Literature DB >> 23476227

Methyl 2-(3-chloro-benzamido)-benzoate.

Abdelaaziz Ouahrouch1, Moha Taourirte, Hassan B Lazrek, Mohamed El Azhari, Mohamed Saadi, Lahcen El Ammari.   

Abstract

In the mol-ecule of the title compound, C15H12ClNO3, the chloro-benzamide and benzoate units are almost co-planar, with a dihedral angle between the six-membered rings of 2.99 (10)°. An intra-molecular N-H⋯O hydrogen bond occurs. In the crystal, each mol-ecule is linked to a symmetry-equivalent counterpart across a twofold rotation axis by weak C-H⋯O and C-H⋯Cl hydrogen bonds, forming dimers. The packing is stabilized through weak π-π stacking along the b-axis direction, leading to π-stacked columns of inversion-related mol-ecules, with an inter-planar distance of 3.46 (2) Å and a centroid-centroid vector of 3.897 (2) Å.

Entities:  

Year:  2012        PMID: 23476227      PMCID: PMC3588991          DOI: 10.1107/S1600536812046934

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For details of the synthesis, see: Shariat & Abdollahi (2004 ▶); Xingwen et al. (2007 ▶); Chandrika et al. (2008 ▶). For background to the potential biological use of benzoxazinone derivatives, see: Kurosaki & Naishi (1983 ▶); Ponchet et al. (1988 ▶); Hedsrom et al. (1984 ▶); Krantz et al. (1990 ▶).

Experimental

Crystal data

C15H12ClNO3 M = 289.71 Monoclinic, a = 25.7464 (10) Å b = 6.9203 (2) Å c = 16.9735 (6) Å β = 116.045 (2)° V = 2717.10 (16) Å3 Z = 8 Mo Kα radiation μ = 0.29 mm−1 T = 296 K 0.36 × 0.31 × 0.27 mm

Data collection

Bruker X8 APEXII diffractometer Absorption correction: multi-scan (SADABS; Bruker, 2009 ▶) T min = 0.957, T max = 0.997 20126 measured reflections 3511 independent reflections 2143 reflections with I > 2σ(I) R int = 0.038

Refinement

R[F 2 > 2σ(F 2)] = 0.047 wR(F 2) = 0.144 S = 1.02 3511 reflections 181 parameters H-atom parameters constrained Δρmax = 0.31 e Å−3 Δρmin = −0.40 e Å−3 Data collection: APEX2 (Bruker, 2009 ▶); cell refinement: SAINT (Bruker, 2009 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012 ▶) and Mercury (Macrae et al. 2008 ▶); software used to prepare material for publication: PLATON (Spek, 2009 ▶) and publCIF (Westrip, 2010 ▶). Click here for additional data file. Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812046934/zl2515sup1.cif Click here for additional data file. Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812046934/zl2515Isup2.hkl Click here for additional data file. Supplementary material file. DOI: 10.1107/S1600536812046934/zl2515Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C15H12ClNO3F(000) = 1200
Mr = 289.71Dx = 1.416 Mg m3
Monoclinic, C2/cMelting point: 361.5 K
Hall symbol: -c 2ycMo Kα radiation, λ = 0.71073 Å
a = 25.7464 (10) ÅCell parameters from 3511 reflections
b = 6.9203 (2) Åθ = 3.1–28.7°
c = 16.9735 (6) ŵ = 0.29 mm1
β = 116.045 (2)°T = 296 K
V = 2717.10 (16) Å3Block, colourless
Z = 80.36 × 0.31 × 0.27 mm
Bruker X8 APEXII diffractometer3511 independent reflections
Radiation source: fine-focus sealed tube2143 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.038
φ and ω scansθmax = 28.7°, θmin = 3.1°
Absorption correction: multi-scan (SADABS; Bruker, 2009)h = −34→34
Tmin = 0.957, Tmax = 0.997k = −6→9
20126 measured reflectionsl = −22→22
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.047Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.144H-atom parameters constrained
S = 1.02w = 1/[σ2(Fo2) + (0.0663P)2 + 1.0088P] where P = (Fo2 + 2Fc2)/3
3511 reflections(Δ/σ)max = 0.001
181 parametersΔρmax = 0.31 e Å3
0 restraintsΔρmin = −0.40 e Å3
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.
xyzUiso*/Ueq
C11.07779 (8)0.3043 (3)0.40699 (12)0.0493 (4)
H11.06010.30840.34600.059*
C21.13694 (8)0.3154 (3)0.45261 (13)0.0532 (5)
C31.16464 (8)0.3122 (3)0.54250 (13)0.0576 (5)
H31.20470.31990.57200.069*
C41.13189 (9)0.2973 (3)0.58835 (13)0.0598 (5)
H41.15000.29620.64930.072*
C51.07250 (8)0.2840 (3)0.54427 (12)0.0523 (5)
H51.05080.27320.57580.063*
C61.04473 (7)0.2867 (2)0.45306 (11)0.0450 (4)
C70.98059 (8)0.2750 (3)0.40006 (12)0.0491 (4)
C80.89076 (8)0.2154 (3)0.41741 (12)0.0479 (4)
C90.85177 (9)0.2244 (3)0.32896 (13)0.0643 (6)
H90.86530.23540.28650.077*
C100.79331 (9)0.2169 (4)0.30448 (14)0.0770 (7)
H100.76770.22450.24530.092*
C110.77171 (9)0.1984 (4)0.36551 (15)0.0751 (7)
H110.73210.19320.34790.090*
C120.80976 (8)0.1878 (3)0.45261 (14)0.0613 (5)
H120.79550.17430.49400.074*
C130.86918 (8)0.1966 (3)0.48050 (11)0.0470 (4)
C140.90870 (8)0.1895 (3)0.57552 (12)0.0497 (4)
C150.91577 (12)0.1812 (5)0.71856 (14)0.0935 (9)
H15A0.89210.15090.74760.112*
H15B0.93330.30570.73750.112*
H15C0.94540.08510.73270.112*
N10.95046 (6)0.2249 (2)0.44555 (10)0.0496 (4)
H20.97120.19460.49960.060*
O10.95798 (6)0.3078 (3)0.32160 (9)0.0813 (5)
O20.96083 (6)0.1874 (2)0.60722 (8)0.0627 (4)
O30.88031 (6)0.1841 (2)0.62469 (9)0.0710 (4)
Cl11.17831 (2)0.33637 (11)0.39517 (4)0.0870 (3)
U11U22U33U12U13U23
C10.0453 (10)0.0606 (11)0.0458 (10)−0.0014 (8)0.0234 (8)−0.0021 (8)
C20.0452 (10)0.0637 (12)0.0583 (11)−0.0011 (8)0.0298 (9)−0.0003 (9)
C30.0397 (10)0.0745 (13)0.0562 (11)−0.0021 (9)0.0190 (9)−0.0015 (9)
C40.0485 (11)0.0805 (14)0.0461 (11)−0.0045 (10)0.0169 (9)−0.0017 (9)
C50.0454 (11)0.0680 (12)0.0473 (10)−0.0040 (9)0.0238 (9)−0.0012 (8)
C60.0406 (9)0.0493 (9)0.0479 (10)−0.0006 (7)0.0219 (8)−0.0016 (8)
C70.0439 (10)0.0626 (11)0.0445 (10)−0.0023 (8)0.0228 (8)−0.0027 (8)
C80.0378 (9)0.0596 (11)0.0458 (10)−0.0027 (8)0.0178 (8)−0.0009 (8)
C90.0446 (11)0.1000 (16)0.0459 (11)−0.0092 (11)0.0175 (9)−0.0012 (10)
C100.0443 (12)0.123 (2)0.0511 (12)−0.0117 (12)0.0092 (10)0.0035 (12)
C110.0351 (10)0.1150 (19)0.0692 (14)−0.0091 (11)0.0173 (10)0.0055 (13)
C120.0434 (11)0.0823 (14)0.0628 (12)−0.0034 (10)0.0276 (10)0.0032 (11)
C130.0405 (10)0.0532 (10)0.0479 (10)−0.0017 (8)0.0198 (8)−0.0001 (8)
C140.0472 (11)0.0575 (11)0.0495 (10)−0.0008 (8)0.0259 (9)0.0026 (8)
C150.0829 (18)0.157 (3)0.0497 (13)0.0046 (17)0.0375 (13)0.0061 (14)
N10.0364 (8)0.0701 (10)0.0430 (8)0.0001 (7)0.0180 (7)0.0044 (7)
O10.0493 (9)0.1499 (15)0.0442 (8)−0.0092 (9)0.0199 (7)0.0100 (8)
O20.0461 (8)0.0951 (11)0.0464 (7)−0.0013 (7)0.0198 (6)0.0058 (7)
O30.0586 (9)0.1105 (12)0.0529 (8)0.0034 (8)0.0326 (7)0.0034 (7)
Cl10.0521 (3)0.1486 (7)0.0740 (4)−0.0057 (3)0.0405 (3)0.0009 (4)
C1—C21.374 (3)C9—C101.375 (3)
C1—C61.391 (2)C9—H90.9300
C1—H10.9300C10—C111.380 (3)
C2—C31.372 (3)C10—H100.9300
C2—Cl11.7374 (18)C11—C121.371 (3)
C3—C41.380 (3)C11—H110.9300
C3—H30.9300C12—C131.390 (3)
C4—C51.379 (3)C12—H120.9300
C4—H40.9300C13—C141.482 (3)
C5—C61.392 (3)C14—O21.207 (2)
C5—H50.9300C14—O31.329 (2)
C6—C71.496 (3)C15—O31.448 (3)
C7—O11.218 (2)C15—H15A0.9600
C7—N11.358 (2)C15—H15B0.9600
C8—C91.394 (3)C15—H15C0.9600
C8—N11.397 (2)N1—H20.8600
C8—C131.412 (2)
C2—C1—C6119.22 (17)C8—C9—H9120.0
C2—C1—H1120.4C9—C10—C11121.7 (2)
C6—C1—H1120.4C9—C10—H10119.2
C3—C2—C1122.16 (17)C11—C10—H10119.2
C3—C2—Cl1118.55 (15)C12—C11—C10118.80 (19)
C1—C2—Cl1119.28 (15)C12—C11—H11120.6
C2—C3—C4118.71 (18)C10—C11—H11120.6
C2—C3—H3120.6C11—C12—C13121.57 (19)
C4—C3—H3120.6C11—C12—H12119.2
C5—C4—C3120.37 (18)C13—C12—H12119.2
C5—C4—H4119.8C12—C13—C8119.09 (17)
C3—C4—H4119.8C12—C13—C14119.73 (16)
C4—C5—C6120.56 (17)C8—C13—C14121.17 (16)
C4—C5—H5119.7O2—C14—O3122.00 (17)
C6—C5—H5119.7O2—C14—C13125.66 (16)
C1—C6—C5118.96 (16)O3—C14—C13112.34 (16)
C1—C6—C7116.94 (16)O3—C15—H15A109.5
C5—C6—C7124.09 (16)O3—C15—H15B109.5
O1—C7—N1123.45 (17)H15A—C15—H15B109.5
O1—C7—C6121.25 (16)O3—C15—H15C109.5
N1—C7—C6115.29 (16)H15A—C15—H15C109.5
C9—C8—N1122.04 (16)H15B—C15—H15C109.5
C9—C8—C13118.94 (17)C7—N1—C8129.44 (16)
N1—C8—C13119.03 (15)C7—N1—H2115.3
C10—C9—C8119.93 (19)C8—N1—H2115.3
C10—C9—H9120.0C14—O3—C15115.88 (17)
D—H···AD—HH···AD···AD—H···A
N1—H2···O20.861.962.6506 (19)137
C1—H1···O1i0.932.673.573 (2)163
C9—H9···Cl1i0.932.873.617 (2)139
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯A D—HH⋯A DA D—H⋯A
N1—H2⋯O20.861.962.6506 (19)137
C1—H1⋯O1i 0.932.673.573 (2)163
C9—H9⋯Cl1i 0.932.873.617 (2)139

Symmetry code: (i) .

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