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The structure of the title compound, C11H10O3, shows pseudo-symmetry. Since the mol­ecule is nearly planar and all non-H atoms lie close to an approximate mirror plane perpendicular to the crystallographic b axis, the structure could almost (85%) be described in space group P21/m. However, the correct space group is P21.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807024142/is2168sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807024142/is2168Isup2.hkl
Contains datablock I

CCDC reference: 651772

Key indicators

  • Single-crystal X-ray study
  • T = 173 K
  • Mean [sigma](C-C) = 0.005 Å
  • R factor = 0.047
  • wR factor = 0.130
  • Data-to-parameter ratio = 7.6

checkCIF/PLATON results

No syntax errors found



Alert level B PLAT111_ALERT_2_B ADDSYM Detects (Pseudo) Centre of Symmetry ..... 85 PerFi
Alert level C PLAT089_ALERT_3_C Poor Data / Parameter Ratio (Zmax .LT. 18) ..... 7.63 PLAT340_ALERT_3_C Low Bond Precision on C-C Bonds (x 1000) Ang ... 5 PLAT369_ALERT_2_C Long C(sp2)-C(sp2) Bond C3 - C4 ... 1.55 Ang.
Alert level G REFLT03_ALERT_4_G 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. From the CIF: _diffrn_reflns_theta_max 25.56 From the CIF: _reflns_number_total 977 Count of symmetry unique reflns 983 Completeness (_total/calc) 99.39% 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 PLAT860_ALERT_3_G Note: Number of Least-Squares Restraints ....... 1
0 ALERT level A = In general: serious problem 1 ALERT level B = Potentially serious problem 3 ALERT level C = Check and explain 2 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 2 ALERT type 2 Indicator that the structure model may be wrong or deficient 3 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

Comment top

Unsaturated α-ketoesters are of great synthetic interest and are widely used as substrates for enantioselective 1,4-additions. For example, Jensen et al. (2001) could develop an highly enantioselective Friedel-Crafts type addition of different electron rich arenes to (E)-methyl 2-oxo-4-phenylbut-3-enoate (Jensen et al., 2001; Jørgensen, 2003). The title compound, (I), was synthesized by an Lewis-Acid catalysed aldol condensation of benzaldehyde and methylpyruvate.

Geometric parameters of (I) are in the normal ranges. The C—C double bond is trans configured and the two carbonyl groups are also trans to each other (Fig. 1). The molecule is almost planar, the r.m.s. deviation for all non-H atoms being 0.208 Å. The structure of (I) shows pseudo-symmetry. The packing diagram (Fig. 2) reveals that the non-H atoms almost lie on a mirror plane perpendicular to the crystallographic b axis. A check for missed symmetry with PLATON (Spek, 2003) suggests space group P21/m with the higher symmetry being fulfilled by 85% of the atoms. However, the correct space group is P21.

Related literature top

For related literature, see: Dujardin et al. (2001); Jørgensen (2003); Jensen et al. (2001); Spek (2003).

Experimental top

The title compound was synthesized by an Lewis-Acid catalysed aldol condensation of benzaldehyde and methylpyruvate (Dujardin et al., 2001).

Refinement top

In the absence of anomalous scatterers Friedel pairs had been merged prior to refinement. The absolute structure was arbitrarily assigned. H atoms were found in a difference map, but they were refined using a riding model with C—H = 0.95 Å and Uiso(H) = 1.2Ueq(C) or C—H = 0.98 Å and Uiso(H) = 1.5Ueq(Cmethyl). The methyl group was allowed to rotate but not to tip.

Structure description top

Unsaturated α-ketoesters are of great synthetic interest and are widely used as substrates for enantioselective 1,4-additions. For example, Jensen et al. (2001) could develop an highly enantioselective Friedel-Crafts type addition of different electron rich arenes to (E)-methyl 2-oxo-4-phenylbut-3-enoate (Jensen et al., 2001; Jørgensen, 2003). The title compound, (I), was synthesized by an Lewis-Acid catalysed aldol condensation of benzaldehyde and methylpyruvate.

Geometric parameters of (I) are in the normal ranges. The C—C double bond is trans configured and the two carbonyl groups are also trans to each other (Fig. 1). The molecule is almost planar, the r.m.s. deviation for all non-H atoms being 0.208 Å. The structure of (I) shows pseudo-symmetry. The packing diagram (Fig. 2) reveals that the non-H atoms almost lie on a mirror plane perpendicular to the crystallographic b axis. A check for missed symmetry with PLATON (Spek, 2003) suggests space group P21/m with the higher symmetry being fulfilled by 85% of the atoms. However, the correct space group is P21.

For related literature, see: Dujardin et al. (2001); Jørgensen (2003); Jensen et al. (2001); Spek (2003).

Computing details top

Data collection: X-AREA (Stoe & Cie, 2001); cell refinement: X-AREA; data reduction: X-AREA; program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); 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.

Figures top
[Figure 1] Fig. 1. Perspective view of (I) with the atom numbering. Displacement ellipsoids of non-H atoms are drawn at the 50% probability level.
[Figure 2] Fig. 2. Packing diagram of (I), viewed onto the bc plane.
(E)-Methyl 2-oxo-4-phenylbut-3-enoate top
Crystal data top
C11H10O3F(000) = 200
Mr = 190.19Dx = 1.311 Mg m3
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ybCell parameters from 5679 reflections
a = 7.1114 (10) Åθ = 3.8–25.2°
b = 6.5381 (6) ŵ = 0.10 mm1
c = 10.5106 (15) ÅT = 173 K
β = 99.527 (11)°Plate, colourless
V = 481.95 (11) Å30.34 × 0.31 × 0.22 mm
Z = 2
Data collection top
Stoe IPDS II two-circle-
diffractometer
937 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.035
Graphite monochromatorθmax = 25.6°, θmin = 3.7°
ω scansh = 88
4453 measured reflectionsk = 77
977 independent reflectionsl = 1212
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)] = 0.047Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.130H-atom parameters constrained
S = 1.19 w = 1/[σ2(Fo2) + (0.043P)2 + 0.4561P]
where P = (Fo2 + 2Fc2)/3
977 reflections(Δ/σ)max < 0.001
128 parametersΔρmax = 0.26 e Å3
1 restraintΔρmin = 0.35 e Å3
Crystal data top
C11H10O3V = 481.95 (11) Å3
Mr = 190.19Z = 2
Monoclinic, P21Mo Kα radiation
a = 7.1114 (10) ŵ = 0.10 mm1
b = 6.5381 (6) ÅT = 173 K
c = 10.5106 (15) Å0.34 × 0.31 × 0.22 mm
β = 99.527 (11)°
Data collection top
Stoe IPDS II two-circle-
diffractometer
937 reflections with I > 2σ(I)
4453 measured reflectionsRint = 0.035
977 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0471 restraint
wR(F2) = 0.130H-atom parameters constrained
S = 1.19Δρmax = 0.26 e Å3
977 reflectionsΔρmin = 0.35 e Å3
128 parameters
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
xyzUiso*/Ueq
C10.6767 (5)0.2097 (7)0.2504 (3)0.0233 (8)
H10.78660.19680.31490.028*
C20.5092 (5)0.2322 (8)0.2914 (3)0.0242 (8)
H20.39590.25090.23050.029*
C30.4997 (5)0.2281 (8)0.4302 (3)0.0257 (8)
O30.6377 (3)0.2281 (8)0.5165 (2)0.0438 (9)
C40.2961 (5)0.2250 (8)0.4643 (3)0.0244 (8)
O40.1529 (3)0.2226 (8)0.3846 (2)0.0442 (9)
O50.3006 (3)0.2202 (6)0.5911 (2)0.0286 (7)
C60.1147 (5)0.2062 (10)0.6332 (3)0.0339 (10)
H6A0.04520.33480.61390.051*
H6B0.13330.18060.72630.051*
H6C0.04140.09360.58760.051*
C110.7074 (5)0.2029 (7)0.1152 (3)0.0229 (8)
C120.5656 (5)0.2600 (6)0.0122 (3)0.0261 (9)
H120.44610.30880.02870.031*
C130.5998 (5)0.2451 (8)0.1155 (3)0.0303 (9)
H130.50440.28510.18530.036*
C140.7741 (6)0.1715 (6)0.1390 (4)0.0309 (10)
H140.79690.16030.22530.037*
C150.9150 (6)0.1141 (8)0.0380 (4)0.0323 (10)
H151.03380.06430.05510.039*
C160.8823 (5)0.1295 (7)0.0884 (4)0.0276 (9)
H160.97930.08990.15740.033*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0243 (15)0.0251 (19)0.0206 (15)0.003 (2)0.0041 (12)0.0008 (18)
C20.0222 (15)0.031 (2)0.0187 (15)0.002 (2)0.0009 (12)0.001 (2)
C30.0219 (15)0.034 (2)0.0210 (15)0.001 (2)0.0029 (12)0.002 (2)
O30.0215 (12)0.087 (3)0.0219 (12)0.003 (2)0.0003 (9)0.001 (2)
C40.0227 (15)0.029 (2)0.0222 (15)0.002 (2)0.0051 (12)0.003 (2)
O40.0223 (12)0.081 (2)0.0268 (13)0.003 (2)0.0029 (10)0.000 (2)
O50.0228 (11)0.0454 (17)0.0186 (11)0.0030 (18)0.0068 (9)0.0006 (17)
C60.0232 (17)0.053 (3)0.0283 (18)0.001 (2)0.0117 (14)0.002 (2)
C110.0257 (16)0.023 (2)0.0195 (16)0.0025 (19)0.0037 (13)0.0008 (18)
C120.0275 (17)0.026 (2)0.0246 (17)0.0041 (18)0.0037 (14)0.0006 (17)
C130.0368 (19)0.032 (2)0.0209 (16)0.000 (2)0.0013 (14)0.004 (2)
C140.040 (2)0.031 (3)0.0235 (17)0.0031 (19)0.0114 (16)0.0015 (17)
C150.034 (2)0.035 (2)0.030 (2)0.001 (2)0.0132 (17)0.0004 (19)
C160.0253 (18)0.030 (2)0.0283 (19)0.0013 (18)0.0078 (15)0.0005 (18)
Geometric parameters (Å, º) top
C1—C21.340 (5)C6—H6C0.9800
C1—C111.473 (4)C11—C121.403 (5)
C1—H10.9500C11—C161.405 (5)
C2—C31.472 (4)C12—C131.407 (5)
C2—H20.9500C12—H120.9500
C3—O31.221 (4)C13—C141.389 (6)
C3—C41.548 (4)C13—H130.9500
C4—O41.207 (4)C14—C151.386 (6)
C4—O51.328 (4)C14—H140.9500
O5—C61.464 (4)C15—C161.390 (5)
C6—H6A0.9800C15—H150.9500
C6—H6B0.9800C16—H160.9500
C2—C1—C11126.5 (3)C12—C11—C16118.9 (3)
C2—C1—H1116.7C12—C11—C1122.3 (3)
C11—C1—H1116.7C16—C11—C1118.8 (3)
C1—C2—C3120.4 (3)C11—C12—C13120.2 (3)
C1—C2—H2119.8C11—C12—H12119.9
C3—C2—H2119.8C13—C12—H12119.9
O3—C3—C2125.0 (3)C14—C13—C12119.6 (3)
O3—C3—C4119.7 (3)C14—C13—H13120.2
C2—C3—C4115.3 (3)C12—C13—H13120.2
O4—C4—O5125.0 (3)C15—C14—C13120.7 (3)
O4—C4—C3123.6 (3)C15—C14—H14119.6
O5—C4—C3111.3 (3)C13—C14—H14119.6
C4—O5—C6115.6 (3)C14—C15—C16119.9 (4)
O5—C6—H6A109.5C14—C15—H15120.0
O5—C6—H6B109.5C16—C15—H15120.0
H6A—C6—H6B109.5C15—C16—C11120.7 (4)
O5—C6—H6C109.5C15—C16—H16119.6
H6A—C6—H6C109.5C11—C16—H16119.6
H6B—C6—H6C109.5
C11—C1—C2—C3177.6 (4)C2—C1—C11—C16164.6 (5)
C1—C2—C3—O38.6 (9)C16—C11—C12—C130.5 (6)
C1—C2—C3—C4171.7 (4)C1—C11—C12—C13178.1 (4)
O3—C3—C4—O4179.2 (7)C11—C12—C13—C140.7 (7)
C2—C3—C4—O41.2 (7)C12—C13—C14—C150.5 (7)
O3—C3—C4—O50.7 (7)C13—C14—C15—C160.2 (7)
C2—C3—C4—O5179.6 (5)C14—C15—C16—C110.0 (7)
O4—C4—O5—C61.5 (8)C12—C11—C16—C150.2 (6)
C3—C4—O5—C6176.9 (4)C1—C11—C16—C15177.9 (4)
C2—C1—C11—C1212.9 (8)

Experimental details

Crystal data
Chemical formulaC11H10O3
Mr190.19
Crystal system, space groupMonoclinic, P21
Temperature (K)173
a, b, c (Å)7.1114 (10), 6.5381 (6), 10.5106 (15)
β (°) 99.527 (11)
V3)481.95 (11)
Z2
Radiation typeMo Kα
µ (mm1)0.10
Crystal size (mm)0.34 × 0.31 × 0.22
Data collection
DiffractometerStoe IPDS II two-circle-
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
4453, 977, 937
Rint0.035
(sin θ/λ)max1)0.607
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.047, 0.130, 1.19
No. of reflections977
No. of parameters128
No. of restraints1
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.26, 0.35

Computer programs: X-AREA (Stoe & Cie, 2001), X-AREA, SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), XP in SHELXTL-Plus (Sheldrick, 1991), SHELXL97.

 

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