.1 |
| C4—C3—C8 | 118.57 (11) | O5—C12—C11 | 111.16 (13) |
| C4—C3—N1 | 124.49 (12) | O5—C12—H12A | 109.4 |
| C8—C3—N1 | 116.94 (11) | C11—C12—H12A | 109.4 |
| C3—C4—C5 | 120.70 (12) | O5—C12—H12B | 109.4 |
| C3—C4—H4 | 119.6 | C11—C12—H12B | 109.4 |
| C5—C4—H4 | 119.6 | H12A—C12—H12B | 108.0 |
| C6—C5—C4 | 120.00 (12) | O5—C13—C14 | 110.89 (13) |
| C6—C5—H5 | 120.0 | O5—C13—H13A | 109.5 |
| C4—C5—H5 | 120.0 | C14—C13—H13A | 109.5 |
| O3—C6—C5 | 125.00 (12) | O5—C13—H13B | 109.5 |
| O3—C6—C7 | 115.48 (12) | C14—C13—H13B | 109.5 |
| C5—C6—C7 | 119.51 (12) | H13A—C13—H13B | 108.0 |
| C8—C7—C6 | 120.36 (12) | N2—C14—C13 | 110.03 (11) |
| C8—C7—H7 | 119.8 | N2—C14—H14A | 109.7 |
| C6—C7—H7 | 119.8 | C13—C14—H14A | 109.7 |
| C7—C8—C3 | 120.84 (12) | N2—C14—H14B | 109.7 |
| C7—C8—H8 | 119.6 | C13—C14—H14B | 109.7 |
| C3—C8—H8 | 119.6 | H14A—C14—H14B | 108.2 |
| O3—C9—C10 | 103.45 (11) | C2—N1—C3 | 128.45 (11) |
| O3—C9—H9A | 111.1 | C2—N1—H1 | 118.1 (11) |
| C10—C9—H9A | 111.1 | C3—N1—H1 | 113.3 (11) |
| O3—C9—H9B | 111.1 | C11—N2—C10 | 111.50 (11) |
| C10—C9—H9B | 111.1 | C11—N2—C14 | 107.90 (11) |
| H9A—C9—H9B | 109.0 | C10—N2—C14 | 108.26 (10) |
| N2—C10—C9 | 113.88 (11) | C6—O3—C9 | 118.64 (10) |
| N2—C10—H10A | 108.8 | C13—O5—C12 | 109.68 (11) |
| C9—C10—H10A | 108.8 | H6A—O6—H6B | 106 (2) |
| C8—C3—C4—C5 | −0.1 (2) | C9—C10—N2—C11 | −68.97 (16) |
| N1—C3—C4—C5 | −179.93 (12) | C9—C10—N2—C14 | 172.48 (13) |
| C3—C4—C5—C6 | −0.6 (2) | C13—C14—N2—C11 | 58.35 (15) |
| C4—C5—C6—O3 | 179.86 (13) | C13—C14—N2—C10 | 179.16 (13) |
| C4—C5—C6—C7 | 0.7 (2) | C5—C6—O3—C9 | 7.5 (2) |
| O3—C6—C7—C8 | −179.30 (14) | C7—C6—O3—C9 | −173.29 (14) |
| C5—C6—C7—C8 | 0.0 (2) | C10—C9—O3—C6 | 177.79 (13) |
| C6—C7—C8—C3 | −0.7 (2) | C14—C13—O5—C12 | 59.49 (16) |
| C4—C3—C8—C7 | 0.8 (2) | C11—C12—O5—C13 | −58.19 (17) |
| N1—C3—C8—C7 | −179.40 (13) | O1—C2—N1—C3 | 4.2 (3) |
| O3—C9—C10—N2 | −169.50 (12) | C1—C2—N1—C3 | −175.68 (13) |
| N2—C11—C12—O5 | 58.19 (16) | C2—N1—C3—C4 | −15.1 (2) |
| O5—C13—C14—N2 | −60.57 (16) | C2—N1—C3—C8 | 165.11 (14) |
| O1—C2—N1—C3 | 4.2 (3) | C7—C6—O3—C9 | −173.29 (14) |
| C1—C2—N1—C3 | −175.68 (13) | C5—C6—O3—C9 | 7.5 (2) |
| C4—C3—N1—C2 | −15.1 (2) | C6—O3—C9—C10 | 177.79 (13) |
| C8—C3—N1—C2 | 165.11 (14) | O3—C9—C10—N2 | −169.50 (12) |
| C12—C11—N2—C10 | −175.90 (11) | C9—C10—N2—C11 | −68.97 (16) |
| C12—C11—N2—C14 | −57.14 (15) | C9—C10—N2—C14 | 172.48 (13) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1···O6i | 0.860 (18) | 2.157 (18) | 3.0148 (17) | 174.8 (14) |
| O6—H6A···O5 | 0.82 (2) | 2.06 (3) | 2.8640 (18) | 165 (2) |
| O6—H6B···N2ii | 0.86 (3) | 2.11 (2) | 2.9586 (17) | 171 (2) |
| C4—H4···O1 | 0.93 | 2.32 | 2.8896 (19) | 120 |
Symmetry codes: (i) x−2, y+1, z; (ii) .
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: JH2248).
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/S1600536810053675/jh2248sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810053675/jh2248Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report



