organic compounds
anti-Ethyl acetohydroximate
aInstitute of Chemistry, University of Silesia, 14 Bankowa Street, 40-007 Katowice, Poland, and bInstitute of Physics, University of Silesia, 4 Uniwersytecka Street, 40-007 Katowice, Poland
*Correspondence e-mail: bhachula@o2.pl
In the 4H9NO2, the O—H⋯N hydrogen bonds link the molecules into supramolecular chains extending along the b-axis direction. The conformation of the NOH group in the nearly planar (r.m.s. deviation = 0.0546 Å) ethyl acetohydroximate molecule is trans to N=C.
of the title compound, CRelated literature
For related structures, see: Kjaer et al. (1977); Larsen (1971). For studies of the IR spectra of hydrogen bonding in oxime derivatives, see: Flakus et al. (2012). For typical bond distances, see: Allen et al. (1987). For hydrogen-bond motifs, see: Bernstein et al. (1995); Etter et al. (1990).
Experimental
Crystal data
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Data collection: CrysAlis CCD (Oxford Diffraction, 2006); cell CrysAlis CCD; data reduction: CrysAlis RED (Oxford Diffraction, 2006); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: Mercury (Macrae et al., 2006); software used to prepare material for publication: publCIF (Westrip, 2010).
Supporting information
10.1107/S1600536813022368/ff2116sup1.cif
contains datablock I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536813022368/ff2116Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536813022368/ff2116Isup3.cml
Ethyl acetohydroximate was purchased from Aldrich-Sigma. Crystals of title compound, suitable for X-ray diffraction, were selected directly from purchased sample.
The H atoms were introduced in geometrically idealized positions with C—H distances of 0.99 Å and Uiso(H) values set at 1.2Ueq(C) for methylene group or 0.98 Å and with Uiso(H) values set at 1.5Ueq(C) for methyl groups. The H atom which takes part in hydrogen bonding was located in a difference Fourier map and was refined with Uiso(H) value set at 1.5Ueq(O).
Data collection: CrysAlis CCD (Oxford Diffraction, 2006); cell
CrysAlis RED (Oxford Diffraction, 2006); data reduction: CrysAlis RED (Oxford Diffraction, 2006); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: Mercury (Macrae et al., 2006); software used to prepare material for publication: publCIF (Westrip, 2010).C4H9NO2 | F(000) = 448 |
Mr = 103.12 | Dx = 1.235 Mg m−3 |
Monoclinic, C2/c | Melting point = 296–298 K |
Hall symbol: -C 2yc | Mo Kα radiation, λ = 0.71073 Å |
a = 19.9481 (9) Å | Cell parameters from 6376 reflections |
b = 4.4138 (1) Å | θ = 3.1–34.4° |
c = 13.3277 (5) Å | µ = 0.10 mm−1 |
β = 109.027 (4)° | T = 100 K |
V = 1109.35 (7) Å3 | Needle, colourless |
Z = 8 | 0.52 × 0.18 × 0.14 mm |
Oxford Diffraction Xcalibur diffractometer with a Sapphire3 detector | 970 independent reflections |
Radiation source: fine-focus sealed tube | 868 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.025 |
Detector resolution: 16.0328 pixels mm-1 | θmax = 25.1°, θmin = 3.2° |
ω–scan | h = −22→23 |
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2006) | k = −2→5 |
Tmin = 0.505, Tmax = 1.000 | l = −15→15 |
6699 measured reflections |
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)] = 0.034 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.098 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.08 | w = 1/[σ2(Fo2) + (0.0616P)2 + 0.5949P] where P = (Fo2 + 2Fc2)/3 |
970 reflections | (Δ/σ)max < 0.001 |
69 parameters | Δρmax = 0.22 e Å−3 |
0 restraints | Δρmin = −0.22 e Å−3 |
C4H9NO2 | V = 1109.35 (7) Å3 |
Mr = 103.12 | Z = 8 |
Monoclinic, C2/c | Mo Kα radiation |
a = 19.9481 (9) Å | µ = 0.10 mm−1 |
b = 4.4138 (1) Å | T = 100 K |
c = 13.3277 (5) Å | 0.52 × 0.18 × 0.14 mm |
β = 109.027 (4)° |
Oxford Diffraction Xcalibur diffractometer with a Sapphire3 detector | 970 independent reflections |
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2006) | 868 reflections with I > 2σ(I) |
Tmin = 0.505, Tmax = 1.000 | Rint = 0.025 |
6699 measured reflections |
R[F2 > 2σ(F2)] = 0.034 | 0 restraints |
wR(F2) = 0.098 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.08 | Δρmax = 0.22 e Å−3 |
970 reflections | Δρmin = −0.22 e Å−3 |
69 parameters |
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 | ||
O1 | 0.31644 (5) | 0.6668 (2) | 0.82875 (7) | 0.0201 (3) | |
O2 | 0.39491 (4) | 0.1706 (2) | 0.69431 (7) | 0.0185 (3) | |
N1 | 0.31725 (5) | 0.4501 (2) | 0.74954 (8) | 0.0165 (3) | |
C1 | 0.38102 (7) | 0.3704 (3) | 0.76216 (10) | 0.0158 (3) | |
C2 | 0.44623 (7) | 0.4799 (3) | 0.84598 (10) | 0.0215 (3) | |
H2A | 0.4568 | 0.6871 | 0.8294 | 0.032* | |
H2B | 0.4862 | 0.3472 | 0.8486 | 0.032* | |
H2C | 0.4385 | 0.4774 | 0.9149 | 0.032* | |
C3 | 0.33586 (7) | 0.0728 (3) | 0.60358 (10) | 0.0187 (3) | |
H3A | 0.3103 | 0.2503 | 0.5636 | 0.022* | |
H3B | 0.3022 | −0.0497 | 0.6271 | 0.022* | |
C4 | 0.36699 (8) | −0.1145 (3) | 0.53500 (11) | 0.0235 (3) | |
H4A | 0.3987 | 0.0118 | 0.5100 | 0.035* | |
H4B | 0.3287 | −0.1929 | 0.4739 | 0.035* | |
H4C | 0.3938 | −0.2843 | 0.5765 | 0.035* | |
H1 | 0.2735 (10) | 0.740 (4) | 0.8065 (13) | 0.035* |
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.0168 (5) | 0.0243 (5) | 0.0190 (5) | 0.0038 (4) | 0.0054 (4) | −0.0041 (4) |
O2 | 0.0153 (5) | 0.0230 (5) | 0.0163 (5) | 0.0012 (3) | 0.0041 (4) | −0.0017 (4) |
N1 | 0.0170 (6) | 0.0172 (6) | 0.0154 (6) | −0.0001 (4) | 0.0052 (4) | 0.0006 (4) |
C1 | 0.0167 (7) | 0.0174 (6) | 0.0140 (6) | 0.0000 (5) | 0.0062 (5) | 0.0034 (5) |
C2 | 0.0152 (7) | 0.0290 (7) | 0.0193 (7) | 0.0011 (5) | 0.0042 (5) | −0.0014 (6) |
C3 | 0.0175 (7) | 0.0201 (7) | 0.0164 (7) | −0.0019 (5) | 0.0026 (5) | 0.0002 (5) |
C4 | 0.0282 (7) | 0.0241 (7) | 0.0188 (7) | −0.0025 (6) | 0.0086 (6) | −0.0006 (5) |
O1—N1 | 1.4286 (13) | C2—H2C | 0.9800 |
O1—H1 | 0.871 (19) | C3—C4 | 1.5082 (17) |
O2—C1 | 1.3547 (15) | C3—H3A | 0.9900 |
O2—C3 | 1.4517 (15) | C3—H3B | 0.9900 |
N1—C1 | 1.2771 (17) | C4—H4A | 0.9800 |
C1—C2 | 1.4922 (17) | C4—H4B | 0.9800 |
C2—H2A | 0.9800 | C4—H4C | 0.9800 |
C2—H2B | 0.9800 | ||
N1—O1—H1 | 104.1 (11) | O2—C3—C4 | 106.57 (10) |
C1—O2—C3 | 117.55 (9) | O2—C3—H3A | 110.4 |
C1—N1—O1 | 109.76 (10) | C4—C3—H3A | 110.4 |
N1—C1—O2 | 120.21 (12) | O2—C3—H3B | 110.4 |
N1—C1—C2 | 126.66 (12) | C4—C3—H3B | 110.4 |
O2—C1—C2 | 113.11 (10) | H3A—C3—H3B | 108.6 |
C1—C2—H2A | 109.5 | C3—C4—H4A | 109.5 |
C1—C2—H2B | 109.5 | C3—C4—H4B | 109.5 |
H2A—C2—H2B | 109.5 | H4A—C4—H4B | 109.5 |
C1—C2—H2C | 109.5 | C3—C4—H4C | 109.5 |
H2A—C2—H2C | 109.5 | H4A—C4—H4C | 109.5 |
H2B—C2—H2C | 109.5 | H4B—C4—H4C | 109.5 |
O1—N1—C1—O2 | −178.49 (9) | C3—O2—C1—C2 | −174.04 (10) |
O1—N1—C1—C2 | 0.24 (17) | C1—O2—C3—C4 | 173.10 (10) |
C3—O2—C1—N1 | 4.85 (16) |
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1···N1i | 0.871 (19) | 1.954 (19) | 2.8196 (14) | 172.4 (16) |
Symmetry code: (i) −x+1/2, y+1/2, −z+3/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1···N1i | 0.871 (19) | 1.954 (19) | 2.8196 (14) | 172.4 (16) |
Symmetry code: (i) −x+1/2, y+1/2, −z+3/2. |
References
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Anti-ethyl acetohydroximate [systematic name: ethyl N-hydroxyacetimidate], (I), was investigated in a continuation of our studies of the IR spectra of hydrogen bonding in oxime derivatives (Flakus et al., 2012). In order to study interactions occurring via hydrogen bonds and molecular packing in this compound, we have now determined the structure of (I) using diffraction data collected at 100 K. Until now, the structures of syn-methyl acetohydroximate and syn- and anti-ethyl benzohydroximate were determined (Kjaer et al., 1977; Larsen et al., 1971). The crystal structure of syn-methyl acetohydroximate is composed of layers of molecules, which form cyclic, hydrogen-bonded trimers, whereas the crystals of syn- and anti-ethyl benzohydroximate are composed of dimers formed by pairs of O—H···N hydrogen- bonded molecules.
The molecule of (I) is nearly planar (r.m.s. deviations 0.0546 Å for all non-H atoms). The lengths of the bonds C=N (1.2771 (17) Å) and N—O (1.4286 (13) Å) in (I) are comparable to the mean values found in other oximes (C=N 1.281 Å; N—O 1.394 Å) (Allen et al., 1987). The conformation of the NOH group in the planar ethyl acetohydroximate molecule is trans to N=C. In the crystal, O—H···N are observed forming infinite chains along the b axis (Fig. 2) with a graph-set motif of C(3) (Etter et al., 1990; Bernstein et al., 1995).