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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2007 Dec 6;64(Pt 1):o88. doi: 10.1107/S1600536807062137

4-Methyl­phenyl 4-chloro­benzoate

B Thimme Gowda a,*, Ingrid Svoboda b, K S Babitha a, Hartmut Fuess b
PMCID: PMC2915044  PMID: 21200965

Abstract

The crystal structure of the title compound, C14H11ClO2, is similar to those of phenyl benzoate, 4-methyl­phenyl benzoate and 4-methyl­phenyl 4-methyl­benzoate. The dihedral angle between the phenyl and benzene rings is 51.86 (4)°. The mol­ecules crystallize in planes parallel to (Inline graphic02).

Related literature

For related literature, see: Adams & Morsi (1976); Gowda, Foro, Babitha & Fuess (2007a ,b ,c ,d ,e ); Gowda, Foro, Nayak & Fuess (2007a ,b ); Nayak & Gowda (2007).graphic file with name e-64-00o88-scheme1.jpg

Experimental

Crystal data

  • C14H11ClO2

  • M r = 246.68

  • Monoclinic, Inline graphic

  • a = 14.6932 (4) Å

  • b = 11.3269 (3) Å

  • c = 7.2386 (2) Å

  • β = 101.050 (3)°

  • V = 1182.37 (6) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.31 mm−1

  • T = 100 (2) K

  • 0.40 × 0.28 × 0.08 mm

Data collection

  • Oxford Diffraction Xcalibur diffractometer with Sapphire CCD detector

  • Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2006) T min = 0.887, T max = 0.976

  • 17127 measured reflections

  • 2407 independent reflections

  • 1889 reflections with I > 2σ(I)

  • R int = 0.023

Refinement

  • R[F 2 > 2σ(F 2)] = 0.034

  • wR(F 2) = 0.096

  • S = 1.04

  • 2407 reflections

  • 155 parameters

  • H-atom parameters constrained

  • Δρmax = 1.04 e Å−3

  • Δρmin = −0.29 e Å−3

Data collection: CrysAlis CCD (Oxford Diffraction, 2006); cell refinement: CrysAlis RED; data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek 2003) and ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536807062137/bt2647sup1.cif

e-64-00o88-sup1.cif (15.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536807062137/bt2647Isup2.hkl

e-64-00o88-Isup2.hkl (118.3KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Acknowledgments

BTG thanks the Alexander von Humboldt Foundation, Bonn, Germany, for extensions of his research fellowship.

supplementary crystallographic information

Comment

In the present work, the structure of 4-methylphenyl 4-chlorobenzoate (4MP4CBA) has been determined, as part of a study of substituent effects on the structures of industrially significant compounds (Gowda, Foro, Babitha & Fuess, 2007a, 2007b; Gowda, Foro, Nayak & Fuess, 2007a, 2007b). The structure of 4MP4CBA (Fig. 1) resembles those of phenyl benzoate (PBA)(Adams & Morsi, 1976), 4-methylphenyl benzoate (4MPBA) (Gowda, Foro, Nayak & Fuess, 2007b), 4-methylphenyl 4-methylbenzoate (4MP4MBA)(Gowda, Foro, Babitha & Fuess, 2007b) and other aryl benzoates (Gowda, Foro, Babitha & Fuess, 2007a; Gowda, Foro, Nayak & Fuess, 2007a). The bond parameters in 4MP4CBA are similar to those in PBA, 4MPBA, 4MP4MBA and other benzoates (Gowda, Foro, Babitha & Fuess, 2007a, 2007b; Gowda, Foro, Nayak & Fuess, 2007a, 2007b). The molecules in the title compound are packed into plane parallel to (-1 0 2) (Fig. 2).

Experimental

The title compound was prepared according to a literature method (Nayak & Gowda, 2007). The purity of the compound was checked by determining its melting point. It was characterized by recording its infrared and NMR spectra (Nayak & Gowda, 2007). Single crystals of the title compound were obtained by slow evaporation of an ethanolic solution and used for X-ray diffraction studies at room temperature.

Refinement

The H atoms of the methyl groups were positioned with idealized geometry using a riding model with C—H = 0.98 Å. The other H atoms were located in difference map and their positions refined.

Figures

Fig. 1.

Fig. 1.

Molecular structure of the title compound, showing the atom labeling. Displacement ellipsoids are drawn at the 50% probability level. H atoms are represented as small spheres of arbitrary radius.

Fig. 2.

Fig. 2.

Molecular packing of the title compound.

Crystal data

C14H11ClO2 F000 = 512
Mr = 246.68 Dx = 1.386 Mg m3
Monoclinic, P21/c Mo Kα radiation λ = 0.71073 Å
Hall symbol: -P2ybc Cell parameters from 5716 reflections
a = 14.6932 (4) Å θ = 2.2–26.9º
b = 11.3269 (3) Å µ = 0.31 mm1
c = 7.2386 (2) Å T = 100 (2) K
β = 101.050 (3)º Prism, colourless
V = 1182.37 (6) Å3 0.40 × 0.28 × 0.08 mm
Z = 4

Data collection

Oxford Diffraction Xcalibur diffractometer with Sapphire CCD detector 2407 independent reflections
Radiation source: Enhance (Mo) X-ray Source 1889 reflections with I > 2σ(I)
Monochromator: graphite Rint = 0.023
Detector resolution: 8.4012 pixels mm-1 θmax = 26.4º
T = 100(2) K θmin = 2.3º
Rotation method data acquisition using ω scans. h = −18→18
Absorption correction: multi-scan(CrysAlis RED; Oxford Diffraction, 2006) k = −13→14
Tmin = 0.887, Tmax = 0.976 l = −9→9
17127 measured reflections

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.034 H-atom parameters constrained
wR(F2) = 0.096   w = 1/[σ2(Fo2) + (0.0437P)2 + 0.873P] where P = (Fo2 + 2Fc2)/3
S = 1.04 (Δ/σ)max < 0.001
2407 reflections Δρmax = 1.04 e Å3
155 parameters Δρmin = −0.29 e Å3
Primary atom site location: structure-invariant direct methods Extinction correction: none

Special details

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)

x y z Uiso*/Ueq
Cl1 −0.39495 (3) 0.43951 (5) 0.00266 (7) 0.03131 (16)
O1 0.06211 (8) 0.40950 (10) 0.28512 (17) 0.0203 (3)
O2 0.02463 (9) 0.23571 (11) 0.40524 (18) 0.0264 (3)
C1 −0.27915 (12) 0.40681 (16) 0.0929 (2) 0.0204 (4)
C2 −0.25731 (12) 0.30158 (16) 0.1886 (2) 0.0214 (4)
H2 −0.3045 0.2473 0.2043 0.026*
C3 −0.16463 (12) 0.27738 (15) 0.2611 (2) 0.0193 (4)
H3 −0.1481 0.2058 0.3275 0.023*
C4 −0.09585 (11) 0.35718 (15) 0.2371 (2) 0.0172 (3)
C5 −0.11937 (12) 0.46239 (15) 0.1393 (2) 0.0184 (4)
H5 −0.0723 0.5167 0.1224 0.022*
C6 −0.21182 (12) 0.48738 (15) 0.0668 (2) 0.0196 (4)
H6 −0.2287 0.5588 0.0002 0.024*
C7 0.00171 (12) 0.32497 (15) 0.3186 (2) 0.0188 (4)
C8 0.15790 (11) 0.38716 (16) 0.3334 (2) 0.0185 (4)
C9 0.19650 (12) 0.28504 (15) 0.2769 (2) 0.0197 (4)
H9 0.1583 0.2245 0.2123 0.024*
C10 0.29215 (12) 0.27312 (15) 0.3169 (2) 0.0208 (4)
H10 0.3193 0.2028 0.2806 0.025*
C11 0.34947 (12) 0.36115 (16) 0.4084 (2) 0.0222 (4)
C12 0.30820 (12) 0.46299 (16) 0.4619 (2) 0.0224 (4)
H12 0.3462 0.5244 0.5243 0.027*
C13 0.21257 (12) 0.47634 (15) 0.4254 (2) 0.0199 (4)
H13 0.1851 0.5460 0.4633 0.024*
C14 0.45367 (13) 0.34475 (18) 0.4483 (3) 0.0327 (5)
H14A 0.4683 0.2603 0.4581 0.049*
H14B 0.4805 0.3840 0.5669 0.049*
H14C 0.4797 0.3794 0.3457 0.049*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cl1 0.0190 (2) 0.0368 (3) 0.0365 (3) 0.00206 (19) 0.00115 (18) 0.0060 (2)
O1 0.0181 (6) 0.0181 (6) 0.0245 (6) −0.0002 (5) 0.0033 (5) 0.0019 (5)
O2 0.0240 (7) 0.0247 (7) 0.0303 (7) 0.0022 (5) 0.0044 (5) 0.0110 (6)
C1 0.0170 (8) 0.0249 (9) 0.0192 (9) 0.0012 (7) 0.0032 (7) −0.0033 (7)
C2 0.0224 (9) 0.0220 (9) 0.0200 (9) −0.0038 (7) 0.0049 (7) −0.0003 (7)
C3 0.0254 (9) 0.0158 (8) 0.0168 (8) −0.0002 (7) 0.0043 (7) 0.0003 (7)
C4 0.0206 (8) 0.0167 (8) 0.0149 (8) 0.0011 (7) 0.0052 (6) −0.0018 (7)
C5 0.0221 (8) 0.0160 (8) 0.0184 (8) −0.0012 (7) 0.0070 (7) −0.0010 (7)
C6 0.0239 (9) 0.0168 (8) 0.0190 (8) 0.0033 (7) 0.0062 (7) 0.0012 (7)
C7 0.0215 (8) 0.0184 (9) 0.0171 (8) −0.0022 (7) 0.0051 (7) −0.0016 (7)
C8 0.0183 (8) 0.0209 (9) 0.0167 (8) 0.0008 (7) 0.0047 (7) 0.0041 (7)
C9 0.0252 (9) 0.0173 (9) 0.0166 (8) −0.0010 (7) 0.0043 (7) 0.0000 (7)
C10 0.0265 (9) 0.0178 (9) 0.0200 (8) 0.0031 (7) 0.0087 (7) 0.0009 (7)
C11 0.0221 (9) 0.0234 (9) 0.0226 (9) 0.0010 (7) 0.0080 (7) 0.0037 (7)
C12 0.0241 (9) 0.0200 (9) 0.0231 (9) −0.0041 (7) 0.0045 (7) −0.0005 (7)
C13 0.0239 (9) 0.0166 (8) 0.0205 (9) 0.0013 (7) 0.0074 (7) −0.0002 (7)
C14 0.0221 (9) 0.0310 (11) 0.0448 (12) 0.0012 (8) 0.0061 (8) 0.0015 (9)

Geometric parameters (Å, °)

Cl1—C1 1.7414 (17) C8—C13 1.380 (2)
O1—C7 1.359 (2) C8—C9 1.384 (2)
O1—C8 1.407 (2) C9—C10 1.386 (2)
O2—C7 1.203 (2) C9—H9 0.9500
C1—C2 1.385 (3) C10—C11 1.389 (3)
C1—C6 1.385 (3) C10—H10 0.9500
C2—C3 1.390 (2) C11—C12 1.392 (3)
C2—H2 0.9500 C11—C14 1.514 (2)
C3—C4 1.391 (2) C12—C13 1.387 (2)
C3—H3 0.9500 C12—H12 0.9500
C4—C5 1.395 (2) C13—H13 0.9500
C4—C7 1.487 (2) C14—H14A 0.9800
C5—C6 1.388 (2) C14—H14B 0.9800
C5—H5 0.9500 C14—H14C 0.9800
C6—H6 0.9500
C7—O1—C8 119.05 (13) C13—C8—O1 116.77 (15)
C2—C1—C6 122.14 (16) C9—C8—O1 121.61 (15)
C2—C1—Cl1 119.12 (14) C8—C9—C10 118.44 (16)
C6—C1—Cl1 118.74 (14) C8—C9—H9 120.8
C1—C2—C3 118.36 (16) C10—C9—H9 120.8
C1—C2—H2 120.8 C9—C10—C11 121.84 (16)
C3—C2—H2 120.8 C9—C10—H10 119.1
C2—C3—C4 120.50 (16) C11—C10—H10 119.1
C2—C3—H3 119.8 C10—C11—C12 118.09 (16)
C4—C3—H3 119.8 C10—C11—C14 120.10 (16)
C3—C4—C5 120.19 (16) C12—C11—C14 121.81 (17)
C3—C4—C7 117.33 (15) C13—C12—C11 121.12 (17)
C5—C4—C7 122.48 (15) C13—C12—H12 119.4
C6—C5—C4 119.67 (16) C11—C12—H12 119.4
C6—C5—H5 120.2 C8—C13—C12 119.11 (16)
C4—C5—H5 120.2 C8—C13—H13 120.4
C1—C6—C5 119.14 (16) C12—C13—H13 120.4
C1—C6—H6 120.4 C11—C14—H14A 109.5
C5—C6—H6 120.4 C11—C14—H14B 109.5
O2—C7—O1 123.92 (15) H14A—C14—H14B 109.5
O2—C7—C4 124.41 (15) C11—C14—H14C 109.5
O1—C7—C4 111.66 (14) H14A—C14—H14C 109.5
C13—C8—C9 121.39 (16) H14B—C14—H14C 109.5
C6—C1—C2—C3 0.4 (3) C3—C4—C7—O1 179.72 (14)
Cl1—C1—C2—C3 −179.45 (13) C5—C4—C7—O1 −0.1 (2)
C1—C2—C3—C4 −0.2 (3) C7—O1—C8—C13 −134.88 (16)
C2—C3—C4—C5 −0.2 (3) C7—O1—C8—C9 50.6 (2)
C2—C3—C4—C7 −179.97 (15) C13—C8—C9—C10 0.8 (3)
C3—C4—C5—C6 0.3 (2) O1—C8—C9—C10 174.97 (14)
C7—C4—C5—C6 −179.89 (15) C8—C9—C10—C11 −1.1 (3)
C2—C1—C6—C5 −0.2 (3) C9—C10—C11—C12 0.6 (3)
Cl1—C1—C6—C5 179.59 (13) C9—C10—C11—C14 −179.67 (17)
C4—C5—C6—C1 −0.1 (3) C10—C11—C12—C13 0.2 (3)
C8—O1—C7—O2 7.9 (2) C14—C11—C12—C13 −179.55 (17)
C8—O1—C7—C4 −172.71 (14) C9—C8—C13—C12 0.0 (3)
C3—C4—C7—O2 −0.9 (3) O1—C8—C13—C12 −174.50 (15)
C5—C4—C7—O2 179.27 (17) C11—C12—C13—C8 −0.5 (3)

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BT2647).

References

  1. Adams, J. M. & Morsi, S. E. (1976). Acta Cryst. B32, 1345–1347.
  2. Farrugia, L. J. (1997). J. Appl. Cryst.30, 565.
  3. Gowda, B. T., Foro, S., Babitha, K. S. & Fuess, H. (2007a). Acta Cryst. E63, o3801.
  4. Gowda, B. T., Foro, S., Babitha, K. S. & Fuess, H. (2007b). Acta Cryst. E63, o3867.
  5. Gowda, B. T., Foro, S., Babitha, K. S. & Fuess, H. (2007c). Acta Cryst. E63, o3876.
  6. Gowda, B. T., Foro, S., Babitha, K. S. & Fuess, H. (2007d). Acta Cryst. E63, o3877.
  7. Gowda, B. T., Foro, S., Babitha, K. S. & Fuess, H. (2007e). Acta Cryst. E63, o4286.
  8. Gowda, B. T., Foro, S., Nayak, R. & Fuess, H. (2007a). Acta Cryst. E63, o3507.
  9. Gowda, B. T., Foro, S., Nayak, R. & Fuess, H. (2007b). Acta Cryst. E63, o3563.
  10. Nayak, R. & Gowda, B. T. (2007). Z. Naturforsch. Teil A, 62 In the press.
  11. Oxford Diffraction (2006). CrysAlis CCD and CrysAlis RED Oxford Diffraction Ltd, Abingdon, Oxfordshire, England.
  12. Sheldrick, G. M. (1997). SHELXS97 and SHELXL97 University of Göttingen, Germany.
  13. Spek, A. L. (2003). J. Appl. Cryst.36, 7–13.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536807062137/bt2647sup1.cif

e-64-00o88-sup1.cif (15.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536807062137/bt2647Isup2.hkl

e-64-00o88-Isup2.hkl (118.3KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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