Abstract
The complete molecule of the title compound, C16H14Cl2N2O2, is generated by crystallographic inversion symmetry. The dihedral angle between the benzene ring and the NH—C(O)—C fragment is 32.8 (1)°. In the crystal, the molecules are linked by N—H⋯O hydrogen bonds into [100] chains.
Related literature
For our study of the effect of substituents on the structures of N-(aryl)-amides, see: Gowda et al. (2000 ▶); Saraswathi et al. (2011 ▶), of N-(aryl)-methanesulfonamides, see: Gowda et al. (2007 ▶) and of N-(substitutedphenyl)-p-substituted-benzenesulfonamides, see: Gowda et al. (2005 ▶).
Experimental
Crystal data
C16H14Cl2N2O2
M r = 337.19
Monoclinic,
a = 8.3412 (8) Å
b = 9.6501 (9) Å
c = 9.5485 (9) Å
β = 91.319 (9)°
V = 768.39 (13) Å3
Z = 2
Mo Kα radiation
μ = 0.43 mm−1
T = 293 K
0.40 × 0.20 × 0.20 mm
Data collection
Oxford Diffraction Xcalibur diffractometer with Sapphire CCD detector
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009 ▶) T min = 0.847, T max = 0.919
2574 measured reflections
1535 independent reflections
1253 reflections with I > 2σ(I)
R int = 0.009
Refinement
R[F 2 > 2σ(F 2)] = 0.037
wR(F 2) = 0.105
S = 1.07
1535 reflections
103 parameters
1 restraint
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.25 e Å−3
Δρmin = −0.34 e Å−3
Data collection: CrysAlis CCD (Oxford Diffraction, 2009 ▶); cell refinement: CrysAlis RED (Oxford Diffraction, 2009 ▶); data reduction: CrysAlis RED; 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: SHELXL97.
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811010440/ds2100sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811010440/ds2100Isup2.hkl
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⋯O1i | 0.81 (2) | 2.10 (2) | 2.8946 (19) | 166 (2) |
Symmetry code: (i)
.
Acknowledgments
BSS thanks the University Grants Commission, Government of India, New Delhi, for the award of a research fellowship under its faculty improvement program.
supplementary crystallographic information
Comment
The amide and sulfonamide moieties are important constituents of many biologically significant compounds. As a part of studying the substituent effects on the structures of this class of compounds(Gowda et al., 2000, 2005, 2007; Saraswathi et al., 2011), in the present work, the structure of N,N-bis(3-chlorophenyl)-succinamide (I) has been determined (Fig.1). The conformations of N—H and C=O bonds in the C—NH—C(O)—C segments are anti to each other and the amide O atoms are anti to the H atoms attached to the adjacent C atoms. Further, conformations of the N—H bonds in the amide fragments are anti to the meta-chloro groups in the adjacent benzene rings, similar to the anti conformations observed with respect to the ortho-methyl groups in N,N-bis(2-methylphenyl)- succinamide (II) (Saraswathi et al., 2011). The dihedral angle between the benzene ring and the NH—C(O)—CH2 segment in the two halves of the molecule is 32.8 (1)°, compared to the value of 62.1 (2)° in (II).
Further, C1—N1—C7—C8 and C1a—N1a—C7a—C8a segments in (I) are nearly linear and so also the C1—N1—C7—O1 and C1a—N1a—C7a—O1a segments, similar to those observed in (II). The torsion angles of C2—C1—N1—C7 and C6—C1—N1—C7 are -35.0 (3)° and 147.5 (2)°, in contrast to the values of -64.0 (4)° and 117.6 (3)° in (II).
The packing of molecules in the crystal linked by of N—H···O hydrogen bonds (Table 1) is shown in Fig. 2.
Experimental
Succinic anhydride (0.01 mol) in toluene (25 ml) was treated drop wise with 3-chloroaniline (0.01 mol) also in toluene (20 ml) with constant stirring. The resulting mixture was stirred for one hour and set aside for an additional hour at room temperature for completion of the reaction. The mixture was then treated with dilute hydrochloric acid to remove unreacted 3-chloroaniline. The resultant solid N-(3-chlorophenyl)-succinamic acid was filtered under suction and washed thoroughly with water to remove the unreacted succinic anhydride and succinic acid. The compound was recrystallized to constant melting point from ethanol. The purity of the compound was checked by elemental analysis and characterized by its infrared and NMR spectra.
The N-(3-chlorophenyl)succinamic acid obtained was then treated with phosphorous oxychloride and excess of 3-chloroaniline at room temperature with constant stirring. The resultant mixture was stirred for 4 h, kept aside for additional 6 h for completion of the reaction and poured slowly into crushed ice with constant stirring. It was kept aside for a day. The resultant solid, N,N-bis(3-chlorophenyl)- succinamide was filtered under suction, washed thoroughly with water, dilute sodium hydroxide solution and finally with water. It was recrystallized to constant melting point from a mixture of acetone and chloroform. The purity of the compound was checked by elemental analysis, and characterized by its infrared and NMR spectra.
Rod like colorless single crystals used in the X-ray diffraction studies were were grown in a mixture of acetone and chloroform at room temperature.
Refinement
The H atom of the NH group was located in a difference map and later restrained to the distance N—H = 0.86 (2) Å. The other H atoms were positioned with idealized geometry using a riding model with the aromatic C—H = 0.93Å and the methylene C—H = 0.97 Å. All H atoms were refined with isotropic displacement parameters (set to 1.2 times of the Ueq of the parent atom).
Figures
Fig. 1.
Molecular structure of (I), showing the atom labelling scheme and displacement ellipsoids are drawn at the 50% probability level.
Fig. 2.
Molecular packing of (I) with hydrogen bonding shown as dashed lines.
Crystal data
| C16H14Cl2N2O2 | F(000) = 348 |
| Mr = 337.19 | Dx = 1.457 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 1492 reflections |
| a = 8.3412 (8) Å | θ = 3.0–28.0° |
| b = 9.6501 (9) Å | µ = 0.43 mm−1 |
| c = 9.5485 (9) Å | T = 293 K |
| β = 91.319 (9)° | Rod, colourless |
| V = 768.39 (13) Å3 | 0.40 × 0.20 × 0.20 mm |
| Z = 2 |
Data collection
| Oxford Diffraction Xcalibur (TM) Single Crystal X-ray Diffractometer with Sapphire CCD Detector. | 1535 independent reflections |
| Radiation source: fine-focus sealed tube | 1253 reflections with I > 2σ(I) |
| graphite | Rint = 0.009 |
| Rotation method data acquisition using ω scans. | θmax = 26.4°, θmin = 3.0° |
| Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009) | h = −10→4 |
| Tmin = 0.847, Tmax = 0.919 | k = −12→11 |
| 2574 measured reflections | l = −10→11 |
Refinement
| 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)] = 0.037 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.105 | H atoms treated by a mixture of independent and constrained refinement |
| S = 1.07 | w = 1/[σ2(Fo2) + (0.0482P)2 + 0.3792P] where P = (Fo2 + 2Fc2)/3 |
| 1535 reflections | (Δ/σ)max = 0.002 |
| 103 parameters | Δρmax = 0.25 e Å−3 |
| 1 restraint | Δρmin = −0.34 e Å−3 |
Special details
| Experimental. Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm. |
| 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 | 0.01685 (8) | 0.54218 (6) | 0.32765 (6) | 0.0639 (2) | |
| O1 | 0.4067 (2) | 0.17690 (15) | 0.16810 (13) | 0.0521 (4) | |
| N1 | 0.3460 (2) | 0.28337 (17) | −0.03736 (15) | 0.0395 (4) | |
| H1N | 0.362 (3) | 0.279 (2) | −0.1207 (17) | 0.047* | |
| C1 | 0.2803 (2) | 0.40783 (19) | 0.01300 (18) | 0.0344 (4) | |
| C2 | 0.1918 (2) | 0.4127 (2) | 0.13434 (19) | 0.0382 (4) | |
| H2 | 0.1761 | 0.3332 | 0.1873 | 0.046* | |
| C3 | 0.1276 (2) | 0.5375 (2) | 0.1747 (2) | 0.0416 (5) | |
| C4 | 0.1467 (3) | 0.6572 (2) | 0.0987 (2) | 0.0508 (5) | |
| H4 | 0.1024 | 0.7404 | 0.1281 | 0.061* | |
| C5 | 0.2335 (3) | 0.6502 (2) | −0.0223 (2) | 0.0520 (5) | |
| H5 | 0.2469 | 0.7298 | −0.0757 | 0.062* | |
| C6 | 0.3006 (2) | 0.5279 (2) | −0.0655 (2) | 0.0429 (5) | |
| H6 | 0.3595 | 0.5253 | −0.1470 | 0.052* | |
| C7 | 0.4051 (2) | 0.17778 (18) | 0.04063 (18) | 0.0363 (4) | |
| C8 | 0.4738 (3) | 0.0598 (2) | −0.04393 (19) | 0.0481 (5) | |
| H8A | 0.3934 | 0.0286 | −0.1118 | 0.058* | |
| H8B | 0.5648 | 0.0938 | −0.0953 | 0.058* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cl1 | 0.0725 (4) | 0.0602 (4) | 0.0602 (4) | 0.0010 (3) | 0.0256 (3) | −0.0182 (3) |
| O1 | 0.0881 (12) | 0.0448 (8) | 0.0235 (7) | 0.0190 (8) | 0.0080 (6) | 0.0013 (6) |
| N1 | 0.0599 (10) | 0.0367 (9) | 0.0220 (7) | 0.0081 (8) | 0.0057 (7) | 0.0004 (6) |
| C1 | 0.0402 (9) | 0.0326 (9) | 0.0304 (9) | 0.0015 (8) | −0.0024 (7) | −0.0012 (7) |
| C2 | 0.0457 (11) | 0.0337 (10) | 0.0353 (9) | −0.0009 (8) | 0.0016 (8) | −0.0019 (7) |
| C3 | 0.0413 (10) | 0.0433 (11) | 0.0402 (10) | 0.0002 (9) | 0.0023 (8) | −0.0088 (8) |
| C4 | 0.0525 (12) | 0.0367 (11) | 0.0631 (14) | 0.0083 (9) | 0.0000 (10) | −0.0066 (10) |
| C5 | 0.0604 (13) | 0.0362 (11) | 0.0593 (13) | 0.0035 (10) | −0.0001 (10) | 0.0108 (10) |
| C6 | 0.0488 (11) | 0.0425 (12) | 0.0376 (10) | 0.0030 (9) | 0.0027 (8) | 0.0067 (8) |
| C7 | 0.0507 (11) | 0.0329 (9) | 0.0254 (8) | 0.0020 (8) | 0.0054 (7) | −0.0010 (7) |
| C8 | 0.0784 (15) | 0.0393 (11) | 0.0266 (9) | 0.0136 (10) | 0.0052 (9) | −0.0022 (8) |
Geometric parameters (Å, °)
| Cl1—C3 | 1.747 (2) | C4—C5 | 1.380 (3) |
| O1—C7 | 1.217 (2) | C4—H4 | 0.9300 |
| N1—C7 | 1.349 (2) | C5—C6 | 1.373 (3) |
| N1—C1 | 1.409 (2) | C5—H5 | 0.9300 |
| N1—H1N | 0.811 (16) | C6—H6 | 0.9300 |
| C1—C2 | 1.389 (3) | C7—C8 | 1.516 (3) |
| C1—C6 | 1.393 (3) | C8—C8i | 1.487 (4) |
| C2—C3 | 1.377 (3) | C8—H8A | 0.9700 |
| C2—H2 | 0.9300 | C8—H8B | 0.9700 |
| C3—C4 | 1.375 (3) | ||
| C7—N1—C1 | 126.55 (15) | C6—C5—C4 | 121.3 (2) |
| C7—N1—H1N | 116.0 (16) | C6—C5—H5 | 119.4 |
| C1—N1—H1N | 116.8 (16) | C4—C5—H5 | 119.4 |
| C2—C1—C6 | 119.64 (18) | C5—C6—C1 | 119.87 (19) |
| C2—C1—N1 | 122.13 (16) | C5—C6—H6 | 120.1 |
| C6—C1—N1 | 118.19 (17) | C1—C6—H6 | 120.1 |
| C3—C2—C1 | 118.72 (18) | O1—C7—N1 | 123.58 (16) |
| C3—C2—H2 | 120.6 | O1—C7—C8 | 122.13 (17) |
| C1—C2—H2 | 120.6 | N1—C7—C8 | 114.28 (15) |
| C4—C3—C2 | 122.47 (19) | C8i—C8—C7 | 113.09 (19) |
| C4—C3—Cl1 | 119.31 (16) | C8i—C8—H8A | 109.0 |
| C2—C3—Cl1 | 118.22 (16) | C7—C8—H8A | 109.0 |
| C3—C4—C5 | 118.03 (19) | C8i—C8—H8B | 109.0 |
| C3—C4—H4 | 121.0 | C7—C8—H8B | 109.0 |
| C5—C4—H4 | 121.0 | H8A—C8—H8B | 107.8 |
| C7—N1—C1—C2 | −35.0 (3) | C3—C4—C5—C6 | −0.7 (3) |
| C7—N1—C1—C6 | 147.5 (2) | C4—C5—C6—C1 | 0.5 (3) |
| C6—C1—C2—C3 | −0.7 (3) | C2—C1—C6—C5 | 0.2 (3) |
| N1—C1—C2—C3 | −178.16 (17) | N1—C1—C6—C5 | 177.74 (19) |
| C1—C2—C3—C4 | 0.6 (3) | C1—N1—C7—O1 | 1.0 (3) |
| C1—C2—C3—Cl1 | −179.87 (14) | C1—N1—C7—C8 | −177.66 (19) |
| C2—C3—C4—C5 | 0.1 (3) | O1—C7—C8—C8i | 5.9 (4) |
| Cl1—C3—C4—C5 | −179.44 (17) | N1—C7—C8—C8i | −175.4 (2) |
Symmetry codes: (i) −x+1, −y, −z.
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1N···O1ii | 0.81 (2) | 2.10 (2) | 2.8946 (19) | 166 (2) |
Symmetry codes: (ii) x, −y+1/2, z−1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: DS2100).
References
- Gowda, B. T., Foro, S. & Fuess, H. (2007). Acta Cryst. E63, o2597.
- Gowda, B. T., Paulus, H. & Fuess, H. (2000). Z. Naturforsch. Teil A, 55, 791–800.
- Gowda, B. T., Shetty, M. & Jayalakshmi, K. L. (2005). Z. Naturforsch. Teil A, 60, 106–112.
- Oxford Diffraction (2009). CrysAlis CCD and CrysAlis RED Oxford Diffraction Ltd, Yarnton, England.
- Saraswathi, B. S., Foro, S. & Gowda, B. T. (2011). Acta Cryst. E67, o607. [DOI] [PMC free article] [PubMed]
- 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 datablocks I, global. DOI: 10.1107/S1600536811010440/ds2100sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811010440/ds2100Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


