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The title molecule, C
18H
14O
2, possesses a crystallographically imposed inversion centre. The carbonyl groups are twisted away from the anthracene mean plane by 21.03 (1)°. The crystal packing is stabilized by C—H
π interactions and C—H
O hydrogen bonds.
Supporting information
CCDC reference: 620782
Key indicators
- Single-crystal X-ray study
- T = 153 K
- Mean (C-C) = 0.001 Å
- R factor = 0.034
- wR factor = 0.108
- Data-to-parameter ratio = 15.5
checkCIF/PLATON results
No syntax errors found
Alert level C
PLAT125_ALERT_4_C No _symmetry_space_group_name_Hall Given ....... ?
0 ALERT level A = In general: serious problem
0 ALERT level B = Potentially serious problem
1 ALERT level C = Check and explain
0 ALERT level G = General alerts; check
0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data
0 ALERT type 2 Indicator that the structure model may be wrong or deficient
0 ALERT type 3 Indicator that the structure quality may be low
1 ALERT type 4 Improvement, methodology, query or suggestion
0 ALERT type 5 Informative message, check
Data collection: RAPID-AUTO (Rigaku, 2004); cell refinement: RAPID-AUTO; data reduction: RAPID-AUTO; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: XP in SHELXTL (Bruker, 1997); software used to prepare material for publication: SHELXTL.
1,5-diacetylanthracene
top
Crystal data top
C18H14O2 | F(000) = 276 |
Mr = 262.29 | Dx = 1.376 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
a = 9.8245 (3) Å | Cell parameters from 5428 reflections |
b = 6.2085 (2) Å | θ = 3.3–27.5° |
c = 10.8823 (3) Å | µ = 0.09 mm−1 |
β = 107.472 (1)° | T = 153 K |
V = 633.15 (3) Å3 | Block, yellow |
Z = 2 | 0.40 × 0.35 × 0.14 mm |
Data collection top
Rigaku R-AXIS RAPID diffractometer | 1327 reflections with I > 2σ(I) |
Radiation source: Rotating Anode | Rint = 0.025 |
Graphite monochromator | θmax = 27.5°, θmin = 3.8° |
ω scans | h = −12→12 |
5967 measured reflections | k = −8→8 |
1445 independent reflections | l = −14→13 |
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)] = 0.034 | H-atom parameters constrained |
wR(F2) = 0.108 | w = 1/[σ2(Fo2) + (0.069P)2 + 0.198P] where P = (Fo2 + 2Fc2)/3 |
S = 1.02 | (Δ/σ)max < 0.001 |
1445 reflections | Δρmax = 0.35 e Å−3 |
93 parameters | Δρmin = −0.20 e Å−3 |
0 restraints | Extinction correction: SHELXL97 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.033 (9) |
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 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 | 0.14358 (8) | 0.14110 (13) | 0.36628 (7) | 0.0263 (2) | |
C1 | 0.57789 (10) | 0.69074 (16) | 0.50455 (9) | 0.0164 (2) | |
H1 | 0.6295 | 0.8208 | 0.5064 | 0.020* | |
C2 | 0.45663 (10) | 0.64994 (15) | 0.39979 (9) | 0.0159 (2) | |
C3 | 0.41660 (11) | 0.80048 (16) | 0.29567 (9) | 0.0183 (3) | |
H3 | 0.4679 | 0.9317 | 0.3014 | 0.022* | |
C4 | 0.30580 (11) | 0.75803 (17) | 0.18838 (10) | 0.0203 (3) | |
H4 | 0.2832 | 0.8560 | 0.1181 | 0.024* | |
C5 | 0.22422 (11) | 0.56756 (17) | 0.18159 (9) | 0.0200 (3) | |
H5 | 0.1471 | 0.5406 | 0.1062 | 0.024* | |
C6 | 0.25323 (10) | 0.42049 (16) | 0.28068 (9) | 0.0171 (2) | |
C7 | 0.37525 (10) | 0.45566 (15) | 0.39354 (9) | 0.0152 (2) | |
C8 | 0.15277 (10) | 0.23605 (17) | 0.27077 (9) | 0.0183 (3) | |
C9 | 0.05500 (12) | 0.17535 (18) | 0.13957 (10) | 0.0239 (3) | |
H9A | 0.0248 | 0.0252 | 0.1409 | 0.029* | |
H9B | 0.1058 | 0.1921 | 0.0752 | 0.029* | |
H9C | −0.0290 | 0.2693 | 0.1175 | 0.029* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
O1 | 0.0262 (4) | 0.0300 (5) | 0.0218 (4) | −0.0091 (3) | 0.0057 (3) | 0.0026 (3) |
C1 | 0.0197 (5) | 0.0149 (5) | 0.0158 (5) | −0.0014 (3) | 0.0070 (4) | −0.0009 (3) |
C2 | 0.0189 (5) | 0.0147 (5) | 0.0153 (5) | 0.0010 (3) | 0.0068 (4) | −0.0006 (3) |
C3 | 0.0217 (5) | 0.0152 (5) | 0.0190 (5) | 0.0003 (3) | 0.0078 (4) | 0.0015 (4) |
C4 | 0.0233 (5) | 0.0202 (5) | 0.0177 (5) | 0.0032 (4) | 0.0065 (4) | 0.0054 (4) |
C5 | 0.0184 (5) | 0.0230 (5) | 0.0170 (5) | 0.0012 (4) | 0.0031 (4) | 0.0002 (4) |
C6 | 0.0170 (5) | 0.0177 (5) | 0.0167 (5) | −0.0002 (4) | 0.0056 (4) | −0.0020 (4) |
C7 | 0.0173 (5) | 0.0158 (5) | 0.0138 (5) | 0.0002 (3) | 0.0065 (3) | −0.0017 (3) |
C8 | 0.0168 (5) | 0.0195 (5) | 0.0187 (5) | 0.0008 (4) | 0.0056 (4) | −0.0017 (4) |
C9 | 0.0234 (5) | 0.0248 (5) | 0.0201 (5) | −0.0047 (4) | 0.0015 (4) | −0.0023 (4) |
Geometric parameters (Å, º) top
O1—C8 | 1.2217 (13) | C5—C6 | 1.3760 (14) |
C1—C7i | 1.4006 (13) | C5—H5 | 0.9500 |
C1—C2 | 1.4027 (13) | C6—C7 | 1.4523 (13) |
C1—H1 | 0.9500 | C6—C8 | 1.4943 (14) |
C2—C3 | 1.4298 (13) | C7—C1i | 1.4006 (13) |
C2—C7 | 1.4374 (13) | C8—C9 | 1.5098 (14) |
C3—C4 | 1.3618 (14) | C9—H9A | 0.9800 |
C3—H3 | 0.9500 | C9—H9B | 0.9800 |
C4—C5 | 1.4179 (15) | C9—H9C | 0.9800 |
C4—H4 | 0.9500 | | |
| | | |
C7i—C1—C2 | 121.56 (9) | C5—C6—C7 | 119.15 (9) |
C7i—C1—H1 | 119.2 | C5—C6—C8 | 118.36 (9) |
C2—C1—H1 | 119.2 | C7—C6—C8 | 122.40 (9) |
C1—C2—C3 | 119.37 (9) | C1i—C7—C2 | 117.47 (9) |
C1—C2—C7 | 120.97 (9) | C1i—C7—C6 | 124.31 (9) |
C3—C2—C7 | 119.62 (9) | C2—C7—C6 | 118.19 (9) |
C4—C3—C2 | 120.78 (9) | O1—C8—C6 | 121.62 (9) |
C4—C3—H3 | 119.6 | O1—C8—C9 | 119.70 (9) |
C2—C3—H3 | 119.6 | C6—C8—C9 | 118.59 (9) |
C3—C4—C5 | 119.99 (9) | C8—C9—H9A | 109.5 |
C3—C4—H4 | 120.0 | C8—C9—H9B | 109.5 |
C5—C4—H4 | 120.0 | H9A—C9—H9B | 109.5 |
C6—C5—C4 | 122.12 (9) | C8—C9—H9C | 109.5 |
C6—C5—H5 | 118.9 | H9A—C9—H9C | 109.5 |
C4—C5—H5 | 118.9 | H9B—C9—H9C | 109.5 |
| | | |
C7i—C1—C2—C3 | −177.47 (9) | C1—C2—C7—C6 | −178.28 (8) |
C7i—C1—C2—C7 | 0.29 (15) | C3—C2—C7—C6 | −0.53 (14) |
C1—C2—C3—C4 | 175.14 (9) | C5—C6—C7—C1i | −174.62 (9) |
C7—C2—C3—C4 | −2.65 (15) | C8—C6—C7—C1i | 8.73 (15) |
C2—C3—C4—C5 | 3.07 (15) | C5—C6—C7—C2 | 3.24 (14) |
C3—C4—C5—C6 | −0.23 (16) | C8—C6—C7—C2 | −173.42 (8) |
C4—C5—C6—C7 | −2.95 (15) | C5—C6—C8—O1 | −156.50 (10) |
C4—C5—C6—C8 | 173.84 (9) | C7—C6—C8—O1 | 20.18 (15) |
C1—C2—C7—C1i | −0.28 (15) | C5—C6—C8—C9 | 20.03 (14) |
C3—C2—C7—C1i | 177.47 (8) | C7—C6—C8—C9 | −163.30 (9) |
Symmetry code: (i) −x+1, −y+1, −z+1. |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
C3—H3···Cg1ii | 0.95 | 2.64 | 3.415 (1) | 140 |
C9—H9C···O1iii | 0.98 | 2.60 | 3.478 (1) | 150 |
Symmetry codes: (ii) −x+1, y+1/2, −z+1/2; (iii) −x, y+1/2, −z+1/2. |
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