organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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ISSN: 2056-9890

Di­ethyl 4,4′-(ethane-1,2-diyldi­­oxy)dibenzoate

aSchool of Chemistry and Chemical Engineering, Guangxi University, Guangxi 530004, People's Republic of China
*Correspondence e-mail: mzmz2009@sohu.com

(Received 25 April 2011; accepted 2 June 2011; online 11 June 2011)

The title compound, C20H22O6, was obtained by the reaction of ethyl 4-hy­droxy­benzoate with 1,2-dichloro­ethane in dimethyl­formamide. The mol­ecule lies around the crystallographic inversion center at (0,0,0), with the asymmetric unit consisting of one half of the mol­ecule. The two ethyl groups are in trans positions. The ethyl, carboxyl, aryl and O—CH2 groups are coplanar with an r.m.s. deviation of 0.0208 (9) Å. The whole mol­ecule is planar with an r.m.s. deviation of 0.0238 (9) Å for the 19 atoms used in the calculation and 0.0071 (9) Å for the two aryl groups in the mol­ecule. A weak inter­molecular C—H⋯O hydrogen bond and a C—H⋯π inter­action help to consolidate the three-dimensional network.

Related literature

For the synthesis and structures of diesters, see Hou & Kan (2007[Hou, L.-M. & Kan, Y.-H. (2007). Acta Cryst. E63, o2157-o2158.]); Tashiro et al. (1990[Tashiro, K., Hou, J., Kobayashi, M. & Inoue, T. (1990). J. Am. Chem. Soc. 112, 8273-8279.]); Zhang et al. (2007[Zhang, L.-P., Jia, Z.-F., Wei, G.-H. & Liu, Y.-Y. (2007). Acta Cryst. E63, o4674.]). For the properties and applications of diesters, see: Chen & Liu (2002[Chen, X. & Liu, G. (2002). Chem. Eur. J. 8, 4811-4817.]). For the synthesis of the title compound, see: Ma & Liu (2002[Ma, Z. & Liu, S.-X. (2002). Chin. J. Struct. Chem. 21, 533-537.]); Ma & Cao (2011[Ma, Z. & Cao, Y. (2011). Acta Cryst. E67, o1503.]). For standard bond lengths, see: Allen et al. (1987[Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans 2, pp. S1-19.]).

[Scheme 1]

Experimental

Crystal data
  • C20H22O6

  • Mr = 358.38

  • Monoclinic, P 21 /c

  • a = 4.8504 (10) Å

  • b = 15.847 (3) Å

  • c = 12.0159 (19) Å

  • β = 104.250 (8)°

  • V = 895.2 (3) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.10 mm−1

  • T = 298 K

  • 0.49 × 0.35 × 0.22 mm

Data collection
  • Bruker SMART CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996[Sheldrick, G. M. (1996). SADABS. University of Göttingen, Germany.]) Tmin = 0.960, Tmax = 0.979

  • 8592 measured reflections

  • 1980 independent reflections

  • 1713 reflections with I > 2σ(I)

  • Rint = 0.032

Refinement
  • R[F2 > 2σ(F2)] = 0.039

  • wR(F2) = 0.130

  • S = 1.02

  • 1980 reflections

  • 119 parameters

  • H-atom parameters constrained

  • Δρmax = 0.34 e Å−3

  • Δρmin = −0.34 e Å−3

Table 1
Hydrogen-bond geometry (Å, °)

Cg is the centroid of the C4–C9 ring.

D—H⋯A D—H H⋯A DA D—H⋯A
C6—H6A⋯O2i 0.93 2.47 3.2784 (16) 146
C10—H10BCgii 0.97 2.65 3.741 (2) 143
Symmetry codes: (i) [x, -y+{\script{1\over 2}}, z-{\script{1\over 2}}]; (ii) x+1, y, z.

Data collection: SMART (Bruker, 2001[Bruker (2001). SMART. Bruker AXS Inc., Madison, Wisconsin, USA.]); cell refinement: SAINT (Bruker, 2002[Bruker (2002). SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.]); data reduction: SAINT; 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: SHELXTL (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); software used to prepare material for publication: SHELXTL.

Supporting information


Comment top

There has been, in recent years, a considerable interest in the study of esters (Hou & Kan, 2007; Tashiro et al., 1990; Zhang et al., 2007), since these compounds are commodity chemicals used as intermediates in the manufacture of acids and to produce many important industrial products. Hence, our current work aims to prepare esters to produce acids and investigate their coordination behaviors with metal ions and study their applications in many fields (Chen & Liu, 2002). Herein, we report a new diester which was obtained by reaction of ethyl 4-hydroxybenzoate with 1,2-dichloroethane in DMF and its structure was confirmed by elemental analysis, IR, NMR spectra and X-ray crystal analysis.

The structure consists of a neutral molecular unit (Fig. 1).The molecule lies on a crystallographic inversion center at (0, 0, 0), thus leading to one half of the molecule being present per asymmetric unit. All bond lengths and angles are within normal ranges (Allen et al., 1987). The ethyl, aryl, carboxyl and the O—CH2 groups of one half molecule are coplanar to form one plane with an r.m.s. deviation of 0.0208 (9) Å. By symmetry, the whole molecule is coplanar with an r.m.s deviation of 0.0238 (9) Å for 19 atoms being used for calculation and 0.0071 (9) Å for the two aryl groups at the molecule. Because of the symmetry of the inversion center, the two ethyl groups at the molecule are in a trans position. One weak hydrogen bond between one hydrogen atom and the oxygen atom of a neighboring molecule is present in the structure: H6A on C6 and O2ii [symmetry code: (ii) x, -y+1/2, z-1/2] (Table 1). The molecules display intermolecular C—H···π interactions between a –CH2-(C10) and a neighboring aryl group [H..Cg 2.647 Å, Cg is the centroid of the six membered ring of C4iii-C9iii, symmetry code: (iii) x+1, y, z].

Related literature top

For the synthesis and structures of diesters, see Hou & Kan (2007); Tashiro et al. (1990); Zhang et al. (2007). For the properties and applications of diesters, see: Chen & Liu (2002). For the synthesis of the title compound, see: Ma & Liu (2002); Ma & Cao (2011). For standard bond lengths, see: Allen et al. (1987).

Experimental top

The title compound was obtained by the reaction of ethyl 4-hydroxybenzoate with 1,2-dichloroethane in N,N'-dimethylformamide (DMF) according to a reported procedure (Ma & Liu, 2002; Ma & Cao, 2011). In a 100 cm3 flask fitted with a funnel, ethyl 4-hydroxybenzoate (8.3 g, 50 mM) and potassium carbonate were mixed in 50 cm3 of DMF. To this solution was added dropwise a stoichiometric quantity of 1,2-dichloroethane (2.5 g, 25 mM) dissolved in 20 cm3 of DMF for a period of an hour with stirring. The mixture was then stirred for 24 h at 353 K. The solution was concentrated under reduced pressure and the white solid formed by adding a large quantity of water (200 cm3) was filtered off and recrystallized from ethanol and decolored with activated carbon. A colorless solid was obtained (yield 30 %, m.p: 388–390 K). Slow evaporation of a solution of the title compound in ethanol and dichloromethane (1:1) led to the formation of colorless crystals, which were suitable for X-ray characterization. Anal. Calcd. for [C20H22O6] (%): C, 67.03; H, 6.19; found: C, 66.75; H, 6.46; IR(KBr), (cm-1): 1711, (C=O), 1605, 1509, 1477 (C=C of aryl), 1280, 1252, 1165, 1105 (CH2—O—CH2), 1045, 1027, 870-715, (Ar—H). 1H NMR (CDCl3): 7.97 (d, 4H, J = 8.8 Hz, aryl, c), 6.94 (d, 4H, J = 8.8 Hz, aryl, d), 4.34 (d, 4H, OCH2CH2, f), 4.31 (d, 4H, COOCH2, g), 1.35 (t, 6H, –CH3, h). 13C NMR: 166.4 (–COO, a), 162.4 (aryl, b), 131.8 (aryl, c), 123.7 (aryl, e), 114.4 (aryl, d), 66.6 (CH2CH2, f), 60.9 (CH2CH2, g), 14.6 (–CH3, h). (see Figure 3 for the NMR atom number assignment).

Refinement top

All H atoms were positioned geometrically and refined using a riding model with C—H = 0.93 - 0.97 Å and with Uiso(H) = 1.2 times Ueq(C).

Computing details top

Data collection: SMART (Bruker, 2001); cell refinement: SAINT (Bruker, 2002); data reduction: SAINT (Bruker, 2002); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound with the atom numbering scheme. Displacement ellipsoids are drawn at the 50% probability level. H atoms are presented as small spheres of arbitrary radius. [Symmetry code: (i) -x, -y, -z]
[Figure 2] Fig. 2. A view of the crystal packing along the a axis. The thin dashed lines are used to show the hydrogen bonds. The thick dashed line is used to show the intermolecular CH-π interactions of –CH2-(C6) and the neighboring aryl groups, from their H atoms to the centroids of the rings of the aryl groups.
[Figure 3] Fig. 3. An additional scheme with the numbering scheme used for the NMR spectra.
Diethyl 4,4'-(ethane-1,2-diyldioxy)dibenzoate top
Crystal data top
C20H22O6F(000) = 380
Mr = 358.38Dx = 1.330 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 8592 reflections
a = 4.8504 (10) Åθ = 2.2–27.2°
b = 15.847 (3) ŵ = 0.10 mm1
c = 12.0159 (19) ÅT = 298 K
β = 104.250 (8)°Prism, colorless
V = 895.2 (3) Å30.49 × 0.35 × 0.22 mm
Z = 2
Data collection top
Bruker SMART CCD area-detector
diffractometer
1980 independent reflections
Radiation source: fine-focus sealed tube1713 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.032
Detector resolution: 0 pixels mm-1θmax = 27.2°, θmin = 2.2°
ϕ and ω scansh = 65
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
k = 2020
Tmin = 0.960, Tmax = 0.979l = 1514
8592 measured reflections
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)] = 0.039Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.130H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0876P)2 + 0.1852P]
where P = (Fo2 + 2Fc2)/3
1980 reflections(Δ/σ)max < 0.001
119 parametersΔρmax = 0.34 e Å3
0 restraintsΔρmin = 0.34 e Å3
Crystal data top
C20H22O6V = 895.2 (3) Å3
Mr = 358.38Z = 2
Monoclinic, P21/cMo Kα radiation
a = 4.8504 (10) ŵ = 0.10 mm1
b = 15.847 (3) ÅT = 298 K
c = 12.0159 (19) Å0.49 × 0.35 × 0.22 mm
β = 104.250 (8)°
Data collection top
Bruker SMART CCD area-detector
diffractometer
1980 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
1713 reflections with I > 2σ(I)
Tmin = 0.960, Tmax = 0.979Rint = 0.032
8592 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0390 restraints
wR(F2) = 0.130H-atom parameters constrained
S = 1.02Δρmax = 0.34 e Å3
1980 reflectionsΔρmin = 0.34 e Å3
119 parameters
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 > 2sigma(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
O11.19587 (17)0.35479 (5)0.09590 (7)0.0219 (2)
O20.9567 (2)0.37413 (6)0.08774 (8)0.0313 (3)
O30.30202 (17)0.06258 (5)0.06554 (7)0.0209 (2)
C11.5949 (3)0.43801 (8)0.19241 (11)0.0302 (3)
H1A1.71990.48330.18430.045*
H1B1.70260.38690.21060.045*
H1C1.50460.45100.25300.045*
C21.3723 (3)0.42675 (7)0.08179 (11)0.0234 (3)
H2A1.25660.47720.06430.028*
H2B1.46170.41640.01920.028*
C30.9916 (2)0.33543 (7)0.00155 (10)0.0199 (3)
C40.8119 (2)0.26316 (7)0.01966 (10)0.0188 (3)
C50.8593 (2)0.21922 (7)0.12413 (10)0.0199 (3)
H5A1.00970.23460.18510.024*
C60.6832 (2)0.15314 (7)0.13669 (10)0.0196 (3)
H6A0.71450.12430.20600.024*
C70.4580 (2)0.12990 (7)0.04481 (10)0.0174 (3)
C80.4063 (2)0.17353 (7)0.05940 (10)0.0197 (3)
H8A0.25490.15840.12010.024*
C90.5851 (2)0.23998 (7)0.07089 (10)0.0197 (3)
H9A0.55260.26930.14000.024*
C100.0671 (2)0.03624 (7)0.02485 (9)0.0182 (3)
H10A0.13170.01790.09120.022*
H10B0.06780.08200.04780.022*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0219 (4)0.0201 (4)0.0220 (4)0.0073 (3)0.0025 (3)0.0001 (3)
O20.0341 (5)0.0299 (5)0.0257 (5)0.0111 (4)0.0005 (4)0.0075 (4)
O30.0185 (4)0.0204 (4)0.0212 (4)0.0056 (3)0.0002 (3)0.0036 (3)
C10.0313 (7)0.0299 (7)0.0275 (7)0.0108 (5)0.0034 (5)0.0042 (5)
C20.0235 (6)0.0183 (5)0.0281 (6)0.0065 (4)0.0058 (5)0.0008 (4)
C30.0199 (6)0.0182 (5)0.0209 (6)0.0009 (4)0.0040 (4)0.0011 (4)
C40.0188 (6)0.0169 (5)0.0210 (6)0.0006 (4)0.0053 (4)0.0014 (4)
C50.0198 (6)0.0192 (5)0.0194 (6)0.0013 (4)0.0025 (4)0.0023 (4)
C60.0217 (6)0.0190 (5)0.0176 (5)0.0001 (4)0.0036 (4)0.0007 (4)
C70.0163 (5)0.0154 (5)0.0210 (6)0.0002 (4)0.0053 (4)0.0007 (4)
C80.0176 (5)0.0200 (5)0.0200 (6)0.0009 (4)0.0019 (4)0.0004 (4)
C90.0208 (6)0.0186 (5)0.0191 (6)0.0001 (4)0.0039 (4)0.0022 (4)
C100.0158 (5)0.0176 (5)0.0200 (5)0.0017 (4)0.0021 (4)0.0008 (4)
Geometric parameters (Å, º) top
O1—C31.3446 (14)C4—C51.4040 (16)
O1—C21.4604 (13)C5—C61.3829 (15)
O2—C31.2109 (15)C5—H5A0.9300
O3—C71.3659 (13)C6—C71.3977 (16)
O3—C101.4294 (13)C6—H6A0.9300
C1—C21.5027 (18)C7—C81.3978 (16)
C1—H1A0.9600C8—C91.3925 (16)
C1—H1B0.9600C8—H8A0.9300
C1—H1C0.9600C9—H9A0.9300
C2—H2A0.9700C10—C10i1.513 (2)
C2—H2B0.9700C10—H10A0.9700
C3—C41.4874 (15)C10—H10B0.9700
C4—C91.3928 (16)
C3—O1—C2114.29 (9)C6—C5—H5A119.9
C7—O3—C10117.60 (8)C4—C5—H5A119.9
C2—C1—H1A109.5C5—C6—C7119.79 (10)
C2—C1—H1B109.5C5—C6—H6A120.1
H1A—C1—H1B109.5C7—C6—H6A120.1
C2—C1—H1C109.5O3—C7—C6114.96 (10)
H1A—C1—H1C109.5O3—C7—C8124.36 (10)
H1B—C1—H1C109.5C6—C7—C8120.68 (10)
O1—C2—C1107.71 (10)C9—C8—C7118.94 (11)
O1—C2—H2A110.2C9—C8—H8A120.5
C1—C2—H2A110.2C7—C8—H8A120.5
O1—C2—H2B110.2C8—C9—C4120.89 (10)
C1—C2—H2B110.2C8—C9—H9A119.6
H2A—C2—H2B108.5C4—C9—H9A119.6
O2—C3—O1123.03 (10)O3—C10—C10i105.17 (11)
O2—C3—C4124.07 (11)O3—C10—H10A110.7
O1—C3—C4112.89 (10)C10i—C10—H10A110.7
C9—C4—C5119.45 (10)O3—C10—H10B110.7
C9—C4—C3117.87 (10)C10i—C10—H10B110.7
C5—C4—C3122.68 (11)H10A—C10—H10B108.8
C6—C5—C4120.23 (11)
C3—O1—C2—C1177.91 (10)C10—O3—C7—C6179.46 (9)
C2—O1—C3—O20.12 (16)C10—O3—C7—C81.26 (16)
C2—O1—C3—C4178.70 (9)C5—C6—C7—O3178.44 (9)
O2—C3—C4—C91.66 (17)C5—C6—C7—C80.88 (16)
O1—C3—C4—C9177.15 (9)O3—C7—C8—C9178.42 (10)
O2—C3—C4—C5179.57 (11)C6—C7—C8—C90.83 (16)
O1—C3—C4—C51.62 (16)C7—C8—C9—C40.16 (16)
C9—C4—C5—C60.41 (16)C5—C4—C9—C80.45 (16)
C3—C4—C5—C6179.16 (10)C3—C4—C9—C8179.26 (10)
C4—C5—C6—C70.25 (16)C7—O3—C10—C10i178.04 (10)
Symmetry code: (i) x, y, z.
Hydrogen-bond geometry (Å, º) top
Cg is the centroid of the C4–C9 ring.
D—H···AD—HH···AD···AD—H···A
C6—H6A···O2ii0.932.473.2784 (16)146
C10—H10B···Cgiii0.972.653.741 (2)143
Symmetry codes: (ii) x, y+1/2, z1/2; (iii) x+1, y, z.

Experimental details

Crystal data
Chemical formulaC20H22O6
Mr358.38
Crystal system, space groupMonoclinic, P21/c
Temperature (K)298
a, b, c (Å)4.8504 (10), 15.847 (3), 12.0159 (19)
β (°) 104.250 (8)
V3)895.2 (3)
Z2
Radiation typeMo Kα
µ (mm1)0.10
Crystal size (mm)0.49 × 0.35 × 0.22
Data collection
DiffractometerBruker SMART CCD area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.960, 0.979
No. of measured, independent and
observed [I > 2σ(I)] reflections
8592, 1980, 1713
Rint0.032
(sin θ/λ)max1)0.644
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.039, 0.130, 1.02
No. of reflections1980
No. of parameters119
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.34, 0.34

Computer programs: SMART (Bruker, 2001), SAINT (Bruker, 2002), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).

Hydrogen-bond geometry (Å, º) top
Cg is the centroid of the C4–C9 ring.
D—H···AD—HH···AD···AD—H···A
C6—H6A···O2i0.932.473.2784 (16)145.8
C10—H10B···Cgii0.972.653.741 (2)143
Symmetry codes: (i) x, y+1/2, z1/2; (ii) x+1, y, z.
 

Acknowledgements

The authors are grateful for financial support from the Scientific Fund of Guangxi University (grant No. X061144).

References

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