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Although mol­ecules of the title compound, 3,4-di­chloro-2,5-dihydro­furan-2,5-dione (di­chloro­maleic anhydride, C4Cl2O3), (I), possess approximate non-crystallographic C2v symmetry, the two chlorine substituents deviate from the ring plane. Their deviations are in the same direction, but with values of 0.0356 (17) and 0.0167 (17) Å, they differ significantly in magnitude. The closest intermolecular contact is of 2.888 (2) Å between a carbonyl O atom and the C atom of a carbonyl group, with the O...C direction orthogonal to the C=O bond [O5...C2i=O2i 93.6 (2)°; symmetry code: (i) 3 \over 2 - x, -½ + y, z]. These contacts form infinite chains of mol­ecules running parallel to the crystallographic b direction.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270100007034/qa0304sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270100007034/qa0304Isup2.hkl
Contains datablock I

CCDC reference: 146107

Computing details top

Data collection: SMART (Bruker, 1998); cell refinement: SMART; data reduction: SAINT (Bruker, 1999); program(s) used to solve structure: SHELXTL (Bruker, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); software used to prepare material for publication: SHELXL97 and PLATON (Spek, 1999).

(I) top
Crystal data top
C4Cl2O3F(000) = 656
Mr = 166.94Dx = 1.941 Mg m3
Orthorhombic, PbcaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2abCell parameters from 5130 reflections
a = 10.6397 (6) Åθ = 3.1–28.6°
b = 8.2558 (5) ŵ = 1.05 mm1
c = 13.0057 (7) ÅT = 150 K
V = 1142.41 (11) Å3Block, colourless
Z = 80.32 × 0.32 × 0.25 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
1372 independent reflections
Radiation source: fine-focus sealed tube1261 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.013
ω scansθmax = 28.6°, θmin = 3.1°
Absorption correction: multi-scan
(SADABS; Bruker, 1996)
h = 014
Tmin = 0.730, Tmax = 0.779k = 011
7980 measured reflectionsl = 017
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.041P)2 + 0.34P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.023(Δ/σ)max = 0.001
wR(F2) = 0.067Δρmax = 0.35 e Å3
S = 1.04Δρmin = 0.21 e Å3
1372 reflectionsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
83 parametersExtinction coefficient: 0.0056 (7)
0 restraints
Special details top

Geometry. Least-squares planes (x,y,z in crystal coordinates) and deviations from them (* indicates atom used to define plane)

5.8224 (0.0054) x + 6.8975 (0.0028) y - 0.6529 (0.0066) z = 4.1943 (0.0036)

* -0.0007 (0.0006) O1 * 0.0023 (0.0006) C2 * -0.0031 (0.0007) C3 * 0.0028 (0.0007) C4 * -0.0012 (0.0006) C5 - 0.0039 (0.0017) O2 - 0.0023 (0.0018) O5 - 0.0356 (0.0017) Cl3 - 0.0167 (0.0017) Cl4

Rms deviation of fitted atoms = 0.0022 ___________________________________________________________________

Short Non-Hydrogen Inter-Molecular Contacts

Contact-Nr Atom I [ARU] Atom J [ARU] d(I—J) Del ——————————————————————- 1 O(2) [1555.01] ··· C(4) [4655.01] = 3.019 - 0.20 2 O(2) [1555.01] ··· C(5) [4655.01] = 3.011 - 0.21 3 O(5) [1555.01] ··· C(2) [7645.01] = 2.888 - 0.33

[4655.01] = 1 - x,1/2 + y,1/2 - z [7645.01] = 3/2 - x,-1/2 + y,z

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
O10.62393 (8)0.09767 (10)0.17283 (6)0.0261 (2)
C20.53423 (10)0.17933 (13)0.23110 (9)0.0241 (2)
O20.44778 (10)0.24782 (10)0.19319 (8)0.0319 (2)
C30.56901 (11)0.15962 (13)0.34126 (9)0.0232 (2)
Cl30.48172 (3)0.23767 (4)0.43703 (3)0.03491 (12)
C40.67404 (10)0.07227 (13)0.34605 (8)0.0223 (2)
Cl40.75628 (3)0.00979 (4)0.44921 (2)0.03129 (12)
C50.71187 (11)0.02966 (14)0.23941 (9)0.0235 (2)
O50.79899 (9)0.04691 (11)0.20904 (7)0.0310 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0300 (4)0.0266 (4)0.0217 (4)0.0028 (3)0.0014 (3)0.0012 (3)
C20.0239 (5)0.0197 (5)0.0287 (6)0.0025 (4)0.0006 (4)0.0003 (4)
O20.0264 (5)0.0297 (5)0.0397 (6)0.0017 (3)0.0057 (4)0.0047 (4)
C30.0244 (5)0.0210 (5)0.0241 (5)0.0036 (4)0.0034 (4)0.0017 (4)
Cl30.0336 (2)0.0363 (2)0.0348 (2)0.00032 (12)0.01382 (12)0.00629 (12)
C40.0235 (5)0.0226 (5)0.0209 (5)0.0039 (4)0.0003 (4)0.0011 (4)
Cl40.03173 (19)0.0370 (2)0.02518 (19)0.00352 (12)0.00609 (11)0.00644 (11)
C50.0250 (5)0.0203 (5)0.0253 (6)0.0020 (4)0.0001 (4)0.0001 (4)
O50.0303 (5)0.0299 (4)0.0327 (5)0.0060 (4)0.0050 (4)0.0028 (4)
Geometric parameters (Å, º) top
O1—C21.3927 (14)C3—Cl31.6820 (12)
O1—C51.3929 (14)C4—C51.4864 (16)
C2—O21.1870 (15)C4—Cl41.6829 (11)
C2—C31.4886 (16)C5—O51.1895 (15)
C3—C41.3314 (17)
C2—O1—C5108.49 (9)C3—C4—C5108.17 (10)
O2—C2—O1122.39 (11)C3—C4—Cl4129.77 (9)
O2—C2—C3130.13 (11)C5—C4—Cl4122.05 (9)
O1—C2—C3107.48 (9)O5—C5—O1122.09 (11)
C4—C3—C2108.23 (10)O5—C5—C4130.29 (11)
C4—C3—Cl3129.51 (9)O1—C5—C4107.62 (10)
C2—C3—Cl3122.25 (9)
C5—O1—C2—O2179.59 (11)C2—C3—C4—Cl4179.23 (9)
C5—O1—C2—C30.27 (11)Cl3—C3—C4—Cl40.15 (18)
O2—C2—C3—C4179.77 (12)C2—O1—C5—O5179.93 (11)
O1—C2—C3—C40.53 (13)C2—O1—C5—C40.05 (11)
O2—C2—C3—Cl30.61 (18)C3—C4—C5—O5179.74 (13)
O1—C2—C3—Cl3178.63 (7)Cl4—C4—C5—O50.94 (18)
C2—C3—C4—C50.55 (13)C3—C4—C5—O10.39 (12)
Cl3—C3—C4—C5178.53 (9)Cl4—C4—C5—O1179.19 (8)
 

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