The experimental charge-density distribution in 2-methyl-1,3-cyclopentanedione in the crystal state was analyzed by synchrotron X-ray diffraction data collection at 0.33 Å resolution. The molecule in the crystal is in the enol form. The experimental electron density was refined using the Hansen–Coppens multipolar model and an alternative modeling, based on spherical atoms and additional charges on the covalent bonds and electron lone-pair sites. The crystallographic refinements, charge-density distributions, molecular electrostatic potentials, dipole moments and intermolecular interaction energies obtained from the different charge-density models were compared. The experimental results are also compared with the theoretical charge densities using theoretical structure factors obtained from periodic quantum calculations at the B3LYP/6-31G** level. A strong intermolecular O—H

O hydrogen bond connects molecules along the [001] direction. The deformation density maps show the resonance within the O=C—C=C—OH fragment and merged lone pair lobes on the hydroxyl O atom. This resonance is further confirmed by the analysis of charges and topology of the electron density.
Supporting information
CCDC reference: 972265
Program(s) used to refine structure: MoPro (J. Appl. Cryst. 2005, 38, 38-54); molecular graphics: MoproViewer.
2-methyl-1,3-cyclopentanedione
top
Crystal data top
C6H8O2 | Z = 4 |
Mr = 112.13 | F(000) = 240 |
Monoclinic, C2/m | Dx = 1.472 Mg m−3 |
Hall symbol: -c_2y | Synchrotron radiation, λ = 0.21784 Å |
a = 12.402 (3) Å | µ = 0.001 mm−1 |
b = 6.470 (2) Å | T = 100 K |
c = 6.321 (2) Å | , colourless |
β = 93.69 (2)° | 0.3 × 0.2 × 0.1 mm |
V = 506.2 (3) Å3 | |
Data collection top
Huber, ID11/ESRF diffractometer | θmax = 19.3°, θmin = 1.0° |
258713 measured reflections | h = −37→36 |
7435 independent reflections | k = 0→19 |
7319 reflections with > 2.0σ(I) | l = 0→19 |
Rint = 0.049 | |
Refinement top
Refinement on F | 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) = 0.031 | Only H-atom coordinates refined |
S = 1.05 | w = 1/[93.*σ2(Fo2)] |
7434 reflections | (Δ/σ)max < 0.001 |
186 parameters | Δρmax = 0.55 e Å−3 |
15 restraints | Δρmin = −0.36 e Å−3 |
Crystal data top
C6H8O2 | V = 506.2 (3) Å3 |
Mr = 112.13 | Z = 4 |
Monoclinic, C2/m | Synchrotron radiation, λ = 0.21784 Å |
a = 12.402 (3) Å | µ = 0.001 mm−1 |
b = 6.470 (2) Å | T = 100 K |
c = 6.321 (2) Å | 0.3 × 0.2 × 0.1 mm |
β = 93.69 (2)° | |
Data collection top
Huber, ID11/ESRF diffractometer | 7319 reflections with > 2.0σ(I) |
258713 measured reflections | Rint = 0.049 |
7435 independent reflections | |
Refinement top
R[F2 > 2σ(F2)] = 0.034 | 15 restraints |
wR(F2) = 0.031 | Only H-atom coordinates refined |
S = 1.05 | Δρmax = 0.55 e Å−3 |
7434 reflections | Δρmin = −0.36 e Å−3 |
186 parameters | |
Special details top
Refinement. Refinement of F1 against reflections. The threshold expression of
F2 > σ(F2) is used for calculating R-factors(gt) 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 | 0.30499 (2) | 0 | 1.06772 (3) | 0.0162 (2) | |
O3 | 0.178900 (10) | 0 | 0.36827 (2) | 0.0129 (2) | |
C1 | 0.302450 (10) | 0 | 0.87585 (2) | 0.0109 (2) | |
C2 | 0.210221 (1) | 0 | 0.73478 (2) | 0.0100 (2) | |
C3 | 0.243333 (1) | 0 | 0.53737 (2) | 0.0095 (2) | |
C4 | 0.361518 (1) | 0 | 0.52858 (2) | 0.0110 (2) | |
C5 | 0.401380 (10) | 0 | 0.75687 (2) | 0.0144 (2) | |
C21 | 0.100080 (10) | 0 | 0.80244 (2) | 0.0142 (2) | |
H3 | 0.22210 | 0 | 0.23608 | 0.02464 | |
H4 | 0.38786 | 0.13621 | 0.44339 | 0.02701 | |
H5 | 0.45004 | 0.13600 | 0.79766 | 0.03256 | |
H21A | 0.04227 | 0 | 0.67142 | 0.03257 | |
H21B | 0.08455 | 0.13300 | 0.89305 | 0.03115 | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
O1 | 0.0156 (6) | 0.0253 (6) | 0.0078 (6) | 0 | 0.00156 (5) | 0 |
O3 | 0.0117 (6) | 0.0178 (6) | 0.0091 (6) | 0 | −0.000006 (4) | 0 |
C1 | 0.0109 (6) | 0.0143 (6) | 0.0077 (6) | 0 | 0.00152 (4) | 0 |
C2 | 0.0094 (6) | 0.0122 (6) | 0.0085 (6) | 0 | 0.00215 (4) | 0 |
C3 | 0.0096 (6) | 0.0111 (6) | 0.0080 (6) | 0 | 0.00136 (4) | 0 |
C4 | 0.0101 (6) | 0.0140 (6) | 0.0091 (6) | 0 | 0.00234 (4) | 0 |
C5 | 0.0099 (6) | 0.0235 (6) | 0.0099 (6) | 0 | 0.00083 (4) | 0 |
C21 | 0.0108 (6) | 0.0180 (6) | 0.0142 (6) | 0 | 0.00403 (5) | 0 |
H3 | 0.0230 | 0.0353 | 0.0158 | 0 | 0.0024 | 0 |
H4 | 0.0263 | 0.0262 | 0.0291 | −0.0049 | 0.0058 | 0.0074 |
H5 | 0.0295 | 0.0412 | 0.0265 | −0.0138 | −0.0023 | −0.0041 |
H21A | 0.0217 | 0.0492 | 0.0262 | 0 | −0.0030 | 0 |
H21B | 0.0339 | 0.0293 | 0.0314 | 0.0036 | 0.0117 | −0.0056 |
Geometric parameters (Å, º) top
O1—C1 | 1.2112 (4) | C3—C4 | 1.4704 (4) |
O3—C3 | 1.2927 (4) | C4—C5 | 1.4950 (5) |
O3—H3 | 1.021 | C4—H4 | 1.094 |
C1—C2 | 1.4043 (4) | C5—H5 | 1.088 |
C1—C5 | 1.4798 (4) | C21—H21B | 1.058 |
C2—C3 | 1.3385 (4) | C21—H21A | 1.060 |
C2—C21 | 1.4574 (4) | | |
| | | |
O1—C1—C2 | 127.12 (6) | C2—C21—H21B | 111.4 |
O1—C1—C5 | 122.68 (5) | C2—C21—H21A | 111.7 |
O3—C3—C2 | 124.09 (3) | C3—O3—H3 | 110.3 |
O3—C3—C4 | 122.23 (4) | C3—C2—C21 | 128.55 (4) |
C1—C2—C3 | 107.80 (4) | C3—C4—C5 | 103.42 (4) |
C1—C2—C21 | 123.65 (3) | C3—C4—H4 | 110.4 |
C1—C5—C4 | 104.90 (4) | C4—C5—H5 | 111.9 |
C1—C5—H5 | 110.2 | C5—C4—H4 | 112.6 |
C2—C3—C4 | 113.68 (2) | H21A—C21—H21B | 106.6 |
C2—C1—C5 | 110.21 (4) | | |
| | | |
O1—C1—C2—C3 | 180 | C2—C3—O3—H3 | 180 |
O1—C1—C2—C21 | 0 | C2—C3—C4—C5 | 0 |
O1—C1—C5—C4 | 180 | C2—C3—C4—H4 | −120.7 |
O1—C1—C5—H5 | −59.4 | C2—C1—C5—C4 | 0 |
O3—C3—C2—C1 | 180 | C2—C1—C5—H5 | 120.6 |
O3—C3—C2—C21 | 0 | C3—C2—C1—C5 | 0 |
O3—C3—C4—C5 | 180 | C3—C2—C21—H21B | −119.1 |
O3—C3—C4—H4 | 59.3 | C3—C2—C21—H21A | 0 |
C1—C2—C3—C4 | 0 | C3—C4—C5—H5 | −119.4 |
C1—C2—C21—H21B | 60.9 | C4—C3—O3—H3 | 0 |
C1—C2—C21—H21A | 180 | C4—C3—C2—C21 | 180 |
C1—C5—C4—C3 | 0 | C5—C1—C2—C21 | 180 |
C1—C5—C4—H4 | 119.2 | H4—C4—C5—H5 | −0.2 |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
O3—H3···O1i | 1.021 | 1.526 | 2.5370 (6) | 169.4 |
Symmetry code: (i) x, y, z−1. |
Experimental details
Crystal data |
Chemical formula | C6H8O2 |
Mr | 112.13 |
Crystal system, space group | Monoclinic, C2/m |
Temperature (K) | 100 |
a, b, c (Å) | 12.402 (3), 6.470 (2), 6.321 (2) |
β (°) | 93.69 (2) |
V (Å3) | 506.2 (3) |
Z | 4 |
Radiation type | Synchrotron, λ = 0.21784 Å |
µ (mm−1) | 0.001 |
Crystal size (mm) | 0.3 × 0.2 × 0.1 |
|
Data collection |
Diffractometer | Huber, ID11/ESRF diffractometer |
Absorption correction | – |
No. of measured, independent and observed [ > 2.0σ(I)] reflections | 258713, 7435, 7319 |
Rint | 0.049 |
(sin θ/λ)max (Å−1) | 1.516 |
|
Refinement |
R[F2 > 2σ(F2)], wR(F2), S | 0.034, 0.031, 1.05 |
No. of reflections | 7434 |
No. of parameters | 186 |
No. of restraints | 15 |
H-atom treatment | Only H-atom coordinates refined |
Δρmax, Δρmin (e Å−3) | 0.55, −0.36 |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
O3—H3···O1i | 1.021 | 1.526 | 2.5370 (6) | 169.4 |
Symmetry code: (i) x, y, z−1. |