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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

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520613031375/pi5017sup1.cif
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520613031375/pi5017Isup2.hkl
Contains datablock I

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2052520613031375/pi5017sup3.pdf
Supplementary tigures and tables

CCDC reference: 972265

Computing details top

Program(s) used to refine structure: MoPro (J. Appl. Cryst. 2005, 38, 38-54); molecular graphics: MoproViewer.

Figures top
[Figure 1]
[Figure 2]
[Figure 3]
[Figure 4]
[Figure 5]
[Figure 6]
[Figure 7]
[Figure 8]
[Figure 9]
[Figure 10]
2-methyl-1,3-cyclopentanedione top
Crystal data top
C6H8O2Z = 4
Mr = 112.13F(000) = 240
Monoclinic, C2/mDx = 1.472 Mg m3
Hall symbol: -c_2ySynchrotron radiation, λ = 0.21784 Å
a = 12.402 (3) ŵ = 0.001 mm1
b = 6.470 (2) ÅT = 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 reflectionsh = 3736
7435 independent reflectionsk = 019
7319 reflections with > 2.0σ(I)l = 019
Rint = 0.049
Refinement top
Refinement on FPrimary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.034Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.031Only H-atom coordinates refined
S = 1.05 w = 1/[93.*σ2(Fo2)]
7434 reflections(Δ/σ)max < 0.001
186 parametersΔρmax = 0.55 e Å3
15 restraintsΔρmin = 0.36 e Å3
Crystal data top
C6H8O2V = 506.2 (3) Å3
Mr = 112.13Z = 4
Monoclinic, C2/mSynchrotron radiation, λ = 0.21784 Å
a = 12.402 (3) ŵ = 0.001 mm1
b = 6.470 (2) ÅT = 100 K
c = 6.321 (2) Å0.3 × 0.2 × 0.1 mm
β = 93.69 (2)°
Data collection top
Huber, ID11/ESRF
diffractometer
7319 reflections with > 2.0σ(I)
258713 measured reflectionsRint = 0.049
7435 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.03415 restraints
wR(F2) = 0.031Only H-atom coordinates refined
S = 1.05Δρmax = 0.55 e Å3
7434 reflectionsΔρmin = 0.36 e Å3
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
xyzUiso*/Ueq
O10.30499 (2)01.06772 (3)0.0162 (2)
O30.178900 (10)00.36827 (2)0.0129 (2)
C10.302450 (10)00.87585 (2)0.0109 (2)
C20.210221 (1)00.73478 (2)0.0100 (2)
C30.243333 (1)00.53737 (2)0.0095 (2)
C40.361518 (1)00.52858 (2)0.0110 (2)
C50.401380 (10)00.75687 (2)0.0144 (2)
C210.100080 (10)00.80244 (2)0.0142 (2)
H30.2221000.236080.02464
H40.387860.136210.443390.02701
H50.450040.136000.797660.03256
H21A0.0422700.671420.03257
H21B0.084550.133000.893050.03115
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0156 (6)0.0253 (6)0.0078 (6)00.00156 (5)0
O30.0117 (6)0.0178 (6)0.0091 (6)00.000006 (4)0
C10.0109 (6)0.0143 (6)0.0077 (6)00.00152 (4)0
C20.0094 (6)0.0122 (6)0.0085 (6)00.00215 (4)0
C30.0096 (6)0.0111 (6)0.0080 (6)00.00136 (4)0
C40.0101 (6)0.0140 (6)0.0091 (6)00.00234 (4)0
C50.0099 (6)0.0235 (6)0.0099 (6)00.00083 (4)0
C210.0108 (6)0.0180 (6)0.0142 (6)00.00403 (5)0
H30.02300.03530.015800.00240
H40.02630.02620.02910.00490.00580.0074
H50.02950.04120.02650.01380.00230.0041
H21A0.02170.04920.026200.00300
H21B0.03390.02930.03140.00360.01170.0056
Geometric parameters (Å, º) top
O1—C11.2112 (4)C3—C41.4704 (4)
O3—C31.2927 (4)C4—C51.4950 (5)
O3—H31.021C4—H41.094
C1—C21.4043 (4)C5—H51.088
C1—C51.4798 (4)C21—H21B1.058
C2—C31.3385 (4)C21—H21A1.060
C2—C211.4574 (4)
O1—C1—C2127.12 (6)C2—C21—H21B111.4
O1—C1—C5122.68 (5)C2—C21—H21A111.7
O3—C3—C2124.09 (3)C3—O3—H3110.3
O3—C3—C4122.23 (4)C3—C2—C21128.55 (4)
C1—C2—C3107.80 (4)C3—C4—C5103.42 (4)
C1—C2—C21123.65 (3)C3—C4—H4110.4
C1—C5—C4104.90 (4)C4—C5—H5111.9
C1—C5—H5110.2C5—C4—H4112.6
C2—C3—C4113.68 (2)H21A—C21—H21B106.6
C2—C1—C5110.21 (4)
O1—C1—C2—C3180C2—C3—O3—H3180
O1—C1—C2—C210C2—C3—C4—C50
O1—C1—C5—C4180C2—C3—C4—H4120.7
O1—C1—C5—H559.4C2—C1—C5—C40
O3—C3—C2—C1180C2—C1—C5—H5120.6
O3—C3—C2—C210C3—C2—C1—C50
O3—C3—C4—C5180C3—C2—C21—H21B119.1
O3—C3—C4—H459.3C3—C2—C21—H21A0
C1—C2—C3—C40C3—C4—C5—H5119.4
C1—C2—C21—H21B60.9C4—C3—O3—H30
C1—C2—C21—H21A180C4—C3—C2—C21180
C1—C5—C4—C30C5—C1—C2—C21180
C1—C5—C4—H4119.2H4—C4—C5—H50.2
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O3—H3···O1i1.0211.5262.5370 (6)169.4
Symmetry code: (i) x, y, z1.

Experimental details

Crystal data
Chemical formulaC6H8O2
Mr112.13
Crystal system, space groupMonoclinic, C2/m
Temperature (K)100
a, b, c (Å)12.402 (3), 6.470 (2), 6.321 (2)
β (°) 93.69 (2)
V3)506.2 (3)
Z4
Radiation typeSynchrotron, λ = 0.21784 Å
µ (mm1)0.001
Crystal size (mm)0.3 × 0.2 × 0.1
Data collection
DiffractometerHuber, ID11/ESRF
diffractometer
Absorption correction
No. of measured, independent and
observed [ > 2.0σ(I)] reflections
258713, 7435, 7319
Rint0.049
(sin θ/λ)max1)1.516
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.034, 0.031, 1.05
No. of reflections7434
No. of parameters186
No. of restraints15
H-atom treatmentOnly H-atom coordinates refined
Δρmax, Δρmin (e Å3)0.55, 0.36

Computer programs: MoPro (J. Appl. Cryst. 2005, 38, 38-54), MoproViewer.

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O3—H3···O1i1.0211.5262.5370 (6)169.4
Symmetry code: (i) x, y, z1.
 

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