organic compounds
(E)-(2,4-Dichlorobenzylidene)amino cyclopropanecarboxylate
aCollege of Chemistry and Chemical Engineering, Beifang University of Nationalities, Yinchuan 750021, People's Republic of China
*Correspondence e-mail: aseonliu@gmail.com
In the title compound C11H9Cl2NO2, the dihedral angle between the benzene and cyclopropane ring planes is 89.95 (13)°. The carbonyl–oxime grouping is almost coplanar with the benzene ring [dihedral angle = 4.08 (6)°]. In the crystal, molecules are linked by C—H⋯O interactions into [100] chains.
Related literature
For further synthetic details, see: Liu et al. (2011b, 2012). For related structures, see: Liu & Liu (2011) Liu et al. (2011d). For the biological activity of related compounds, see: Liu et al. (2010, 2011a,c).
Experimental
Crystal data
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Refinement
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Data collection: CrystalClear (Rigaku/MSC, 2005); cell 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.
Supporting information
10.1107/S1600536812018016/hb6735sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536812018016/hb6735Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536812018016/hb6735Isup3.cml
Dropwised the cyclopropanecarbonyl chloride to 2,4-dichlorobenzaldehyde oxime (7.50 mmol in 25 ml THF) and 7.5 mmol Et3N, then vigorously stirred at ambient temperature for overnight. The corresponding product precipitated immediately. Compound was dissolved in hot alcohol and the resulting solution was allowed to stand in air at room temperature to give colourless blocks of the title compound.
All the H atoms were positioned geometrically (C—H = 0.93–0.97 Å) and refined as riding with Uiso(H) = 1.2Ueq(C) or 1.5Ueq(methyl C).
Data collection: CrystalClear (Rigaku/MSC, 2005); cell
CrystalClear (Rigaku/MSC, 2005); data reduction: CrystalClear (Rigaku/MSC, 2005); 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 (Sheldrick, 2008.Fig. 1. The molecular structure of (I). Displacement ellipsoids are drawn at the 30% probability level. |
C11H9Cl2NO2 | Z = 2 |
Mr = 258.09 | F(000) = 264 |
Triclinic, P1 | Dx = 1.540 Mg m−3 |
a = 6.4381 (13) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 7.6030 (15) Å | Cell parameters from 1887 reflections |
c = 11.956 (2) Å | θ = 1.8–27.9° |
α = 94.90 (3)° | µ = 0.57 mm−1 |
β = 100.42 (3)° | T = 113 K |
γ = 102.70 (3)° | Block, coloress |
V = 556.71 (19) Å3 | 0.24 × 0.20 × 0.10 mm |
Rigaku Saturn CCD diffractometer | 1937 independent reflections |
Radiation source: rotating anode | 1563 reflections with I > 2σ(I) |
Confocal monochromator | Rint = 0.030 |
ω scans | θmax = 25.0°, θmin = 1.8° |
Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2005) | h = −7→7 |
Tmin = 0.876, Tmax = 0.946 | k = −9→6 |
3737 measured reflections | l = −14→14 |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.027 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.076 | H-atom parameters constrained |
S = 1.03 | w = 1/[σ2(Fo2) + (0.0407P)2] where P = (Fo2 + 2Fc2)/3 |
1937 reflections | (Δ/σ)max = 0.001 |
145 parameters | Δρmax = 0.24 e Å−3 |
0 restraints | Δρmin = −0.21 e Å−3 |
C11H9Cl2NO2 | γ = 102.70 (3)° |
Mr = 258.09 | V = 556.71 (19) Å3 |
Triclinic, P1 | Z = 2 |
a = 6.4381 (13) Å | Mo Kα radiation |
b = 7.6030 (15) Å | µ = 0.57 mm−1 |
c = 11.956 (2) Å | T = 113 K |
α = 94.90 (3)° | 0.24 × 0.20 × 0.10 mm |
β = 100.42 (3)° |
Rigaku Saturn CCD diffractometer | 1937 independent reflections |
Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2005) | 1563 reflections with I > 2σ(I) |
Tmin = 0.876, Tmax = 0.946 | Rint = 0.030 |
3737 measured reflections |
R[F2 > 2σ(F2)] = 0.027 | 0 restraints |
wR(F2) = 0.076 | H-atom parameters constrained |
S = 1.03 | Δρmax = 0.24 e Å−3 |
1937 reflections | Δρmin = −0.21 e Å−3 |
145 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
Cl1 | 0.32359 (6) | 0.70035 (5) | 0.47089 (3) | 0.02317 (14) | |
Cl2 | 1.15092 (6) | 0.98054 (6) | 0.68823 (4) | 0.02531 (14) | |
O1 | 0.08882 (17) | 0.30779 (16) | 0.94813 (9) | 0.0263 (3) | |
O2 | 0.00692 (16) | 0.37138 (15) | 0.76492 (9) | 0.0186 (3) | |
N1 | 0.2306 (2) | 0.46280 (18) | 0.78101 (11) | 0.0202 (3) | |
C1 | −0.3868 (2) | 0.2548 (2) | 0.94150 (14) | 0.0217 (4) | |
H1A | −0.2971 | 0.3293 | 1.0106 | 0.026* | |
H1B | −0.5348 | 0.2689 | 0.9234 | 0.026* | |
C2 | −0.3504 (3) | 0.0724 (2) | 0.91336 (14) | 0.0208 (4) | |
H2A | −0.4764 | −0.0249 | 0.8783 | 0.025* | |
H2B | −0.2388 | 0.0354 | 0.9655 | 0.025* | |
C3 | −0.2777 (2) | 0.2198 (2) | 0.84222 (14) | 0.0198 (4) | |
H3 | −0.3629 | 0.2113 | 0.7644 | 0.024* | |
C4 | −0.0426 (2) | 0.3004 (2) | 0.86199 (13) | 0.0177 (4) | |
C5 | 0.2637 (2) | 0.5304 (2) | 0.69054 (14) | 0.0177 (4) | |
H5 | 0.1511 | 0.5129 | 0.6268 | 0.021* | |
C6 | 0.4823 (2) | 0.6365 (2) | 0.68810 (14) | 0.0164 (4) | |
C7 | 0.5265 (3) | 0.7218 (2) | 0.59348 (13) | 0.0168 (4) | |
C8 | 0.7305 (2) | 0.8271 (2) | 0.59131 (13) | 0.0188 (4) | |
H8 | 0.7566 | 0.8836 | 0.5275 | 0.023* | |
C9 | 0.8947 (2) | 0.8453 (2) | 0.68750 (14) | 0.0187 (4) | |
C10 | 0.8595 (3) | 0.7612 (2) | 0.78232 (14) | 0.0196 (4) | |
H10 | 0.9725 | 0.7736 | 0.8453 | 0.024* | |
C11 | 0.6539 (2) | 0.6579 (2) | 0.78256 (14) | 0.0177 (4) | |
H11 | 0.6293 | 0.6016 | 0.8466 | 0.021* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cl1 | 0.0227 (2) | 0.0314 (3) | 0.0143 (2) | 0.00420 (18) | 0.00140 (17) | 0.00786 (18) |
Cl2 | 0.0192 (2) | 0.0275 (2) | 0.0273 (3) | −0.00120 (17) | 0.00716 (17) | 0.00581 (18) |
O1 | 0.0182 (6) | 0.0425 (8) | 0.0166 (7) | 0.0021 (5) | 0.0021 (5) | 0.0121 (6) |
O2 | 0.0123 (5) | 0.0267 (6) | 0.0165 (6) | 0.0012 (5) | 0.0038 (4) | 0.0082 (5) |
N1 | 0.0117 (6) | 0.0267 (8) | 0.0213 (8) | 0.0005 (6) | 0.0039 (5) | 0.0072 (6) |
C1 | 0.0179 (8) | 0.0266 (9) | 0.0221 (10) | 0.0051 (7) | 0.0073 (7) | 0.0061 (7) |
C2 | 0.0191 (8) | 0.0226 (9) | 0.0198 (9) | 0.0004 (7) | 0.0059 (7) | 0.0054 (7) |
C3 | 0.0151 (8) | 0.0264 (9) | 0.0160 (9) | 0.0002 (7) | 0.0027 (7) | 0.0059 (7) |
C4 | 0.0187 (8) | 0.0201 (8) | 0.0162 (9) | 0.0045 (7) | 0.0070 (7) | 0.0059 (7) |
C5 | 0.0178 (8) | 0.0218 (9) | 0.0145 (9) | 0.0048 (7) | 0.0041 (7) | 0.0056 (7) |
C6 | 0.0184 (8) | 0.0158 (8) | 0.0162 (9) | 0.0042 (6) | 0.0061 (7) | 0.0031 (6) |
C7 | 0.0185 (8) | 0.0193 (8) | 0.0134 (9) | 0.0070 (6) | 0.0019 (6) | 0.0024 (6) |
C8 | 0.0244 (9) | 0.0189 (9) | 0.0165 (10) | 0.0057 (7) | 0.0100 (7) | 0.0071 (7) |
C9 | 0.0181 (8) | 0.0170 (8) | 0.0223 (9) | 0.0038 (7) | 0.0082 (7) | 0.0024 (7) |
C10 | 0.0189 (8) | 0.0226 (9) | 0.0183 (9) | 0.0077 (7) | 0.0022 (7) | 0.0040 (7) |
C11 | 0.0194 (8) | 0.0206 (9) | 0.0166 (9) | 0.0079 (7) | 0.0065 (7) | 0.0073 (7) |
Cl1—C7 | 1.7477 (16) | C3—C4 | 1.470 (2) |
Cl2—C9 | 1.7394 (16) | C3—H3 | 0.9800 |
O1—C4 | 1.1976 (18) | C5—C6 | 1.467 (2) |
O2—C4 | 1.3800 (19) | C5—H5 | 0.9300 |
O2—N1 | 1.4253 (16) | C6—C7 | 1.394 (2) |
N1—C5 | 1.269 (2) | C6—C11 | 1.401 (2) |
C1—C2 | 1.478 (2) | C7—C8 | 1.385 (2) |
C1—C3 | 1.517 (2) | C8—C9 | 1.389 (2) |
C1—H1A | 0.9700 | C8—H8 | 0.9300 |
C1—H1B | 0.9700 | C9—C10 | 1.378 (2) |
C2—C3 | 1.508 (2) | C10—C11 | 1.383 (2) |
C2—H2A | 0.9700 | C10—H10 | 0.9300 |
C2—H2B | 0.9700 | C11—H11 | 0.9300 |
C4—O2—N1 | 112.18 (11) | O2—C4—C3 | 109.31 (12) |
C5—N1—O2 | 109.05 (12) | N1—C5—C6 | 118.94 (14) |
C2—C1—C3 | 60.45 (11) | N1—C5—H5 | 120.5 |
C2—C1—H1A | 117.7 | C6—C5—H5 | 120.5 |
C3—C1—H1A | 117.7 | C7—C6—C11 | 117.60 (14) |
C2—C1—H1B | 117.7 | C7—C6—C5 | 121.71 (14) |
C3—C1—H1B | 117.7 | C11—C6—C5 | 120.69 (15) |
H1A—C1—H1B | 114.8 | C8—C7—C6 | 122.37 (14) |
C1—C2—C3 | 61.08 (11) | C8—C7—Cl1 | 116.74 (13) |
C1—C2—H2A | 117.7 | C6—C7—Cl1 | 120.89 (12) |
C3—C2—H2A | 117.7 | C7—C8—C9 | 117.79 (15) |
C1—C2—H2B | 117.7 | C7—C8—H8 | 121.1 |
C3—C2—H2B | 117.7 | C9—C8—H8 | 121.1 |
H2A—C2—H2B | 114.8 | C10—C9—C8 | 121.89 (15) |
C4—C3—C2 | 116.62 (14) | C10—C9—Cl2 | 119.36 (12) |
C4—C3—C1 | 115.92 (13) | C8—C9—Cl2 | 118.75 (13) |
C2—C3—C1 | 58.47 (11) | C9—C10—C11 | 119.14 (14) |
C4—C3—H3 | 117.5 | C9—C10—H10 | 120.4 |
C2—C3—H3 | 117.5 | C11—C10—H10 | 120.4 |
C1—C3—H3 | 117.5 | C10—C11—C6 | 121.20 (15) |
O1—C4—O2 | 123.97 (14) | C10—C11—H11 | 119.4 |
O1—C4—C3 | 126.72 (15) | C6—C11—H11 | 119.4 |
C4—O2—N1—C5 | −177.60 (13) | C5—C6—C7—C8 | 177.96 (16) |
C1—C2—C3—C4 | 105.44 (16) | C11—C6—C7—Cl1 | 179.11 (13) |
C2—C1—C3—C4 | −106.64 (16) | C5—C6—C7—Cl1 | −2.0 (2) |
N1—O2—C4—O1 | −3.1 (2) | C6—C7—C8—C9 | 0.4 (3) |
N1—O2—C4—C3 | 176.04 (13) | Cl1—C7—C8—C9 | −179.65 (12) |
C2—C3—C4—O1 | −25.6 (3) | C7—C8—C9—C10 | 0.6 (3) |
C1—C3—C4—O1 | 40.4 (2) | C7—C8—C9—Cl2 | −178.69 (13) |
C2—C3—C4—O2 | 155.33 (15) | C8—C9—C10—C11 | −1.1 (3) |
C1—C3—C4—O2 | −138.66 (14) | Cl2—C9—C10—C11 | 178.24 (13) |
O2—N1—C5—C6 | 178.12 (13) | C9—C10—C11—C6 | 0.5 (3) |
N1—C5—C6—C7 | −176.72 (16) | C7—C6—C11—C10 | 0.5 (2) |
N1—C5—C6—C11 | 2.2 (3) | C5—C6—C11—C10 | −178.44 (16) |
C11—C6—C7—C8 | −1.0 (3) |
D—H···A | D—H | H···A | D···A | D—H···A |
C1—H1B···O1i | 0.97 | 2.57 | 3.5008 (19) | 161 |
Symmetry code: (i) x−1, y, z. |
Experimental details
Crystal data | |
Chemical formula | C11H9Cl2NO2 |
Mr | 258.09 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 113 |
a, b, c (Å) | 6.4381 (13), 7.6030 (15), 11.956 (2) |
α, β, γ (°) | 94.90 (3), 100.42 (3), 102.70 (3) |
V (Å3) | 556.71 (19) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 0.57 |
Crystal size (mm) | 0.24 × 0.20 × 0.10 |
Data collection | |
Diffractometer | Rigaku Saturn CCD diffractometer |
Absorption correction | Multi-scan (CrystalClear; Rigaku/MSC, 2005) |
Tmin, Tmax | 0.876, 0.946 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 3737, 1937, 1563 |
Rint | 0.030 |
(sin θ/λ)max (Å−1) | 0.595 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.027, 0.076, 1.03 |
No. of reflections | 1937 |
No. of parameters | 145 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.24, −0.21 |
Computer programs: CrystalClear (Rigaku/MSC, 2005), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008.
D—H···A | D—H | H···A | D···A | D—H···A |
C1—H1B···O1i | 0.97 | 2.57 | 3.5008 (19) | 161 |
Symmetry code: (i) x−1, y, z. |
Acknowledgements
This research work was supported by the Research Program of Beifang University of Nationalities (2010Y047) and the Key Laboratory of Chemical Technology of the SEAC (2010SY16).
References
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