Literature DB >> 22798876

5,6-Dimethyl-1,2,9,10-tetra-hydro-pyrano[3,2-f]chromene-3,8-dione.

Shailesh K Goswami1, Lyall R Hanton, C John McAdam, Stephen C Moratti, Jim Simpson.   

Abstract

The title mol-ecule, C(14)H(14)O(4), lies on a twofold rotation axis that bis-ects the central benzene ring, with only one half-mol-ecule in the asymmetric unit. The pyran-one systems adopt distorted twist- boat conformations, with the two methyl-ene C atoms displaced by 0.537 (1) and 0.163 (2) Å from the best-fit plane through the remaining five C and O atoms (r.m.s. deviation = 0.073 Å). In the crystal, bifurcated C-H⋯(O,O) hydrogen bonds link pairs of adjacent mol-ecules in an obverse fashion, stacking mol-ecules along c. These contacts are further stabilized by very weak π-π inter-actions between adjacent benzene rings with centroid-centroid distances of 4.1951 (4) Å. Additional C-H⋯O contacts link these stacks, giving a three-dimensional network.

Entities:  

Year:  2012        PMID: 22798876      PMCID: PMC3394011          DOI: 10.1107/S1600536812027699

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For the synthesis, see: Lecea et al. (2010 ▶). For details of the Cambridge Structural Database, see: Allen (2002 ▶) and for related structures, see: Cameron et al. (2011 ▶); Goswami et al. (2011 ▶). For standard bond lengths, see: Allen et al. (1987 ▶).

Experimental

Crystal data

C14H14O4 M = 246.25 Monoclinic, a = 16.0726 (2) Å b = 8.7982 (1) Å c = 8.0555 (1) Å β = 96.1134 (7)° V = 1132.65 (2) Å3 Z = 4 Mo Kα radiation μ = 0.11 mm−1 T = 92 K 0.53 × 0.50 × 0.22 mm

Data collection

Bruker APEXII CCD area-detector diffractometer Absorption correction: multi-scan (SADABS; Bruker, 2011 ▶) T min = 0.570, T max = 0.748 9744 measured reflections 2989 independent reflections 2358 reflections with I > 2σ(I) R int = 0.038

Refinement

R[F 2 > 2σ(F 2)] = 0.050 wR(F 2) = 0.148 S = 1.08 2989 reflections 83 parameters H-atom parameters constrained Δρmax = 0.47 e Å−3 Δρmin = −0.38 e Å−3 Data collection: APEX2 (Bruker, 2011 ▶); cell refinement: APEX2 (Bruker, 2011 ▶) and SAINT (Bruker, 2011 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶) and TITAN2000 (Hunter & Simpson, 1999 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶) and TITAN2000; molecular graphics: SHELXTL (Sheldrick, 2008 ▶) and Mercury (Macrae et al., 2008 ▶); software used to prepare material for publication: SHELXL97, enCIFer (Allen et al., 2004 ▶), PLATON (Spek, 2009 ▶) and publCIF (Westrip 2010 ▶). Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812027699/bt5941sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812027699/bt5941Isup2.hkl Supplementary material file. DOI: 10.1107/S1600536812027699/bt5941Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C14H14O4F(000) = 520
Mr = 246.25Dx = 1.444 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 3955 reflections
a = 16.0726 (2) Åθ = 2.6–38.3°
b = 8.7982 (1) ŵ = 0.11 mm1
c = 8.0555 (1) ÅT = 92 K
β = 96.1134 (7)°Rectangular block, yellow
V = 1132.65 (2) Å30.53 × 0.50 × 0.22 mm
Z = 4
Bruker APEXII CCD area-detector diffractometer2989 independent reflections
Radiation source: fine-focus sealed tube2358 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.038
φ & ω scansθmax = 39.3°, θmin = 3.6°
Absorption correction: multi-scan (SADABS; Bruker, 2011)h = −27→26
Tmin = 0.570, Tmax = 0.748k = −14→7
9744 measured reflectionsl = −13→14
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.050Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.148H-atom parameters constrained
S = 1.08w = 1/[σ2(Fo2) + (0.0702P)2 + 0.4368P] where P = (Fo2 + 2Fc2)/3
2989 reflections(Δ/σ)max < 0.001
83 parametersΔρmax = 0.47 e Å3
0 restraintsΔρmin = −0.38 e Å3
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.
xyzUiso*/Ueq
O10.76307 (4)−0.03359 (9)0.53742 (9)0.02826 (17)
C10.70230 (5)−0.04789 (10)0.61199 (10)0.01983 (16)
O20.64973 (4)0.07377 (7)0.61147 (8)0.01902 (14)
C20.68037 (5)−0.18492 (10)0.70770 (10)0.02081 (16)
H2A0.6997−0.17000.82740.025*
H2B0.7099−0.27450.66820.025*
C30.58596 (5)−0.21578 (9)0.68795 (10)0.01919 (15)
H3A0.5684−0.25330.57370.023*
H3B0.5728−0.29520.76810.023*
C40.53894 (4)−0.07275 (8)0.71898 (9)0.01485 (14)
C50.57500 (4)0.06647 (8)0.68637 (9)0.01470 (14)
C60.53839 (4)0.20612 (8)0.71558 (9)0.01519 (14)
C610.57956 (5)0.35308 (10)0.67541 (12)0.02167 (17)
H61A0.60300.40220.77920.033*
H61B0.53800.42040.61560.033*
H61C0.62450.33250.60530.033*
U11U22U33U12U13U23
O10.0216 (3)0.0340 (4)0.0307 (3)0.0048 (2)0.0097 (2)0.0013 (3)
C10.0175 (3)0.0226 (4)0.0194 (3)0.0039 (2)0.0021 (2)−0.0023 (3)
O20.0158 (2)0.0186 (3)0.0232 (3)0.00139 (18)0.0047 (2)0.0013 (2)
C20.0214 (3)0.0204 (4)0.0207 (3)0.0070 (3)0.0026 (3)0.0000 (3)
C30.0220 (3)0.0143 (3)0.0212 (3)0.0028 (2)0.0018 (2)−0.0018 (2)
C40.0165 (3)0.0124 (3)0.0152 (3)0.0007 (2)−0.0003 (2)−0.0005 (2)
C50.0140 (3)0.0145 (3)0.0154 (3)0.0003 (2)0.0009 (2)0.0001 (2)
C60.0150 (3)0.0122 (3)0.0178 (3)−0.0004 (2)−0.0007 (2)0.0006 (2)
C610.0196 (3)0.0149 (3)0.0302 (4)−0.0028 (2)0.0012 (3)0.0024 (3)
O1—C11.2065 (10)C3—H3B0.9900
C1—O21.3634 (10)C4—C51.3920 (10)
C1—C21.4934 (13)C4—C4i1.3962 (14)
O2—C51.4018 (9)C5—C61.3931 (10)
C2—C31.5329 (11)C6—C6i1.4058 (14)
C2—H2A0.9900C6—C611.5033 (11)
C2—H2B0.9900C61—H61A0.9800
C3—C41.5025 (11)C61—H61B0.9800
C3—H3A0.9900C61—H61C0.9800
O1—C1—O2116.80 (8)C5—C4—C4i118.34 (4)
O1—C1—C2126.11 (8)C5—C4—C3118.59 (7)
O2—C1—C2117.07 (7)C4i—C4—C3123.06 (4)
C1—O2—C5121.45 (6)C4—C5—C6123.53 (7)
C1—C2—C3112.01 (7)C4—C5—O2120.97 (6)
C1—C2—H2A109.2C6—C5—O2115.40 (6)
C3—C2—H2A109.2C5—C6—C6i118.10 (4)
C1—C2—H2B109.2C5—C6—C61121.25 (7)
C3—C2—H2B109.2C6i—C6—C61120.66 (4)
H2A—C2—H2B107.9C6—C61—H61A109.5
C4—C3—C2110.14 (7)C6—C61—H61B109.5
C4—C3—H3A109.6H61A—C61—H61B109.5
C2—C3—H3A109.6C6—C61—H61C109.5
C4—C3—H3B109.6H61A—C61—H61C109.5
C2—C3—H3B109.6H61B—C61—H61C109.5
H3A—C3—H3B108.1
O1—C1—O2—C5176.44 (7)C4i—C4—C5—O2−174.81 (8)
C2—C1—O2—C5−4.87 (11)C3—C4—C5—O25.95 (11)
O1—C1—C2—C3−142.07 (9)C1—O2—C5—C4−19.48 (11)
O2—C1—C2—C339.38 (10)C1—O2—C5—C6164.02 (7)
C1—C2—C3—C4−49.20 (9)C4—C5—C6—C6i1.15 (14)
C2—C3—C4—C527.91 (10)O2—C5—C6—C6i177.55 (8)
C2—C3—C4—C4i−151.29 (9)C4—C5—C6—C61−179.02 (7)
C4i—C4—C5—C61.40 (14)O2—C5—C6—C61−2.62 (11)
C3—C4—C5—C6−177.84 (7)
D—H···AD—HH···AD···AD—H···A
C61—H61A···O1ii0.982.543.3907 (11)145
C2—H2A···O1iii0.992.603.4301 (12)142
C2—H2A···O2iii0.992.643.4813 (10)143
C2—H2B···O1iv0.992.443.3528 (11)154
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯A D—HH⋯A DA D—H⋯A
C61—H61A⋯O1i 0.982.543.3907 (11)145
C2—H2A⋯O1ii 0.992.603.4301 (12)142
C2—H2A⋯O2ii 0.992.643.4813 (10)143
C2—H2B⋯O1iii 0.992.443.3528 (11)154

Symmetry codes: (i) ; (ii) ; (iii) .

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Authors:  Mercedes Lecea; Gloria Hernández-Torres; Antonio Urbano; M Carmen Carreño; Françoise Colobert
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