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Geometric parameters of the title compound, C9H10O3, are in the usual ranges. The dioxolane ring adopts an envelope conformation with one of the ring O atoms deviating by 0.477 (4) Å from the plane of the remaining four atoms [C—O—C—C torsion angle = −0.6 (3)°]. The mol­ecules are linked by an O—H...O hydrogen bond, forming zigzag chains running along the a axis.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807056103/ng2361sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807056103/ng2361Isup2.hkl
Contains datablock I

CCDC reference: 674089

Key indicators

  • Single-crystal X-ray study
  • T = 173 K
  • Mean [sigma](C-C)= 0.004 Å
  • R factor = 0.049
  • wR factor = 0.093
  • Data-to-parameter ratio = 12.8

checkCIF/PLATON results

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Comment top

We report here the X-ray crystal structure analysis of salicylaldehyde ethylene cyclic acetal. Recently, we have synthesized complexes with redox-active hydroquinone / quinone ligands (Lerner et al., 2006; Kretz et al., 2007). To get more information about ligand properties we focus our interest now on the synthesis of complexes with identical geometrical parameters but with redox-inactive ("innocent") ligands coordinate on the transition metal centers. Therefore we decided to prepare the salicylaldehyde ethylene cyclic acetal as starting material of these "innocent" ligands.

Geometric parameters of the title compound are in the usual ranges. The dioxolane ring adopts an envelope conformation with one of the ring O atoms deviating by 0.477 (4) Å from the plane of the remaining four atoms [torsion angle C11—O12—C13—C14 - 0.6 (3)°]. The molecules are linked by a O—H···O hydrogen bond to zigzag chains running along the a axis.

Related literature top

For related literature, see: Kretz et al. (2007); Lerner et al. (2006).

Experimental top

A mixture of commercially available salicylaldehyde (2.8 g, 23 mmol), ethylene glycole (3.3 g, 53 mmol), and toluene (40 mL), and p-toluenesulfonic acid (0.1 g) was boiled for six hours in a flask fitted with a water-separator head. Single crystals of title compound were obtained from the reaction mixture at ambient temperature.

Refinement top

H atoms bonded to C were refined with fixed individual displacement parameters [U(H) = 1.2 Ueq(C,O)] using a riding model with O—H = 0.84 Å and C—H ranging from 0.95 Å to 1.0 Å. The hydroxy group was allowed to rotate but not to tip.

Computing details top

Data collection: X-AREA (Stoe & Cie, 2001); cell refinement: X-AREA (Stoe & Cie, 2001); data reduction: X-AREA (Stoe & Cie, 2001); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: XP in SHELXTL-Plus (Sheldrick, 1991); software used to prepare material for publication: SHELXL97 (Sheldrick, 1997) and PLATON (Spek, 2003).

Figures top
[Figure 1] Fig. 1. Perspective view of the title compound with the atom numbering; displacement ellipsoids are at the 50% probability level.
[Figure 2] Fig. 2. Partial packing diagram of the title compound. Hydrogen bonds shown as dashed lines.
2-(1,3-Dioxolan-2-yl)phenol top
Crystal data top
C9H10O3F(000) = 704
Mr = 166.17Dx = 1.350 Mg m3
Orthorhombic, PbcaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2abCell parameters from 2262 reflections
a = 7.4564 (15) Åθ = 3.6–25.2°
b = 11.172 (2) ŵ = 0.10 mm1
c = 19.633 (4) ÅT = 173 K
V = 1635.5 (6) Å3Plate, colourless
Z = 80.24 × 0.12 × 0.03 mm
Data collection top
Stoe IPDSII two-circle
diffractometer
774 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.082
Graphite monochromatorθmax = 25.0°, θmin = 3.7°
ω scansh = 88
5325 measured reflectionsk = 1313
1413 independent reflectionsl = 2223
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)] = 0.049Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.093H-atom parameters constrained
S = 0.86 w = 1/[σ2(Fo2) + (0.0241P)2]
where P = (Fo2 + 2Fc2)/3
1413 reflections(Δ/σ)max < 0.001
110 parametersΔρmax = 0.19 e Å3
0 restraintsΔρmin = 0.20 e Å3
Crystal data top
C9H10O3V = 1635.5 (6) Å3
Mr = 166.17Z = 8
Orthorhombic, PbcaMo Kα radiation
a = 7.4564 (15) ŵ = 0.10 mm1
b = 11.172 (2) ÅT = 173 K
c = 19.633 (4) Å0.24 × 0.12 × 0.03 mm
Data collection top
Stoe IPDSII two-circle
diffractometer
774 reflections with I > 2σ(I)
5325 measured reflectionsRint = 0.082
1413 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0490 restraints
wR(F2) = 0.093H-atom parameters constrained
S = 0.86Δρmax = 0.19 e Å3
1413 reflectionsΔρmin = 0.20 e Å3
110 parameters
Special details top

Experimental. ;

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
C10.5283 (4)0.3479 (2)0.62327 (12)0.0247 (6)
C20.6308 (4)0.2789 (2)0.57795 (12)0.0294 (7)
O20.6007 (3)0.29787 (18)0.50973 (8)0.0396 (6)
H20.64810.24250.48710.048*
C30.7516 (5)0.1944 (2)0.60194 (13)0.0351 (7)
H30.81930.14760.57080.042*
C40.7735 (5)0.1784 (3)0.67196 (13)0.0394 (8)
H40.85560.12040.68870.047*
C50.6755 (5)0.2469 (2)0.71662 (14)0.0359 (8)
H50.69040.23610.76430.043*
C60.5561 (4)0.3312 (2)0.69295 (12)0.0306 (7)
H60.49140.37880.72460.037*
C110.3905 (5)0.4325 (2)0.59682 (13)0.0295 (7)
H110.43650.47470.55540.035*
O120.2257 (3)0.36945 (17)0.58096 (9)0.0373 (5)
C130.0756 (5)0.4432 (3)0.60146 (18)0.0490 (9)
H13A0.00100.40200.63600.059*
H13B0.00040.46430.56190.059*
C140.1629 (5)0.5515 (3)0.63072 (18)0.0472 (9)
H14A0.16350.61770.59720.057*
H14B0.09860.57850.67210.057*
O150.3404 (3)0.51632 (15)0.64692 (10)0.0393 (6)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0240 (18)0.0245 (12)0.0255 (13)0.0032 (12)0.0018 (12)0.0038 (10)
C20.0288 (19)0.0295 (13)0.0298 (14)0.0025 (13)0.0028 (13)0.0032 (11)
O20.0542 (17)0.0432 (11)0.0215 (10)0.0140 (11)0.0020 (9)0.0046 (8)
C30.0321 (19)0.0335 (14)0.0395 (15)0.0047 (16)0.0017 (15)0.0049 (12)
C40.036 (2)0.0406 (16)0.0418 (17)0.0061 (16)0.0024 (15)0.0064 (13)
C50.0307 (19)0.0474 (17)0.0297 (14)0.0042 (14)0.0040 (13)0.0021 (12)
C60.0319 (19)0.0332 (14)0.0268 (14)0.0031 (14)0.0030 (13)0.0059 (11)
C110.034 (2)0.0244 (13)0.0301 (14)0.0009 (14)0.0057 (13)0.0052 (11)
O120.0283 (14)0.0363 (10)0.0473 (11)0.0056 (10)0.0091 (10)0.0151 (9)
C130.039 (2)0.0544 (19)0.0535 (19)0.0139 (16)0.0095 (17)0.0176 (16)
C140.037 (2)0.0367 (15)0.068 (2)0.0049 (15)0.0060 (19)0.0116 (15)
O150.0324 (15)0.0324 (10)0.0530 (12)0.0053 (10)0.0044 (11)0.0200 (10)
Geometric parameters (Å, º) top
C1—C61.396 (4)C6—H60.9500
C1—C21.404 (4)C11—O151.408 (3)
C1—C111.490 (4)C11—O121.450 (4)
C2—O21.374 (3)C11—H111.0000
C2—C31.387 (4)O12—C131.447 (4)
O2—H20.8400C13—C141.489 (4)
C3—C41.396 (4)C13—H13A0.9900
C3—H30.9500C13—H13B0.9900
C4—C51.374 (4)C14—O151.417 (4)
C4—H40.9500C14—H14A0.9900
C5—C61.376 (4)C14—H14B0.9900
C5—H50.9500
C6—C1—C2117.8 (3)O15—C11—C1111.2 (2)
C6—C1—C11121.9 (2)O12—C11—C1110.6 (2)
C2—C1—C11120.2 (2)O15—C11—H11110.2
O2—C2—C3122.8 (2)O12—C11—H11110.2
O2—C2—C1116.4 (2)C1—C11—H11110.2
C3—C2—C1120.8 (2)C13—O12—C11108.6 (2)
C2—O2—H2109.5O12—C13—C14103.4 (3)
C2—C3—C4119.8 (3)O12—C13—H13A111.1
C2—C3—H3120.1C14—C13—H13A111.1
C4—C3—H3120.1O12—C13—H13B111.1
C5—C4—C3119.7 (3)C14—C13—H13B111.1
C5—C4—H4120.2H13A—C13—H13B109.0
C3—C4—H4120.2O15—C14—C13105.6 (2)
C4—C5—C6120.6 (3)O15—C14—H14A110.6
C4—C5—H5119.7C13—C14—H14A110.6
C6—C5—H5119.7O15—C14—H14B110.6
C5—C6—C1121.2 (3)C13—C14—H14B110.6
C5—C6—H6119.4H14A—C14—H14B108.7
C1—C6—H6119.4C11—O15—C14106.0 (2)
O15—C11—O12104.4 (2)
C6—C1—C2—O2179.8 (3)C6—C1—C11—O1519.3 (4)
C11—C1—C2—O22.4 (4)C2—C1—C11—O15162.9 (2)
C6—C1—C2—C32.0 (4)C6—C1—C11—O1296.2 (3)
C11—C1—C2—C3175.9 (3)C2—C1—C11—O1281.6 (3)
O2—C2—C3—C4178.9 (3)O15—C11—O12—C1321.0 (3)
C1—C2—C3—C40.7 (5)C1—C11—O12—C13140.6 (2)
C2—C3—C4—C50.3 (5)C11—O12—C13—C140.6 (3)
C3—C4—C5—C60.0 (5)O12—C13—C14—O1519.9 (3)
C4—C5—C6—C11.3 (5)O12—C11—O15—C1433.9 (3)
C2—C1—C6—C52.2 (4)C1—C11—O15—C14153.1 (2)
C11—C1—C6—C5175.6 (3)C13—C14—O15—C1134.0 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2—H2···O12i0.841.922.745 (3)167
Symmetry code: (i) x+1/2, y+1/2, z+1.

Experimental details

Crystal data
Chemical formulaC9H10O3
Mr166.17
Crystal system, space groupOrthorhombic, Pbca
Temperature (K)173
a, b, c (Å)7.4564 (15), 11.172 (2), 19.633 (4)
V3)1635.5 (6)
Z8
Radiation typeMo Kα
µ (mm1)0.10
Crystal size (mm)0.24 × 0.12 × 0.03
Data collection
DiffractometerStoe IPDSII two-circle
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
5325, 1413, 774
Rint0.082
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.049, 0.093, 0.86
No. of reflections1413
No. of parameters110
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.19, 0.20

Computer programs: X-AREA (Stoe & Cie, 2001), SHELXS97 (Sheldrick, 1997), XP in SHELXTL-Plus (Sheldrick, 1991), SHELXL97 (Sheldrick, 1997) and PLATON (Spek, 2003).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2—H2···O12i0.841.922.745 (3)167
Symmetry code: (i) x+1/2, y+1/2, z+1.
 

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