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The half-chair conformation of the dynamically disordered molecular ring of 2-methyl-1,3-cyclohexanedione, C
H
O
, transforms to a sofa below
= 244 K, when the crystal undergoes a continuous phase transition induced by the onset of halting large-amplitude vibrations of methylene groups C(4)H
and C(5)H
. The temperature dependence of the crystal structure has been investigated by X-ray diffraction. The
Ibam symmetry of the crystal reduces below
to space group
Pccn. The mechanism of the phase transition and of the conversion of the ring conformation is discussed.
Supporting information
| Crystallographic Information File (CIF) https://doi.org/10.1107/S0108768100005905/hr0044sup1.cif Contains datablocks 123, 170, 180, 220, 225, 239, 240, 242, 250, 293, global |
| Structure factor file (CIF format) https://doi.org/10.1107/S0108768100005905/hr0044123sup2.hkl Contains datablock 123 |
| Structure factor file (CIF format) https://doi.org/10.1107/S0108768100005905/hr0044170sup3.hkl Contains datablock 170 |
| Structure factor file (CIF format) https://doi.org/10.1107/S0108768100005905/hr0044180sup4.hkl Contains datablock 180 |
| Structure factor file (CIF format) https://doi.org/10.1107/S0108768100005905/hr0044220sup5.hkl Contains datablock 220 |
| Structure factor file (CIF format) https://doi.org/10.1107/S0108768100005905/hr0044225sup6.hkl Contains datablock 225 |
| Structure factor file (CIF format) https://doi.org/10.1107/S0108768100005905/hr0044239sup7.hkl Contains datablock 239 |
| Structure factor file (CIF format) https://doi.org/10.1107/S0108768100005905/hr0044240sup8.hkl Contains datablock 240 |
| Structure factor file (CIF format) https://doi.org/10.1107/S0108768100005905/hr0044242sup9.hkl Contains datablock 242 |
| Structure factor file (CIF format) https://doi.org/10.1107/S0108768100005905/hr0044250sup10.hkl Supplementary material |
| Structure factor file (CIF format) https://doi.org/10.1107/S0108768100005905/hr0044293sup11.hkl Supplementary material |
CCDC references: 153328; 153329; 153330; 153331; 153332; 153333; 153334; 153335; 153336; 153337
For all compounds, program(s) used to solve structure: SHELXS86 (Sheldrick, 1990); program(s) used to refine structure: SHELXL93 (Sheldrick, 1993).
Crystal data top
C7H10O2 | Z = 8 |
Mr = 126.15 | F(000) = 544 |
Orthorhombic, Pccn | Dx = 1.313 Mg m−3 |
Hall symbol: -P 2ab 2ac | Mo Kα radiation, λ = 0.71073 Å |
a = 13.427 (3) Å | µ = 0.10 mm−1 |
b = 13.689 (3) Å | T = 123 K |
c = 6.946 (2) Å | Plate, colourless |
V = 1276.7 (5) Å3 | 0.3 × 0.3 × 0.2 mm |
Data collection top
KUMA-4-CCD diffractometer | Rint = 0.055 |
Radiation source: fine-focus sealed tube | θmax = 29.7°, θmin = 3.0° |
Graphite monochromator | h = −17→16 |
6596 measured reflections | k = −18→18 |
1616 independent reflections | l = −7→9 |
1322 reflections with I > 2σ(I) | |
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)] = 0.053 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.157 | Calculated w = 1/[σ2(Fo2) + (0.1052P)2] where P = (Fo2 + 2Fc2)/3 |
S = 1.10 | (Δ/σ)max = −0.014 |
1616 reflections | Δρmax = 0.44 e Å−3 |
117 parameters | Δρmin = −0.31 e Å−3 |
0 restraints | |
Crystal data top
C7H10O2 | V = 1276.7 (5) Å3 |
Mr = 126.15 | Z = 8 |
Orthorhombic, Pccn | Mo Kα radiation |
a = 13.427 (3) Å | µ = 0.10 mm−1 |
b = 13.689 (3) Å | T = 123 K |
c = 6.946 (2) Å | 0.3 × 0.3 × 0.2 mm |
Data collection top
KUMA-4-CCD diffractometer | 1322 reflections with I > 2σ(I) |
6596 measured reflections | Rint = 0.055 |
1616 independent reflections | |
Refinement top
R[F2 > 2σ(F2)] = 0.053 | 117 parameters |
wR(F2) = 0.157 | 0 restraints |
S = 1.10 | Δρmax = 0.44 e Å−3 |
1616 reflections | Δρmin = −0.31 e Å−3 |
Special details top
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 on F2 for ALL reflections except for 0 with very negative
F2 or flagged by the user for potential systematic errors. Weighted
R-factors wR and all goodnesses of fit S are based on
F2, conventional R-factors R are based on F,
with F set to zero for negative F2. The observed criterion of
F2 > σ(F2) is used only for calculating _R_factor_obs
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 | 0.56748 (7) | 0.45070 (6) | 0.23059 (14) | 0.0204 (3) | |
H1 | 0.5274 (18) | 0.3894 (17) | 0.229 (3) | 0.046 (7)* | |
O2 | 0.52702 (8) | 0.78702 (7) | 0.2790 (2) | 0.0248 (3) | |
C1 | 0.50884 (10) | 0.52910 (9) | 0.2458 (2) | 0.0155 (3) | |
C2 | 0.55143 (10) | 0.61931 (9) | 0.2478 (2) | 0.0165 (3) | |
C7 | 0.66143 (10) | 0.63485 (10) | 0.2226 (2) | 0.0253 (4) | |
H7A | 0.67266 (10) | 0.6811 (6) | 0.1210 (10) | 0.033* | |
H7B | 0.69266 (15) | 0.5739 (2) | 0.1905 (15) | 0.033* | |
H7C | 0.6893 (2) | 0.6595 (7) | 0.3403 (5) | 0.033* | |
C3 | 0.48991 (10) | 0.70373 (9) | 0.2796 (2) | 0.0175 (3) | |
C4 | 0.37998 (9) | 0.68976 (9) | 0.3210 (2) | 0.0205 (3) | |
H4A | 0.3435 (13) | 0.7508 (13) | 0.289 (2) | 0.025* | |
H4B | 0.3761 (11) | 0.6800 (10) | 0.459 (3) | 0.025* | |
C5 | 0.33758 (9) | 0.60178 (9) | 0.2154 (2) | 0.0195 (3) | |
H5A | 0.2630 (15) | 0.5867 (13) | 0.254 (2) | 0.023* | |
H5B | 0.3401 (11) | 0.6117 (11) | 0.079 (2) | 0.023* | |
C6 | 0.39853 (10) | 0.51077 (9) | 0.2618 (2) | 0.0181 (3) | |
H6A | 0.3857 (11) | 0.4891 (11) | 0.397 (2) | 0.022* | |
H6B | 0.3817 (12) | 0.4569 (12) | 0.179 (3) | 0.022* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
O1 | 0.0196 (5) | 0.0104 (5) | 0.0313 (7) | 0.0016 (3) | 0.0001 (4) | −0.0018 (3) |
O2 | 0.0272 (5) | 0.0104 (5) | 0.0367 (7) | −0.0005 (3) | −0.0032 (4) | −0.0010 (4) |
C1 | 0.0189 (6) | 0.0118 (6) | 0.0156 (7) | 0.0010 (4) | −0.0012 (4) | 0.0006 (4) |
C2 | 0.0171 (6) | 0.0112 (6) | 0.0212 (7) | 0.0003 (4) | −0.0021 (4) | 0.0005 (4) |
C7 | 0.0179 (6) | 0.0170 (7) | 0.0411 (9) | −0.0027 (4) | −0.0009 (5) | −0.0008 (5) |
C3 | 0.0211 (6) | 0.0117 (6) | 0.0196 (8) | 0.0002 (4) | −0.0028 (5) | −0.0003 (4) |
C4 | 0.0211 (6) | 0.0153 (6) | 0.0250 (8) | 0.0034 (4) | 0.0030 (5) | −0.0017 (5) |
C5 | 0.0169 (6) | 0.0166 (6) | 0.0249 (8) | 0.0018 (4) | −0.0005 (5) | −0.0002 (5) |
C6 | 0.0164 (6) | 0.0129 (6) | 0.0249 (8) | −0.0019 (4) | −0.0004 (4) | 0.0009 (5) |
Geometric parameters (Å, º) top
O1—C1 | 1.3353 (15) | C3—C4 | 1.516 (2) |
O1—H1 | 1.00 (2) | C4—C5 | 1.521 (2) |
O2—C3 | 1.2443 (15) | C4—H4A | 0.99 (2) |
C1—C2 | 1.361 (2) | C4—H4B | 0.97 (2) |
C1—C6 | 1.506 (2) | C5—C6 | 1.525 (2) |
C2—C3 | 1.438 (2) | C5—H5A | 1.06 (2) |
C2—C7 | 1.502 (2) | C5—H5B | 0.96 (2) |
C7—H7A | 0.96 | C6—H6A | 1.00 (2) |
C7—H7B | 0.96 | C6—H6B | 0.96 (2) |
C7—H7C | 0.96 | | |
| | | |
C1—O1—H1 | 111.1 (13) | C3—C4—H4A | 109.4 (10) |
O1—C1—C2 | 118.84 (12) | C5—C4—H4A | 112.0 (10) |
O1—C1—C6 | 116.85 (11) | C3—C4—H4B | 104.9 (9) |
C2—C1—C6 | 124.30 (12) | C5—C4—H4B | 110.3 (9) |
C1—C2—C3 | 119.31 (12) | H4A—C4—H4B | 108.0 (13) |
C1—C2—C7 | 122.71 (12) | C4—C5—C6 | 110.11 (11) |
C3—C2—C7 | 117.96 (11) | C4—C5—H5A | 112.8 (9) |
C2—C7—H7A | 109.47 (7) | C6—C5—H5A | 107.2 (10) |
C2—C7—H7B | 109.47 (7) | C4—C5—H5B | 110.6 (9) |
H7A—C7—H7B | 109.5 | C6—C5—H5B | 107.8 (9) |
C2—C7—H7C | 109.47 (7) | H5A—C5—H5B | 108.1 (12) |
H7A—C7—H7C | 109.5 | C1—C6—C5 | 112.08 (10) |
H7B—C7—H7C | 109.5 | C1—C6—H6A | 106.7 (9) |
O2—C3—C2 | 120.40 (12) | C5—C6—H6A | 110.4 (9) |
O2—C3—C4 | 120.41 (11) | C1—C6—H6B | 108.3 (10) |
C2—C3—C4 | 119.16 (10) | C5—C6—H6B | 111.9 (10) |
C3—C4—C5 | 111.90 (11) | H6A—C6—H6B | 107.2 (13) |
| | | |
O1—C1—C2—C3 | −175.04 (11) | C7—C2—C3—C4 | −175.28 (12) |
C6—C1—C2—C3 | 4.3 (2) | O2—C3—C4—C5 | 148.88 (13) |
O1—C1—C2—C7 | 3.5 (2) | C2—C3—C4—C5 | −33.3 (2) |
C6—C1—C2—C7 | −177.20 (11) | C3—C4—C5—C6 | 54.4 (2) |
C1—C2—C3—O2 | −178.86 (11) | O1—C1—C6—C5 | −162.03 (12) |
C7—C2—C3—O2 | 2.6 (2) | C2—C1—C6—C5 | 18.6 (2) |
C1—C2—C3—C4 | 3.3 (2) | C4—C5—C6—C1 | −47.0 (2) |
Crystal data top
C7H10O2 | Z = 8 |
Mr = 126.15 | F(000) = 544 |
Orthorhombic, Pccn | Dx = 1.305 Mg m−3 |
Hall symbol: -P 2ab 2ac | Mo Kα radiation, λ = 0.71069 Å |
a = 13.426 (4) Å | µ = 0.10 mm−1 |
b = 13.690 (4) Å | T = 170 K |
c = 6.987 (2) Å | Plate, colourless |
V = 1284.2 (6) Å3 | 0.3 × 0.3 × 0.2 mm |
Data collection top
KUMA-4 diffractometer | Rint = 0.000 |
Radiation source: fine-focus sealed tube | θmax = 28.1°, θmin = 2.1° |
Graphite monochromator | h = 0→17 |
846 measured reflections | k = 0→18 |
846 independent reflections | l = 0→9 |
742 reflections with I > 2σ(I) | |
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)] = 0.040 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.118 | Calculated w = 1/[σ2(Fo2) + (0.0807P)2 + 0.3895P] where P = (Fo2 + 2Fc2)/3 |
S = 1.04 | (Δ/σ)max = 0.014 |
846 reflections | Δρmax = 0.38 e Å−3 |
91 parameters | Δρmin = −0.14 e Å−3 |
0 restraints | |
Crystal data top
C7H10O2 | V = 1284.2 (6) Å3 |
Mr = 126.15 | Z = 8 |
Orthorhombic, Pccn | Mo Kα radiation |
a = 13.426 (4) Å | µ = 0.10 mm−1 |
b = 13.690 (4) Å | T = 170 K |
c = 6.987 (2) Å | 0.3 × 0.3 × 0.2 mm |
Data collection top
KUMA-4 diffractometer | 742 reflections with I > 2σ(I) |
846 measured reflections | Rint = 0.000 |
846 independent reflections | |
Refinement top
R[F2 > 2σ(F2)] = 0.040 | 91 parameters |
wR(F2) = 0.118 | 0 restraints |
S = 1.04 | Δρmax = 0.38 e Å−3 |
846 reflections | Δρmin = −0.14 e Å−3 |
Special details top
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 on F2 for ALL reflections except for 0 with very negative
F2 or flagged by the user for potential systematic errors. Weighted
R-factors wR and all goodnesses of fit S are based on
F2, conventional R-factors R are based on F,
with F set to zero for negative F2. The observed criterion of
F2 > σ(F2) is used only for calculating _R_factor_obs
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 | 0.56773 (9) | 0.45101 (8) | 0.238 (11) | 0.028 (5) | |
H1 | 0.528 (2) | 0.3913 (18) | 0.212 (6) | 0.049 (9)* | |
O2 | 0.52638 (10) | 0.78717 (9) | 0.2790 (8) | 0.0303 (12) | |
C1 | 0.50905 (12) | 0.52962 (11) | 0.2370 (6) | 0.0150 (4) | |
C2 | 0.55142 (12) | 0.61959 (11) | 0.233 (3) | 0.014 (2) | |
C7 | 0.66109 (14) | 0.63493 (13) | 0.2239 (12) | 0.0282 (15) | |
H7A | 0.6857 (2) | 0.6505 (14) | 0.3492 (13) | 0.055 (6)* | |
H7B | 0.6756 (2) | 0.6878 (10) | 0.138 (3) | 0.055 (6)* | |
H7C | 0.6927 (2) | 0.5764 (5) | 0.179 (3) | 0.055 (6)* | |
C3 | 0.48967 (13) | 0.70385 (11) | 0.2793 (6) | 0.0195 (10) | |
C4 | 0.38005 (13) | 0.68972 (14) | 0.3192 (3) | 0.0245 (4) | |
H4A | 0.34392 (13) | 0.74761 (14) | 0.2793 (3) | 0.036 (4)* | |
H4B | 0.37017 (13) | 0.68158 (14) | 0.4558 (3) | 0.036 (4)* | |
C5 | 0.33843 (13) | 0.60127 (13) | 0.2150 (4) | 0.0254 (8) | |
H5A | 0.26956 (13) | 0.59127 (13) | 0.2520 (4) | 0.039 (4)* | |
H5B | 0.34029 (13) | 0.61268 (13) | 0.0780 (4) | 0.039 (4)* | |
C6 | 0.39884 (12) | 0.51075 (12) | 0.263 (3) | 0.0205 (12) | |
H6A | 0.38597 (12) | 0.49167 (12) | 0.394 (3) | 0.032 (5)* | |
H6B | 0.37849 (12) | 0.45738 (12) | 0.180 (3) | 0.032 (5)* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
O1 | 0.0201 (5) | 0.0117 (5) | 0.052 (14) | 0.0022 (3) | 0.000 (2) | −0.001 (2) |
O2 | 0.0315 (7) | 0.0109 (5) | 0.049 (4) | 0.0000 (4) | −0.0042 (8) | −0.0007 (7) |
C1 | 0.0183 (6) | 0.0134 (6) | 0.0134 (6) | 0.0021 (4) | −0.0013 (13) | −0.0036 (12) |
C2 | 0.0169 (6) | 0.0140 (6) | 0.012 (6) | 0.0004 (5) | −0.0007 (10) | −0.0005 (9) |
C7 | 0.0174 (7) | 0.0213 (8) | 0.046 (5) | −0.0038 (5) | 0.0000 (11) | −0.0007 (11) |
C3 | 0.0222 (7) | 0.0128 (7) | 0.024 (3) | 0.0013 (5) | −0.0029 (7) | −0.0001 (7) |
C4 | 0.0209 (9) | 0.0183 (8) | 0.0341 (9) | 0.0054 (6) | 0.0026 (7) | −0.0015 (7) |
C5 | 0.0164 (7) | 0.0212 (8) | 0.038 (3) | 0.0021 (5) | −0.0012 (7) | 0.0001 (7) |
C6 | 0.0175 (6) | 0.0156 (6) | 0.029 (3) | −0.0018 (5) | −0.0012 (15) | 0.000 (2) |
Geometric parameters (Å, º) top
O1—C1 | 1.334 (2) | C3—C4 | 1.510 (3) |
O1—H1 | 0.99 (3) | C4—C5 | 1.519 (3) |
O2—C3 | 1.243 (2) | C4—H4A | 0.97 |
C1—C2 | 1.357 (2) | C4—H4B | 0.97 |
C1—C6 | 1.513 (3) | C5—C6 | 1.518 (4) |
C2—C3 | 1.457 (5) | C5—H5A | 0.97 |
C2—C7 | 1.489 (2) | C5—H5B | 0.97 |
C7—H7A | 0.96 | C6—H6A | 0.97 |
C7—H7B | 0.96 | C6—H6B | 0.97 |
C7—H7C | 0.96 | | |
| | | |
C1—O1—H1 | 110.4 (18) | C3—C4—H4A | 109.25 (10) |
O1—C1—C2 | 119.0 (2) | C5—C4—H4A | 109.25 (10) |
O1—C1—C6 | 116.1 (4) | C3—C4—H4B | 109.2 (2) |
C2—C1—C6 | 124.6 (2) | C5—C4—H4B | 109.25 (12) |
C1—C2—C3 | 118.4 (4) | H4A—C4—H4B | 107.9 |
C1—C2—C7 | 122.92 (15) | C6—C5—C4 | 110.4 (4) |
C3—C2—C7 | 117.4 (3) | C6—C5—H5A | 109.6 (2) |
C2—C7—H7A | 109.5 (8) | C4—C5—H5A | 109.58 (10) |
C2—C7—H7B | 109.5 (6) | C6—C5—H5B | 109.6 (6) |
H7A—C7—H7B | 109.5 | C4—C5—H5B | 109.58 (12) |
C2—C7—H7C | 109.5 (3) | H5A—C5—H5B | 108.1 |
H7A—C7—H7C | 109.5 | C1—C6—C5 | 110.9 (4) |
H7B—C7—H7C | 109.5 | C1—C6—H6A | 109.5 (6) |
O2—C3—C2 | 120.0 (2) | C5—C6—H6A | 109.5 (6) |
O2—C3—C4 | 120.3 (2) | C1—C6—H6B | 109.5 (5) |
C2—C3—C4 | 119.6 (2) | C5—C6—H6B | 109.5 (5) |
C3—C4—C5 | 111.8 (2) | H6A—C6—H6B | 108.0 |
| | | |
O1—C1—C2—C3 | −165 (4) | C7—C2—C3—C4 | −170.9 (9) |
C6—C1—C2—C3 | 8 (2) | O2—C3—C4—C5 | 149.3 (4) |
O1—C1—C2—C7 | 2 (4) | C2—C3—C4—C5 | −28.1 (10) |
C6—C1—C2—C7 | 174.6 (13) | C3—C4—C5—C6 | 54.5 (6) |
C1—C2—C3—O2 | 179.1 (11) | O1—C1—C6—C5 | −167 (4) |
C7—C2—C3—O2 | 11.7 (18) | C2—C1—C6—C5 | 19.7 (17) |
C1—C2—C3—C4 | −3.5 (19) | C4—C5—C6—C1 | −50.0 (11) |
Crystal data top
C7H10O2 | Z = 8 |
Mr = 126.15 | F(000) = 544 |
Orthorhombic, Pccn | Dx = 1.289 Mg m−3 |
Hall symbol: -P 2ab 2ac | Mo Kα radiation, λ = 0.71073 Å |
a = 13.466 (4) Å | µ = 0.09 mm−1 |
b = 13.691 (4) Å | T = 180 K |
c = 7.053 (2) Å | Plate, colourless |
V = 1300.3 (7) Å3 | 0.4 × 0.3 × 0.2 mm |
Data collection top
KUMA-4-CCD diffractometer | Rint = 0.077 |
Radiation source: fine-focus sealed tube | θmax = 29.7°, θmin = 2.1° |
Graphite monochromator | h = −18→15 |
7637 measured reflections | k = −17→18 |
1712 independent reflections | l = −7→9 |
1088 reflections with I > 2σ(I) | |
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)] = 0.092 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.278 | Calculated w = 1/[σ2(Fo2) + (0.1519P)2] where P = (Fo2 + 2Fc2)/3 |
S = 1.15 | (Δ/σ)max = 0.007 |
1712 reflections | Δρmax = 0.66 e Å−3 |
117 parameters | Δρmin = −0.30 e Å−3 |
0 restraints | |
Crystal data top
C7H10O2 | V = 1300.3 (7) Å3 |
Mr = 126.15 | Z = 8 |
Orthorhombic, Pccn | Mo Kα radiation |
a = 13.466 (4) Å | µ = 0.09 mm−1 |
b = 13.691 (4) Å | T = 180 K |
c = 7.053 (2) Å | 0.4 × 0.3 × 0.2 mm |
Data collection top
KUMA-4-CCD diffractometer | 1088 reflections with I > 2σ(I) |
7637 measured reflections | Rint = 0.077 |
1712 independent reflections | |
Refinement top
R[F2 > 2σ(F2)] = 0.092 | 117 parameters |
wR(F2) = 0.278 | 0 restraints |
S = 1.15 | Δρmax = 0.66 e Å−3 |
1712 reflections | Δρmin = −0.30 e Å−3 |
Special details top
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 on F2 for ALL reflections except for 0 with very negative
F2 or flagged by the user for potential systematic errors. Weighted
R-factors wR and all goodnesses of fit S are based on
F2, conventional R-factors R are based on F,
with F set to zero for negative F2. The observed criterion of
F2 > σ(F2) is used only for calculating _R_factor_obs
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 | 0.56745 (13) | 0.45111 (14) | 0.2322 (3) | 0.0418 (6) | |
H1 | 0.528 (3) | 0.378 (3) | 0.232 (5) | 0.075 (14)* | |
O2 | 0.52617 (15) | 0.78690 (15) | 0.2775 (3) | 0.0489 (7) | |
C1 | 0.5088 (2) | 0.5297 (2) | 0.2461 (3) | 0.0341 (6) | |
C2 | 0.5514 (2) | 0.6194 (2) | 0.2484 (4) | 0.0349 (7) | |
C7 | 0.6615 (2) | 0.6352 (3) | 0.2258 (6) | 0.0503 (9) | |
H7A | 0.678 (3) | 0.683 (3) | 0.109 (6) | 0.090 (8)* | |
H7B | 0.686 (3) | 0.583 (4) | 0.195 (6) | 0.090 (8)* | |
H7C | 0.684 (3) | 0.665 (3) | 0.330 (6) | 0.090 (8)* | |
C3 | 0.4900 (2) | 0.7042 (2) | 0.2776 (4) | 0.0362 (7) | |
C4 | 0.3796 (2) | 0.6895 (2) | 0.3176 (5) | 0.0443 (8) | |
H4A | 0.347 (2) | 0.754 (3) | 0.283 (4) | 0.056 (6)* | |
H4B | 0.377 (2) | 0.679 (2) | 0.463 (5) | 0.056 (6)* | |
C5 | 0.3383 (2) | 0.6008 (2) | 0.2154 (4) | 0.0405 (7) | |
H5A | 0.339 (2) | 0.612 (2) | 0.070 (4) | 0.047 (6)* | |
H5B | 0.265 (3) | 0.586 (3) | 0.258 (4) | 0.047 (6)* | |
C6 | 0.3984 (2) | 0.5109 (2) | 0.2609 (4) | 0.0383 (7) | |
H6A | 0.385 (3) | 0.486 (3) | 0.404 (5) | 0.063 (7)* | |
H6B | 0.381 (3) | 0.456 (3) | 0.173 (5) | 0.063 (7)* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
O1 | 0.0263 (10) | 0.0326 (11) | 0.0665 (14) | 0.0017 (7) | −0.0011 (8) | −0.0016 (8) |
O2 | 0.0361 (11) | 0.0329 (11) | 0.078 (2) | −0.0010 (8) | −0.0051 (9) | 0.0006 (9) |
C1 | 0.0236 (11) | 0.0334 (14) | 0.0453 (14) | 0.0022 (9) | −0.0023 (10) | 0.0010 (10) |
C2 | 0.0252 (12) | 0.0315 (14) | 0.048 (2) | 0.0025 (9) | −0.0051 (10) | −0.0024 (10) |
C7 | 0.0238 (13) | 0.042 (2) | 0.085 (3) | −0.0038 (11) | 0.0018 (14) | −0.002 (2) |
C3 | 0.0292 (13) | 0.0337 (14) | 0.046 (2) | 0.0017 (10) | −0.0035 (10) | −0.0021 (10) |
C4 | 0.0292 (14) | 0.0381 (15) | 0.066 (2) | 0.0066 (10) | 0.0021 (13) | −0.0010 (14) |
C5 | 0.0203 (12) | 0.043 (2) | 0.058 (2) | 0.0020 (10) | 0.0025 (11) | 0.0003 (13) |
C6 | 0.0233 (12) | 0.0362 (14) | 0.055 (2) | −0.0022 (10) | −0.0026 (11) | 0.0013 (12) |
Geometric parameters (Å, º) top
O1—C1 | 1.338 (3) | C3—C4 | 1.525 (4) |
O1—H1 | 1.13 (4) | C4—C5 | 1.518 (4) |
O2—C3 | 1.233 (3) | C4—H4A | 1.02 (4) |
C1—C2 | 1.355 (4) | C4—H4B | 1.03 (3) |
C1—C6 | 1.513 (4) | C5—C6 | 1.508 (4) |
C2—C3 | 1.440 (3) | C5—H5A | 1.04 (3) |
C2—C7 | 1.507 (4) | C5—H5B | 1.05 (4) |
C7—H7A | 1.07 (4) | C6—H6A | 1.08 (3) |
C7—H7B | 0.82 (5) | C6—H6B | 1.00 (4) |
C7—H7C | 0.89 (4) | | |
| | | |
C1—O1—H1 | 116 (2) | C5—C4—H4A | 115.1 (19) |
O1—C1—C2 | 118.7 (2) | C3—C4—H4A | 105.3 (19) |
O1—C1—C6 | 116.6 (2) | C5—C4—H4B | 109.9 (17) |
C2—C1—C6 | 124.7 (2) | C3—C4—H4B | 103.9 (17) |
C1—C2—C3 | 119.3 (2) | H4A—C4—H4B | 110 (2) |
C1—C2—C7 | 123.0 (3) | C6—C5—C4 | 110.8 (2) |
C3—C2—C7 | 117.7 (2) | C6—C5—H5A | 109.3 (15) |
C2—C7—H7A | 112 (2) | C4—C5—H5A | 110.4 (15) |
C2—C7—H7B | 108 (3) | C6—C5—H5B | 106.3 (19) |
H7A—C7—H7B | 104 (4) | C4—C5—H5B | 111.6 (17) |
C2—C7—H7C | 108 (3) | H5A—C5—H5B | 108 (2) |
H7A—C7—H7C | 107 (4) | C5—C6—C1 | 111.9 (2) |
H7B—C7—H7C | 119 (4) | C5—C6—H6A | 111.4 (18) |
O2—C3—C2 | 120.9 (2) | C1—C6—H6A | 106.7 (18) |
O2—C3—C4 | 120.4 (2) | C5—C6—H6B | 111 (2) |
C2—C3—C4 | 118.7 (2) | C1—C6—H6B | 108 (2) |
C5—C4—C3 | 112.0 (2) | H6A—C6—H6B | 108 (3) |
| | | |
O1—C1—C2—C3 | −175.4 (2) | C7—C2—C3—C4 | −174.9 (3) |
C6—C1—C2—C3 | 3.7 (4) | O2—C3—C4—C5 | 149.6 (3) |
O1—C1—C2—C7 | 3.3 (4) | C2—C3—C4—C5 | −33.1 (4) |
C6—C1—C2—C7 | −177.6 (3) | C3—C4—C5—C6 | 54.0 (3) |
C1—C2—C3—O2 | −178.8 (2) | C4—C5—C6—C1 | −46.5 (3) |
C7—C2—C3—O2 | 2.4 (4) | O1—C1—C6—C5 | −162.3 (2) |
C1—C2—C3—C4 | 3.9 (4) | C2—C1—C6—C5 | 18.5 (4) |
Crystal data top
C7H10O2 | Z = 8 |
Mr = 126.15 | F(000) = 544 |
Orthorhombic, Pccn | Dx = 1.289 Mg m−3 |
Hall symbol: -P 2ab 2ac | Mo Kα radiation, λ = 0.71073 Å |
a = 13.466 (4) Å | µ = 0.09 mm−1 |
b = 13.691 (4) Å | T = 220 K |
c = 7.053 (2) Å | Plate, colourless |
V = 1300.3 (7) Å3 | 0.3 × 0.3 × 0.2 mm |
Data collection top
KUMA-4 diffractometer | Rint = 0.000 |
Radiation source: fine-focus sealed tube | θmax = 28.1°, θmin = 2.1° |
Graphite monochromator | h = 0→17 |
856 measured reflections | k = 0→18 |
856 independent reflections | l = 0→9 |
723 reflections with I > 2σ(I) | |
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)] = 0.044 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.135 | Calculated w = 1/[σ2(Fo2) + (0.099P)2 + 0.2039P] where P = (Fo2 + 2Fc2)/3 |
S = 1.04 | (Δ/σ)max = 0.047 |
856 reflections | Δρmax = 0.18 e Å−3 |
91 parameters | Δρmin = −0.39 e Å−3 |
0 restraints | |
Crystal data top
C7H10O2 | V = 1300.3 (7) Å3 |
Mr = 126.15 | Z = 8 |
Orthorhombic, Pccn | Mo Kα radiation |
a = 13.466 (4) Å | µ = 0.09 mm−1 |
b = 13.691 (4) Å | T = 220 K |
c = 7.053 (2) Å | 0.3 × 0.3 × 0.2 mm |
Data collection top
KUMA-4 diffractometer | 723 reflections with I > 2σ(I) |
856 measured reflections | Rint = 0.000 |
856 independent reflections | |
Refinement top
R[F2 > 2σ(F2)] = 0.044 | 91 parameters |
wR(F2) = 0.135 | 0 restraints |
S = 1.04 | Δρmax = 0.18 e Å−3 |
856 reflections | Δρmin = −0.39 e Å−3 |
Special details top
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 on F2 for ALL reflections except for 0 with very negative
F2 or flagged by the user for potential systematic errors. Weighted
R-factors wR and all goodnesses of fit S are based on
F2, conventional R-factors R are based on F,
with F set to zero for negative F2. The observed criterion of
F2 > σ(F2) is used only for calculating _R_factor_obs
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 | 0.56810 (9) | 0.45141 (8) | 0.234 (6) | 0.034 (4) | |
H1 | 0.529 (2) | 0.390 (2) | 0.213 (6) | 0.057 (10)* | |
O2 | 0.52514 (11) | 0.78711 (10) | 0.2783 (11) | 0.040 (2) | |
C1 | 0.50914 (12) | 0.52959 (12) | 0.234 (5) | 0.020 (3) | |
C2 | 0.55107 (12) | 0.61977 (12) | 0.233 (4) | 0.021 (3) | |
C7 | 0.66039 (14) | 0.63522 (14) | 0.2249 (18) | 0.038 (2) | |
H7A | 0.6748 (2) | 0.6904 (8) | 0.146 (3) | 0.063 (6)* | |
H7B | 0.6917 (2) | 0.5781 (5) | 0.174 (3) | 0.063 (6)* | |
H7C | 0.6852 (2) | 0.6471 (13) | 0.3504 (18) | 0.063 (6)* | |
C3 | 0.48909 (14) | 0.70370 (12) | 0.2771 (10) | 0.0274 (14) | |
C4 | 0.37972 (14) | 0.68935 (15) | 0.3143 (3) | 0.0343 (5) | |
H4A | 0.34373 (14) | 0.74685 (15) | 0.2726 (3) | 0.051 (5)* | |
H4B | 0.36904 (14) | 0.68208 (15) | 0.4496 (3) | 0.051 (5)* | |
C5 | 0.33917 (13) | 0.60035 (14) | 0.2127 (5) | 0.0376 (12) | |
H5A | 0.34148 (13) | 0.61099 (14) | 0.0768 (5) | 0.055 (5)* | |
H5B | 0.27041 (13) | 0.59024 (14) | 0.2487 (5) | 0.055 (5)* | |
C6 | 0.39953 (13) | 0.51045 (13) | 0.263 (3) | 0.0290 (13) | |
H6A | 0.38755 (13) | 0.49286 (13) | 0.394 (3) | 0.044 (6)* | |
H6B | 0.37889 (13) | 0.45615 (13) | 0.184 (3) | 0.044 (6)* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
O1 | 0.0265 (6) | 0.0147 (5) | 0.061 (11) | 0.0032 (4) | 0.0013 (15) | −0.002 (2) |
O2 | 0.0406 (7) | 0.0142 (6) | 0.066 (5) | 0.0000 (4) | −0.0048 (10) | −0.0004 (8) |
C1 | 0.0223 (6) | 0.0159 (6) | 0.022 (9) | 0.0020 (5) | 0.0013 (12) | −0.0003 (11) |
C2 | 0.0212 (6) | 0.0158 (7) | 0.027 (8) | −0.0001 (5) | −0.0006 (11) | −0.0008 (11) |
C7 | 0.0209 (7) | 0.0268 (9) | 0.066 (6) | −0.0046 (5) | 0.0006 (14) | −0.0009 (14) |
C3 | 0.0291 (8) | 0.0155 (8) | 0.038 (4) | 0.0016 (5) | −0.0023 (9) | 0.0008 (8) |
C4 | 0.0273 (9) | 0.0228 (9) | 0.0528 (12) | 0.0067 (7) | 0.0051 (8) | 0.0002 (8) |
C5 | 0.0218 (8) | 0.0282 (10) | 0.063 (4) | 0.0025 (6) | −0.0020 (9) | 0.0027 (10) |
C6 | 0.0217 (7) | 0.0205 (7) | 0.045 (4) | −0.0035 (5) | −0.003 (2) | 0.001 (2) |
Geometric parameters (Å, º) top
O1—C1 | 1.333 (2) | C3—C4 | 1.509 (3) |
O1—H1 | 1.00 (3) | C4—C5 | 1.515 (3) |
O2—C3 | 1.241 (2) | C4—H4A | 0.97 |
C1—C2 | 1.358 (2) | C4—H4B | 0.97 |
C1—C6 | 1.513 (5) | C5—C6 | 1.517 (5) |
C2—C3 | 1.454 (6) | C5—H5A | 0.97 |
C2—C7 | 1.488 (3) | C5—H5B | 0.97 |
C7—H7A | 0.96 | C6—H6A | 0.97 |
C7—H7B | 0.96 | C6—H6B | 0.97 |
C7—H7C | 0.96 | | |
| | | |
C1—O1—H1 | 111.2 (16) | C3—C4—H4A | 109.22 (14) |
O1—C1—C2 | 118.9 (2) | C5—C4—H4A | 109.22 (12) |
O1—C1—C6 | 116.2 (4) | C3—C4—H4B | 109.2 (3) |
C2—C1—C6 | 124.3 (4) | C5—C4—H4B | 109.22 (15) |
C1—C2—C3 | 118.6 (6) | H4A—C4—H4B | 107.9 |
C1—C2—C7 | 122.7 (2) | C4—C5—C6 | 110.4 (5) |
C3—C2—C7 | 117.6 (4) | C4—C5—H5A | 109.56 (15) |
C2—C7—H7A | 109.5 (7) | C6—C5—H5A | 109.6 (7) |
C2—C7—H7B | 109.5 (5) | C4—C5—H5B | 109.56 (11) |
H7A—C7—H7B | 109.5 | C6—C5—H5B | 109.6 (3) |
C2—C7—H7C | 109.5 (12) | H5A—C5—H5B | 108.1 |
H7A—C7—H7C | 109.5 | C1—C6—C5 | 110.5 (5) |
H7B—C7—H7C | 109.5 | C1—C6—H6A | 109.5 (13) |
O2—C3—C2 | 120.3 (2) | C5—C6—H6A | 109.6 (7) |
O2—C3—C4 | 120.0 (2) | C1—C6—H6B | 109.5 (9) |
C2—C3—C4 | 119.7 (2) | C5—C6—H6B | 109.5 (5) |
C3—C4—C5 | 112.0 (2) | H6A—C6—H6B | 108.1 |
| | | |
O1—C1—C2—C3 | −166 (3) | C7—C2—C3—C4 | −171.3 (13) |
C6—C1—C2—C3 | 5 (4) | O2—C3—C4—C5 | 150.2 (6) |
O1—C1—C2—C7 | 2 (5) | C2—C3—C4—C5 | −27.5 (13) |
C6—C1—C2—C7 | 173 (2) | C3—C4—C5—C6 | 54.3 (7) |
C1—C2—C3—O2 | 180 (2) | O1—C1—C6—C5 | −166 (3) |
C7—C2—C3—O2 | 11 (3) | C2—C1—C6—C5 | 23 (3) |
C1—C2—C3—C4 | −3 (3) | C4—C5—C6—C1 | −51.2 (17) |
Crystal data top
C7H10O2 | Z = 8 |
Mr = 126.15 | F(000) = 544 |
Orthorhombic, Pccn | Dx = 1.286 Mg m−3 |
Hall symbol: -P 2ab 2ac | Mo Kα radiation, λ = 0.71073 Å |
a = 13.472 (4) Å | µ = 0.09 mm−1 |
b = 13.692 (4) Å | T = 225 K |
c = 7.062 (2) Å | Plate, colourless |
V = 1302.6 (7) Å3 | 0.4 × 0.3 × 0.2 mm |
Data collection top
KUMA-4-CCD diffractometer | Rint = 0.044 |
Radiation source: fine-focus sealed tube | θmax = 29.7°, θmin = 3.0° |
Graphite monochromator | h = −18→15 |
8309 measured reflections | k = −18→18 |
1756 independent reflections | l = −7→9 |
1097 reflections with I > 2σ(I) | |
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)] = 0.091 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.272 | Calculated w = 1/[σ2(Fo2) + (0.1436P)2] where P = (Fo2 + 2Fc2)/3 |
S = 1.17 | (Δ/σ)max = 0.017 |
1756 reflections | Δρmax = 0.51 e Å−3 |
117 parameters | Δρmin = −0.24 e Å−3 |
0 restraints | |
Crystal data top
C7H10O2 | V = 1302.6 (7) Å3 |
Mr = 126.15 | Z = 8 |
Orthorhombic, Pccn | Mo Kα radiation |
a = 13.472 (4) Å | µ = 0.09 mm−1 |
b = 13.692 (4) Å | T = 225 K |
c = 7.062 (2) Å | 0.4 × 0.3 × 0.2 mm |
Data collection top
KUMA-4-CCD diffractometer | 1097 reflections with I > 2σ(I) |
8309 measured reflections | Rint = 0.044 |
1756 independent reflections | |
Refinement top
R[F2 > 2σ(F2)] = 0.091 | 117 parameters |
wR(F2) = 0.272 | 0 restraints |
S = 1.17 | Δρmax = 0.51 e Å−3 |
1756 reflections | Δρmin = −0.24 e Å−3 |
Special details top
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 on F2 for ALL reflections except for 0 with very negative
F2 or flagged by the user for potential systematic errors. Weighted
R-factors wR and all goodnesses of fit S are based on
F2, conventional R-factors R are based on F,
with F set to zero for negative F2. The observed criterion of
F2 > σ(F2) is used only for calculating _R_factor_obs
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 | 0.56807 (13) | 0.45129 (14) | 0.2343 (3) | 0.0455 (6) | |
H1 | 0.533 (3) | 0.383 (3) | 0.233 (4) | 0.085 (14)* | |
O2 | 0.5250 (2) | 0.78678 (14) | 0.2741 (3) | 0.0565 (7) | |
C1 | 0.5090 (2) | 0.5297 (2) | 0.2475 (3) | 0.0348 (6) | |
C2 | 0.5510 (2) | 0.6196 (2) | 0.2492 (3) | 0.0382 (6) | |
C7 | 0.6604 (2) | 0.6356 (3) | 0.2296 (6) | 0.0562 (9) | |
H7A | 0.673 (3) | 0.677 (4) | 0.104 (6) | 0.128 (11)* | |
H7B | 0.689 (4) | 0.579 (5) | 0.213 (6) | 0.128 (11)* | |
H7C | 0.681 (4) | 0.667 (4) | 0.325 (7) | 0.128 (11)* | |
C3 | 0.4891 (2) | 0.7036 (2) | 0.2747 (4) | 0.0394 (7) | |
C4 | 0.3794 (2) | 0.6891 (2) | 0.3108 (5) | 0.0531 (8) | |
H4A | 0.342 (3) | 0.748 (4) | 0.279 (5) | 0.095 (9)* | |
H4B | 0.373 (3) | 0.671 (3) | 0.457 (6) | 0.095 (9)* | |
C5 | 0.3391 (2) | 0.6000 (2) | 0.2153 (5) | 0.0525 (9) | |
H5A | 0.343 (2) | 0.619 (2) | 0.063 (5) | 0.075 (7)* | |
H5B | 0.261 (4) | 0.582 (3) | 0.253 (4) | 0.075 (7)* | |
C6 | 0.3993 (2) | 0.5106 (2) | 0.2601 (4) | 0.0417 (7) | |
H6A | 0.386 (3) | 0.483 (3) | 0.391 (5) | 0.078 (8)* | |
H6B | 0.384 (3) | 0.458 (3) | 0.186 (5) | 0.078 (8)* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
O1 | 0.0333 (10) | 0.0295 (11) | 0.0738 (14) | 0.0022 (7) | 0.0007 (8) | −0.0019 (8) |
O2 | 0.0492 (13) | 0.0288 (11) | 0.092 (2) | −0.0004 (8) | −0.0037 (10) | −0.0014 (8) |
C1 | 0.0294 (11) | 0.0313 (13) | 0.0437 (13) | 0.0014 (9) | −0.0018 (9) | 0.0000 (9) |
C2 | 0.0274 (12) | 0.0319 (13) | 0.055 (2) | 0.0003 (9) | −0.0039 (10) | −0.0022 (10) |
C7 | 0.0278 (13) | 0.043 (2) | 0.098 (3) | −0.0045 (11) | −0.0012 (14) | −0.002 (2) |
C3 | 0.0352 (13) | 0.0308 (13) | 0.0522 (15) | 0.0019 (9) | −0.0039 (10) | −0.0012 (10) |
C4 | 0.0354 (14) | 0.041 (2) | 0.083 (2) | 0.0089 (11) | 0.0055 (14) | −0.0006 (15) |
C5 | 0.0288 (13) | 0.042 (2) | 0.087 (2) | 0.0045 (10) | 0.0026 (13) | 0.0015 (14) |
C6 | 0.0286 (12) | 0.0355 (13) | 0.061 (2) | −0.0033 (10) | −0.0013 (11) | −0.0006 (12) |
Geometric parameters (Å, º) top
O1—C1 | 1.339 (3) | C3—C4 | 1.512 (4) |
O1—H1 | 1.05 (5) | C4—C5 | 1.496 (4) |
O2—C3 | 1.238 (3) | C4—H4A | 0.97 (5) |
C1—C2 | 1.355 (3) | C4—H4B | 1.06 (4) |
C1—C6 | 1.504 (4) | C5—C6 | 1.502 (4) |
C2—C3 | 1.432 (3) | C5—H5A | 1.11 (3) |
C2—C7 | 1.497 (4) | C5—H5B | 1.11 (5) |
C7—H7A | 1.06 (5) | C6—H6A | 1.02 (3) |
C7—H7B | 0.87 (6) | C6—H6B | 0.92 (4) |
C7—H7C | 0.84 (5) | | |
| | | |
C1—O1—H1 | 117 (2) | C5—C4—H4A | 113 (3) |
O1—C1—C2 | 118.8 (2) | C3—C4—H4A | 111 (3) |
O1—C1—C6 | 116.7 (2) | C5—C4—H4B | 102 (2) |
C2—C1—C6 | 124.6 (2) | C3—C4—H4B | 106.1 (18) |
C1—C2—C3 | 119.2 (2) | H4A—C4—H4B | 112 (3) |
C1—C2—C7 | 122.9 (3) | C4—C5—C6 | 111.9 (3) |
C3—C2—C7 | 117.9 (2) | C4—C5—H5A | 103.1 (16) |
C2—C7—H7A | 108 (2) | C6—C5—H5A | 111.6 (16) |
C2—C7—H7B | 108 (4) | C4—C5—H5B | 115 (2) |
H7A—C7—H7B | 106 (4) | C6—C5—H5B | 106 (2) |
C2—C7—H7C | 109 (3) | H5A—C5—H5B | 110 (2) |
H7A—C7—H7C | 110 (4) | C5—C6—C1 | 112.1 (2) |
H7B—C7—H7C | 114 (5) | C5—C6—H6A | 113 (2) |
O2—C3—C2 | 120.7 (2) | C1—C6—H6A | 107 (2) |
O2—C3—C4 | 120.3 (2) | C5—C6—H6B | 114 (3) |
C2—C3—C4 | 119.0 (2) | C1—C6—H6B | 109 (3) |
C5—C4—C3 | 112.7 (2) | H6A—C6—H6B | 101 (3) |
| | | |
O1—C1—C2—C3 | −176.3 (2) | C7—C2—C3—C4 | −175.1 (3) |
C6—C1—C2—C3 | 3.6 (4) | O2—C3—C4—C5 | 150.9 (3) |
O1—C1—C2—C7 | 2.3 (4) | C2—C3—C4—C5 | −31.6 (4) |
C6—C1—C2—C7 | −177.8 (3) | C3—C4—C5—C6 | 51.8 (4) |
C1—C2—C3—O2 | −178.9 (2) | C4—C5—C6—C1 | −44.5 (4) |
C7—C2—C3—O2 | 2.4 (4) | O1—C1—C6—C5 | −162.7 (2) |
C1—C2—C3—C4 | 3.6 (4) | C2—C1—C6—C5 | 17.5 (4) |
Crystal data top
C7H10O2 | Z = 8 |
Mr = 126.15 | F(000) = 544 |
Orthorhombic, Pccn | Dx = 1.281 Mg m−3 |
Hall symbol: -P 2ab 2ac | Mo Kα radiation, λ = 0.71073 Å |
a = 13.472 (4) Å | µ = 0.09 mm−1 |
b = 13.692 (4) Å | T = 239.K K |
c = 7.090 (2) Å | Plate, colourless |
V = 1307.8 (7) Å3 | 0.4 × 0.3 × 0.2 mm |
Data collection top
KUMA-4-CCD diffractometer | Rint = 0.035 |
Radiation source: fine-focus sealed tube | θmax = 29.6°, θmin = 3.0° |
Graphite monochromator | h = −18→16 |
8221 measured reflections | k = −18→18 |
1758 independent reflections | l = −7→9 |
1073 reflections with I > 2σ(I) | |
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)] = 0.107 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.329 | Calculated w = 1/[σ2(Fo2) + (0.1617P)2] where P = (Fo2 + 2Fc2)/3 |
S = 1.26 | (Δ/σ)max = 0.045 |
1758 reflections | Δρmax = 0.50 e Å−3 |
117 parameters | Δρmin = −0.21 e Å−3 |
0 restraints | |
Crystal data top
C7H10O2 | V = 1307.8 (7) Å3 |
Mr = 126.15 | Z = 8 |
Orthorhombic, Pccn | Mo Kα radiation |
a = 13.472 (4) Å | µ = 0.09 mm−1 |
b = 13.692 (4) Å | T = 239.K K |
c = 7.090 (2) Å | 0.4 × 0.3 × 0.2 mm |
Data collection top
KUMA-4-CCD diffractometer | 1073 reflections with I > 2σ(I) |
8221 measured reflections | Rint = 0.035 |
1758 independent reflections | |
Refinement top
R[F2 > 2σ(F2)] = 0.107 | 117 parameters |
wR(F2) = 0.329 | 0 restraints |
S = 1.26 | Δρmax = 0.50 e Å−3 |
1758 reflections | Δρmin = −0.21 e Å−3 |
Special details top
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 on F2 for ALL reflections except for 0 with very negative
F2 or flagged by the user for potential systematic errors. Weighted
R-factors wR and all goodnesses of fit S are based on
F2, conventional R-factors R are based on F,
with F set to zero for negative F2. The observed criterion of
F2 > σ(F2) is used only for calculating _R_factor_obs
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 | 0.5686 (2) | 0.4513 (2) | 0.2380 (3) | 0.0479 (8) | |
H1 | 0.533 (4) | 0.390 (4) | 0.241 (4) | 0.072 (14)* | |
O2 | 0.5241 (2) | 0.7868 (2) | 0.2690 (4) | 0.0610 (9) | |
C1 | 0.5091 (2) | 0.5294 (2) | 0.2478 (4) | 0.0353 (7) | |
C2 | 0.5510 (2) | 0.6196 (2) | 0.2494 (4) | 0.0383 (8) | |
C7 | 0.6600 (2) | 0.6358 (3) | 0.2352 (7) | 0.0579 (12) | |
H7A | 0.674 (4) | 0.681 (5) | 0.109 (8) | 0.148 (16)* | |
H7B | 0.685 (6) | 0.588 (6) | 0.224 (8) | 0.148 (16)* | |
H7C | 0.685 (5) | 0.676 (5) | 0.349 (8) | 0.148 (16)* | |
C3 | 0.4884 (2) | 0.7033 (2) | 0.2692 (4) | 0.0433 (9) | |
C4 | 0.3787 (3) | 0.6888 (3) | 0.3012 (7) | 0.0650 (13) | |
H4A | 0.337 (4) | 0.749 (5) | 0.276 (6) | 0.101 (11)* | |
H4B | 0.371 (3) | 0.663 (3) | 0.466 (6) | 0.101 (11)* | |
C5 | 0.3400 (3) | 0.5993 (3) | 0.2186 (7) | 0.0692 (14) | |
H5A | 0.355 (3) | 0.632 (3) | 0.054 (7) | 0.103 (11)* | |
H5B | 0.266 (5) | 0.582 (5) | 0.253 (5) | 0.103 (11)* | |
C6 | 0.3998 (2) | 0.5100 (2) | 0.2588 (5) | 0.0423 (8) | |
H6A | 0.395 (4) | 0.477 (3) | 0.382 (6) | 0.088 (11)* | |
H6B | 0.390 (4) | 0.464 (4) | 0.176 (6) | 0.088 (11)* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
O1 | 0.0353 (12) | 0.0262 (12) | 0.082 (2) | 0.0019 (8) | 0.0007 (10) | −0.0010 (9) |
O2 | 0.053 (2) | 0.0261 (12) | 0.104 (2) | −0.0004 (10) | −0.0012 (12) | −0.0007 (10) |
C1 | 0.0316 (14) | 0.0275 (15) | 0.047 (2) | 0.0018 (10) | −0.0015 (11) | −0.0010 (11) |
C2 | 0.0293 (14) | 0.0287 (15) | 0.057 (2) | 0.0019 (11) | −0.0031 (12) | 0.0004 (12) |
C7 | 0.028 (2) | 0.038 (2) | 0.108 (3) | −0.0045 (12) | −0.002 (2) | 0.003 (2) |
C3 | 0.037 (2) | 0.028 (2) | 0.065 (2) | 0.0018 (11) | 0.0001 (13) | −0.0006 (12) |
C4 | 0.035 (2) | 0.037 (2) | 0.123 (4) | 0.0083 (14) | 0.005 (2) | −0.003 (2) |
C5 | 0.030 (2) | 0.039 (2) | 0.139 (4) | 0.0022 (13) | 0.001 (2) | 0.005 (2) |
C6 | 0.0309 (15) | 0.033 (2) | 0.063 (2) | −0.0046 (11) | 0.0006 (14) | 0.0012 (14) |
Geometric parameters (Å, º) top
O1—C1 | 1.337 (3) | C3—C4 | 1.508 (5) |
O1—H1 | 0.98 (5) | C4—C5 | 1.454 (6) |
O2—C3 | 1.240 (4) | C4—H4A | 1.01 (6) |
C1—C2 | 1.357 (4) | C4—H4B | 1.22 (4) |
C1—C6 | 1.499 (4) | C5—C6 | 1.493 (5) |
C2—C3 | 1.430 (4) | C5—H5A | 1.27 (5) |
C2—C7 | 1.489 (4) | C5—H5B | 1.05 (7) |
C7—H7A | 1.10 (6) | C6—H6A | 0.98 (4) |
C7—H7B | 0.74 (8) | C6—H6B | 0.87 (5) |
C7—H7C | 1.03 (6) | | |
| | | |
C1—O1—H1 | 113 (3) | C5—C4—H4A | 114 (3) |
O1—C1—C2 | 118.6 (3) | C3—C4—H4A | 114 (3) |
O1—C1—C6 | 116.7 (2) | C5—C4—H4B | 96 (2) |
C2—C1—C6 | 124.7 (3) | C3—C4—H4B | 105 (2) |
C1—C2—C3 | 119.1 (3) | H4A—C4—H4B | 111 (3) |
C1—C2—C7 | 123.0 (3) | C4—C5—C6 | 114.8 (3) |
C3—C2—C7 | 117.9 (3) | C4—C5—H5A | 91 (2) |
C2—C7—H7A | 108 (3) | C6—C5—H5A | 112 (2) |
C2—C7—H7B | 109 (6) | C4—C5—H5B | 116 (3) |
H7A—C7—H7B | 109 (6) | C6—C5—H5B | 107 (4) |
C2—C7—H7C | 111 (3) | H5A—C5—H5B | 116 (3) |
H7A—C7—H7C | 106 (5) | C5—C6—C1 | 112.0 (3) |
H7B—C7—H7C | 114 (6) | C5—C6—H6A | 120 (3) |
O2—C3—C2 | 120.7 (3) | C1—C6—H6A | 101 (3) |
O2—C3—C4 | 120.1 (3) | C5—C6—H6B | 112 (3) |
C2—C3—C4 | 119.1 (3) | C1—C6—H6B | 104 (4) |
C5—C4—C3 | 113.7 (3) | H6A—C6—H6B | 105 (4) |
| | | |
O1—C1—C2—C3 | −176.9 (2) | C7—C2—C3—C4 | −174.6 (4) |
C6—C1—C2—C3 | 2.2 (4) | O2—C3—C4—C5 | 154.2 (4) |
O1—C1—C2—C7 | 1.9 (5) | C2—C3—C4—C5 | −29.1 (5) |
C6—C1—C2—C7 | −179.0 (3) | C3—C4—C5—C6 | 47.5 (6) |
C1—C2—C3—O2 | −179.1 (3) | C4—C5—C6—C1 | −40.6 (5) |
C7—C2—C3—O2 | 2.0 (5) | O1—C1—C6—C5 | −165.1 (3) |
C1—C2—C3—C4 | 4.2 (4) | C2—C1—C6—C5 | 15.8 (5) |
Crystal data top
C7H10O2 | Z = 8 |
Mr = 126.15 | F(000) = 544 |
Orthorhombic, Pccn | Dx = 1.279 Mg m−3 |
Hall symbol: -P 2ab 2ac | Mo Kα radiation, λ = 0.71073 Å |
a = 13.492 (4) Å | µ = 0.09 mm−1 |
b = 13.692 (4) Å | T = 240 K |
c = 7.091 (2) Å | Plate, colourless |
V = 1309.9 (7) Å3 | 0.4 × 0.3 × 0.2 mm |
Data collection top
KUMA-4-CCD diffractometer | Rint = 0.066 |
Radiation source: fine-focus sealed tube | θmax = 29.9°, θmin = 2.1° |
Graphite monochromator | h = −18→16 |
8148 measured reflections | k = −18→18 |
1777 independent reflections | l = −7→9 |
948 reflections with I > 2σ(I) | |
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)] = 0.196 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.490 | Calculated w = 1/[σ2(Fo2) + (0.1986P)2 + 0.544P] where P = (Fo2 + 2Fc2)/3 |
S = 1.31 | (Δ/σ)max = 0.114 |
1777 reflections | Δρmax = 0.57 e Å−3 |
91 parameters | Δρmin = −0.32 e Å−3 |
0 restraints | |
Crystal data top
C7H10O2 | V = 1309.9 (7) Å3 |
Mr = 126.15 | Z = 8 |
Orthorhombic, Pccn | Mo Kα radiation |
a = 13.492 (4) Å | µ = 0.09 mm−1 |
b = 13.692 (4) Å | T = 240 K |
c = 7.091 (2) Å | 0.4 × 0.3 × 0.2 mm |
Data collection top
KUMA-4-CCD diffractometer | 948 reflections with I > 2σ(I) |
8148 measured reflections | Rint = 0.066 |
1777 independent reflections | |
Refinement top
R[F2 > 2σ(F2)] = 0.196 | 0 restraints |
wR(F2) = 0.490 | (Δ/σ)max = 0.114 |
S = 1.31 | Δρmax = 0.57 e Å−3 |
1777 reflections | Δρmin = −0.32 e Å−3 |
91 parameters | |
Special details top
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 on F2 for ALL reflections except for 0 with very negative
F2 or flagged by the user for potential systematic errors. Weighted
R-factors wR and all goodnesses of fit S are based on
F2, conventional R-factors R are based on F,
with F set to zero for negative F2. The observed criterion of
F2 > σ(F2) is used only for calculating _R_factor_obs
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 | 0.5690 (3) | 0.4522 (3) | 0.2386 (6) | 0.0530 (14) | |
H1 | 0.531 (7) | 0.406 (8) | 0.231 (10) | 0.09 (3)* | |
O2 | 0.5252 (4) | 0.7866 (3) | 0.2697 (7) | 0.063 (2) | |
C1 | 0.5088 (4) | 0.5290 (4) | 0.2471 (7) | 0.0372 (14) | |
C2 | 0.5512 (4) | 0.6192 (4) | 0.2481 (7) | 0.0411 (15) | |
C7 | 0.6606 (4) | 0.6355 (5) | 0.2365 (9) | 0.061 (2) | |
H7A | 0.6770 (7) | 0.663 (4) | 0.116 (3) | 0.17 (3)* | |
H7B | 0.6945 (5) | 0.5744 (8) | 0.253 (8) | 0.17 (3)* | |
H7C | 0.6807 (8) | 0.680 (3) | 0.334 (5) | 0.17 (3)* | |
C3 | 0.4886 (4) | 0.7030 (4) | 0.2694 (8) | 0.045 (2) | |
C4 | 0.3790 (5) | 0.6887 (5) | 0.2986 (13) | 0.074 (3) | |
H4A | 0.3651 (5) | 0.6899 (5) | 0.4328 (13) | 0.14 (3)* | |
H4B | 0.3439 (5) | 0.7431 (5) | 0.2415 (13) | 0.14 (3)* | |
C5 | 0.3415 (5) | 0.5994 (5) | 0.2210 (12) | 0.072 (3) | |
H5A | 0.3363 (5) | 0.6071 (5) | 0.0853 (12) | 0.086 (19)* | |
H5B | 0.2750 (5) | 0.5892 (5) | 0.2692 (12) | 0.086 (19)* | |
C6 | 0.4006 (4) | 0.5101 (4) | 0.2599 (7) | 0.047 (2) | |
H6A | 0.3826 (4) | 0.4596 (4) | 0.1701 (7) | 0.17 (4)* | |
H6B | 0.3849 (4) | 0.4862 (4) | 0.3852 (7) | 0.17 (4)* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
O1 | 0.039 (2) | 0.026 (2) | 0.094 (4) | 0.004 (2) | −0.006 (2) | 0.002 (2) |
O2 | 0.060 (3) | 0.030 (2) | 0.100 (4) | 0.001 (2) | 0.001 (2) | 0.001 (2) |
C1 | 0.037 (3) | 0.030 (3) | 0.045 (3) | −0.001 (2) | −0.009 (2) | 0.005 (2) |
C2 | 0.030 (3) | 0.036 (3) | 0.057 (4) | 0.001 (2) | 0.006 (2) | −0.002 (3) |
C7 | 0.030 (3) | 0.054 (4) | 0.100 (6) | −0.002 (3) | −0.007 (3) | 0.013 (4) |
C3 | 0.032 (3) | 0.034 (3) | 0.070 (4) | 0.002 (2) | −0.006 (3) | −0.006 (3) |
C4 | 0.036 (4) | 0.050 (4) | 0.137 (7) | 0.010 (3) | 0.004 (4) | −0.003 (4) |
C5 | 0.035 (3) | 0.038 (4) | 0.143 (8) | 0.000 (3) | −0.006 (4) | 0.014 (4) |
C6 | 0.031 (3) | 0.041 (3) | 0.068 (4) | −0.003 (2) | 0.021 (3) | 0.005 (3) |
Geometric parameters (Å, º) top
O1—C1 | 1.330 (6) | C3—C4 | 1.506 (9) |
O1—H1 | 0.82 (10) | C4—C5 | 1.434 (10) |
O2—C3 | 1.247 (7) | C4—H4A | 0.97 |
C1—C2 | 1.361 (7) | C4—H4B | 0.97 |
C1—C6 | 1.485 (8) | C5—C6 | 1.486 (8) |
C2—C3 | 1.433 (7) | C5—H5A | 0.97 |
C2—C7 | 1.496 (8) | C5—H5B | 0.97 |
C7—H7A | 0.96 | C6—H6A | 0.97 |
C7—H7B | 0.96 | C6—H6B | 0.97 |
C7—H7C | 0.96 | | |
| | | |
C1—O1—H1 | 103 (7) | C5—C4—H4A | 108.8 (5) |
O1—C1—C2 | 117.4 (5) | C3—C4—H4A | 108.8 (4) |
O1—C1—C6 | 117.8 (5) | C5—C4—H4B | 108.8 (4) |
C2—C1—C6 | 124.8 (5) | C3—C4—H4B | 108.8 (4) |
C1—C2—C3 | 118.7 (5) | H4A—C4—H4B | 107.7 |
C1—C2—C7 | 123.4 (5) | C4—C5—C6 | 116.2 (6) |
C3—C2—C7 | 117.9 (5) | C4—C5—H5A | 108.3 (5) |
C2—C7—H7A | 109.5 (3) | C6—C5—H5A | 108.2 (4) |
C2—C7—H7B | 109.5 (4) | C4—C5—H5B | 108.2 (4) |
H7A—C7—H7B | 109.5 | C6—C5—H5B | 108.2 (3) |
C2—C7—H7C | 109.5 (3) | H5A—C5—H5B | 107.4 |
H7A—C7—H7C | 109.5 | C5—C6—C1 | 111.9 (5) |
H7B—C7—H7C | 109.5 | C5—C6—H6A | 109.2 (4) |
O2—C3—C2 | 120.1 (5) | C1—C6—H6A | 109.2 (3) |
O2—C3—C4 | 120.6 (5) | C5—C6—H6B | 109.2 (4) |
C2—C3—C4 | 119.3 (5) | C1—C6—H6B | 109.2 (3) |
C5—C4—C3 | 113.8 (6) | H6A—C6—H6B | 107.9 |
| | | |
O1—C1—C2—C3 | −176.0 (5) | C7—C2—C3—C4 | −174.7 (6) |
C6—C1—C2—C3 | 2.3 (8) | O2—C3—C4—C5 | 155.8 (7) |
O1—C1—C2—C7 | 1.2 (8) | C2—C3—C4—C5 | −26.5 (10) |
C6—C1—C2—C7 | 179.5 (5) | C3—C4—C5—C6 | 45.7 (10) |
C1—C2—C3—O2 | −179.6 (5) | C4—C5—C6—C1 | −40.1 (9) |
C7—C2—C3—O2 | 3.1 (8) | O1—C1—C6—C5 | −165.9 (5) |
C1—C2—C3—C4 | 2.7 (8) | C2—C1—C6—C5 | 15.8 (8) |
Crystal data top
C7H10O2 | Z = 8 |
Mr = 126.15 | F(000) = 544 |
Orthorhombic, Pccn | Dx = 1.278 Mg m−3 |
Hall symbol: -P 2ab 2ac | Mo Kα radiation, λ = 0.71073 Å |
a = 13.498 (4) Å | µ = 0.09 mm−1 |
b = 13.691 (4) Å | T = 242 K |
c = 7.095 (2) Å | Plate, colourless |
V = 1311.2 (7) Å3 | 0.4 × 0.3 × 0.2 mm |
Data collection top
KUMA-4-CCD diffractometer | 889 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.066 |
Graphite monochromator | θmax = 29.8°, θmin = 2.1° |
rotation scans | h = −18→16 |
8192 measured reflections | k = −18→18 |
1778 independent reflections | l = −7→9 |
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)] = 0.186 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.510 | Calculated w = 1/[σ2(Fo2) + (0.1975P)2 + 1.2779P] where P = (Fo2 + 2Fc2)/3 |
S = 1.29 | (Δ/σ)max = 0.017 |
1778 reflections | Δρmax = 0.50 e Å−3 |
91 parameters | Δρmin = −0.35 e Å−3 |
0 restraints | |
Crystal data top
C7H10O2 | V = 1311.2 (7) Å3 |
Mr = 126.15 | Z = 8 |
Orthorhombic, Pccn | Mo Kα radiation |
a = 13.498 (4) Å | µ = 0.09 mm−1 |
b = 13.691 (4) Å | T = 242 K |
c = 7.095 (2) Å | 0.4 × 0.3 × 0.2 mm |
Data collection top
KUMA-4-CCD diffractometer | 889 reflections with I > 2σ(I) |
8192 measured reflections | Rint = 0.066 |
1778 independent reflections | |
Refinement top
R[F2 > 2σ(F2)] = 0.186 | 91 parameters |
wR(F2) = 0.510 | 0 restraints |
S = 1.29 | Δρmax = 0.50 e Å−3 |
1778 reflections | Δρmin = −0.35 e Å−3 |
Special details top
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 on F2 for ALL reflections except for 0 with very negative
F2 or flagged by the user for potential systematic errors. Weighted
R-factors wR and all goodnesses of fit S are based on
F2, conventional R-factors R are based on F,
with F set to zero for negative F2. The observed criterion of
F2 > σ(F2) is used only for calculating _R_factor_obs
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 | 0.5684 (3) | 0.4522 (3) | 0.2412 (6) | 0.0547 (15) | |
H1 | 0.524 (8) | 0.396 (8) | 0.239 (10) | 0.11 (4)* | |
O2 | 0.5249 (4) | 0.7869 (3) | 0.2676 (7) | 0.068 (2) | |
C1 | 0.5093 (4) | 0.5291 (4) | 0.2469 (8) | 0.0413 (15) | |
C2 | 0.5512 (4) | 0.6187 (4) | 0.2467 (8) | 0.046 (2) | |
C7 | 0.6607 (5) | 0.6361 (5) | 0.2393 (10) | 0.064 (2) | |
H7A | 0.6773 (8) | 0.668 (4) | 0.123 (4) | 0.18 (3)* | |
H7B | 0.6949 (5) | 0.5748 (6) | 0.247 (9) | 0.18 (3)* | |
H7C | 0.6800 (9) | 0.677 (4) | 0.344 (5) | 0.18 (3)* | |
C3 | 0.4883 (5) | 0.7030 (5) | 0.2676 (9) | 0.051 (2) | |
C4 | 0.3788 (5) | 0.6881 (6) | 0.2895 (15) | 0.090 (3) | |
H4A | 0.3624 (5) | 0.6939 (6) | 0.4222 (15) | 0.18 (4)* | |
H4B | 0.3449 (5) | 0.7404 (6) | 0.2237 (15) | 0.18 (4)* | |
C5 | 0.3416 (5) | 0.5996 (5) | 0.2242 (14) | 0.085 (3) | |
H5A | 0.3317 (5) | 0.6055 (5) | 0.0893 (14) | 0.15 (3)* | |
H5B | 0.2769 (5) | 0.5899 (5) | 0.2807 (14) | 0.15 (3)* | |
C6 | 0.4003 (5) | 0.5108 (5) | 0.2582 (8) | 0.053 (2) | |
H6A | 0.3823 (5) | 0.4617 (5) | 0.1658 (8) | 0.17 (4)* | |
H6B | 0.3844 (5) | 0.4852 (5) | 0.3821 (8) | 0.17 (4)* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
O1 | 0.042 (3) | 0.029 (2) | 0.093 (4) | 0.004 (2) | −0.013 (2) | 0.003 (2) |
O2 | 0.068 (3) | 0.028 (2) | 0.108 (4) | −0.001 (2) | 0.002 (3) | −0.004 (2) |
C1 | 0.034 (3) | 0.035 (3) | 0.055 (3) | 0.004 (2) | −0.013 (3) | 0.011 (3) |
C2 | 0.034 (3) | 0.037 (3) | 0.068 (4) | −0.002 (2) | 0.014 (3) | 0.003 (3) |
C7 | 0.033 (3) | 0.051 (4) | 0.108 (6) | −0.005 (3) | −0.010 (3) | −0.004 (4) |
C3 | 0.038 (3) | 0.040 (3) | 0.075 (5) | 0.008 (2) | −0.009 (3) | −0.013 (3) |
C4 | 0.038 (4) | 0.053 (5) | 0.180 (10) | 0.012 (3) | 0.007 (5) | −0.003 (5) |
C5 | 0.039 (4) | 0.031 (3) | 0.185 (10) | 0.002 (3) | −0.016 (4) | 0.023 (4) |
C6 | 0.036 (3) | 0.044 (3) | 0.078 (5) | −0.003 (3) | 0.026 (3) | 0.010 (3) |
Geometric parameters (Å, º) top
O1—C1 | 1.322 (7) | C3—C4 | 1.500 (10) |
O1—H1 | 0.97 (11) | C4—C5 | 1.391 (11) |
O2—C3 | 1.250 (7) | C4—H4A | 0.97 |
C1—C2 | 1.351 (8) | C4—H4B | 0.97 |
C1—C6 | 1.494 (9) | C5—C6 | 1.471 (9) |
C2—C3 | 1.442 (8) | C5—H5A | 0.97 |
C2—C7 | 1.497 (9) | C5—H5B | 0.97 |
C7—H7A | 0.96 | C6—H6A | 0.97 |
C7—H7B | 0.96 | C6—H6B | 0.97 |
C7—H7C | 0.96 | | |
| | | |
C1—O1—H1 | 105 (6) | C5—C4—H4A | 108.3 (6) |
O1—C1—C2 | 118.1 (5) | C3—C4—H4A | 108.3 (5) |
O1—C1—C6 | 117.5 (5) | C5—C4—H4B | 108.3 (5) |
C2—C1—C6 | 124.4 (5) | C3—C4—H4B | 108.3 (4) |
C1—C2—C3 | 118.7 (5) | H4A—C4—H4B | 107.4 |
C1—C2—C7 | 123.9 (6) | C4—C5—C6 | 118.1 (7) |
C3—C2—C7 | 117.2 (5) | C4—C5—H5A | 107.8 (6) |
C2—C7—H7A | 109.5 (3) | C6—C5—H5A | 107.8 (5) |
C2—C7—H7B | 109.5 (4) | C4—C5—H5B | 107.8 (5) |
H7A—C7—H7B | 109.5 | C6—C5—H5B | 107.8 (4) |
C2—C7—H7C | 109.5 (4) | H5A—C5—H5B | 107.1 |
H7A—C7—H7C | 109.5 | C5—C6—C1 | 112.5 (5) |
H7B—C7—H7C | 109.5 | C5—C6—H6A | 109.1 (4) |
O2—C3—C2 | 120.1 (6) | C1—C6—H6A | 109.1 (3) |
O2—C3—C4 | 121.0 (6) | C5—C6—H6B | 109.1 (4) |
C2—C3—C4 | 118.8 (6) | C1—C6—H6B | 109.1 (3) |
C5—C4—C3 | 116.1 (7) | H6A—C6—H6B | 107.8 |
| | | |
O1—C1—C2—C3 | −175.2 (5) | C7—C2—C3—C4 | −175.7 (7) |
C6—C1—C2—C3 | 3.1 (9) | O2—C3—C4—C5 | 158.5 (8) |
O1—C1—C2—C7 | 0.3 (9) | C2—C3—C4—C5 | −21.6 (12) |
C6—C1—C2—C7 | 178.7 (5) | C3—C4—C5—C6 | 39.9 (13) |
C1—C2—C3—O2 | −179.9 (6) | C4—C5—C6—C1 | −35.5 (11) |
C7—C2—C3—O2 | 4.2 (9) | O1—C1—C6—C5 | −168.1 (6) |
C1—C2—C3—C4 | 0.2 (9) | C2—C1—C6—C5 | 13.5 (9) |
Crystal data top
C7H10O2 | Z = 8 |
Mr = 126.15 | F(000) = 544 |
Orthorhombic, Ibam | Dx = 1.274 Mg m−3 |
Hall symbol: -I 2 2c | Mo Kα radiation, λ = 0.71069 Å |
a = 13.510 (3) Å | µ = 0.09 mm−1 |
b = 13.690 (3) Å | T = 250 K |
c = 7.111 (1) Å | Plate, colourless |
V = 1315.2 (5) Å3 | 0.3 × 0.3 × 0.2 mm |
Data collection top
KUMA-4 diffractometer | Rint = 0.000 |
Radiation source: fine-focus sealed tube | θmax = 28.1°, θmin = 2.1° |
Graphite monochromator | h = 0→17 |
θ–2θ scans | k = 0→18 |
866 measured reflections | l = 0→9 |
866 independent reflections | 2 standard reflections every 100 reflections |
655 reflections with I > 2σ(I) | intensity decay: none |
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)] = 0.045 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.138 | Calculated w = 1/[σ2(Fo2) + (0.1P)2 + 0.0891P] where P = (Fo2 + 2Fc2)/3 |
S = 1.03 | (Δ/σ)max = 0.013 |
866 reflections | Δρmax = 0.25 e Å−3 |
104 parameters | Δρmin = −0.18 e Å−3 |
0 restraints | |
Crystal data top
C7H10O2 | V = 1315.2 (5) Å3 |
Mr = 126.15 | Z = 8 |
Orthorhombic, Ibam | Mo Kα radiation |
a = 13.510 (3) Å | µ = 0.09 mm−1 |
b = 13.690 (3) Å | T = 250 K |
c = 7.111 (1) Å | 0.3 × 0.3 × 0.2 mm |
Data collection top
KUMA-4 diffractometer | Rint = 0.000 |
866 measured reflections | 2 standard reflections every 100 reflections |
866 independent reflections | intensity decay: none |
655 reflections with I > 2σ(I) | |
Refinement top
R[F2 > 2σ(F2)] = 0.045 | 104 parameters |
wR(F2) = 0.138 | 0 restraints |
S = 1.03 | Δρmax = 0.25 e Å−3 |
866 reflections | Δρmin = −0.18 e Å−3 |
Special details top
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 on F2 for ALL reflections except for 0 with very negative
F2 or flagged by the user for potential systematic errors. Weighted
R-factors wR and all goodnesses of fit S are based on
F2, conventional R-factors R are based on F,
with F set to zero for negative F2. The observed criterion of
F2 > σ(F2) is used only for calculating _R_factor_obs
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 | Occ. (<1) |
O1 | 0.31902 (8) | 0.20153 (8) | 0.0000 | 0.0524 (4) | |
O2 | 0.27336 (11) | 0.53660 (9) | 0.0000 | 0.0710 (6) | |
C1 | 0.25946 (11) | 0.27924 (10) | 0.0000 | 0.0380 (4) | |
C2 | 0.30069 (10) | 0.36961 (10) | 0.0000 | 0.0396 (4) | |
C7 | 0.40993 (13) | 0.38555 (14) | 0.0000 | 0.0595 (7) | |
H71 | 0.425 (5) | 0.447 (5) | 0.0000 | 0.09 (3)* | 0.47 (6) |
H72 | 0.438 (3) | 0.341 (4) | 0.121 (7) | 0.082 (19)* | 0.47 (6) |
H73 | 0.426 (2) | 0.423 (2) | 0.126 (4) | 0.046 (12)* | 0.53 (6) |
H74 | 0.444 (4) | 0.330 (5) | 0.0000 | 0.080 (18)* | 0.53 (6) |
C3 | 0.23808 (13) | 0.45325 (11) | 0.0000 | 0.0522 (5) | |
C4 | 0.1283 (2) | 0.4382 (2) | −0.0525 (4) | 0.0523 (11) | 0.50 |
H41 | 0.0928 (18) | 0.501 (2) | −0.041 (4) | 0.053 (8)* | 0.50 |
H42 | 0.119 (3) | 0.434 (3) | −0.175 (5) | 0.061 (10)* | 0.50 |
C5 | 0.0904 (2) | 0.3484 (2) | 0.0489 (5) | 0.056 (2) | 0.50 |
H51 | 0.103 (2) | 0.361 (2) | 0.188 (5) | 0.056 (9)* | 0.50 |
H52 | 0.0187 (18) | 0.3351 (17) | 0.042 (4) | 0.043 (8)* | 0.50 |
C6 | 0.15042 (12) | 0.25947 (12) | 0.0000 | 0.0465 (5) | |
H61 | 0.139 (2) | 0.202 (2) | 0.065 (4) | 0.046 (8)* | 0.50 |
H62 | 0.137 (2) | 0.237 (2) | −0.149 (4) | 0.053 (8)* | 0.50 |
H1 | 0.283 (2) | 0.140 (2) | 0.0000 | 0.086 (9)* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
O1 | 0.0343 (6) | 0.0210 (6) | 0.1018 (11) | 0.0024 (4) | 0.000 | 0.000 |
O2 | 0.0523 (8) | 0.0204 (6) | 0.1403 (15) | 0.0013 (5) | 0.000 | 0.000 |
C1 | 0.0295 (7) | 0.0229 (7) | 0.0618 (9) | 0.0018 (5) | 0.000 | 0.000 |
C2 | 0.0274 (7) | 0.0225 (7) | 0.0691 (10) | −0.0003 (5) | 0.000 | 0.000 |
C7 | 0.0280 (8) | 0.0329 (9) | 0.118 (2) | −0.0056 (5) | 0.000 | 0.000 |
C3 | 0.0362 (9) | 0.0226 (8) | 0.0980 (14) | 0.0031 (5) | 0.000 | 0.000 |
C4 | 0.0350 (11) | 0.0346 (11) | 0.087 (3) | 0.0096 (7) | −0.0055 (10) | 0.0005 (10) |
C5 | 0.0280 (9) | 0.0387 (12) | 0.103 (5) | 0.0028 (7) | 0.0042 (11) | −0.0051 (12) |
C6 | 0.0292 (8) | 0.0293 (8) | 0.0808 (12) | −0.0046 (6) | 0.000 | 0.000 |
Geometric parameters (Å, º) top
O1—C1 | 1.334 (2) | C4—C4i | 0.747 (6) |
O1—H1 | 0.97 (3) | C4—C5i | 1.332 (3) |
O2—C3 | 1.237 (2) | C4—C5 | 1.514 (4) |
C1—C2 | 1.357 (2) | C4—H41 | 0.99 (3) |
C1—C6 | 1.498 (2) | C4—H42 | 0.88 (3) |
C2—C3 | 1.424 (2) | C5—C5i | 0.696 (7) |
C2—C7 | 1.492 (2) | C5—C4i | 1.332 (3) |
C7—H71 | 0.86 (7) | C5—C6 | 1.504 (3) |
C7—H72 | 1.12 (5) | C5—H51 | 1.02 (3) |
C7—H73 | 1.05 (3) | C5—H52 | 0.99 (2) |
C7—H74 | 0.89 (7) | C6—C5i | 1.504 (3) |
C3—C4 | 1.544 (3) | C6—H61 | 0.93 (3) |
C3—C4i | 1.544 (3) | C6—H62 | 1.12 (3) |
| | | |
C1—O1—H1 | 112.7 (18) | C3—C4—H41 | 109.3 (15) |
O1—C1—C2 | 118.66 (14) | C4i—C4—H42 | 171 (2) |
O1—C1—C6 | 116.69 (13) | C5i—C4—H42 | 84 (2) |
C2—C1—C6 | 124.65 (13) | C5—C4—H42 | 112 (2) |
C1—C2—C3 | 119.30 (13) | C3—C4—H42 | 112 (2) |
C1—C2—C7 | 122.65 (14) | H41—C4—H42 | 94 (3) |
C3—C2—C7 | 118.05 (14) | C5i—C5—C4i | 91.1 (2) |
C2—C7—H71 | 112 (5) | C5i—C5—C6 | 76.62 (12) |
C2—C7—H72 | 105 (2) | C4i—C5—C6 | 123.0 (2) |
H71—C7—H72 | 117 (3) | C5i—C5—C4 | 61.5 (2) |
C2—C7—H73 | 106.0 (15) | C4i—C5—C4 | 29.6 (2) |
H71—C7—H73 | 58.7 (14) | C6—C5—C4 | 111.4 (2) |
H72—C7—H73 | 63 (2) | C5i—C5—H51 | 166.7 (18) |
C2—C7—H74 | 113 (4) | C4i—C5—H51 | 76.6 (18) |
H71—C7—H74 | 136 (6) | C6—C5—H51 | 105.6 (18) |
H72—C7—H74 | 50 (2) | C4—C5—H51 | 106.1 (18) |
H73—C7—H74 | 108 (2) | C5i—C5—H52 | 86.9 (15) |
O2—C3—C2 | 120.87 (15) | C4i—C5—H52 | 123.3 (14) |
O2—C3—C4 | 119.57 (15) | C6—C5—H52 | 111.6 (14) |
C2—C3—C4 | 117.64 (14) | C4—C5—H52 | 117.1 (14) |
O2—C3—C4i | 119.57 (15) | H51—C5—H52 | 104 (2) |
C2—C3—C4i | 117.64 (14) | C1—C6—C5 | 112.58 (14) |
C4—C3—C4i | 28.0 (2) | C1—C6—C5i | 112.58 (14) |
C4i—C4—C5i | 88.9 (2) | C5—C6—C5i | 26.8 (3) |
C4i—C4—C5 | 61.5 (2) | C1—C6—H61 | 108.7 (19) |
C5i—C4—C5 | 27.3 (3) | C5—C6—H61 | 118.9 (18) |
C4i—C4—C3 | 75.99 (11) | C5i—C6—H61 | 135.5 (19) |
C5i—C4—C3 | 119.2 (2) | C1—C6—H62 | 102.1 (17) |
C5—C4—C3 | 108.5 (2) | C5—C6—H62 | 110.6 (17) |
C4i—C4—H41 | 85.4 (17) | C5i—C6—H62 | 85.0 (17) |
C5i—C4—H41 | 128.0 (15) | H61—C6—H62 | 102 (3) |
C5—C4—H41 | 120.3 (16) | | |
| | | |
O1—C1—C2—C3 | 180.0 | C4i—C4—C5—C5i | 180.000 (1) |
C6—C1—C2—C3 | 0.0 | C5i—C4—C5—C5i | 0.0 |
O1—C1—C2—C7 | 0.0 | C3—C4—C5—C5i | −118.1 (2) |
C6—C1—C2—C7 | 180.0 | C4i—C4—C5—C4i | 0.000 (1) |
C1—C2—C3—O2 | 180.0 | C5i—C4—C5—C4i | 180.000 (1) |
C7—C2—C3—O2 | 0.0 | C3—C4—C5—C4i | 61.9 (2) |
C1—C2—C3—C4 | −15.85 (12) | C4i—C4—C5—C6 | −119.7 (2) |
C7—C2—C3—C4 | 164.15 (12) | C5i—C4—C5—C6 | 60.3 (2) |
C1—C2—C3—C4i | 15.85 (12) | C3—C4—C5—C6 | −57.8 (3) |
C7—C2—C3—C4i | −164.15 (12) | O1—C1—C6—C5 | 165.49 (14) |
O2—C3—C4—C4i | −98.13 (8) | C2—C1—C6—C5 | −14.51 (14) |
C2—C3—C4—C4i | 97.50 (7) | O1—C1—C6—C5i | −165.49 (14) |
C4i—C3—C4—C4i | 0.0 | C2—C1—C6—C5i | 14.51 (14) |
O2—C3—C4—C5i | −178.8 (2) | C5i—C5—C6—C1 | 95.67 (7) |
C2—C3—C4—C5i | 16.8 (3) | C4i—C5—C6—C1 | 13.2 (3) |
C4i—C3—C4—C5i | −80.7 (3) | C4—C5—C6—C1 | 43.9 (2) |
O2—C3—C4—C5 | −151.17 (15) | C5i—C5—C6—C5i | 0.0 |
C2—C3—C4—C5 | 44.5 (2) | C4i—C5—C6—C5i | −82.5 (3) |
C4i—C3—C4—C5 | −53.0 (2) | C4—C5—C6—C5i | −51.7 (2) |
Symmetry code: (i) x, y, −z. |
Crystal data top
C7H10O2 | Z = 8 |
Mr = 126.15 | F(000) = 544 |
Orthorhombic, Ibam | Dx = 1.258 Mg m−3 |
Hall symbol: -I 2 2c | Mo Kα radiation, λ = 0.71069 Å |
a = 13.558 (3) Å | µ = 0.09 mm−1 |
b = 13.696 (3) Å | T = 293 K |
c = 7.174 (1) Å | Plate, colourless |
V = 1332.1 (5) Å3 | 0.5 × 0.4 × 0.2 mm |
Data collection top
KUMA-4 diffractometer | Rint = 0.019 |
Radiation source: fine-focus sealed tube | θmax = 26.0°, θmin = 2.1° |
Graphite monochromator | h = −12→−1 |
θ–2θ scans | k = −16→0 |
568 measured reflections | l = 0→8 |
566 independent reflections | 2 standard reflections every 100 reflections |
526 reflections with I > 2σ(I) | intensity decay: none |
Refinement top
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.044 | Calculated w = 1/[σ2(Fo2) + (0.0993P)2 + 0.0875P] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.116 | (Δ/σ)max = 3.670 |
S = 1.03 | Δρmax = 0.22 e Å−3 |
566 reflections | Δρmin = −0.18 e Å−3 |
105 parameters | Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.0649 (72) |
Primary atom site location: structure-invariant direct methods | |
Crystal data top
C7H10O2 | V = 1332.1 (5) Å3 |
Mr = 126.15 | Z = 8 |
Orthorhombic, Ibam | Mo Kα radiation |
a = 13.558 (3) Å | µ = 0.09 mm−1 |
b = 13.696 (3) Å | T = 293 K |
c = 7.174 (1) Å | 0.5 × 0.4 × 0.2 mm |
Data collection top
KUMA-4 diffractometer | Rint = 0.019 |
568 measured reflections | 2 standard reflections every 100 reflections |
566 independent reflections | intensity decay: none |
526 reflections with I > 2σ(I) | |
Refinement top
R[F2 > 2σ(F2)] = 0.044 | 0 restraints |
wR(F2) = 0.116 | (Δ/σ)max = 3.670 |
S = 1.03 | Δρmax = 0.22 e Å−3 |
566 reflections | Δρmin = −0.18 e Å−3 |
105 parameters | |
Special details top
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 on F2 for ALL reflections except for 0 with very negative
F2 or flagged by the user for potential systematic errors. Weighted
R-factors wR and all goodnesses of fit S are based on
F2, conventional R-factors R are based on F,
with F set to zero for negative F2. The observed criterion of
F2 > σ(F2) is used only for calculating _R_factor_obs
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 | Occ. (<1) |
O1 | 0.31952 (9) | 0.20214 (8) | 0.0000 | 0.0654 (5) | |
O2 | 0.27230 (12) | 0.53650 (9) | 0.0000 | 0.0856 (6) | |
C1 | 0.25952 (14) | 0.27921 (10) | 0.0000 | 0.0492 (5) | |
C2 | 0.30043 (12) | 0.36966 (12) | 0.0000 | 0.0528 (6) | |
C7 | 0.4090 (2) | 0.38588 (14) | 0.0000 | 0.0778 (8) | |
H71 | 0.417 (6) | 0.448 (8) | 0.0000 | 0.11 (3)* | 0.37 (6) |
H72 | 0.444 (3) | 0.338 (3) | 0.117 (6) | 0.062 (18)* | 0.37 (6) |
H73 | 0.428 (2) | 0.425 (3) | 0.122 (4) | 0.087 (13)* | 0.63 (6) |
H74 | 0.444 (3) | 0.329 (4) | 0.0000 | 0.077 (13)* | 0.63 (6) |
C3 | 0.2374 (2) | 0.45319 (12) | 0.0000 | 0.0630 (6) | |
C4 | 0.1281 (2) | 0.4377 (2) | −0.0472 (6) | 0.071 (2) | 0.50 |
H41 | 0.0934 (17) | 0.496 (2) | −0.041 (4) | 0.056 (7)* | 0.50 |
H42 | 0.122 (3) | 0.432 (4) | −0.192 (6) | 0.109 (15)* | 0.50 |
C5 | 0.0915 (2) | 0.3476 (2) | 0.0530 (4) | 0.0684 (14) | 0.50 |
H51 | 0.103 (2) | 0.360 (3) | 0.196 (5) | 0.079 (9)* | 0.50 |
H52 | 0.019 (2) | 0.3348 (19) | 0.040 (4) | 0.063 (9)* | 0.50 |
C6 | 0.15149 (15) | 0.25900 (13) | 0.0000 | 0.0591 (6) | |
H61 | 0.136 (2) | 0.199 (3) | 0.065 (4) | 0.068 (10)* | 0.50 |
H62 | 0.137 (2) | 0.238 (3) | −0.141 (5) | 0.069 (9)* | 0.50 |
H1 | 0.283 (3) | 0.145 (3) | 0.0000 | 0.110 (10)* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
O1 | 0.0452 (10) | 0.0298 (7) | 0.1213 (12) | 0.0026 (4) | 0.000 | 0.000 |
O2 | 0.0692 (11) | 0.0286 (7) | 0.159 (2) | 0.0008 (5) | 0.000 | 0.000 |
C1 | 0.0431 (12) | 0.0322 (8) | 0.0723 (10) | 0.0017 (5) | 0.000 | 0.000 |
C2 | 0.0400 (12) | 0.0332 (9) | 0.0853 (13) | −0.0006 (6) | 0.000 | 0.000 |
C7 | 0.0435 (14) | 0.0422 (11) | 0.148 (2) | −0.0054 (7) | 0.000 | 0.000 |
C3 | 0.0494 (13) | 0.0332 (9) | 0.1064 (14) | 0.0027 (6) | 0.000 | 0.000 |
C4 | 0.049 (2) | 0.0445 (12) | 0.121 (7) | 0.0119 (9) | −0.0044 (12) | 0.0022 (12) |
C5 | 0.040 (2) | 0.0539 (14) | 0.111 (4) | 0.0017 (9) | 0.0050 (10) | −0.0047 (11) |
C6 | 0.0445 (13) | 0.0376 (9) | 0.0951 (15) | −0.0067 (7) | 0.000 | 0.000 |
Geometric parameters (Å, º) top
O1—C1 | 1.333 (2) | C4—C4i | 0.678 (8) |
O1—H1 | 0.93 (4) | C4—C5i | 1.331 (4) |
O2—C3 | 1.235 (2) | C4—C5 | 1.513 (4) |
C1—C2 | 1.357 (2) | C4—H41 | 0.93 (3) |
C1—C6 | 1.491 (3) | C4—H42 | 1.04 (4) |
C2—C3 | 1.428 (2) | C5—C5i | 0.761 (6) |
C2—C7 | 1.489 (3) | C5—C4i | 1.331 (4) |
C7—H71 | 0.85 (11) | C5—C6 | 1.509 (3) |
C7—H72 | 1.17 (5) | C5—H51 | 1.05 (4) |
C7—H73 | 1.06 (3) | C5—H52 | 1.01 (3) |
C7—H74 | 0.91 (5) | C6—C5i | 1.509 (3) |
C3—C4 | 1.536 (4) | C6—H61 | 0.97 (3) |
C3—C4i | 1.536 (4) | C6—H62 | 1.07 (3) |
| | | |
C1—O1—H1 | 110 (2) | C3—C4—H41 | 111.0 (14) |
O1—C1—C2 | 118.3 (2) | C4i—C4—H42 | 174 (2) |
O1—C1—C6 | 116.92 (14) | C5i—C4—H42 | 83 (3) |
C2—C1—C6 | 124.81 (15) | C5—C4—H42 | 113 (3) |
C1—C2—C3 | 119.1 (2) | C3—C4—H42 | 108 (2) |
C1—C2—C7 | 122.7 (2) | H41—C4—H42 | 94 (3) |
C3—C2—C7 | 118.15 (15) | C5i—C5—C4i | 88.2 (2) |
C2—C7—H71 | 106 (6) | C5i—C5—C6 | 75.40 (11) |
C2—C7—H72 | 108.8 (19) | C4i—C5—C6 | 122.4 (2) |
H71—C7—H72 | 121 (4) | C5i—C5—C4 | 61.6 (2) |
C2—C7—H73 | 108.4 (15) | C4i—C5—C4 | 26.6 (3) |
H71—C7—H73 | 58.1 (19) | C6—C5—C4 | 111.1 (2) |
H72—C7—H73 | 66 (2) | C5i—C5—H51 | 167.2 (18) |
C2—C7—H74 | 113 (3) | C4i—C5—H51 | 80 (2) |
H71—C7—H74 | 142 (6) | C6—C5—H51 | 106.9 (19) |
H72—C7—H74 | 46 (2) | C4—C5—H51 | 107 (2) |
H73—C7—H74 | 108 (2) | C5i—C5—H52 | 84.8 (16) |
O2—C3—C2 | 120.8 (2) | C4i—C5—H52 | 121.6 (15) |
O2—C3—C4 | 119.8 (2) | C6—C5—H52 | 111.5 (16) |
C2—C3—C4 | 117.83 (15) | C4—C5—H52 | 114.9 (15) |
O2—C3—C4i | 119.8 (2) | H51—C5—H52 | 106 (2) |
C2—C3—C4i | 117.83 (15) | C1—C6—C5 | 112.4 (2) |
C4—C3—C4i | 25.5 (3) | C1—C6—C5i | 112.4 (2) |
C4i—C4—C5i | 91.8 (2) | C5—C6—C5i | 29.2 (2) |
C4i—C4—C5 | 61.6 (2) | C1—C6—H61 | 112.0 (19) |
C5i—C4—C5 | 30.2 (2) | C5—C6—H61 | 116 (2) |
C4i—C4—C3 | 77.3 (2) | C5i—C6—H61 | 133.1 (19) |
C5i—C4—C3 | 119.6 (2) | C1—C6—H62 | 103.1 (17) |
C5—C4—C3 | 108.9 (2) | C5—C6—H62 | 111.1 (19) |
C4i—C4—H41 | 87.3 (16) | C5i—C6—H62 | 83.3 (19) |
C5i—C4—H41 | 127.7 (15) | H61—C6—H62 | 101 (3) |
C5—C4—H41 | 121.0 (15) | | |
| | | |
O1—C1—C2—C3 | 180.0 | C4i—C4—C5—C5i | 180.000 (1) |
C6—C1—C2—C3 | 0.0 | C5i—C4—C5—C5i | 0.000 (1) |
O1—C1—C2—C7 | 0.0 | C3—C4—C5—C5i | −116.8 (2) |
C6—C1—C2—C7 | 180.0 | C4i—C4—C5—C4i | 0.000 (1) |
C1—C2—C3—O2 | 180.0 | C5i—C4—C5—C4i | 180.000 (2) |
C7—C2—C3—O2 | 0.0 | C3—C4—C5—C4i | 63.2 (2) |
C1—C2—C3—C4 | −14.4 (2) | C4i—C4—C5—C6 | −121.0 (2) |
C7—C2—C3—C4 | 165.6 (2) | C5i—C4—C5—C6 | 59.0 (2) |
C1—C2—C3—C4i | 14.4 (2) | C3—C4—C5—C6 | −57.8 (3) |
C7—C2—C3—C4i | −165.6 (2) | O1—C1—C6—C5 | 164.18 (12) |
O2—C3—C4—C4i | −97.44 (10) | C2—C1—C6—C5 | −15.82 (12) |
C2—C3—C4—C4i | 96.86 (9) | O1—C1—C6—C5i | −164.18 (12) |
C4i—C3—C4—C4i | 0.0 | C2—C1—C6—C5i | 15.82 (12) |
O2—C3—C4—C5i | 177.8 (2) | C5i—C5—C6—C1 | 96.16 (7) |
C2—C3—C4—C5i | 12.1 (4) | C4i—C5—C6—C1 | 17.9 (3) |
C4i—C3—C4—C5i | −84.7 (3) | C4—C5—C6—C1 | 45.0 (2) |
O2—C3—C4—C5 | −151.1 (2) | C5i—C5—C6—C5i | 0.0 |
C2—C3—C4—C5 | 43.2 (3) | C4i—C5—C6—C5i | −78.2 (3) |
C4i—C3—C4—C5 | −53.6 (2) | C4—C5—C6—C5i | −51.2 (2) |
Symmetry code: (i) x, y, −z. |
Experimental details
| (123) | (170) | (180) | (220) |
Crystal data |
Chemical formula | C7H10O2 | C7H10O2 | C7H10O2 | C7H10O2 |
Mr | 126.15 | 126.15 | 126.15 | 126.15 |
Crystal system, space group | Orthorhombic, Pccn | Orthorhombic, Pccn | Orthorhombic, Pccn | Orthorhombic, Pccn |
Temperature (K) | 123 | 170 | 180 | 220 |
a, b, c (Å) | 13.427 (3), 13.689 (3), 6.946 (2) | 13.426 (4), 13.690 (4), 6.987 (2) | 13.466 (4), 13.691 (4), 7.053 (2) | 13.466 (4), 13.691 (4), 7.053 (2) |
V (Å3) | 1276.7 (5) | 1284.2 (6) | 1300.3 (7) | 1300.3 (7) |
Z | 8 | 8 | 8 | 8 |
Radiation type | Mo Kα | Mo Kα | Mo Kα | Mo Kα |
µ (mm−1) | 0.10 | 0.10 | 0.09 | 0.09 |
Crystal size (mm) | 0.3 × 0.3 × 0.2 | 0.3 × 0.3 × 0.2 | 0.4 × 0.3 × 0.2 | 0.3 × 0.3 × 0.2 |
|
Data collection |
Diffractometer | KUMA-4-CCD diffractometer | KUMA-4 diffractometer | KUMA-4-CCD diffractometer | KUMA-4 diffractometer |
Absorption correction | – | – | – | – |
No. of measured, independent and observed [I > 2σ(I)] reflections | 6596, 1616, 1322 | 846, 846, 742 | 7637, 1712, 1088 | 856, 856, 723 |
Rint | 0.055 | 0.000 | 0.077 | 0.000 |
(sin θ/λ)max (Å−1) | 0.698 | 0.662 | 0.698 | 0.662 |
|
Refinement |
R[F2 > 2σ(F2)], wR(F2), S | 0.053, 0.157, 1.10 | 0.040, 0.118, 1.04 | 0.092, 0.278, 1.15 | 0.044, 0.135, 1.04 |
No. of reflections | 1616 | 846 | 1712 | 856 |
No. of parameters | 117 | 91 | 117 | 91 |
(Δ/σ)max | −0.014 | 0.014 | 0.007 | 0.047 |
Δρmax, Δρmin (e Å−3) | 0.44, −0.31 | 0.38, −0.14 | 0.66, −0.30 | 0.18, −0.39 |
| (225) | (239) | (240) | (242) |
Crystal data |
Chemical formula | C7H10O2 | C7H10O2 | C7H10O2 | C7H10O2 |
Mr | 126.15 | 126.15 | 126.15 | 126.15 |
Crystal system, space group | Orthorhombic, Pccn | Orthorhombic, Pccn | Orthorhombic, Pccn | Orthorhombic, Pccn |
Temperature (K) | 225 | 239.K | 240 | 242 |
a, b, c (Å) | 13.472 (4), 13.692 (4), 7.062 (2) | 13.472 (4), 13.692 (4), 7.090 (2) | 13.492 (4), 13.692 (4), 7.091 (2) | 13.498 (4), 13.691 (4), 7.095 (2) |
V (Å3) | 1302.6 (7) | 1307.8 (7) | 1309.9 (7) | 1311.2 (7) |
Z | 8 | 8 | 8 | 8 |
Radiation type | Mo Kα | Mo Kα | Mo Kα | Mo Kα |
µ (mm−1) | 0.09 | 0.09 | 0.09 | 0.09 |
Crystal size (mm) | 0.4 × 0.3 × 0.2 | 0.4 × 0.3 × 0.2 | 0.4 × 0.3 × 0.2 | 0.4 × 0.3 × 0.2 |
|
Data collection |
Diffractometer | KUMA-4-CCD diffractometer | KUMA-4-CCD diffractometer | KUMA-4-CCD diffractometer | KUMA-4-CCD diffractometer |
Absorption correction | – | – | – | – |
No. of measured, independent and observed [I > 2σ(I)] reflections | 8309, 1756, 1097 | 8221, 1758, 1073 | 8148, 1777, 948 | 8192, 1778, 889 |
Rint | 0.044 | 0.035 | 0.066 | 0.066 |
(sin θ/λ)max (Å−1) | 0.696 | 0.696 | 0.701 | 0.699 |
|
Refinement |
R[F2 > 2σ(F2)], wR(F2), S | 0.091, 0.272, 1.17 | 0.107, 0.329, 1.26 | 0.196, 0.490, 1.31 | 0.186, 0.510, 1.29 |
No. of reflections | 1756 | 1758 | 1777 | 1778 |
No. of parameters | 117 | 117 | 91 | 91 |
(Δ/σ)max | 0.017 | 0.045 | 0.114 | 0.017 |
Δρmax, Δρmin (e Å−3) | 0.51, −0.24 | 0.50, −0.21 | 0.57, −0.32 | 0.50, −0.35 |
| (250) | (293) |
Crystal data |
Chemical formula | C7H10O2 | C7H10O2 |
Mr | 126.15 | 126.15 |
Crystal system, space group | Orthorhombic, Ibam | Orthorhombic, Ibam |
Temperature (K) | 250 | 293 |
a, b, c (Å) | 13.510 (3), 13.690 (3), 7.111 (1) | 13.558 (3), 13.696 (3), 7.174 (1) |
V (Å3) | 1315.2 (5) | 1332.1 (5) |
Z | 8 | 8 |
Radiation type | Mo Kα | Mo Kα |
µ (mm−1) | 0.09 | 0.09 |
Crystal size (mm) | 0.3 × 0.3 × 0.2 | 0.5 × 0.4 × 0.2 |
|
Data collection |
Diffractometer | KUMA-4 diffractometer | KUMA-4 diffractometer |
Absorption correction | – | – |
No. of measured, independent and observed [I > 2σ(I)] reflections | 866, 866, 655 | 568, 566, 526 |
Rint | 0.000 | 0.019 |
(sin θ/λ)max (Å−1) | 0.662 | 0.616 |
|
Refinement |
R[F2 > 2σ(F2)], wR(F2), S | 0.045, 0.138, 1.03 | 0.044, 0.116, 1.03 |
No. of reflections | 866 | 566 |
No. of parameters | 104 | 105 |
(Δ/σ)max | 0.013 | 3.670 |
Δρmax, Δρmin (e Å−3) | 0.25, −0.18 | 0.22, −0.18 |
Hydrogen-bond dimensions in
2-methyl-1,3-cyclohexanedione at varied temperatures.
Angle $ρho$ between the line passing through O(1) and O(2) of
one molecule and the [010] direction describes the inclination
of the molecules to the direction of the chains.
Also the deviations of methylene atoms C(4) and C(5) from the
least-squares plane fitted to the remaining non-H atoms of the
molecule, denoted d[C(4)] and d[C(5)] respectively,
have been given.
The negative sign of d[C(5)] indicate the location of C(5)
on the opposite site of the plane than C(4). top | 123K | 170K | 180K | 220K | 225K | 239K | 250K | 293K |
O(1)···O(2i) | 2.576 (1) | 2.577 (4) | 2.578 (3) | 2.578 (2) | 2.579 (3) | 2.576 (3) | 2.580 (2) | 2.588 (2) |
O(1)–H(1) | 1.00 (2) | 0.99 (3) | 1.13 (4) | 1.00 (3) | 1.05 (5) | 0.98 (5) | 0.97 (3) | 0.93 (3) |
H(1)···O(2i) | 1.58 (2) | 1.60 (3) | 1.45 (4) | 1.59 (3) | 1.53 (5) | 1.60 (5) | 1.61 (3) | 1.66 (3) |
O(1)–H(1)···O(2i) | 175 (2) | 166 (5) | 177 (3) | 168 (4) | 175 (4) | 176 (3) | 178 (3) | 175 (3) |
C(1)–O(1)–H(1)(ηd) | 111.1 (13) | 110.4 (18) | 115 (2) | 111.2 (16) | 117 (3) | 113 (3) | 112.7 (18) | 110.3 (19) |
H(1)···O(2i)=C(3i)(ηa) | 128.8 (8) | 129.4 (9) | 126 (2) | 129.3 (10) | 126 (2) | 128.6 (18) | 129.2 (11) | 130.6 (12) |
C(1)–O(1)···O(2i)(η'd) | 114.25 (8) | 114.4 (2) | 114.49 (16) | 114.25 (14) | 114.37 (15) | 114.2 (2) | 113.97 (10) | 113.63 (11) |
O(1)···O(2i)=C(3i)(η'a) | 126.86 (9) | 127.20 (13) | 127.42 (17) | 127.76 (13) | 127.82 | 128.2 (2) | 128.40 (12) | 128.75 (14) |
$ρho$ | 7.90 (2) | 7.7 (4) | 7.94 (4) | 8.1 (3) | 7.98 (4) | 7.90 (4) | 7.66 (9) | 7.96 (3) |
$d$[C(4)][{AA}] | 0.114 (2) | 0.159 (9) | 0.125 (5) | 0.160 (21) | 0.118 (5) | 0.126 (7) | 0.373 (3) | 0.339 (4) |
$d$[C(5)] | -0.614 (2) | -0.556 (8) | -0.586 (6) | -0.529 (30) | -0.547 (7) | -0.449 (8) | -0.348 (3) | -0.381 (3) |
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