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In the title compound, C19H14Cl2N2O3S, which was synthesized by the intermolecular [3 + 2]-cyclo­addition of 2,6-di­chloro­benzo­nitrile oxide and 5-benzyl­idene-3-ethyl-thia­zolidine-2,4-dione, there is a spiro connection between an isoxazoline ring and a thia­zolidine ring. The thia­zolidine ring is essentially planar, but the isoxazoline ring has a mean deviation from the plane of 0.0177 (3) Å. The dihedral angle between the mean planes of the rings is 88.5 (4)°.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536803003003/cf6237sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536803003003/cf6237Isup2.hkl
Contains datablock I

CCDC reference: 206782

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.005 Å
  • R factor = 0.052
  • wR factor = 0.110
  • Data-to-parameter ratio = 13.6

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry








Computing details top

Data collection: SMART (Bruker, 1998); cell refinement: SMART; data reduction: SAINT (Bruker, 1998); program(s) used to solve structure: SHELXTL (Bruker, 1998); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

3-(2,6-Dichlorophenyl)-8-ethyl-4-phenyl-1-oxa-6-thia-2,8-diazaspiro[4.4]non- 2-ene-7,9-dione top
Crystal data top
C19H14Cl2N2O3SDx = 1.469 Mg m3
Mr = 421.28Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PbcaCell parameters from 864 reflections
a = 10.0339 (9) Åθ = 2.7–21.2°
b = 12.5618 (12) ŵ = 0.47 mm1
c = 30.220 (3) ÅT = 293 K
V = 3809.1 (7) Å3Plate, colorless
Z = 80.26 × 0.24 × 0.16 mm
F(000) = 1728
Data collection top
Bruker SMART CCD area-detector
diffractometer
3335 independent reflections
Radiation source: fine-focus sealed tube2148 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.057
φ and ω scansθmax = 25.0°, θmin = 1.4°
Absorption correction: multi-scan
(SADABS; Bruker, 1998)
h = 911
Tmin = 0.825, Tmax = 0.927k = 1414
13516 measured reflectionsl = 3533
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.052 w = 1/[σ2(Fo2) + (0.084P)2]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.110(Δ/σ)max < 0.001
S = 1.07Δρmax = 0.36 e Å3
3335 reflectionsΔρmin = 0.33 e Å3
245 parameters
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
S10.12407 (10)0.47626 (8)0.46069 (3)0.0582 (3)
Cl10.28598 (11)0.33697 (8)0.27374 (3)0.0688 (3)
Cl20.03391 (12)0.67094 (8)0.31535 (4)0.0833 (4)
N10.3347 (3)0.3573 (2)0.47022 (9)0.0514 (8)
N20.2437 (3)0.5770 (3)0.35317 (9)0.0605 (9)
O10.2129 (3)0.3869 (2)0.53316 (9)0.0770 (9)
O20.4271 (3)0.3571 (3)0.40150 (10)0.1123 (14)
O30.2809 (3)0.5541 (2)0.39765 (8)0.0750 (9)
C10.2306 (4)0.4008 (3)0.49435 (12)0.0517 (9)
C20.3407 (4)0.3839 (3)0.42664 (13)0.0613 (11)
C30.2243 (3)0.4544 (3)0.41168 (11)0.0475 (9)
C40.1537 (3)0.4089 (3)0.37016 (10)0.0393 (8)
H40.20560.34790.35960.047*
C50.1750 (3)0.5004 (3)0.33819 (10)0.0406 (8)
C60.4353 (4)0.2884 (3)0.49189 (14)0.0671 (11)
H6A0.47120.23900.47030.081*
H6B0.39270.24730.51510.081*
C70.5473 (4)0.3527 (3)0.51148 (15)0.0803 (14)
H7A0.59240.39080.48840.120*
H7B0.60910.30590.52600.120*
H7C0.51190.40240.53260.120*
C80.0103 (3)0.3735 (3)0.37547 (10)0.0379 (8)
C90.0200 (4)0.2668 (3)0.37114 (11)0.0507 (9)
H90.04620.21830.36360.061*
C100.1499 (4)0.2321 (3)0.37810 (13)0.0650 (11)
H100.17040.16030.37490.078*
C110.2473 (4)0.3023 (3)0.38958 (12)0.0561 (10)
H110.33360.27820.39460.067*
C120.2186 (4)0.4074 (3)0.39364 (11)0.0527 (9)
H120.28530.45540.40130.063*
C130.0900 (3)0.4432 (3)0.38640 (11)0.0476 (9)
H130.07120.51550.38900.057*
C140.1258 (3)0.5055 (2)0.29201 (10)0.0404 (8)
C150.1724 (3)0.4356 (3)0.25966 (11)0.0461 (9)
C160.1335 (4)0.4427 (3)0.21599 (12)0.0610 (11)
H160.16820.39600.19510.073*
C170.0437 (5)0.5187 (4)0.20362 (14)0.0740 (12)
H170.01680.52320.17420.089*
C180.0071 (4)0.5883 (4)0.23403 (14)0.0692 (12)
H180.06880.63950.22540.083*
C190.0340 (4)0.5823 (3)0.27798 (12)0.0528 (10)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0514 (6)0.0792 (7)0.0439 (5)0.0127 (5)0.0001 (4)0.0091 (5)
Cl10.0706 (7)0.0682 (6)0.0677 (6)0.0179 (5)0.0087 (5)0.0122 (5)
Cl20.0988 (9)0.0611 (6)0.0899 (8)0.0282 (6)0.0247 (7)0.0090 (6)
N10.0463 (19)0.0584 (19)0.0496 (19)0.0027 (15)0.0077 (15)0.0078 (15)
N20.071 (2)0.065 (2)0.0450 (18)0.0225 (18)0.0013 (17)0.0045 (16)
O10.090 (2)0.095 (2)0.0465 (17)0.0104 (18)0.0014 (15)0.0064 (15)
O20.0519 (19)0.223 (4)0.0622 (19)0.047 (2)0.0023 (16)0.019 (2)
O30.085 (2)0.086 (2)0.0537 (16)0.0430 (17)0.0141 (15)0.0014 (15)
C10.057 (3)0.052 (2)0.046 (2)0.0067 (19)0.003 (2)0.0066 (18)
C20.037 (2)0.099 (3)0.048 (2)0.003 (2)0.0052 (19)0.017 (2)
C30.038 (2)0.064 (2)0.0411 (19)0.0045 (18)0.0005 (16)0.0032 (17)
C40.037 (2)0.0444 (19)0.0368 (18)0.0020 (15)0.0000 (15)0.0065 (15)
C50.0371 (19)0.0421 (19)0.0428 (19)0.0050 (16)0.0054 (15)0.0047 (16)
C60.066 (3)0.057 (2)0.078 (3)0.010 (2)0.018 (2)0.007 (2)
C70.073 (3)0.074 (3)0.094 (3)0.005 (2)0.036 (3)0.008 (3)
C80.038 (2)0.0426 (19)0.0330 (17)0.0003 (16)0.0034 (15)0.0010 (15)
C90.048 (2)0.046 (2)0.059 (2)0.0033 (18)0.0082 (18)0.0027 (18)
C100.067 (3)0.048 (2)0.080 (3)0.017 (2)0.008 (2)0.003 (2)
C110.043 (2)0.070 (3)0.055 (2)0.011 (2)0.0016 (19)0.001 (2)
C120.040 (2)0.062 (2)0.056 (2)0.0077 (19)0.0003 (18)0.0019 (19)
C130.048 (2)0.039 (2)0.056 (2)0.0026 (17)0.0036 (18)0.0019 (17)
C140.039 (2)0.0411 (19)0.0411 (18)0.0093 (16)0.0046 (16)0.0017 (15)
C150.047 (2)0.048 (2)0.043 (2)0.0080 (17)0.0026 (17)0.0000 (17)
C160.078 (3)0.060 (3)0.045 (2)0.015 (2)0.005 (2)0.0079 (19)
C170.088 (3)0.082 (3)0.051 (2)0.018 (3)0.008 (2)0.011 (2)
C180.066 (3)0.071 (3)0.071 (3)0.000 (2)0.012 (2)0.027 (2)
C190.053 (2)0.047 (2)0.058 (2)0.0052 (19)0.0085 (19)0.0069 (19)
Geometric parameters (Å, º) top
S1—C11.754 (4)C7—H7B0.960
S1—C31.811 (3)C7—H7C0.960
Cl1—C151.737 (4)C8—C131.374 (4)
Cl2—C191.726 (4)C8—C91.381 (4)
N1—C21.360 (5)C9—C101.390 (5)
N1—C11.387 (4)C9—H90.930
N1—C61.481 (4)C10—C111.361 (5)
N2—C51.268 (4)C10—H100.930
N2—O31.425 (4)C11—C121.357 (5)
O1—C11.199 (4)C11—H110.930
O2—C21.201 (4)C12—C131.384 (5)
O3—C31.440 (4)C12—H120.930
C2—C31.534 (5)C13—H130.930
C3—C41.550 (4)C14—C151.395 (4)
C4—C81.514 (4)C14—C191.399 (5)
C4—C51.516 (4)C15—C161.379 (5)
C4—H40.980C16—C171.365 (6)
C5—C141.482 (4)C16—H160.930
C6—C71.505 (5)C17—C181.367 (6)
C6—H6A0.970C17—H170.930
C6—H6B0.970C18—C191.393 (5)
C7—H7A0.960C18—H180.930
C1—S1—C393.10 (17)H7B—C7—H7C109.5
C2—N1—C1116.5 (3)C13—C8—C9118.7 (3)
C2—N1—C6122.8 (3)C13—C8—C4122.3 (3)
C1—N1—C6120.7 (3)C9—C8—C4119.0 (3)
C5—N2—O3109.0 (3)C8—C9—C10119.8 (3)
N2—O3—C3110.5 (2)C8—C9—H9120.1
O1—C1—N1124.7 (4)C10—C9—H9120.1
O1—C1—S1123.8 (3)C11—C10—C9120.6 (4)
N1—C1—S1111.5 (3)C11—C10—H10119.7
O2—C2—N1125.1 (4)C9—C10—H10119.7
O2—C2—C3121.7 (4)C12—C11—C10120.0 (4)
N1—C2—C3113.2 (3)C12—C11—H11120.0
O3—C3—C2106.7 (3)C10—C11—H11120.0
O3—C3—C4105.2 (3)C11—C12—C13120.0 (3)
C2—C3—C4112.0 (3)C11—C12—H12120.0
O3—C3—S1109.1 (2)C13—C12—H12120.0
C2—C3—S1105.6 (2)C8—C13—C12120.9 (3)
C4—C3—S1117.7 (2)C8—C13—H13119.5
C8—C4—C5115.1 (3)C12—C13—H13119.5
C8—C4—C3117.2 (3)C15—C14—C19116.2 (3)
C5—C4—C399.9 (3)C15—C14—C5121.4 (3)
C8—C4—H4108.0C19—C14—C5122.4 (3)
C5—C4—H4108.0C16—C15—C14122.4 (3)
C3—C4—H4108.0C16—C15—Cl1117.8 (3)
N2—C5—C14119.0 (3)C14—C15—Cl1119.8 (3)
N2—C5—C4115.1 (3)C17—C16—C15119.6 (4)
C14—C5—C4125.9 (3)C17—C16—H16120.2
N1—C6—C7111.7 (3)C15—C16—H16120.2
N1—C6—H6A109.3C16—C17—C18120.6 (4)
C7—C6—H6A109.3C16—C17—H17119.7
N1—C6—H6B109.3C18—C17—H17119.7
C7—C6—H6B109.3C17—C18—C19119.7 (4)
H6A—C6—H6B107.9C17—C18—H18120.1
C6—C7—H7A109.5C19—C18—H18120.1
C6—C7—H7B109.5C18—C19—C14121.4 (4)
H7A—C7—H7B109.5C18—C19—Cl2118.2 (3)
C6—C7—H7C109.5C14—C19—Cl2120.4 (3)
H7A—C7—H7C109.5
C5—N2—O3—C32.5 (4)C3—C4—C5—C14178.3 (3)
C2—N1—C1—O1178.5 (4)C2—N1—C6—C791.1 (4)
C6—N1—C1—O10.3 (5)C1—N1—C6—C786.8 (4)
C2—N1—C1—S13.2 (4)C5—C4—C8—C1353.7 (4)
C6—N1—C1—S1178.7 (3)C3—C4—C8—C1363.2 (4)
C3—S1—C1—O1179.6 (3)C5—C4—C8—C9129.2 (3)
C3—S1—C1—N12.0 (3)C3—C4—C8—C9113.8 (3)
C1—N1—C2—O2176.7 (4)C13—C8—C9—C100.4 (5)
C6—N1—C2—O21.4 (6)C4—C8—C9—C10176.8 (3)
C1—N1—C2—C32.9 (5)C8—C9—C10—C110.6 (6)
C6—N1—C2—C3179.1 (3)C9—C10—C11—C121.0 (6)
N2—O3—C3—C2123.4 (3)C10—C11—C12—C130.4 (6)
N2—O3—C3—C44.3 (4)C9—C8—C13—C121.0 (5)
N2—O3—C3—S1122.9 (3)C4—C8—C13—C12176.0 (3)
O2—C2—C3—O362.3 (5)C11—C12—C13—C80.6 (5)
N1—C2—C3—O3117.3 (3)N2—C5—C14—C15113.2 (4)
O2—C2—C3—C452.4 (5)C4—C5—C14—C1565.4 (4)
N1—C2—C3—C4128.1 (3)N2—C5—C14—C1964.6 (4)
O2—C2—C3—S1178.4 (4)C4—C5—C14—C19116.8 (4)
N1—C2—C3—S11.2 (4)C19—C14—C15—C161.6 (5)
C1—S1—C3—O3114.0 (2)C5—C14—C15—C16176.4 (3)
C1—S1—C3—C20.5 (3)C19—C14—C15—Cl1179.7 (2)
C1—S1—C3—C4126.3 (3)C5—C14—C15—Cl12.4 (4)
O3—C3—C4—C8129.1 (3)C14—C15—C16—C171.6 (6)
C2—C3—C4—C8115.3 (3)Cl1—C15—C16—C17179.6 (3)
S1—C3—C4—C87.4 (4)C15—C16—C17—C180.5 (6)
O3—C3—C4—C54.2 (3)C16—C17—C18—C190.5 (6)
C2—C3—C4—C5119.7 (3)C17—C18—C19—C140.6 (6)
S1—C3—C4—C5117.6 (3)C17—C18—C19—Cl2179.4 (3)
O3—N2—C5—C14179.3 (3)C15—C14—C19—C180.4 (5)
O3—N2—C5—C40.6 (4)C5—C14—C19—C18177.5 (3)
C8—C4—C5—N2129.5 (3)C15—C14—C19—Cl2178.3 (2)
C3—C4—C5—N23.1 (4)C5—C14—C19—Cl23.8 (4)
C8—C4—C5—C1451.9 (4)
 

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