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The phenyl and di­chloro­phenyl rings of the title mol­ecule, C21H13Cl2NO, are oriented at angles of 39.3 (1) and 77.8 (1)°, respectively, with respect to the central indoline ring. The crystal structure is stabilized by van der Waals interactions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S160053680201111X/ci6135sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S160053680201111X/ci6135Isup2.hkl
Contains datablock I

CCDC reference: 193759

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.004 Å
  • R factor = 0.042
  • wR factor = 0.107
  • Data-to-parameter ratio = 13.6

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry








Computing details top

Data collection: CAD-4 EXPRESS (Enraf-Nonius, 1994); cell refinement: CAD-4 EXPRESS; data reduction: MolEN (Fair, 1990); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: WinGX (Farrugia, 1999); software used to prepare material for publication: SHELXL97.

3-Benzylidene-[N-(2,6-dichlorophenyl)-indolin-2-one] top
Crystal data top
C21H13Cl2NOF(000) = 752
Mr = 366.22Dx = 1.378 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 25 reflections
a = 9.242 (5) Åθ = 10–15°
b = 19.232 (12) ŵ = 0.38 mm1
c = 10.319 (5) ÅT = 293 K
β = 105.80 (4)°Plate, white
V = 1764.8 (17) Å30.30 × 0.25 × 0.20 mm
Z = 4
Data collection top
Enraf-Nonius CAD-4
diffractometer
2276 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.013
Graphite monochromatorθmax = 25.0°, θmin = 2.1°
ω–2θ scansh = 010
Absorption correction: ψ scan
(North et al., 1968)
k = 022
Tmin = 0.896, Tmax = 0.929l = 1211
3290 measured reflections2 standard reflections every 100 reflections
3090 independent reflections intensity decay: none
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.042H-atom parameters constrained
wR(F2) = 0.107 w = 1/[σ2(Fo2) + (0.0294P)2 + 1.0794P]
where P = (Fo2 + 2Fc2)/3
S = 1.11(Δ/σ)max < 0.001
3090 reflectionsΔρmax = 0.27 e Å3
227 parametersΔρmin = 0.29 e Å3
0 restraintsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0058 (8)
Special details top

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) top
xyzUiso*/Ueq
Cl10.47556 (11)0.27210 (4)0.10827 (10)0.0924 (3)
Cl20.15949 (9)0.50626 (4)0.05194 (9)0.0811 (3)
O10.3571 (2)0.44759 (10)0.28208 (19)0.0645 (5)
N10.2359 (2)0.37615 (11)0.1072 (2)0.0513 (5)
C10.2566 (3)0.40735 (13)0.2324 (3)0.0482 (6)
C20.1302 (3)0.38254 (12)0.2858 (2)0.0460 (6)
C30.0696 (3)0.28542 (14)0.1842 (3)0.0616 (7)
H30.11410.28410.25490.074*
C40.1196 (3)0.24138 (16)0.0755 (3)0.0728 (9)
H40.19770.21050.07340.087*
C50.0549 (3)0.24278 (17)0.0299 (3)0.0770 (9)
H50.09160.21360.10330.092*
C60.0642 (3)0.28698 (15)0.0285 (3)0.0669 (8)
H60.10900.28750.09900.080*
C70.1129 (3)0.32973 (13)0.0807 (3)0.0500 (6)
C80.0471 (2)0.33167 (12)0.1880 (2)0.0461 (6)
C90.3255 (3)0.39048 (13)0.0189 (2)0.0497 (6)
C100.3016 (3)0.44970 (14)0.0610 (3)0.0544 (6)
C110.3901 (3)0.46469 (16)0.1456 (3)0.0670 (8)
H110.37300.50480.19800.080*
C120.5031 (3)0.42005 (16)0.1515 (3)0.0697 (8)
H120.56270.43000.20870.084*
C130.5301 (3)0.36092 (16)0.0750 (3)0.0695 (8)
H130.60690.33080.08060.083*
C140.4421 (3)0.34636 (14)0.0108 (3)0.0580 (7)
C150.1149 (3)0.41034 (13)0.4003 (3)0.0519 (6)
H150.19480.43790.44720.062*
C160.0092 (3)0.40376 (12)0.4625 (2)0.0516 (6)
C170.1573 (3)0.39822 (15)0.3861 (3)0.0640 (7)
H170.17860.39660.29270.077*
C180.2739 (4)0.39499 (17)0.4457 (4)0.0800 (9)
H180.37280.39170.39290.096*
C190.2426 (5)0.39672 (18)0.5828 (4)0.0918 (11)
H190.32060.39330.62340.110*
C200.0982 (5)0.40346 (17)0.6609 (4)0.0868 (11)
H200.07860.40490.75410.104*
C210.0189 (4)0.40815 (14)0.6018 (3)0.0671 (8)
H210.11680.41430.65530.081*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.0994 (6)0.0695 (5)0.1249 (8)0.0220 (4)0.0586 (6)0.0289 (5)
Cl20.0662 (5)0.0833 (6)0.1008 (6)0.0203 (4)0.0346 (4)0.0217 (5)
O10.0558 (11)0.0755 (13)0.0667 (12)0.0196 (10)0.0243 (9)0.0112 (10)
N10.0488 (12)0.0565 (12)0.0556 (12)0.0109 (10)0.0262 (10)0.0035 (10)
C10.0446 (13)0.0486 (14)0.0541 (15)0.0005 (11)0.0180 (11)0.0029 (12)
C20.0438 (13)0.0455 (13)0.0511 (14)0.0021 (10)0.0169 (11)0.0072 (11)
C30.0540 (15)0.0620 (17)0.0772 (19)0.0073 (13)0.0322 (14)0.0019 (15)
C40.0600 (17)0.0661 (19)0.100 (2)0.0217 (14)0.0338 (17)0.0153 (17)
C50.0712 (19)0.078 (2)0.086 (2)0.0246 (16)0.0282 (17)0.0265 (17)
C60.0649 (17)0.0745 (19)0.0692 (18)0.0154 (15)0.0320 (15)0.0154 (15)
C70.0460 (13)0.0494 (14)0.0577 (15)0.0047 (11)0.0194 (12)0.0003 (12)
C80.0414 (12)0.0462 (13)0.0534 (14)0.0008 (10)0.0176 (11)0.0057 (11)
C90.0471 (13)0.0556 (15)0.0524 (14)0.0085 (11)0.0236 (12)0.0034 (12)
C100.0474 (14)0.0603 (16)0.0587 (16)0.0020 (12)0.0200 (12)0.0031 (13)
C110.0696 (18)0.0719 (19)0.0660 (18)0.0057 (15)0.0295 (15)0.0120 (15)
C120.076 (2)0.080 (2)0.0682 (19)0.0128 (16)0.0455 (16)0.0057 (16)
C130.0663 (18)0.0706 (19)0.086 (2)0.0012 (15)0.0451 (17)0.0090 (17)
C140.0603 (16)0.0527 (15)0.0672 (17)0.0026 (12)0.0280 (14)0.0027 (13)
C150.0545 (14)0.0520 (14)0.0518 (15)0.0025 (12)0.0189 (12)0.0041 (12)
C160.0641 (16)0.0434 (13)0.0547 (15)0.0004 (12)0.0284 (13)0.0016 (11)
C170.0626 (18)0.0715 (18)0.0644 (17)0.0077 (14)0.0284 (14)0.0026 (14)
C180.0687 (19)0.088 (2)0.097 (3)0.0025 (17)0.0460 (18)0.0050 (19)
C190.106 (3)0.090 (2)0.107 (3)0.010 (2)0.076 (3)0.015 (2)
C200.131 (3)0.079 (2)0.070 (2)0.008 (2)0.062 (2)0.0138 (18)
C210.087 (2)0.0616 (17)0.0591 (17)0.0056 (15)0.0307 (16)0.0098 (14)
Geometric parameters (Å, º) top
Cl1—C141.725 (3)C10—C111.379 (4)
Cl2—C101.728 (3)C11—C121.366 (4)
O1—C11.210 (3)C11—H110.93
N1—C11.389 (3)C12—C131.368 (4)
N1—C71.412 (3)C12—H120.93
N1—C91.416 (3)C13—C141.385 (4)
C1—C21.498 (3)C13—H130.93
C2—C151.339 (3)C15—C161.465 (3)
C2—C81.464 (3)C15—H150.93
C3—C41.381 (4)C16—C171.385 (4)
C3—C81.391 (3)C16—C211.392 (4)
C3—H30.93C17—C181.380 (4)
C4—C51.376 (4)C17—H170.93
C4—H40.93C18—C191.365 (5)
C5—C61.388 (4)C18—H180.93
C5—H50.93C19—C201.364 (5)
C6—C71.369 (4)C19—H190.93
C6—H60.93C20—C211.382 (4)
C7—C81.401 (3)C20—H200.93
C9—C101.388 (4)C21—H210.93
C9—C141.392 (3)
C1—N1—C7110.68 (19)C12—C11—C10119.3 (3)
C1—N1—C9123.9 (2)C12—C11—H11120.4
C7—N1—C9125.4 (2)C10—C11—H11120.4
O1—C1—N1124.5 (2)C11—C12—C13121.2 (3)
O1—C1—C2129.3 (2)C11—C12—H12119.4
N1—C1—C2106.3 (2)C13—C12—H12119.4
C15—C2—C8135.5 (2)C12—C13—C14119.4 (3)
C15—C2—C1118.5 (2)C12—C13—H13120.3
C8—C2—C1105.9 (2)C14—C13—H13120.3
C4—C3—C8120.0 (3)C13—C14—C9120.9 (3)
C4—C3—H3120.0C13—C14—Cl1119.8 (2)
C8—C3—H3120.0C9—C14—Cl1119.3 (2)
C5—C4—C3120.6 (3)C2—C15—C16129.5 (2)
C5—C4—H4119.7C2—C15—H15115.3
C3—C4—H4119.7C16—C15—H15115.3
C4—C5—C6121.2 (3)C17—C16—C21118.1 (2)
C4—C5—H5119.4C17—C16—C15121.8 (2)
C6—C5—H5119.4C21—C16—C15120.0 (3)
C7—C6—C5117.3 (3)C18—C17—C16121.4 (3)
C7—C6—H6121.4C18—C17—H17119.3
C5—C6—H6121.4C16—C17—H17119.3
C6—C7—C8123.4 (2)C19—C18—C17119.3 (3)
C6—C7—N1127.3 (2)C19—C18—H18120.3
C8—C7—N1109.3 (2)C17—C18—H18120.3
C3—C8—C7117.5 (2)C20—C19—C18120.8 (3)
C3—C8—C2134.8 (2)C20—C19—H19119.6
C7—C8—C2107.7 (2)C18—C19—H19119.6
C10—C9—C14117.7 (2)C19—C20—C21120.2 (3)
C10—C9—N1121.1 (2)C19—C20—H20119.9
C14—C9—N1121.2 (2)C21—C20—H20119.9
C11—C10—C9121.4 (2)C20—C21—C16120.2 (3)
C11—C10—Cl2119.6 (2)C20—C21—H21119.9
C9—C10—Cl2118.98 (19)C16—C21—H21119.9
C7—N1—C1—O1177.4 (2)C1—N1—C9—C1499.5 (3)
C9—N1—C1—O13.5 (4)C7—N1—C9—C1481.6 (3)
C7—N1—C1—C24.2 (3)C14—C9—C10—C110.1 (4)
C9—N1—C1—C2174.9 (2)N1—C9—C10—C11178.9 (2)
O1—C1—C2—C154.8 (4)C14—C9—C10—Cl2179.1 (2)
N1—C1—C2—C15173.5 (2)N1—C9—C10—Cl20.2 (3)
O1—C1—C2—C8177.1 (3)C9—C10—C11—C120.4 (4)
N1—C1—C2—C84.7 (2)Cl2—C10—C11—C12179.5 (2)
C8—C3—C4—C50.1 (5)C10—C11—C12—C130.1 (5)
C3—C4—C5—C61.6 (5)C11—C12—C13—C140.5 (5)
C4—C5—C6—C70.9 (5)C12—C13—C14—C90.9 (4)
C5—C6—C7—C81.2 (4)C12—C13—C14—Cl1179.8 (2)
C5—C6—C7—N1176.6 (3)C10—C9—C14—C130.6 (4)
C1—N1—C7—C6176.1 (3)N1—C9—C14—C13179.5 (2)
C9—N1—C7—C64.9 (4)C10—C9—C14—Cl1179.9 (2)
C1—N1—C7—C82.0 (3)N1—C9—C14—Cl11.1 (3)
C9—N1—C7—C8177.0 (2)C8—C2—C15—C167.9 (5)
C4—C3—C8—C72.0 (4)C1—C2—C15—C16169.6 (2)
C4—C3—C8—C2177.4 (3)C2—C15—C16—C1734.1 (4)
C6—C7—C8—C32.7 (4)C2—C15—C16—C21150.7 (3)
N1—C7—C8—C3175.5 (2)C21—C16—C17—C181.9 (4)
C6—C7—C8—C2179.3 (2)C15—C16—C17—C18177.2 (3)
N1—C7—C8—C21.1 (3)C16—C17—C18—C190.5 (5)
C15—C2—C8—C310.1 (5)C17—C18—C19—C201.8 (5)
C1—C2—C8—C3172.2 (3)C18—C19—C20—C210.5 (6)
C15—C2—C8—C7174.2 (3)C19—C20—C21—C162.1 (5)
C1—C2—C8—C73.5 (3)C17—C16—C21—C203.2 (4)
C1—N1—C9—C1079.5 (3)C15—C16—C21—C20178.6 (3)
C7—N1—C9—C1099.5 (3)
 

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