Download citation
Download citation
link to html
In the solid state, the non-centrosymmetric structure of the title compound, C10H8O, is stabilized both by van der Waals interactions and by O—H...O intermolecular hydrogen bonds. These hydrogen bonds link every mol­ecule with two neighbouring non-equivalent mol­ecules, forming chains. The asymmetric unit contains two mol­ecules, which are related to each other by a pseudo-inversion centre.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536802022808/cf6223sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536802022808/cf6223Isup2.hkl
Contains datablock I

CCDC reference: 203002

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.006 Å
  • R factor = 0.045
  • wR factor = 0.093
  • Data-to-parameter ratio = 8.5

checkCIF results

No syntax errors found


Amber Alert Alert Level B:
PLAT_111 Alert B ADDSYM Detects (Pseudo) Centre of Symmetry ... 100 Perc Fit General Notes
REFLT_03 From the CIF: _diffrn_reflns_theta_max 27.45 From the CIF: _reflns_number_total 1744 Count of symmetry unique reflns 1744 Completeness (_total/calc) 100.00% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 0 Fraction of Friedel pairs measured 0.000 Are heavy atom types Z>Si present no Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF.
0 Alert Level A = Potentially serious problem
1 Alert Level B = Potential problem
0 Alert Level C = Please check

Computing details top

Data collection: DARCH package (Burevestnik, 1991); cell refinement: DARCH package; data reduction: DARCH package; program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 (Farrugia, 1997) and PLATON (Spek, 2003); software used to prepare material for publication: SHELXL97.

(I) top
Crystal data top
C10H8ODx = 1.263 Mg m3
Mr = 144.16Melting point: 123 K
Monoclinic, CcMo Kα radiation, λ = 0.71069 Å
a = 32.074 (6) ÅCell parameters from 30 reflections
b = 5.931 (1) Åθ = 1.2–28.0°
c = 8.127 (2) ŵ = 0.08 mm1
β = 101.18 (3)°T = 293 K
V = 1516.7 (5) Å3Needle, pale yellow
Z = 80.4 × 0.06 × 0.03 mm
F(000) = 608
Data collection top
DARCH-1
diffractometer
1339 reflections with I > 2σ(I)
Radiation source: BSW x-ray tubeRint = 0.020
Graphite monochromatorθmax = 27.5°, θmin = 1.3°
ω–2θ scansh = 4140
Absorption correction: part of the refinement model (ΔF)
(DIFABS; Walker & Stuart, 1983)
k = 77
Tmin = 0.958, Tmax = 0.998l = 010
1875 measured reflections3 standard reflections every 120 min
1744 independent reflections intensity decay: 5%
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.045Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.093H-atom parameters constrained
S = 1.30 w = 1/[σ2(Fo2) + (0.0121P)2]
where P = (Fo2 + 2Fc2)/3
1744 reflections(Δ/σ)max = 0.007
204 parametersΔρmax = 0.09 e Å3
2 restraintsΔρmin = 0.14 e Å3
Special details top

Experimental. The DIFABS only insignificantly reduced the R value, but it enabled us much better refinement of the structure parameters.

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
xyzUiso*/Ueq
O10.26010 (9)0.8581 (4)0.2004 (4)0.0870 (7)
H10.25860.99540.20960.130*
C10.30146 (14)0.7886 (7)0.2607 (6)0.0869 (12)
C20.32747 (14)0.9230 (8)0.3703 (6)0.0888 (12)
H20.31751.06110.40050.107*
C30.36958 (15)0.8568 (7)0.4395 (6)0.0888 (12)
C40.39776 (12)0.9928 (7)0.5500 (6)0.0856 (11)
H40.38901.13390.57990.103*
C50.43793 (15)0.9203 (7)0.6142 (6)0.0896 (11)
H50.45541.00690.69480.108*
C60.45332 (14)0.7177 (6)0.5610 (5)0.0798 (10)
H60.48160.67560.59660.096*
C70.42577 (15)0.5842 (8)0.4556 (6)0.0958 (13)
H70.43540.44400.42760.115*
C80.38384 (14)0.6449 (7)0.3867 (5)0.0857 (11)
C90.35595 (17)0.5133 (9)0.2751 (7)0.1030 (14)
H90.36510.37450.24230.124*
C100.31602 (16)0.5807 (8)0.2130 (6)0.0987 (14)
H100.29800.48890.13810.118*
O20.22878 (9)0.2095 (4)0.3642 (4)0.0905 (8)
H2A0.23860.31560.42400.136*
C110.18700 (12)0.2519 (6)0.2957 (5)0.0748 (10)
C120.16206 (13)0.1045 (6)0.1936 (5)0.0825 (10)
H120.17370.03160.16760.099*
C130.11971 (13)0.1504 (6)0.1265 (5)0.0785 (10)
C140.09277 (14)0.0033 (7)0.0178 (6)0.0918 (12)
H140.10350.13330.01190.110*
C150.05175 (15)0.0564 (7)0.0441 (6)0.0911 (12)
H150.03460.04550.11330.109*
C160.03480 (15)0.2636 (7)0.0053 (6)0.0869 (11)
H160.00700.30330.05310.104*
C170.05940 (13)0.4037 (7)0.1023 (6)0.0841 (11)
H170.04770.53740.13230.101*
C180.10132 (14)0.3564 (7)0.1697 (5)0.0853 (11)
C190.12873 (16)0.5065 (8)0.2786 (7)0.1074 (15)
H190.11810.64390.30710.129*
C200.16999 (15)0.4536 (8)0.3416 (6)0.1001 (14)
H200.18690.55180.41530.120*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0912 (17)0.0816 (14)0.0892 (18)0.0035 (13)0.0202 (14)0.0036 (15)
C10.093 (3)0.079 (2)0.090 (3)0.006 (2)0.020 (2)0.003 (2)
C20.088 (3)0.084 (2)0.097 (3)0.0010 (19)0.023 (2)0.004 (2)
C30.095 (3)0.085 (2)0.086 (3)0.003 (2)0.017 (3)0.003 (2)
C40.084 (3)0.085 (2)0.087 (3)0.004 (2)0.016 (2)0.001 (2)
C50.089 (3)0.092 (3)0.087 (3)0.002 (2)0.014 (2)0.000 (2)
C60.076 (2)0.082 (2)0.081 (3)0.0029 (19)0.014 (2)0.001 (2)
C70.102 (3)0.089 (3)0.100 (3)0.001 (2)0.027 (3)0.001 (2)
C80.082 (3)0.086 (2)0.090 (3)0.002 (2)0.018 (2)0.000 (2)
C90.112 (3)0.101 (3)0.100 (4)0.000 (3)0.030 (3)0.002 (3)
C100.102 (4)0.094 (3)0.100 (4)0.004 (2)0.020 (3)0.002 (2)
O20.0917 (18)0.0925 (16)0.0863 (19)0.0019 (14)0.0147 (15)0.0009 (14)
C110.071 (2)0.0766 (19)0.076 (3)0.0046 (16)0.0133 (19)0.0009 (18)
C120.085 (3)0.082 (2)0.081 (3)0.0027 (19)0.017 (2)0.0001 (19)
C130.073 (2)0.0795 (19)0.083 (3)0.0014 (17)0.014 (2)0.0001 (19)
C140.099 (3)0.088 (2)0.089 (3)0.007 (2)0.021 (3)0.001 (2)
C150.093 (3)0.091 (3)0.090 (3)0.001 (2)0.017 (2)0.003 (2)
C160.087 (3)0.086 (2)0.088 (3)0.001 (2)0.017 (2)0.002 (2)
C170.079 (2)0.088 (2)0.085 (3)0.0020 (19)0.016 (2)0.002 (2)
C180.091 (3)0.084 (2)0.080 (3)0.000 (2)0.015 (2)0.003 (2)
C190.104 (3)0.108 (3)0.107 (4)0.002 (3)0.014 (3)0.007 (3)
C200.098 (3)0.109 (3)0.092 (3)0.002 (2)0.016 (3)0.001 (2)
Geometric parameters (Å, º) top
O1—C11.385 (5)O2—C111.371 (5)
O1—H10.820O2—H2A0.820
C1—C21.355 (6)C11—C121.355 (5)
C1—C101.400 (6)C11—C201.395 (6)
C2—C31.414 (6)C12—C131.389 (6)
C2—H20.930C12—H120.930
C3—C41.400 (6)C13—C141.411 (6)
C3—C81.432 (5)C13—C181.430 (5)
C4—C51.362 (6)C14—C151.351 (6)
C4—H40.930C14—H140.930
C5—C61.399 (6)C15—C161.405 (6)
C5—H50.930C15—H150.930
C6—C71.359 (6)C16—C171.345 (6)
C6—H60.930C16—H160.930
C7—C81.400 (7)C17—C181.379 (6)
C7—H70.930C17—H170.930
C8—C91.385 (7)C18—C191.431 (6)
C9—C101.343 (7)C19—C201.360 (6)
C9—H90.930C19—H190.930
C10—H100.930C20—H200.930
C1—O1—H1109.5C11—O2—H2A109.5
C2—C1—O1118.9 (4)C12—C11—O2123.0 (3)
C2—C1—C10120.3 (4)C12—C11—C20120.1 (4)
O1—C1—C10120.8 (4)O2—C11—C20116.8 (3)
C1—C2—C3121.1 (4)C11—C12—C13122.0 (4)
C1—C2—H2119.4C11—C12—H12119.0
C3—C2—H2119.4C13—C12—H12119.0
C4—C3—C2122.9 (4)C12—C13—C14123.9 (4)
C4—C3—C8119.6 (4)C12—C13—C18119.3 (4)
C2—C3—C8117.4 (4)C14—C13—C18116.7 (4)
C5—C4—C3120.6 (4)C15—C14—C13121.5 (4)
C5—C4—H4119.7C15—C14—H14119.2
C3—C4—H4119.7C13—C14—H14119.2
C4—C5—C6121.1 (4)C14—C15—C16120.8 (4)
C4—C5—H5119.4C14—C15—H15119.6
C6—C5—H5119.4C16—C15—H15119.6
C7—C6—C5118.0 (4)C17—C16—C15118.9 (5)
C7—C6—H6121.0C17—C16—H16120.6
C5—C6—H6121.0C15—C16—H16120.6
C6—C7—C8124.0 (4)C16—C17—C18122.4 (4)
C6—C7—H7118.0C16—C17—H17118.8
C8—C7—H7118.0C18—C17—H17118.8
C9—C8—C7124.4 (4)C17—C18—C13119.6 (4)
C9—C8—C3119.2 (4)C17—C18—C19123.6 (4)
C7—C8—C3116.4 (4)C13—C18—C19116.8 (4)
C10—C9—C8121.7 (5)C20—C19—C18121.7 (5)
C10—C9—H9119.1C20—C19—H19119.2
C8—C9—H9119.1C18—C19—H19119.2
C9—C10—C1120.2 (5)C19—C20—C11120.0 (5)
C9—C10—H10119.9C19—C20—H20120.0
C1—C10—H10119.9C11—C20—H20120.0
O1—C1—C2—C3178.1 (4)O2—C11—C12—C13179.6 (4)
C10—C1—C2—C30.3 (7)C20—C11—C12—C132.3 (6)
C1—C2—C3—C4178.5 (5)C11—C12—C13—C14179.0 (4)
C1—C2—C3—C81.2 (7)C11—C12—C13—C181.7 (7)
C2—C3—C4—C5179.5 (4)C12—C13—C14—C15179.9 (4)
C8—C3—C4—C53.3 (7)C18—C13—C14—C150.9 (7)
C3—C4—C5—C65.5 (7)C13—C14—C15—C161.6 (7)
C4—C5—C6—C76.3 (7)C14—C15—C16—C173.6 (7)
C5—C6—C7—C85.2 (8)C15—C16—C17—C183.2 (7)
C6—C7—C8—C9177.8 (5)C16—C17—C18—C130.7 (7)
C6—C7—C8—C33.1 (7)C16—C17—C18—C19177.2 (5)
C4—C3—C8—C9178.9 (5)C12—C13—C18—C17179.4 (4)
C2—C3—C8—C91.5 (6)C14—C13—C18—C171.3 (6)
C4—C3—C8—C72.0 (6)C12—C13—C18—C191.3 (6)
C2—C3—C8—C7179.4 (4)C14—C13—C18—C19179.4 (4)
C7—C8—C9—C10179.9 (5)C17—C18—C19—C20179.6 (5)
C3—C8—C9—C101.0 (8)C13—C18—C19—C201.6 (7)
C8—C9—C10—C10.1 (8)C18—C19—C20—C112.2 (8)
C2—C1—C10—C90.3 (8)C12—C11—C20—C192.6 (7)
O1—C1—C10—C9178.6 (4)O2—C11—C20—C19179.9 (4)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1···O2i0.822.142.764 (3)133
O2—H2A···O1ii0.822.452.752 (3)103
Symmetry codes: (i) x, y+1, z; (ii) x, y+1, z+1/2.
 

Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds