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In the title compound, C13H10ClNO3, the dihedral angle between the two rings is 68.9 (3)°. The crystal structure is stabilized by weak inter­molecular C—H...O hydrogen bonds.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805039838/bh6055sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536805039838/bh6055Isup2.hkl
Contains datablock I

CCDC reference: 296522

Key indicators

  • Single-crystal X-ray study
  • T = 298 K
  • Mean [sigma](C-C) = 0.004 Å
  • R factor = 0.049
  • wR factor = 0.150
  • Data-to-parameter ratio = 12.8

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT029_ALERT_3_C _diffrn_measured_fraction_theta_full Low ....... 0.97 PLAT150_ALERT_1_C Volume as Calculated Differs from that Given ... 1214.40 Ang-3 PLAT340_ALERT_3_C Low Bond Precision on C-C bonds (x 1000) Ang ... 5
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 3 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion

Comment top

We have investigated the photo-induced reaction of 3,4-dichloromaleimide (3,4-dichloro-pyrrole-2,5-dione) and 2-trimethylsiloxyphenylethene, and obtained the title compound, (I), as one of the products. An X-ray crystallographic analysis was undertaken to establish its structure and configuration.

In the structure of (I) (Fig. 1), bond lengths and angles are in good agreement with the expected values (Allen et al., 1987). Both the maleimide ring and the phenyl ring are planar to within ±0.02 Å. The carbonyl group linked to the phenyl ring is nearly in the plane of the phenyl ring, with atom C7 deviating by 0.019 (3) Å. Similarly, atom Cll is in the plane of the maleimide ring, with a deviation of 0.045 (3) Å. On the other hand, the methylene group lies approximately on the cross line of the two ring planes. The calculated deviations for this atom from the phenyl and maleimide rings are 0.058 (2) and 0.100 (2) Å, respectively. Finally, the dihedral angle between the phenyl and maleimide rings is 68.9 (3)°.

In the packing of the title compound, the molecules are linked into layers (Fig. 2) by C3—H3A···O3 and C8—H8B···O1 intermolecular contacts (Table 2). No significant ππ interactions are observed in the crystal structure.

Experimental top

The title compound was one of the products of a photo-induced reaction between 3,4-dichloromaleimide (3,4-dichloro-pyrrole-2,5-dione) and an excess amount of 2-trimethylsiloxyphenylethene in benzene [Please give brief details of quantities, volume of solvent, wavelength of radiation, time etc.]. The title compound was isolated using column chromatography (yield 35%). Single crystals suitable for X-ray diffraction analysis were obtained by slow evaporation of a petroleum ether–ethyl acetate (4:1) solution.

Refinement top

H atoms were positioned geometrically and treated as riding on their parent C atoms, with C—H distances constrained to 0.93 (aromatic CH), 0.97 (methylene CH2) or 0.96 Å (methyl CH3), and with Uiso(H) = 1.2Ueq(C) for aromatic CH and methylene CH2, or 1.5Ueq(C) for the methyl group.

Computing details top

Data collection: CAD-4 Software (Enraf–Nonius, 1989); cell refinement: CAD-4 Software; data reduction: XCAD4 (Harms & Wocadlo, 1995); program(s) used to solve structure: SHELXTL (Sheldrick, 1997); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 2003).

Figures top
[Figure 1] Fig. 1. The structure of (I), showing 30% probability displacement ellipsoids and the atom-numbering scheme.
[Figure 2] Fig. 2. The packing structure of (I), viewed along [100].
3-Benzoylmethyl-2-chloro-N-methylmaleimide top
Crystal data top
C13H10ClNO3F(000) = 544
Mr = 263.67Dx = 1.442 Mg m3
Monoclinic, P21/nMelting point: 448.2 K
Hall symbol: -P 2ynMo Kα radiation, λ = 0.71073 Å
a = 5.474 (2) ÅCell parameters from 25 reflections
b = 24.185 (3) Åθ = 1.7–25.0°
c = 9.283 (2) ŵ = 0.31 mm1
β = 98.78 (3)°T = 298 K
V = 1214.4 (5) Å3Block, colourless
Z = 40.40 × 0.40 × 0.10 mm
Data collection top
Enraf–Nonius CAD-4
diffractometer
1321 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.066
Graphite monochromatorθmax = 25.0°, θmin = 1.7°
ω/2θ scansh = 06
Absorption correction: ψ scan
(XCAD4; Harms & Wocadlo, 1995)
k = 028
Tmin = 0.885, Tmax = 0.965l = 1110
2298 measured reflections3 standard reflections every 200 reflections
2085 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)] = 0.049H-atom parameters constrained
wR(F2) = 0.150 w = 1/[σ2(Fo2) + (0.0337P)2 + P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max = 0.003
2085 reflectionsΔρmax = 0.32 e Å3
163 parametersΔρmin = 0.26 e Å3
0 restraintsExtinction correction: SHELXTL (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.022 (3)
Crystal data top
C13H10ClNO3V = 1214.4 (5) Å3
Mr = 263.67Z = 4
Monoclinic, P21/nMo Kα radiation
a = 5.474 (2) ŵ = 0.31 mm1
b = 24.185 (3) ÅT = 298 K
c = 9.283 (2) Å0.40 × 0.40 × 0.10 mm
β = 98.78 (3)°
Data collection top
Enraf–Nonius CAD-4
diffractometer
1321 reflections with I > 2σ(I)
Absorption correction: ψ scan
(XCAD4; Harms & Wocadlo, 1995)
Rint = 0.066
Tmin = 0.885, Tmax = 0.9653 standard reflections every 200 reflections
2298 measured reflections intensity decay: none
2085 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0490 restraints
wR(F2) = 0.150H-atom parameters constrained
S = 1.03Δρmax = 0.32 e Å3
2085 reflectionsΔρmin = 0.26 e Å3
163 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
N0.1184 (4)0.11267 (11)0.4283 (3)0.0471 (6)
O10.2122 (4)0.27081 (9)0.2373 (3)0.0677 (7)
O20.2164 (4)0.19502 (9)0.5287 (2)0.0599 (6)
O30.0564 (5)0.04984 (10)0.2877 (3)0.0679 (7)
C10.2725 (7)0.42659 (15)0.4167 (4)0.0636 (10)
H1A0.42010.44100.46520.076*
C20.0843 (8)0.46136 (15)0.3606 (4)0.0674 (11)
H2A0.10650.49940.36980.081*
C30.1370 (7)0.44084 (15)0.2909 (4)0.0649 (10)
H3A0.26490.46480.25520.078*
C40.1677 (6)0.38457 (14)0.2744 (3)0.0530 (8)
H4A0.31660.37060.22650.064*
C50.0209 (5)0.34839 (12)0.3283 (3)0.0422 (7)
C60.2421 (6)0.36993 (13)0.4009 (4)0.0512 (8)
H6A0.36960.34620.43890.061*
C70.0222 (5)0.28831 (13)0.3063 (3)0.0424 (7)
C80.1775 (6)0.24851 (13)0.3731 (4)0.0482 (8)
H8A0.31910.25190.32240.058*
H8B0.23040.25860.47430.058*
C90.0931 (5)0.19025 (12)0.3660 (3)0.0411 (7)
C100.0976 (5)0.16902 (13)0.4524 (3)0.0443 (7)
C110.0328 (6)0.09613 (13)0.3307 (3)0.0455 (7)
C120.1621 (5)0.14741 (12)0.2931 (3)0.0436 (7)
C130.2828 (7)0.07543 (15)0.4933 (4)0.0643 (10)
H13A0.26300.03840.45970.097*
H13B0.45110.08690.46510.097*
H13C0.24180.07660.59750.097*
Cl0.36553 (16)0.14479 (4)0.17204 (9)0.0645 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N0.0496 (15)0.0452 (16)0.0495 (15)0.0031 (12)0.0172 (12)0.0047 (11)
O10.0555 (15)0.0588 (15)0.0793 (16)0.0098 (12)0.0202 (13)0.0021 (12)
O20.0616 (14)0.0650 (16)0.0573 (14)0.0040 (12)0.0224 (12)0.0097 (11)
O30.0755 (17)0.0481 (16)0.0850 (17)0.0023 (12)0.0283 (14)0.0060 (12)
C10.069 (2)0.059 (2)0.066 (2)0.0207 (19)0.0246 (19)0.0201 (18)
C20.094 (3)0.044 (2)0.077 (3)0.004 (2)0.052 (2)0.0083 (18)
C30.071 (2)0.054 (2)0.074 (2)0.0184 (18)0.029 (2)0.0080 (18)
C40.0515 (19)0.055 (2)0.0566 (19)0.0056 (15)0.0205 (15)0.0031 (16)
C50.0448 (17)0.0464 (18)0.0379 (15)0.0001 (13)0.0142 (13)0.0011 (13)
C60.0486 (18)0.054 (2)0.0523 (18)0.0066 (15)0.0108 (15)0.0038 (15)
C70.0411 (17)0.0490 (18)0.0370 (15)0.0045 (14)0.0053 (13)0.0030 (13)
C80.0441 (16)0.0469 (18)0.0531 (18)0.0034 (13)0.0060 (14)0.0025 (14)
C90.0399 (16)0.0419 (17)0.0411 (16)0.0008 (13)0.0046 (12)0.0034 (13)
C100.0449 (17)0.0474 (18)0.0400 (16)0.0016 (14)0.0046 (14)0.0010 (14)
C110.0484 (17)0.0417 (18)0.0457 (17)0.0026 (14)0.0052 (14)0.0014 (14)
C120.0414 (16)0.0509 (18)0.0400 (16)0.0022 (13)0.0111 (13)0.0057 (14)
C130.064 (2)0.065 (2)0.069 (2)0.0120 (18)0.0271 (19)0.0113 (18)
Cl0.0606 (6)0.0790 (7)0.0604 (5)0.0022 (4)0.0299 (4)0.0015 (4)
Geometric parameters (Å, º) top
N—C111.377 (4)C5—C61.394 (4)
N—C101.383 (4)C5—C71.481 (4)
N—C131.466 (4)C6—H6A0.9300
O1—C71.211 (3)C7—C81.516 (4)
O2—C101.208 (4)C8—C91.481 (4)
O3—C111.202 (3)C8—H8A0.9700
C1—C21.369 (5)C8—H8B0.9700
C1—C61.385 (4)C9—C121.324 (4)
C1—H1A0.9300C9—C101.501 (4)
C2—C31.376 (5)C11—C121.495 (4)
C2—H2A0.9300C12—Cl1.700 (3)
C3—C41.377 (5)C13—H13A0.9600
C3—H3A0.9300C13—H13B0.9600
C4—C51.387 (4)C13—H13C0.9600
C4—H4A0.9300
C11—N—C10110.6 (3)C9—C8—C7112.6 (3)
C11—N—C13124.1 (3)C9—C8—H8A109.1
C10—N—C13125.4 (3)C7—C8—H8A109.1
C2—C1—C6119.8 (3)C9—C8—H8B109.1
C2—C1—H1A120.0C7—C8—H8B109.1
C6—C1—H1A120.0H8A—C8—H8B107.8
C1—C2—C3120.9 (3)C12—C9—C8131.1 (3)
C1—C2—H2A119.8C12—C9—C10106.3 (3)
C3—C2—H2A119.8C8—C9—C10122.6 (3)
C4—C3—C2119.8 (4)O2—C10—N124.7 (3)
C4—C3—H3A120.1O2—C10—C9127.8 (3)
C2—C3—H3A120.1N—C10—C9107.1 (3)
C3—C4—C5120.7 (3)O3—C11—N126.5 (3)
C3—C4—H4A119.7O3—C11—C12128.0 (3)
C5—C4—H4A119.7N—C11—C12105.5 (3)
C6—C5—C4118.6 (3)C9—C12—C11110.4 (3)
C6—C5—C7123.1 (3)C9—C12—Cl129.2 (3)
C4—C5—C7118.3 (3)C11—C12—Cl120.4 (2)
C1—C6—C5120.3 (3)N—C13—H13A109.5
C1—C6—H6A119.9N—C13—H13B109.5
C5—C6—H6A119.9H13A—C13—H13B109.5
O1—C7—C5121.7 (3)N—C13—H13C109.5
O1—C7—C8119.8 (3)H13A—C13—H13C109.5
C5—C7—C8118.5 (3)H13B—C13—H13C109.5
C6—C1—C2—C31.1 (6)C11—N—C10—C92.3 (3)
C1—C2—C3—C41.3 (6)C13—N—C10—C9179.4 (3)
C2—C3—C4—C50.3 (5)C12—C9—C10—O2176.2 (3)
C3—C4—C5—C60.7 (5)C8—C9—C10—O25.2 (5)
C3—C4—C5—C7179.5 (3)C12—C9—C10—N3.0 (3)
C2—C1—C6—C50.1 (5)C8—C9—C10—N175.5 (3)
C4—C5—C6—C10.8 (5)C10—N—C11—O3180.0 (3)
C7—C5—C6—C1179.4 (3)C13—N—C11—O31.7 (6)
C6—C5—C7—O1176.7 (3)C10—N—C11—C120.8 (3)
C4—C5—C7—O13.5 (5)C13—N—C11—C12179.1 (3)
C6—C5—C7—C83.5 (4)C8—C9—C12—C11175.8 (3)
C4—C5—C7—C8176.3 (3)C10—C9—C12—C112.6 (3)
O1—C7—C8—C910.1 (4)C8—C9—C12—Cl3.7 (5)
C5—C7—C8—C9169.7 (3)C10—C9—C12—Cl177.9 (2)
C7—C8—C9—C12113.5 (4)O3—C11—C12—C9177.9 (3)
C7—C8—C9—C1068.3 (4)N—C11—C12—C91.3 (4)
C11—N—C10—O2177.0 (3)O3—C11—C12—Cl1.6 (5)
C13—N—C10—O21.3 (5)N—C11—C12—Cl179.2 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C13—H13A···O30.952.552.925 (5)102
C3—H3A···O3i0.932.593.499 (5)163
C8—H8B···O1ii0.972.513.375 (5)147
Symmetry codes: (i) x1/2, y+1/2, z+1/2; (ii) x+1/2, y+1/2, z+1/2.

Experimental details

Crystal data
Chemical formulaC13H10ClNO3
Mr263.67
Crystal system, space groupMonoclinic, P21/n
Temperature (K)298
a, b, c (Å)5.474 (2), 24.185 (3), 9.283 (2)
β (°) 98.78 (3)
V3)1214.4 (5)
Z4
Radiation typeMo Kα
µ (mm1)0.31
Crystal size (mm)0.40 × 0.40 × 0.10
Data collection
DiffractometerEnraf–Nonius CAD-4
diffractometer
Absorption correctionψ scan
(XCAD4; Harms & Wocadlo, 1995)
Tmin, Tmax0.885, 0.965
No. of measured, independent and
observed [I > 2σ(I)] reflections
2298, 2085, 1321
Rint0.066
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.049, 0.150, 1.03
No. of reflections2085
No. of parameters163
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.32, 0.26

Computer programs: CAD-4 Software (Enraf–Nonius, 1989), CAD-4 Software, XCAD4 (Harms & Wocadlo, 1995), SHELXTL (Sheldrick, 1997), SHELXTL and PLATON (Spek, 2003).

Selected geometric parameters (Å, º) top
O1—C71.211 (3)C7—C81.516 (4)
C5—C71.481 (4)C12—Cl1.700 (3)
C5—C7—C8118.5 (3)C11—C12—Cl120.4 (2)
C9—C8—C7112.6 (3)
C6—C5—C7—C83.5 (4)C7—C8—C9—C1068.3 (4)
C5—C7—C8—C9169.7 (3)N—C11—C12—Cl179.2 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C3—H3A···O3i0.932.593.499 (5)163
C8—H8B···O1ii0.972.513.375 (5)147
Symmetry codes: (i) x1/2, y+1/2, z+1/2; (ii) x+1/2, y+1/2, z+1/2.
 

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