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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Apr 25;68(Pt 5):o1534. doi: 10.1107/S1600536812017242

Ethyl 2-(4-nitro­phen­oxy)acetate

Su-Wen Sun a,*
PMCID: PMC3344636  PMID: 22590398

Abstract

In the title mol­ecule, C10H11NO5, the methyl C atom deviates by 0.830 (6) Å from the mean plane of the remaining non-H atoms. In the crystal, weak C—H⋯O hydrogen bonds link the mol­ecules into layers parallel to the bc plane.

Related literature  

For the structure of tert-butyl 2-(4-nitro­phen­oxy)acetate, see: Ali et al. (2011). For general background to ferroelectric organics, see: Fu et al. (2009); Ye et al. (2006).graphic file with name e-68-o1534-scheme1.jpg

Experimental  

Crystal data  

  • C10H11NO5

  • M r = 225.20

  • Monoclinic, Inline graphic

  • a = 5.3848 (11) Å

  • b = 8.4482 (17) Å

  • c = 24.238 (5) Å

  • β = 92.59 (3)°

  • V = 1101.5 (4) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.11 mm−1

  • T = 293 K

  • 0.3 × 0.3 × 0.2 mm

Data collection  

  • Rigaku Mercury CCD diffractometer

  • Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) T min = 0.968, T max = 0.978

  • 9279 measured reflections

  • 2169 independent reflections

  • 1157 reflections with I > 2σ(I)

  • R int = 0.089

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.068

  • wR(F 2) = 0.156

  • S = 1.01

  • 2169 reflections

  • 146 parameters

  • H-atom parameters constrained

  • Δρmax = 0.20 e Å−3

  • Δρmin = −0.21 e Å−3

Data collection: CrystalClear (Rigaku, 2005); cell refinement: CrystalClear; data reduction: CrystalClear; 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: SHELXL97.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812017242/cv5259sup1.cif

e-68-o1534-sup1.cif (14.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812017242/cv5259Isup2.hkl

e-68-o1534-Isup2.hkl (106.7KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812017242/cv5259Isup3.cml

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

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
C2—H2A⋯O4i 0.93 2.53 3.177 (4) 127
C10—H10B⋯O1ii 0.96 2.58 3.513 (6) 164

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Acknowledgments

The author is grateful to the starter fund of Southeast University for financial support to buy the X-ray diffractometer.

supplementary crystallographic information

Comment

The title compound, (I), has been obtain during the search for new organic compounds which demonstrate ferroelectric phase changes (Fu et al., 2009; Ye et al., 2006). Though the measured dielectric constant of (I) showed no dielectric disuniformity in the range 120–385 K (mp.393–402 K), herewith we present its crystal structure.

In (I) (Fig. 1), all bond lengths and angles are normal and correspond to those observed in tert-butyl 2-(4-nitrophenoxy)acetate (Ali et al., 2011). Atom C10 deviates at 0.830 (6) Å from the mean plane of the rest non-H atoms.Weak intermolecular C—H···O hydrogen bonds (Table 1) link the molecules into layers parallel to bc plane.

Experimental

4-Nitro-phenol (7 g) and 1-Bromo-butan-2-one (8.5 g) were dissolved in acetone, kalium carbonicum (7.5 g) was added to the mixture. Then the mixture was heated and refluxed by mechanical stirring at 70°C. Yellow solid was filtered off. This solid was dissolved in ethanol and single crystals suitable for X-ray structure analysis were obtained by the slow evaporation of the above solution after 3 days in air.

Refinement

All H atoms were placed in calculated positions (N—H = 0.89 Å; C—H = 0.93 Å for Csp2 atoms and C—H = 0.96 Å and 0.97 Å for Csp3 atoms), assigned fixed Uiso values [Uiso = 1.2Ueq(Csp2) and 1.5Ueq(Csp3,N)] and allowed to ride.

Figures

Fig. 1.

Fig. 1.

The molecular structure of (I) showing the atomic numbering and 40% probability displacement ellipsoids.

Crystal data

C10H11NO5 F(000) = 472
Mr = 225.20 Dx = 1.358 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 3450 reflections
a = 5.3848 (11) Å θ = 3.4–26.0°
b = 8.4482 (17) Å µ = 0.11 mm1
c = 24.238 (5) Å T = 293 K
β = 92.59 (3)° Block, colourless
V = 1101.5 (4) Å3 0.3 × 0.3 × 0.2 mm
Z = 4

Data collection

Rigaku Mercury CCD diffractometer 2169 independent reflections
Radiation source: fine-focus sealed tube 1157 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.089
ω scans θmax = 26.0°, θmin = 3.4°
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) h = −6→6
Tmin = 0.968, Tmax = 0.978 k = −10→10
9279 measured reflections l = −29→29

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)] = 0.068 H-atom parameters constrained
wR(F2) = 0.156 w = 1/[σ2(Fo2) + (0.05P)2 + 0.35P] where P = (Fo2 + 2Fc2)/3
S = 1.01 (Δ/σ)max < 0.001
2169 reflections Δρmax = 0.20 e Å3
146 parameters Δρmin = −0.21 e Å3
0 restraints Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.011 (2)

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
O3 0.2402 (3) 0.9062 (2) 0.43476 (7) 0.0593 (5)
C4 0.3764 (4) 0.8226 (3) 0.47348 (10) 0.0502 (6)
C3 0.2863 (5) 0.8248 (3) 0.52630 (10) 0.0559 (7)
H3A 0.1438 0.8824 0.5331 0.067*
C1 0.6184 (5) 0.6596 (3) 0.55727 (11) 0.0540 (7)
C7 0.3224 (5) 0.9043 (3) 0.38008 (10) 0.0598 (7)
H7A 0.3228 0.7968 0.3661 0.072*
H7B 0.4902 0.9458 0.3794 0.072*
C6 0.7118 (5) 0.6582 (3) 0.50557 (11) 0.0600 (7)
H6A 0.8565 0.6024 0.4992 0.072*
O5 0.2362 (4) 1.0156 (3) 0.29508 (8) 0.0930 (8)
C5 0.5909 (4) 0.7396 (3) 0.46316 (11) 0.0568 (7)
H5A 0.6527 0.7389 0.4279 0.068*
N1 0.7460 (5) 0.5687 (3) 0.60109 (11) 0.0713 (7)
C2 0.4062 (5) 0.7424 (3) 0.56848 (11) 0.0588 (7)
H2A 0.3454 0.7424 0.6038 0.071*
O1 0.6650 (5) 0.5737 (3) 0.64727 (10) 0.1141 (10)
O2 0.9260 (4) 0.4885 (3) 0.59049 (9) 0.0938 (8)
C8 0.1488 (5) 1.0048 (4) 0.34495 (11) 0.0640 (8)
O4 −0.0361 (4) 1.0635 (3) 0.35870 (9) 0.1103 (10)
C9 0.0983 (7) 1.1139 (6) 0.25442 (15) 0.1140 (14)
H9A −0.0259 1.0504 0.2344 0.137*
H9B 0.0140 1.1987 0.2730 0.137*
C10 0.2659 (8) 1.1779 (7) 0.21723 (18) 0.157 (2)
H10A 0.1762 1.2415 0.1902 0.235*
H10B 0.3491 1.0935 0.1991 0.235*
H10C 0.3863 1.2424 0.2371 0.235*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O3 0.0581 (11) 0.0663 (12) 0.0541 (11) 0.0116 (9) 0.0075 (8) 0.0024 (9)
C4 0.0496 (15) 0.0462 (15) 0.0547 (15) −0.0030 (12) 0.0012 (12) −0.0033 (13)
C3 0.0522 (15) 0.0567 (17) 0.0594 (16) −0.0004 (13) 0.0083 (12) −0.0025 (14)
C1 0.0535 (16) 0.0467 (15) 0.0612 (17) −0.0028 (13) −0.0046 (13) 0.0025 (14)
C7 0.0612 (16) 0.0655 (18) 0.0534 (16) 0.0049 (14) 0.0104 (13) 0.0001 (14)
C6 0.0551 (16) 0.0554 (17) 0.0694 (18) 0.0060 (13) 0.0020 (14) −0.0043 (16)
O5 0.0837 (14) 0.130 (2) 0.0668 (13) 0.0279 (14) 0.0152 (11) 0.0294 (14)
C5 0.0539 (16) 0.0596 (17) 0.0574 (15) 0.0025 (13) 0.0079 (12) −0.0056 (14)
N1 0.0725 (17) 0.0681 (17) 0.0725 (18) −0.0037 (14) −0.0054 (14) 0.0084 (15)
C2 0.0636 (17) 0.0562 (17) 0.0568 (16) −0.0076 (14) 0.0050 (13) 0.0006 (14)
O1 0.1161 (19) 0.153 (3) 0.0734 (16) 0.0334 (17) 0.0087 (14) 0.0313 (17)
O2 0.0892 (16) 0.0956 (17) 0.0954 (17) 0.0293 (14) −0.0086 (13) 0.0132 (14)
C8 0.0609 (17) 0.076 (2) 0.0554 (16) 0.0006 (16) 0.0055 (14) 0.0000 (15)
O4 0.0937 (17) 0.161 (3) 0.0771 (15) 0.0615 (17) 0.0125 (13) 0.0127 (15)
C9 0.101 (3) 0.160 (4) 0.080 (2) 0.023 (3) −0.002 (2) 0.043 (3)
C10 0.149 (4) 0.196 (5) 0.129 (4) 0.053 (4) 0.043 (3) 0.081 (4)

Geometric parameters (Å, º)

O3—C4 1.362 (3) O5—C8 1.320 (3)
O3—C7 1.416 (3) O5—C9 1.465 (4)
C4—C5 1.384 (3) C5—H5A 0.9300
C4—C3 1.390 (3) N1—O2 1.220 (3)
C3—C2 1.374 (3) N1—O1 1.220 (3)
C3—H3A 0.9300 C2—H2A 0.9300
C1—C6 1.371 (3) C8—O4 1.174 (3)
C1—C2 1.377 (3) C9—C10 1.412 (5)
C1—N1 1.458 (3) C9—H9A 0.9700
C7—C8 1.499 (4) C9—H9B 0.9700
C7—H7A 0.9700 C10—H10A 0.9600
C7—H7B 0.9700 C10—H10B 0.9600
C6—C5 1.376 (3) C10—H10C 0.9600
C6—H6A 0.9300
C4—O3—C7 117.25 (19) C4—C5—H5A 120.4
O3—C4—C5 124.5 (2) O2—N1—O1 122.2 (3)
O3—C4—C3 115.4 (2) O2—N1—C1 119.5 (3)
C5—C4—C3 120.1 (2) O1—N1—C1 118.3 (3)
C2—C3—C4 120.5 (2) C3—C2—C1 118.5 (2)
C2—C3—H3A 119.8 C3—C2—H2A 120.8
C4—C3—H3A 119.8 C1—C2—H2A 120.8
C6—C1—C2 121.8 (2) O4—C8—O5 125.0 (3)
C6—C1—N1 118.8 (2) O4—C8—C7 126.4 (3)
C2—C1—N1 119.5 (2) O5—C8—C7 108.7 (2)
O3—C7—C8 108.2 (2) C10—C9—O5 109.1 (3)
O3—C7—H7A 110.1 C10—C9—H9A 109.9
C8—C7—H7A 110.1 O5—C9—H9A 109.9
O3—C7—H7B 110.1 C10—C9—H9B 109.9
C8—C7—H7B 110.1 O5—C9—H9B 109.9
H7A—C7—H7B 108.4 H9A—C9—H9B 108.3
C1—C6—C5 119.8 (2) C9—C10—H10A 109.5
C1—C6—H6A 120.1 C9—C10—H10B 109.5
C5—C6—H6A 120.1 H10A—C10—H10B 109.5
C8—O5—C9 117.7 (3) C9—C10—H10C 109.5
C6—C5—C4 119.3 (2) H10A—C10—H10C 109.5
C6—C5—H5A 120.4 H10B—C10—H10C 109.5

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
C2—H2A···O4i 0.93 2.53 3.177 (4) 127
C10—H10B···O1ii 0.96 2.58 3.513 (6) 164

Symmetry codes: (i) −x, −y+2, −z+1; (ii) x, −y+3/2, z−1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: CV5259).

References

  1. Ali, Q., Anis, I., Raza Shah, M. & Ng, S. W. (2011). Acta Cryst. E67, o532. [DOI] [PMC free article] [PubMed]
  2. Fu, D.-W., Ge, J.-Z., Dai, J., Ye, H.-Y. & Qu, Z.-R. (2009). Inorg. Chem. Commun. 12, 994–997.
  3. Rigaku (2005). CrystalClear Rigaku Corporation, Tokyo, Japan.
  4. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  5. Ye, Q., Song, Y.-M., Wang, G.-X., Chen, K. & Fu, D.-W. (2006). J. Am. Chem. Soc. 128, 6554–6555. [DOI] [PubMed]

Associated Data

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

Supplementary Materials

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812017242/cv5259sup1.cif

e-68-o1534-sup1.cif (14.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812017242/cv5259Isup2.hkl

e-68-o1534-Isup2.hkl (106.7KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812017242/cv5259Isup3.cml

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


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