Abstract
The molecule of the title compound, C11H13ClN2O3, is planar (r.m.s. deviation = 0.0587 Å for non-H atoms) and adopts a Z conformation about the C=N double bond. In the crystal, molecules are linked via an N—H⋯O hydrogen bond, forming zigzag chains propagating along [010]. These chains are consolidated by C—H⋯O hydrogen bonds.
Related literature
For closely related structures, see: Asiri et al. (2011a
▶,b
▶). For graph-set notation, see: Bernstein et al. (1995 ▶).
Experimental
Crystal data
C11H13ClN2O3
M r = 256.68
Monoclinic,
a = 4.7480 (2) Å
b = 9.9256 (4) Å
c = 13.3084 (4) Å
β = 91.468 (3)°
V = 626.98 (4) Å3
Z = 2
Cu Kα radiation
μ = 2.71 mm−1
T = 296 K
0.23 × 0.11 × 0.06 mm
Data collection
Agilent SuperNova (Dual, Cu at zero, Atlas) CCD diffractometer
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2012 ▶) T min = 0.860, T max = 1.000
3153 measured reflections
1824 independent reflections
1685 reflections with I > 2σ(I)
R int = 0.018
Refinement
R[F 2 > 2σ(F 2)] = 0.038
wR(F 2) = 0.109
S = 1.07
1824 reflections
159 parameters
1 restraint
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.16 e Å−3
Δρmin = −0.20 e Å−3
Absolute structure: Flack (1983 ▶), 466 Friedel pairs
Flack parameter: 0.01 (2)
Data collection: CrysAlis PRO (Agilent, 2012 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: PLATON (Spek, 2009 ▶); software used to prepare material for publication: WinGX (Farrugia, 2012 ▶).
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812044285/su2515sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812044285/su2515Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812044285/su2515Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N1—H1N⋯O2i | 0.97 (4) | 2.11 (4) | 3.053 (3) | 164 (3) |
| C6—H6⋯O2i | 0.93 | 2.59 | 3.368 (3) | 141 |
Symmetry code: (i)
.
Acknowledgments
We would like to thank the Deanship of Scientific Research at King Abdulaziz University for the support of this research via a Research Group Track Grant (No. 3-102/428).
supplementary crystallographic information
Comment
The present structure analysis is a continuation of our interest in related compounds already reported by our group, that is, 1-Chloro-1-[(4-methoxyphenyl)hydrazinylidene]propan-2-one (Asiri et al., 2011a) and 1-Chloro-1-[(4-methylphenyl)hydrazinylidene]propan-2-one (Asiri et al., 2011b).
In the title compound, Fig. 1, the methoxy aromatic ring (C1—C6) is oriented at a dihedral angle of 3.05 (2) ° with respect to the mean plane of the ester moiety (N1/N2/C7-Cl1; planar to within 0.0 \%A). The molecule adopts a Z conformation around the C7═N2 double bond.
In the crystal, N-H···O and C-H···O hydrogen bonds connect the molecules to form zigzag chains along the b axis, enclosing six membered R12(6) ring motifs (Bernstein et al., 1995) - see Table 1 and Fig. 2.
Experimental
The molecule was synthesised according to the literature procedure (Asiri et al., 2011a) and recrystallized from ethanol giving yellow needle-like crystals.
Refinement
The NH H atom was located in a difference Fourier map and refined with Uiso(H) = 1.2Ueq(N). The C-bound H-atoms were included in calculated positions and treated as riding atoms: C-H = 0.93, 0.96 and 0.97 Å for CH(aromatic), CH3, and CH2 H atoms, respectively, with Uiso(H) = k × Ueq(parent C-atom), where k = 1.5 for CH3 H atoms and = 1.2 for other H atoms.
Figures
Fig. 1.

A view of the molecular structure of the title molecule with the atom numbering. The displacement ellipsoids are drawn at the 50% probability level.
Fig. 2.
A partial view along the a axis of the crystal packing of the title compound. The N-H···O and C-H···O hydrogen bonds are shown as dashed lines - see Table 1 for details.
Crystal data
| C11H13ClN2O3 | F(000) = 268 |
| Mr = 256.68 | Dx = 1.360 Mg m−3 |
| Monoclinic, P21 | Cu Kα radiation, λ = 1.54184 Å |
| Hall symbol: P 2yb | Cell parameters from 2064 reflections |
| a = 4.7480 (2) Å | θ = 4.5–75.6° |
| b = 9.9256 (4) Å | µ = 2.71 mm−1 |
| c = 13.3084 (4) Å | T = 296 K |
| β = 91.468 (3)° | Needle, yellow |
| V = 626.98 (4) Å3 | 0.23 × 0.11 × 0.06 mm |
| Z = 2 |
Data collection
| Agilent SuperNova (Dual, Cu at zero, Atlas) CCD diffractometer | 1824 independent reflections |
| Radiation source: SuperNova (Cu) X-ray Source | 1685 reflections with I > 2σ(I) |
| Mirror monochromator | Rint = 0.018 |
| ω scans | θmax = 75.8°, θmin = 5.6° |
| Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2012) | h = −5→5 |
| Tmin = 0.860, Tmax = 1.000 | k = −12→9 |
| 3153 measured reflections | l = −16→16 |
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)] = 0.038 | H atoms treated by a mixture of independent and constrained refinement |
| wR(F2) = 0.109 | w = 1/[σ2(Fo2) + (0.0575P)2 + 0.0434P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.07 | (Δ/σ)max < 0.001 |
| 1824 reflections | Δρmax = 0.16 e Å−3 |
| 159 parameters | Δρmin = −0.20 e Å−3 |
| 1 restraint | Absolute structure: Flack (1983), 466 Friedel pairs |
| Primary atom site location: structure-invariant direct methods | Flack parameter: 0.01 (2) |
Special details
| 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)
| x | y | z | Uiso*/Ueq | ||
| Cl1 | 1.03853 (17) | 0.46169 (11) | 0.45757 (5) | 0.0873 (3) | |
| O1 | 0.1393 (5) | 0.2136 (3) | 0.96956 (16) | 0.0895 (7) | |
| O2 | 1.4090 (4) | 0.6817 (2) | 0.52714 (16) | 0.0785 (6) | |
| O3 | 1.2764 (5) | 0.6800 (2) | 0.68691 (15) | 0.0735 (6) | |
| N1 | 0.7239 (5) | 0.3882 (3) | 0.63734 (15) | 0.0607 (5) | |
| N2 | 0.9085 (4) | 0.4860 (2) | 0.64964 (14) | 0.0566 (5) | |
| C1 | 0.5738 (5) | 0.3420 (3) | 0.72120 (18) | 0.0542 (5) | |
| C2 | 0.6135 (6) | 0.4022 (3) | 0.81488 (19) | 0.0616 (6) | |
| H2 | 0.7405 | 0.4728 | 0.8235 | 0.074* | |
| C3 | 0.4620 (6) | 0.3557 (3) | 0.89470 (19) | 0.0675 (7) | |
| H3 | 0.4869 | 0.3960 | 0.9574 | 0.081* | |
| C4 | 0.2750 (6) | 0.2509 (3) | 0.8836 (2) | 0.0656 (7) | |
| C5 | 0.2349 (6) | 0.1908 (3) | 0.7907 (2) | 0.0666 (7) | |
| H5 | 0.1083 | 0.1199 | 0.7824 | 0.080* | |
| C6 | 0.3865 (6) | 0.2378 (3) | 0.7097 (2) | 0.0637 (7) | |
| H6 | 0.3604 | 0.1979 | 0.6469 | 0.076* | |
| C7 | 1.0590 (6) | 0.5288 (3) | 0.57810 (18) | 0.0584 (6) | |
| C8 | 1.2652 (6) | 0.6375 (3) | 0.59250 (18) | 0.0605 (6) | |
| C9 | 1.4822 (8) | 0.7834 (4) | 0.7110 (2) | 0.0894 (10) | |
| H9A | 1.6681 | 0.7533 | 0.6923 | 0.107* | |
| H9B | 1.4376 | 0.8647 | 0.6734 | 0.107* | |
| C10 | 1.4804 (13) | 0.8107 (5) | 0.8152 (3) | 0.1310 (18) | |
| H10A | 1.2976 | 0.8430 | 0.8329 | 0.197* | |
| H10B | 1.6195 | 0.8780 | 0.8315 | 0.197* | |
| H10C | 1.5228 | 0.7297 | 0.8520 | 0.197* | |
| C11 | −0.0364 (8) | 0.1011 (4) | 0.9655 (3) | 0.0903 (11) | |
| H11A | −0.1846 | 0.1157 | 0.9162 | 0.135* | |
| H11B | −0.1166 | 0.0869 | 1.0301 | 0.135* | |
| H11C | 0.0709 | 0.0233 | 0.9473 | 0.135* | |
| H1N | 0.712 (7) | 0.330 (5) | 0.579 (3) | 0.108* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cl1 | 0.1022 (6) | 0.1004 (6) | 0.0602 (4) | −0.0065 (5) | 0.0182 (3) | −0.0155 (4) |
| O1 | 0.0895 (14) | 0.112 (2) | 0.0679 (12) | −0.0237 (15) | 0.0142 (10) | 0.0084 (13) |
| O2 | 0.0887 (14) | 0.0810 (15) | 0.0666 (11) | −0.0067 (12) | 0.0164 (9) | 0.0181 (10) |
| O3 | 0.0847 (13) | 0.0763 (13) | 0.0597 (10) | −0.0197 (11) | 0.0073 (9) | 0.0004 (9) |
| N1 | 0.0667 (12) | 0.0627 (13) | 0.0528 (11) | −0.0039 (11) | 0.0032 (9) | −0.0050 (9) |
| N2 | 0.0595 (11) | 0.0586 (14) | 0.0518 (9) | 0.0038 (10) | 0.0020 (8) | 0.0034 (9) |
| C1 | 0.0548 (13) | 0.0542 (13) | 0.0537 (12) | 0.0056 (11) | 0.0003 (9) | −0.0011 (10) |
| C2 | 0.0642 (14) | 0.0615 (15) | 0.0591 (14) | −0.0054 (13) | 0.0007 (10) | −0.0026 (11) |
| C3 | 0.0701 (16) | 0.0773 (19) | 0.0551 (13) | −0.0018 (15) | 0.0021 (11) | −0.0052 (13) |
| C4 | 0.0605 (14) | 0.0745 (18) | 0.0619 (15) | 0.0016 (14) | 0.0031 (11) | 0.0094 (13) |
| C5 | 0.0634 (15) | 0.0655 (17) | 0.0708 (15) | −0.0077 (14) | −0.0009 (11) | 0.0018 (13) |
| C6 | 0.0685 (16) | 0.0640 (16) | 0.0583 (14) | −0.0046 (14) | −0.0035 (11) | −0.0065 (12) |
| C7 | 0.0618 (14) | 0.0601 (15) | 0.0533 (12) | 0.0101 (12) | 0.0053 (10) | 0.0017 (10) |
| C8 | 0.0687 (15) | 0.0577 (15) | 0.0554 (12) | 0.0069 (13) | 0.0042 (10) | 0.0079 (11) |
| C9 | 0.106 (3) | 0.083 (2) | 0.0788 (19) | −0.026 (2) | 0.0017 (17) | 0.0007 (17) |
| C10 | 0.191 (5) | 0.103 (3) | 0.098 (3) | −0.042 (4) | −0.014 (3) | −0.020 (3) |
| C11 | 0.081 (2) | 0.088 (3) | 0.103 (2) | −0.006 (2) | 0.0184 (18) | 0.020 (2) |
Geometric parameters (Å, º)
| Cl1—C7 | 1.737 (3) | C3—H3 | 0.9300 |
| O1—C4 | 1.378 (3) | C4—C5 | 1.381 (4) |
| O1—C11 | 1.394 (5) | C5—C6 | 1.393 (4) |
| O2—C8 | 1.202 (3) | C5—H5 | 0.9300 |
| O3—C8 | 1.325 (3) | C6—H6 | 0.9300 |
| O3—C9 | 1.447 (4) | C7—C8 | 1.466 (4) |
| N1—N2 | 1.315 (3) | C9—C10 | 1.414 (5) |
| N1—C1 | 1.416 (3) | C9—H9A | 0.9700 |
| N1—H1N | 0.97 (4) | C9—H9B | 0.9700 |
| N2—C7 | 1.277 (3) | C10—H10A | 0.9600 |
| C1—C6 | 1.370 (4) | C10—H10B | 0.9600 |
| C1—C2 | 1.391 (3) | C10—H10C | 0.9600 |
| C2—C3 | 1.378 (4) | C11—H11A | 0.9600 |
| C2—H2 | 0.9300 | C11—H11B | 0.9600 |
| C3—C4 | 1.373 (4) | C11—H11C | 0.9600 |
| C4—O1—C11 | 118.3 (3) | N2—C7—C8 | 122.1 (2) |
| C8—O3—C9 | 116.5 (2) | N2—C7—Cl1 | 122.8 (2) |
| N2—N1—C1 | 119.3 (2) | C8—C7—Cl1 | 115.10 (19) |
| N2—N1—H1N | 124 (2) | O2—C8—O3 | 124.1 (3) |
| C1—N1—H1N | 115 (2) | O2—C8—C7 | 124.3 (3) |
| C7—N2—N1 | 122.4 (2) | O3—C8—C7 | 111.6 (2) |
| C6—C1—C2 | 119.8 (2) | C10—C9—O3 | 109.4 (3) |
| C6—C1—N1 | 119.7 (2) | C10—C9—H9A | 109.8 |
| C2—C1—N1 | 120.5 (3) | O3—C9—H9A | 109.8 |
| C3—C2—C1 | 119.1 (3) | C10—C9—H9B | 109.8 |
| C3—C2—H2 | 120.5 | O3—C9—H9B | 109.8 |
| C1—C2—H2 | 120.5 | H9A—C9—H9B | 108.2 |
| C4—C3—C2 | 121.3 (2) | C9—C10—H10A | 109.5 |
| C4—C3—H3 | 119.4 | C9—C10—H10B | 109.5 |
| C2—C3—H3 | 119.4 | H10A—C10—H10B | 109.5 |
| C3—C4—O1 | 115.4 (3) | C9—C10—H10C | 109.5 |
| C3—C4—C5 | 119.9 (2) | H10A—C10—H10C | 109.5 |
| O1—C4—C5 | 124.8 (3) | H10B—C10—H10C | 109.5 |
| C4—C5—C6 | 119.1 (3) | O1—C11—H11A | 109.5 |
| C4—C5—H5 | 120.5 | O1—C11—H11B | 109.5 |
| C6—C5—H5 | 120.5 | H11A—C11—H11B | 109.5 |
| C1—C6—C5 | 120.9 (2) | O1—C11—H11C | 109.5 |
| C1—C6—H6 | 119.6 | H11A—C11—H11C | 109.5 |
| C5—C6—H6 | 119.6 | H11B—C11—H11C | 109.5 |
| C1—N1—N2—C7 | 177.1 (2) | C2—C1—C6—C5 | −0.1 (4) |
| N2—N1—C1—C6 | −178.3 (2) | N1—C1—C6—C5 | −179.6 (3) |
| N2—N1—C1—C2 | 2.2 (4) | C4—C5—C6—C1 | 0.1 (4) |
| C6—C1—C2—C3 | −0.2 (4) | N1—N2—C7—C8 | −179.7 (2) |
| N1—C1—C2—C3 | 179.4 (3) | N1—N2—C7—Cl1 | −0.6 (4) |
| C1—C2—C3—C4 | 0.5 (5) | C9—O3—C8—O2 | −1.8 (4) |
| C2—C3—C4—O1 | 179.4 (3) | C9—O3—C8—C7 | 177.3 (3) |
| C2—C3—C4—C5 | −0.4 (5) | N2—C7—C8—O2 | −179.3 (3) |
| C11—O1—C4—C3 | −175.0 (3) | Cl1—C7—C8—O2 | 1.5 (4) |
| C11—O1—C4—C5 | 4.9 (5) | N2—C7—C8—O3 | 1.6 (4) |
| C3—C4—C5—C6 | 0.1 (5) | Cl1—C7—C8—O3 | −177.6 (2) |
| O1—C4—C5—C6 | −179.7 (3) | C8—O3—C9—C10 | −176.1 (4) |
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1N···O2i | 0.97 (4) | 2.11 (4) | 3.053 (3) | 164 (3) |
| C6—H6···O2i | 0.93 | 2.59 | 3.368 (3) | 141 |
Symmetry code: (i) −x+2, y−1/2, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SU2515).
References
- Agilent (2012). CrysAlis PRO Agilent Technologies, Yarnton, Oxfordshire, England.
- Asiri, A. M., Al-Youbi, A. O., Zayed, M. E. M. & Ng, S. W. (2011a). Acta Cryst. E67, o1961. [DOI] [PMC free article] [PubMed]
- Asiri, A. M., Al-Youbi, A. O., Zayed, M. E. M. & Ng, S. W. (2011b). Acta Cryst. E67, o1964. [DOI] [PMC free article] [PubMed]
- Bernstein, J., Davis, R. E., Shimoni, L. & Chang, N.-L. (1995). Angew. Chem. Int. Ed. Engl. 34, 1555-1573.
- Farrugia, L. J. (2012). J. Appl. Cryst. 45, 849–854.
- Flack, H. D. (1983). Acta Cryst. A39, 876–881.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Spek, A. L. (2009). Acta Cryst. D65, 148–155. [DOI] [PMC free article] [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/S1600536812044285/su2515sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812044285/su2515Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812044285/su2515Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

