The title compound, C
5H
6N
2O, was obtained as a side product during the synthesis of diimidazo[1,5-
a;1′,5′-
d]pyrazine-5,10-dione. The molecule is almost planar with the acetyl group inclined to the mean plane of the imidazole ring by 1.52 (12)°. In the crystal structure, molecules are linked by C—H
O and C—H
N hydrogen bonds, forming a sheet-like structure.
Supporting information
CCDC reference: 636658
Key indicators
- Single-crystal X-ray study
- T = 173 K
- Mean (C-C)= 0.001 Å
- R factor = 0.037
- wR factor = 0.099
- Data-to-parameter ratio = 14.2
checkCIF/PLATON results
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Data collection: X-AREA (Stoe & Cie, 2005); cell refinement: X-AREA; data reduction: X-RED32 (Stoe & Cie, 2005); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 2003); software used to prepare material for publication: SHELXL97.
1-(1
H-Imidazol-1-yl)ethanone
top
Crystal data top
C5H6N2O | F(000) = 232 |
Mr = 110.12 | Dx = 1.434 Mg m−3 |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2yn | Cell parameters from 6792 reflections |
a = 7.5263 (8) Å | θ = 2.7–29.6° |
b = 7.5835 (10) Å | µ = 0.10 mm−1 |
c = 9.0853 (10) Å | T = 173 K |
β = 100.361 (8)° | Rod, colourless |
V = 510.09 (10) Å3 | 0.50 × 0.34 × 0.23 mm |
Z = 4 | |
Data collection top
Stoe IPDS-2 diffractometer | 1208 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.064 |
Graphite monochromator | θmax = 29.2°, θmin = 3.2° |
ω and φ scans | h = −9→10 |
6541 measured reflections | k = −10→10 |
1380 independent reflections | l = −11→12 |
Refinement top
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)] = 0.037 | Hydrogen site location: difference Fourier map |
wR(F2) = 0.099 | All H-atom parameters refined |
S = 1.08 | w = 1/[σ2(Fo2) + (0.0443P)2 + 0.1063P] where P = (Fo2 + 2Fc2)/3 |
1380 reflections | (Δ/σ)max = 0.002 |
97 parameters | Δρmax = 0.31 e Å−3 |
0 restraints | Δρmin = −0.18 e Å−3 |
Special details top
Geometry. Bond distances, angles etc. have been calculated using the rounded
fractional coordinates. All su's are estimated from the variances of the
(full) variance-covariance matrix. The cell e.s.d.'s are taken into account in
the estimation of distances, angles and torsion angles |
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) top | x | y | z | Uiso*/Ueq | |
O1 | 0.54967 (10) | 0.09548 (9) | 0.27123 (8) | 0.0273 (2) | |
N1 | 0.73130 (10) | 0.00829 (10) | 0.48493 (9) | 0.0193 (2) | |
N2 | 0.90493 (12) | −0.11678 (11) | 0.68045 (10) | 0.0265 (2) | |
C1 | 0.84817 (13) | 0.03262 (13) | 0.61753 (11) | 0.0230 (3) | |
C2 | 0.82040 (14) | −0.24598 (13) | 0.58337 (12) | 0.0242 (3) | |
C3 | 0.71450 (13) | −0.17296 (12) | 0.46345 (11) | 0.0212 (2) | |
C4 | 0.64752 (12) | 0.13917 (12) | 0.38522 (11) | 0.0202 (2) | |
C5 | 0.69090 (14) | 0.32584 (13) | 0.43316 (12) | 0.0255 (3) | |
H1 | 0.8815 (19) | 0.1487 (19) | 0.6561 (17) | 0.033 (4)* | |
H2 | 0.8378 (19) | −0.3686 (18) | 0.6071 (17) | 0.031 (3)* | |
H3 | 0.6391 (18) | −0.2203 (18) | 0.3790 (17) | 0.028 (3)* | |
H4 | 0.818 (2) | 0.351 (2) | 0.4395 (18) | 0.041 (4)* | |
H5 | 0.626 (2) | 0.404 (2) | 0.363 (2) | 0.041 (4)* | |
H6 | 0.668 (2) | 0.348 (2) | 0.5363 (19) | 0.042 (4)* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
O1 | 0.0317 (4) | 0.0253 (4) | 0.0222 (4) | 0.0004 (3) | −0.0022 (3) | −0.0007 (3) |
N1 | 0.0211 (4) | 0.0173 (4) | 0.0191 (4) | −0.0016 (3) | 0.0023 (3) | −0.0011 (3) |
N2 | 0.0295 (4) | 0.0224 (4) | 0.0248 (4) | 0.0001 (3) | −0.0027 (3) | 0.0010 (3) |
C1 | 0.0249 (4) | 0.0207 (4) | 0.0214 (5) | −0.0013 (3) | −0.0011 (4) | −0.0012 (3) |
C2 | 0.0271 (5) | 0.0183 (4) | 0.0267 (5) | −0.0002 (3) | 0.0034 (4) | 0.0006 (3) |
C3 | 0.0231 (4) | 0.0181 (4) | 0.0226 (4) | −0.0025 (3) | 0.0046 (3) | −0.0029 (3) |
C4 | 0.0209 (4) | 0.0200 (4) | 0.0199 (4) | 0.0002 (3) | 0.0040 (3) | 0.0008 (3) |
C5 | 0.0283 (5) | 0.0178 (4) | 0.0288 (5) | −0.0005 (3) | 0.0007 (4) | 0.0010 (4) |
Geometric parameters (Å, º) top
O1—C4 | 1.2043 (12) | C4—C5 | 1.4997 (14) |
N1—C1 | 1.3704 (13) | C1—H1 | 0.964 (15) |
N1—C3 | 1.3909 (12) | C2—H2 | 0.958 (14) |
N1—C4 | 1.4135 (12) | C3—H3 | 0.940 (15) |
N2—C1 | 1.3058 (13) | C5—H4 | 0.967 (15) |
N2—C2 | 1.3931 (14) | C5—H5 | 0.940 (16) |
C2—C3 | 1.3478 (14) | C5—H6 | 0.997 (17) |
| | | |
C1—N1—C3 | 106.51 (8) | N2—C1—H1 | 126.2 (9) |
C1—N1—C4 | 127.64 (8) | N2—C2—H2 | 120.8 (9) |
C3—N1—C4 | 125.82 (8) | C3—C2—H2 | 128.1 (9) |
C1—N2—C2 | 104.88 (9) | N1—C3—H3 | 121.2 (9) |
N1—C1—N2 | 112.07 (9) | C2—C3—H3 | 133.3 (9) |
N2—C2—C3 | 111.05 (9) | C4—C5—H4 | 111.4 (9) |
N1—C3—C2 | 105.49 (8) | C4—C5—H5 | 109.8 (10) |
O1—C4—N1 | 119.42 (8) | C4—C5—H6 | 111.5 (9) |
O1—C4—C5 | 125.24 (9) | H4—C5—H5 | 107.7 (13) |
N1—C4—C5 | 115.34 (8) | H4—C5—H6 | 104.3 (13) |
N1—C1—H1 | 121.8 (9) | H5—C5—H6 | 112.0 (14) |
| | | |
C3—N1—C1—N2 | −0.20 (11) | C3—N1—C4—O1 | 1.18 (14) |
C4—N1—C1—N2 | −178.22 (9) | C3—N1—C4—C5 | −178.70 (9) |
C1—N1—C3—C2 | 0.27 (11) | C2—N2—C1—N1 | 0.04 (11) |
C4—N1—C3—C2 | 178.34 (9) | C1—N2—C2—C3 | 0.15 (12) |
C1—N1—C4—O1 | 178.83 (9) | N2—C2—C3—N1 | −0.26 (12) |
C1—N1—C4—C5 | −1.05 (14) | | |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
C1—H1···O1i | 0.964 (15) | 2.446 (15) | 3.3826 (13) | 163.9 (12) |
C3—H3···N2ii | 0.940 (15) | 2.597 (15) | 3.5252 (14) | 169.7 (12) |
Symmetry codes: (i) x+1/2, −y+1/2, z+1/2; (ii) x−1/2, −y−1/2, z−1/2. |