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ISSN: 2056-9890

Whole-mol­ecule disordered (E)-2-(1-hy­dr­oxy-3-phenylprop-2-en-1-yl­­idene)-4,5-dimeth­oxycyclo­pent-4-ene-1,3-dione isolated from Lindera oxyphylla (Lauraceae)

aDepartment of Chemistry, University of Malaya, 50603 Kuala Lumpur, Malaysia, and bInstitute of Biological Sciences, University of Malaya, 50603 Kuala Lumpur, Malaysia
*Correspondence e-mail: seikweng@um.edu.my

(Received 21 May 2011; accepted 23 May 2011; online 28 May 2011)

In the mol­ecule of the title compound, C16H14O5, all non-H atoms are approximately co-planar [maximum atomic deviation = 0.064 (5) Å]. The hy­droxy group is a hydrogen-bond donor to a carbonyl O atom. Weak intermolecular C—H⋯O hydrogen bonding is present in the crystal structure. The crystal structure is 'whole-mol­ecule disordered' about an axis that runs approximately along the length of the mol­ecule; the occupancy of the two disorder components was set as exactly 0.5. An intra­molecular O—-H⋯O hydrogen bond exists in each component.

Related literature

For the spectroscopic characterization of linderone and methyl linderone isolated from Lindera pipericarpa, see: Kiang et al. (1962[Kiang, A. K., Lee, H. H. & Sim, K. Y. (1962). J. Chem. Soc. pp. 4338-4345.]). For the crystal structure of methyl linderone isolated from Lindera poliantha, see: Syah et al. (2005[Syah, Y. M., Suastri, N. S., Latip, J. & Yamin, B. M. (2005). Acta Cryst. E61, o1530-o1531.]).

[Scheme 1]

Experimental

Crystal data
  • C16H14O5

  • Mr = 286.27

  • Monoclinic, P 21 /n

  • a = 7.3195 (5) Å

  • b = 9.8635 (7) Å

  • c = 18.6724 (11) Å

  • β = 96.586 (6)°

  • V = 1339.17 (15) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.11 mm−1

  • T = 100 K

  • 0.20 × 0.20 × 0.10 mm

Data collection
  • Agilent SuperNova Dual diffractometer with an Atlas detector

  • Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010[Agilent (2010). CrysAlis PRO. Agilent Technologies, Yarnton, England.]) Tmin = 0.979, Tmax = 0.990

  • 8436 measured reflections

  • 2369 independent reflections

  • 1965 reflections with I > 2σ(I)

  • Rint = 0.032

Refinement
  • R[F2 > 2σ(F2)] = 0.068

  • wR(F2) = 0.190

  • S = 1.05

  • 2369 reflections

  • 308 parameters

  • 30 restraints

  • H-atom parameters constrained

  • Δρmax = 0.56 e Å−3

  • Δρmin = −0.34 e Å−3

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
O1—H1⋯O2 0.84 1.93 2.600 (5) 136
O1′—H1′⋯O2′ 0.84 1.97 2.623 (4) 134
C2—H2⋯O2i 0.95 2.26 3.091 (8) 145
C16′—H16D⋯O1′ii 0.98 2.05 2.885 (11) 142
Symmetry codes: (i) x, y+1, z; (ii) x, y-1, z.

Data collection: CrysAlis PRO (Agilent, 2010[Agilent (2010). CrysAlis PRO. Agilent Technologies, Yarnton, England.]); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); molecular graphics: X-SEED (Barbour, 2001[Barbour, L. J. (2001). J. Supramol. Chem. 1, 189-191.]); software used to prepare material for publication: publCIF (Westrip, 2010[Westrip, S. P. (2010). J. Appl. Cryst. 43, 920-925.]).

Supporting information


Comment top

Linderone (Scheme I) was isolated from Lindera pipericarpa and its formulation was established by solution 1H-NMR spectrocopy (Kiang et al., 1962) nearly 50 years ago. This plant genus also yields methyl linderone, which differs from linderone in having a methyl group in place of the hydroxy H atom. Methyl linderone, isolated from Lindera poliantha, exists as a planar molecule (Syah et al., 2005). Linderone is similarly a planar molecule; however, the molecule is 'whole-molecule' disordered (Fig. 1) about an axis that runs approximately along the length of the flat molecule. The three-atom chain connecting the five-membered and six-membered rings exists in an E-configuration; the hydroxy group is hydrogen-bond donor to the carbonyl O atom.

Related literature top

For the spectroscopic characterization of linderone and methyl linderone isolated from Lindera pipericarpa, see: Kiang et al. (1962). For the crystal structure of methyl linderone isolated from Lindera poliantha, see: Syah et al. (2005).

Experimental top

Lindera oxyphylla (Lauraceae) was collected from Ulu Muda, Baling, Kedah, Malaysia. Some 4 kg of dried and ground bark of Lindera oxyphylla were extracted with hexane (10 L) for 3 days. The hexane extract was concentrated under reduced pressure to give a crude material (13 g). This was subjected to column chromatography on silica gel-60 (2 x 75 cm, 70–230 mesh ASTM) by using a step gradient of hexane and dichloromethane. The separation afforded 30 fractions; fractions 22–30 were purified by using dichloromethane–methanol (98:2) to yield (E)- 2-(1-hydroxy-3-phenyl-2-propen-1-ylidene)-4,5-dimethoxy-4-cyclopentene-1,3-dione. Its formulation was established by solution NMR spectroscopic analysis. Deep yellow prisms were obtained upon recrystallization from dichloromethane.

Refinement top

Carbon- and oxygen-bound H-atoms were placed in calculated positions [C—H 0.95 to 0.98. O–H 0.84 Å, Uiso(H) 1.2 to 1.5Ueq(C,O)], and were included in the refinement in the riding model approximation. An sp2-type of hybridization was assumed for the hydroxy H atom.

The crystal structure is a 'whole-molecule disordered' crystal structure. As the occupancy refined to near 1:1, the occupancy of the two disorder components was set as exactly 0.5.

The phenyl ring was refined as a rigid hexagon of 1.39 Å sides and the five-membered ring a rigid pentagon of 1.42 Å sides. The temperature factors of the atoms constituting the five-membered ring were set to those of the umprimed ones, and the anisotropic temperature factors were restrained to be nearly isotropic.

The extinction was refined; although the value is small, its refinement improved the refinement somewhat.

The crystal used for the measurements was a twinned crystal of low mosaicity; fortunately, the presence of the minor twin component did not affect the diffraction intensities of the major component only the diffraction intensities of the major component were integrated. On the other hand, the simultaneous integration of both components lead to a less satisfactory refinement. Other crystals were also measured but these demonstrated varying mosaicities and degrees of twinning (from 0 to 50%), and neither were the refinements improved by the use of copper radiation in place of molybdenum radiation.

Computing details top

Data collection: CrysAlis PRO (Agilent, 2010); cell refinement: CrysAlis PRO (Agilent, 2010); data reduction: CrysAlis PRO (Agilent, 2010); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: X-SEED (Barbour, 2001); software used to prepare material for publication: publCIF (Westrip, 2010).

Figures top
[Figure 1] Fig. 1. Thermal ellipsoid plot (Barbour, 2001) of one of the whole-molcule disordered components of C16H14O5 at the 70% probability level; hydrogen atoms are drawn as spheres of arbitrary radius.
(E)-2-(1-hydroxy-3-phenylprop-2-en-1-ylidene)-4,5-dimethoxycyclopent- 4-ene-1,3-dione top
Crystal data top
C16H14O5F(000) = 600
Mr = 286.27Dx = 1.420 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 4706 reflections
a = 7.3195 (5) Åθ = 2.2–25.0°
b = 9.8635 (7) ŵ = 0.11 mm1
c = 18.6724 (11) ÅT = 100 K
β = 96.586 (6)°Prism, yellow
V = 1339.17 (15) Å30.20 × 0.20 × 0.10 mm
Z = 4
Data collection top
Agilent SuperNova Dual
diffractometer with an Atlas detector
2369 independent reflections
Radiation source: SuperNova (Mo) X-ray Source1965 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.032
Detector resolution: 10.4041 pixels mm-1θmax = 25.1°, θmin = 2.2°
ω scansh = 88
Absorption correction: multi-scan
(CrysAlis PRO; Agilent, 2010)
k = 1110
Tmin = 0.979, Tmax = 0.990l = 2222
8436 measured reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.068H-atom parameters constrained
wR(F2) = 0.190 w = 1/[σ2(Fo2) + (0.0883P)2 + 1.2962P]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max = 0.001
2369 reflectionsΔρmax = 0.56 e Å3
308 parametersΔρmin = 0.34 e Å3
30 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0014 (11)
Crystal data top
C16H14O5V = 1339.17 (15) Å3
Mr = 286.27Z = 4
Monoclinic, P21/nMo Kα radiation
a = 7.3195 (5) ŵ = 0.11 mm1
b = 9.8635 (7) ÅT = 100 K
c = 18.6724 (11) Å0.20 × 0.20 × 0.10 mm
β = 96.586 (6)°
Data collection top
Agilent SuperNova Dual
diffractometer with an Atlas detector
2369 independent reflections
Absorption correction: multi-scan
(CrysAlis PRO; Agilent, 2010)
1965 reflections with I > 2σ(I)
Tmin = 0.979, Tmax = 0.990Rint = 0.032
8436 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.06830 restraints
wR(F2) = 0.190H-atom parameters constrained
S = 1.05Δρmax = 0.56 e Å3
2369 reflectionsΔρmin = 0.34 e Å3
308 parameters
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
O10.1902 (5)0.2729 (4)0.58692 (19)0.0387 (8)0.50
H10.19940.18940.57930.058*0.50
O20.2649 (5)0.0774 (4)0.50156 (19)0.0417 (9)0.50
O30.3802 (5)0.0354 (4)0.3530 (2)0.0405 (9)0.50
O40.4003 (4)0.3167 (3)0.29148 (16)0.0326 (8)0.50
O50.3180 (4)0.5067 (4)0.39499 (17)0.0341 (8)0.50
C10.1608 (5)0.7931 (7)0.6029 (2)0.0322 (14)0.50
H1a0.19430.78280.55550.039*0.50
C20.1349 (12)0.9219 (5)0.6302 (4)0.038 (2)0.50
H20.15070.99960.60150.046*0.50
C30.0859 (18)0.9370 (5)0.6995 (5)0.031 (3)0.50
H30.06821.02500.71820.037*0.50
C40.0629 (17)0.8233 (7)0.7415 (3)0.033 (3)0.50
H40.02940.83360.78890.040*0.50
C50.0888 (9)0.6945 (6)0.7142 (3)0.0282 (16)0.50
H50.07300.61680.74290.034*0.50
C60.1377 (5)0.6794 (5)0.6449 (3)0.0245 (16)0.50
C70.1602 (6)0.5419 (5)0.6182 (2)0.0302 (10)0.50
H70.13800.47050.65030.036*0.50
C80.2094 (11)0.5036 (8)0.5527 (4)0.0241 (15)0.50
H80.23310.57010.51820.029*0.50
C90.2249 (6)0.3619 (5)0.5364 (2)0.0284 (10)0.50
C100.2768 (5)0.3111 (4)0.47099 (16)0.0217 (10)0.50
C110.2933 (6)0.1698 (3)0.45873 (17)0.0324 (11)0.50
C120.3440 (6)0.1517 (3)0.38819 (19)0.0183 (11)0.50
C130.3588 (5)0.2819 (4)0.35685 (14)0.0219 (9)0.50
C140.3172 (5)0.3804 (2)0.4080 (2)0.0254 (8)0.50
C150.3509 (17)0.0907 (11)0.3878 (5)0.051 (2)0.50
H15A0.38230.16580.35710.077*0.50
H15B0.22150.09800.39620.077*0.50
H15C0.42890.09470.43410.077*0.50
C160.4447 (17)0.2108 (10)0.2420 (6)0.032 (2)0.50
H16A0.47250.25200.19680.049*0.50
H16B0.33960.14940.23230.049*0.50
H16C0.55190.15970.26370.049*0.50
O1'0.3120 (4)0.6031 (3)0.42276 (16)0.0284 (7)0.50
H1'0.34340.58480.38200.043*0.50
O2'0.3866 (4)0.4149 (3)0.33121 (15)0.0286 (7)0.50
O3'0.3939 (4)0.1087 (4)0.31727 (17)0.0303 (7)0.50
O4'0.2841 (5)0.0061 (3)0.46004 (18)0.0356 (8)0.50
O5'0.2174 (5)0.2272 (3)0.54512 (19)0.0349 (8)0.50
C1'0.1246 (5)0.6426 (4)0.6802 (3)0.0236 (11)0.50
H1'a0.13500.54710.67540.028*0.50
C2'0.0771 (10)0.6978 (7)0.7440 (3)0.0290 (16)0.50
H2'0.05500.64010.78280.035*0.50
C3'0.0618 (17)0.8376 (7)0.7510 (4)0.031 (2)0.50
H3'0.02930.87530.79460.037*0.50
C4'0.0942 (18)0.9221 (4)0.6942 (5)0.036 (3)0.50
H4'0.08381.01750.69900.043*0.50
C5'0.1418 (11)0.8668 (5)0.6304 (3)0.0274 (16)0.50
H5'0.16390.92460.59160.033*0.50
C6'0.1570 (5)0.7271 (5)0.6234 (2)0.0202 (15)0.50
C7'0.2082 (5)0.6752 (4)0.5545 (2)0.0220 (9)0.50
H7'0.23060.74100.51930.026*0.50
C8'0.2262 (12)0.5464 (7)0.5363 (5)0.0237 (15)0.50
H8'0.20280.47890.57040.028*0.50
C9'0.2790 (5)0.5022 (4)0.4682 (2)0.0219 (9)0.50
C10'0.2968 (5)0.3663 (3)0.4479 (2)0.0217 (10)0.50
C11'0.3503 (5)0.3338 (3)0.37918 (18)0.0324 (11)0.50
C12'0.3537 (6)0.1904 (3)0.37286 (15)0.0183 (11)0.50
C13'0.3024 (6)0.1342 (2)0.43766 (18)0.0219 (9)0.50
C14'0.2673 (5)0.2429 (4)0.48403 (13)0.0254 (8)0.50
C15'0.4107 (15)0.1709 (10)0.2489 (7)0.034 (2)0.50
H15D0.44070.10170.21450.051*0.50
H15E0.50880.23910.25460.051*0.50
H15F0.29420.21460.23090.051*0.50
C16'0.3136 (18)0.1051 (11)0.4120 (5)0.054 (3)0.50
H16D0.29540.19140.43620.081*0.50
H16E0.43940.10090.39890.081*0.50
H16F0.22600.09830.36830.081*0.50
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.053 (2)0.035 (2)0.0288 (19)0.0007 (16)0.0099 (16)0.0090 (16)
O20.061 (2)0.034 (2)0.0326 (18)0.0009 (17)0.0146 (16)0.0108 (17)
O30.056 (2)0.0259 (19)0.042 (2)0.0032 (16)0.0153 (17)0.0052 (17)
O40.0370 (18)0.0352 (19)0.0273 (16)0.0001 (14)0.0109 (13)0.0018 (15)
O50.0366 (18)0.037 (2)0.0295 (17)0.0010 (15)0.0076 (14)0.0037 (16)
C10.025 (3)0.051 (5)0.021 (3)0.001 (3)0.005 (2)0.001 (3)
C20.031 (3)0.041 (5)0.043 (4)0.003 (4)0.006 (3)0.006 (4)
C30.030 (5)0.037 (4)0.026 (5)0.002 (4)0.006 (4)0.009 (4)
C40.021 (5)0.049 (7)0.029 (3)0.005 (4)0.004 (3)0.010 (4)
C50.028 (3)0.032 (3)0.025 (4)0.000 (2)0.006 (3)0.008 (4)
C60.020 (2)0.028 (4)0.027 (4)0.004 (2)0.007 (2)0.002 (3)
C70.026 (2)0.038 (3)0.026 (2)0.0021 (19)0.0014 (17)0.000 (2)
C80.023 (3)0.032 (4)0.018 (3)0.001 (3)0.004 (2)0.001 (3)
C90.025 (2)0.039 (3)0.022 (2)0.0005 (19)0.0043 (17)0.0036 (19)
C100.0244 (15)0.022 (2)0.019 (2)0.0003 (17)0.0042 (14)0.0059 (18)
C110.034 (2)0.033 (2)0.030 (2)0.0013 (18)0.0023 (17)0.0119 (19)
C120.0202 (12)0.015 (2)0.0199 (18)0.0023 (15)0.0056 (12)0.0068 (19)
C130.0227 (16)0.0248 (19)0.0181 (17)0.0019 (14)0.0022 (14)0.0051 (16)
C140.0220 (16)0.0245 (19)0.029 (2)0.0042 (14)0.0012 (14)0.0090 (17)
C150.077 (5)0.023 (4)0.057 (7)0.008 (3)0.024 (5)0.006 (4)
C160.049 (5)0.034 (5)0.017 (3)0.011 (3)0.011 (3)0.012 (3)
O1'0.0424 (18)0.0215 (17)0.0233 (15)0.0008 (13)0.0116 (13)0.0016 (13)
O2'0.0358 (17)0.0301 (18)0.0210 (15)0.0019 (13)0.0086 (12)0.0009 (13)
O3'0.0394 (18)0.0311 (18)0.0220 (16)0.0042 (14)0.0098 (13)0.0035 (15)
O4'0.055 (2)0.0233 (17)0.0293 (17)0.0025 (15)0.0097 (15)0.0069 (15)
O5'0.058 (2)0.0294 (19)0.0205 (17)0.0003 (15)0.0178 (16)0.0020 (15)
C1'0.029 (2)0.021 (3)0.023 (3)0.003 (2)0.011 (2)0.003 (3)
C2'0.030 (3)0.035 (4)0.024 (4)0.001 (2)0.009 (3)0.009 (3)
C3'0.028 (5)0.028 (5)0.036 (4)0.002 (3)0.002 (3)0.012 (4)
C4'0.026 (5)0.026 (4)0.055 (8)0.001 (3)0.002 (5)0.013 (4)
C5'0.028 (3)0.029 (5)0.025 (3)0.000 (3)0.005 (2)0.004 (3)
C6'0.020 (2)0.023 (4)0.018 (3)0.002 (2)0.003 (2)0.006 (3)
C7'0.020 (2)0.025 (2)0.021 (2)0.0014 (16)0.0053 (16)0.0032 (17)
C8'0.027 (3)0.018 (4)0.026 (4)0.001 (3)0.003 (2)0.007 (2)
C9'0.0173 (19)0.025 (2)0.023 (2)0.0011 (16)0.0002 (16)0.0006 (17)
C10'0.0244 (15)0.022 (2)0.019 (2)0.0003 (17)0.0042 (14)0.0059 (18)
C11'0.034 (2)0.033 (2)0.030 (2)0.0013 (18)0.0023 (17)0.0119 (19)
C12'0.0202 (12)0.015 (2)0.0199 (18)0.0023 (15)0.0056 (12)0.0068 (19)
C13'0.0227 (16)0.0248 (19)0.0181 (17)0.0019 (14)0.0022 (14)0.0051 (16)
C14'0.0220 (16)0.0245 (19)0.029 (2)0.0042 (14)0.0012 (14)0.0090 (17)
C15'0.025 (4)0.042 (6)0.035 (4)0.000 (4)0.011 (3)0.010 (4)
C16'0.101 (8)0.021 (4)0.041 (6)0.001 (4)0.017 (4)0.011 (4)
Geometric parameters (Å, º) top
O1—C91.334 (6)O1'—C9'1.347 (5)
O1—H10.8400O1'—H1'0.8400
O2—C111.246 (4)O2'—C11'1.252 (4)
O3—C121.364 (4)O3'—C12'1.373 (4)
O3—C151.431 (10)O3'—C15'1.434 (11)
O4—C131.336 (4)O4'—C13'1.342 (4)
O4—C161.455 (11)O4'—C16'1.449 (10)
O5—C141.269 (4)O5'—C14'1.247 (4)
C1—C21.3900C1'—C2'1.3900
C1—C61.3900C1'—C6'1.3900
C1—H1A0.9500C1'—H1'A0.9500
C2—C31.3900C2'—C3'1.3900
C2—H20.9500C2'—H2'0.9500
C3—C41.3900C3'—C4'1.3900
C3—H30.9500C3'—H3'0.9500
C4—C51.3900C4'—C5'1.3900
C4—H40.9500C4'—H4'0.9500
C5—C61.3900C5'—C6'1.3900
C5—H50.9500C5'—H5'0.9500
C6—C71.460 (6)C6'—C7'1.473 (5)
C7—C81.367 (10)C7'—C8'1.326 (10)
C7—H70.9500C7'—H7'0.9500
C8—C91.437 (10)C8'—C9'1.438 (10)
C8—H80.9500C8'—H8'0.9500
C9—C101.412 (5)C9'—C10'1.404 (5)
C10—C111.4200C10'—C11'1.4200
C10—C141.4200C10'—C14'1.4200
C11—C121.4200C11'—C12'1.4200
C12—C131.4200C12'—C13'1.4200
C13—C141.4200C13'—C14'1.4200
C15—H15A0.9800C15'—H15D0.9800
C15—H15B0.9800C15'—H15E0.9800
C15—H15C0.9800C15'—H15F0.9800
C16—H16A0.9800C16'—H16D0.9800
C16—H16B0.9800C16'—H16E0.9800
C16—H16C0.9800C16'—H16F0.9800
C9—O1—H1120.0C9'—O1'—H1'120.0
C12—O3—C15117.7 (5)C12'—O3'—C15'118.0 (5)
C13—O4—C16119.1 (5)C13'—O4'—C16'119.5 (5)
C2—C1—C6120.0C2'—C1'—C6'120.0
C2—C1—H1A120.0C2'—C1'—H1'A120.0
C6—C1—H1A120.0C6'—C1'—H1'A120.0
C1—C2—C3120.0C3'—C2'—C1'120.0
C1—C2—H2120.0C3'—C2'—H2'120.0
C3—C2—H2120.0C1'—C2'—H2'120.0
C4—C3—C2120.0C2'—C3'—C4'120.0
C4—C3—H3120.0C2'—C3'—H3'120.0
C2—C3—H3120.0C4'—C3'—H3'120.0
C5—C4—C3120.0C5'—C4'—C3'120.0
C5—C4—H4120.0C5'—C4'—H4'120.0
C3—C4—H4120.0C3'—C4'—H4'120.0
C4—C5—C6120.0C4'—C5'—C6'120.0
C4—C5—H5120.0C4'—C5'—H5'120.0
C6—C5—H5120.0C6'—C5'—H5'120.0
C5—C6—C1120.0C5'—C6'—C1'120.0
C5—C6—C7117.9 (5)C5'—C6'—C7'117.3 (4)
C1—C6—C7122.1 (5)C1'—C6'—C7'122.7 (4)
C8—C7—C6127.8 (5)C8'—C7'—C6'126.8 (5)
C8—C7—H7116.1C8'—C7'—H7'116.6
C6—C7—H7116.1C6'—C7'—H7'116.6
C7—C8—C9119.6 (6)C7'—C8'—C9'124.1 (5)
C7—C8—H8120.2C7'—C8'—H8'117.9
C9—C8—H8120.2C9'—C8'—H8'117.9
O1—C9—C10118.1 (4)O1'—C9'—C10'120.4 (4)
O1—C9—C8117.6 (5)O1'—C9'—C8'114.8 (4)
C10—C9—C8124.3 (5)C10'—C9'—C8'124.8 (4)
C9—C10—C11121.6 (4)C9'—C10'—C11'120.2 (3)
C9—C10—C14130.4 (4)C9'—C10'—C14'131.8 (3)
C11—C10—C14108.0C11'—C10'—C14'108.0
O2—C11—C12125.7 (4)O2'—C11'—C12'124.7 (3)
O2—C11—C10126.2 (4)O2'—C11'—C10'127.3 (3)
C12—C11—C10108.0C12'—C11'—C10'108.0
O3—C12—C13122.3 (3)O3'—C12'—C11'131.0 (3)
O3—C12—C11129.7 (3)O3'—C12'—C13'121.0 (3)
C13—C12—C11108.0C11'—C12'—C13'108.0
O4—C13—C12130.1 (3)O4'—C13'—C14'119.3 (3)
O4—C13—C14121.9 (3)O4'—C13'—C12'132.7 (3)
C12—C13—C14108.0C14'—C13'—C12'108.0
O5—C14—C13122.4 (4)O5'—C14'—C13'123.8 (3)
O5—C14—C10129.6 (4)O5'—C14'—C10'128.2 (3)
C13—C14—C10108.0C13'—C14'—C10'108.0
O3—C15—H15A109.5O3'—C15'—H15D109.5
O3—C15—H15B109.5O3'—C15'—H15E109.5
H15A—C15—H15B109.5H15D—C15'—H15E109.5
O3—C15—H15C109.5O3'—C15'—H15F109.5
H15A—C15—H15C109.5H15D—C15'—H15F109.5
H15B—C15—H15C109.5H15E—C15'—H15F109.5
O4—C16—H16A109.5O4'—C16'—H16D109.5
O4—C16—H16B109.5O4'—C16'—H16E109.5
H16A—C16—H16B109.5H16D—C16'—H16E109.5
O4—C16—H16C109.5O4'—C16'—H16F109.5
H16A—C16—H16C109.5H16D—C16'—H16F109.5
H16B—C16—H16C109.5H16E—C16'—H16F109.5
C6—C1—C2—C30.0C6'—C1'—C2'—C3'0.0
C1—C2—C3—C40.0C1'—C2'—C3'—C4'0.0
C2—C3—C4—C50.0C2'—C3'—C4'—C5'0.0
C3—C4—C5—C60.0C3'—C4'—C5'—C6'0.0
C4—C5—C6—C10.0C4'—C5'—C6'—C1'0.0
C4—C5—C6—C7179.0 (5)C4'—C5'—C6'—C7'179.9 (5)
C2—C1—C6—C50.0C2'—C1'—C6'—C5'0.0
C2—C1—C6—C7178.9 (5)C2'—C1'—C6'—C7'179.9 (5)
C5—C6—C7—C8179.2 (6)C5'—C6'—C7'—C8'178.5 (6)
C1—C6—C7—C81.9 (7)C1'—C6'—C7'—C8'1.6 (7)
C6—C7—C8—C9179.8 (5)C6'—C7'—C8'—C9'179.2 (5)
C7—C8—C9—O10.1 (9)C7'—C8'—C9'—O1'0.7 (9)
C7—C8—C9—C10179.2 (5)C7'—C8'—C9'—C10'179.3 (6)
O1—C9—C10—C110.4 (5)O1'—C9'—C10'—C11'0.1 (5)
C8—C9—C10—C11178.7 (5)C8'—C9'—C10'—C11'179.9 (5)
O1—C9—C10—C14178.4 (3)O1'—C9'—C10'—C14'178.5 (3)
C8—C9—C10—C142.5 (7)C8'—C9'—C10'—C14'1.5 (7)
C9—C10—C11—O20.4 (5)C9'—C10'—C11'—O2'0.2 (5)
C14—C10—C11—O2178.6 (5)C14'—C10'—C11'—O2'179.2 (4)
C9—C10—C11—C12179.0 (4)C9'—C10'—C11'—C12'178.9 (4)
C14—C10—C11—C120.0C14'—C10'—C11'—C12'0.0
C15—O3—C12—C13176.5 (6)C15'—O3'—C12'—C11'10.5 (7)
C15—O3—C12—C115.5 (8)C15'—O3'—C12'—C13'168.5 (5)
O2—C11—C12—O33.2 (5)O2'—C11'—C12'—O3'0.1 (5)
C10—C11—C12—O3178.2 (5)C10'—C11'—C12'—O3'179.1 (5)
O2—C11—C12—C13178.7 (5)O2'—C11'—C12'—C13'179.2 (4)
C10—C11—C12—C130.0C10'—C11'—C12'—C13'0.0
C16—O4—C13—C122.2 (7)C16'—O4'—C13'—C14'177.9 (7)
C16—O4—C13—C14178.9 (6)C16'—O4'—C13'—C12'2.3 (8)
O3—C12—C13—O42.6 (5)O3'—C12'—C13'—O4'1.0 (5)
C11—C12—C13—O4179.0 (4)C11'—C12'—C13'—O4'179.8 (5)
O3—C12—C13—C14178.4 (4)O3'—C12'—C13'—C14'179.2 (4)
C11—C12—C13—C140.0C11'—C12'—C13'—C14'0.0
O4—C13—C14—O50.4 (4)O4'—C13'—C14'—O5'0.9 (5)
C12—C13—C14—O5179.5 (4)C12'—C13'—C14'—O5'179.3 (4)
O4—C13—C14—C10179.1 (4)O4'—C13'—C14'—C10'179.8 (4)
C12—C13—C14—C100.0C12'—C13'—C14'—C10'0.0
C9—C10—C14—O50.5 (5)C9'—C10'—C14'—O5'0.5 (6)
C11—C10—C14—O5179.5 (4)C11'—C10'—C14'—O5'179.3 (4)
C9—C10—C14—C13178.9 (4)C9'—C10'—C14'—C13'178.8 (4)
C11—C10—C14—C130.0C11'—C10'—C14'—C13'0.0
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1···O20.841.932.600 (5)136
O1—H1···O20.841.972.623 (4)134
C2—H2···O2i0.952.263.091 (8)145
C16—H16D···O1ii0.982.052.885 (11)142
Symmetry codes: (i) x, y+1, z; (ii) x, y1, z.

Experimental details

Crystal data
Chemical formulaC16H14O5
Mr286.27
Crystal system, space groupMonoclinic, P21/n
Temperature (K)100
a, b, c (Å)7.3195 (5), 9.8635 (7), 18.6724 (11)
β (°) 96.586 (6)
V3)1339.17 (15)
Z4
Radiation typeMo Kα
µ (mm1)0.11
Crystal size (mm)0.20 × 0.20 × 0.10
Data collection
DiffractometerAgilent SuperNova Dual
diffractometer with an Atlas detector
Absorption correctionMulti-scan
(CrysAlis PRO; Agilent, 2010)
Tmin, Tmax0.979, 0.990
No. of measured, independent and
observed [I > 2σ(I)] reflections
8436, 2369, 1965
Rint0.032
(sin θ/λ)max1)0.596
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.068, 0.190, 1.05
No. of reflections2369
No. of parameters308
No. of restraints30
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.56, 0.34

Computer programs: CrysAlis PRO (Agilent, 2010), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), X-SEED (Barbour, 2001), publCIF (Westrip, 2010).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1···O20.841.932.600 (5)136
O1'—H1'···O2'0.841.972.623 (4)134
C2—H2···O2i0.952.263.091 (8)145
C16'—H16D···O1'ii0.982.052.885 (11)142
Symmetry codes: (i) x, y+1, z; (ii) x, y1, z.
 

Acknowledgements

This work was carried under the aegis of a University of Malaya–CNRS (France) collaborative framework. We thank the University of Malaya (grant No. RG045/11BIO) for financial support.

References

First citationAgilent (2010). CrysAlis PRO. Agilent Technologies, Yarnton, England.  Google Scholar
First citationBarbour, L. J. (2001). J. Supramol. Chem. 1, 189–191.  CrossRef CAS Google Scholar
First citationKiang, A. K., Lee, H. H. & Sim, K. Y. (1962). J. Chem. Soc. pp. 4338–4345.  CrossRef Google Scholar
First citationSheldrick, G. M. (2008). Acta Cryst. A64, 112–122.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationSyah, Y. M., Suastri, N. S., Latip, J. & Yamin, B. M. (2005). Acta Cryst. E61, o1530–o1531.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationWestrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.  Web of Science CrossRef CAS IUCr Journals Google Scholar

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