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The title compound, C10H12N2O4, crystallizes as discrete mol­ecules disposed about crystallographic centres of symmetry, with two independent half-mol­ecules constituting the asymmetric unit of the unit cell. The succin­imide rings are essentially planar. No unusual features are observed in the molecular geometry.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805008226/lh6386sup1.cif
Contains datablocks global, 2

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536805008226/lh63862sup2.hkl
Contains datablock 2

CCDC reference: 270486

Key indicators

  • Single-crystal X-ray study
  • T = 295 K
  • Mean [sigma](C-C) = 0.002 Å
  • R factor = 0.048
  • wR factor = 0.137
  • Data-to-parameter ratio = 16.5

checkCIF/PLATON results

No syntax errors found


No errors found in this datablock

Computing details top

Data collection: MSC/AFC7 Diffractometer Control Software (Molecular Structure Corporation, 1999); cell refinement: MSC/AFC7 Diffractometer Control Software; data reduction: TEXSAN for Windows (Molecular Structure Corporation, 2001); program(s) used to solve structure: TEXSAN for Windows; program(s) used to refine structure: TEXSAN for Windows and SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: TEXSAN for Windows and PLATON (Spek, 2003).

N,N'-ethylenedisuccinimide top
Crystal data top
C10H12N2O4F(000) = 472
Mr = 224.22Dx = 1.428 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.7107 Å
Hall symbol: -P 2ybcCell parameters from 25 reflections
a = 12.5653 (13) Åθ = 8.3–10.6°
b = 8.3613 (10) ŵ = 0.11 mm1
c = 9.9285 (15) ÅT = 295 K
β = 90.694 (10)°Prismatic, colorless
V = 1043.0 (2) Å30.50 × 0.40 × 0.30 mm
Z = 4
Data collection top
Rigaku AFC-7R
diffractometer
Rint = 0.031
Radiation source: Rigaku rotating anodeθmax = 27.5°, θmin = 2.9°
Graphite monochromatorh = 716
ω–2θ scansk = 010
2655 measured reflectionsl = 1212
2396 independent reflections3 standard reflections every 150 reflections
1825 reflections with I > 2σ(I) intensity decay: 1.2%
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.048Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.137H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.0858P)2 + 0.1556P]
where P = (Fo2 + 2Fc2)/3
2396 reflections(Δ/σ)max < 0.001
145 parametersΔρmax = 0.20 e Å3
0 restraintsΔρmin = 0.34 e Å3
Special details top

Experimental. The scan width was (1.70 + 0.30tanθ)° with an ω scan speed of 16° per minute (up to 4 scans to achieve I/σ(I) > 10). Stationary background counts were recorded at each end of the scan, and the scan time:background time ratio was 2:1.

Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su's are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles

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 > 2σ(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
O210.27827 (8)0.14811 (15)0.44453 (11)0.0479 (4)
O510.51818 (10)0.14448 (18)0.21134 (13)0.0623 (5)
N10.40577 (9)0.01381 (14)0.35400 (11)0.0326 (3)
C110.45740 (11)0.05978 (17)0.47970 (14)0.0364 (4)
C210.31874 (10)0.08840 (17)0.34728 (14)0.0334 (4)
C310.28656 (12)0.1055 (2)0.20148 (15)0.0435 (5)
C410.36857 (13)0.0112 (2)0.12343 (15)0.0431 (4)
C510.44123 (11)0.06040 (19)0.22852 (15)0.0378 (4)
O220.21295 (8)0.30734 (14)0.06096 (11)0.0472 (3)
O520.03527 (9)0.57812 (17)0.29858 (13)0.0599 (5)
N20.07448 (9)0.44313 (14)0.15613 (11)0.0342 (3)
C120.00104 (11)0.42676 (18)0.04488 (15)0.0389 (4)
C220.17597 (10)0.37805 (16)0.15513 (14)0.0337 (4)
C320.22731 (12)0.4122 (2)0.29009 (16)0.0449 (5)
C420.14505 (13)0.50345 (19)0.36953 (15)0.0424 (4)
C520.04993 (11)0.51648 (18)0.27671 (14)0.0376 (4)
H11A0.493600.158600.467900.0440*
H11B0.405300.071900.547600.0440*
H31A0.287400.214900.175400.0520*
H31B0.217300.062900.186500.0520*
H41A0.407200.079900.065500.0520*
H41B0.335000.070400.071700.0520*
H12A0.070300.409700.079400.0470*
H12B0.018600.338200.009400.0470*
H32A0.289600.475100.279200.0540*
H32B0.245400.315200.334500.0540*
H42A0.170900.606700.392900.0510*
H42B0.127300.446800.449100.0510*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O210.0437 (6)0.0538 (7)0.0461 (6)0.0098 (5)0.0021 (5)0.0039 (5)
O510.0515 (7)0.0746 (9)0.0607 (8)0.0214 (7)0.0013 (6)0.0183 (7)
N10.0297 (5)0.0358 (6)0.0321 (6)0.0017 (4)0.0067 (4)0.0010 (5)
C110.0341 (7)0.0399 (7)0.0349 (7)0.0011 (6)0.0093 (5)0.0073 (6)
C210.0277 (6)0.0348 (7)0.0376 (7)0.0015 (5)0.0051 (5)0.0014 (5)
C310.0376 (7)0.0536 (9)0.0389 (8)0.0024 (7)0.0125 (6)0.0059 (7)
C410.0471 (8)0.0491 (8)0.0330 (7)0.0063 (7)0.0071 (6)0.0021 (6)
C510.0343 (7)0.0407 (7)0.0382 (7)0.0022 (6)0.0041 (6)0.0072 (6)
O220.0414 (6)0.0504 (6)0.0498 (6)0.0032 (5)0.0060 (5)0.0085 (5)
O520.0443 (7)0.0713 (9)0.0641 (8)0.0138 (6)0.0029 (6)0.0178 (7)
N20.0311 (6)0.0378 (6)0.0336 (6)0.0026 (5)0.0058 (4)0.0021 (5)
C120.0343 (7)0.0410 (8)0.0413 (8)0.0027 (6)0.0090 (6)0.0002 (6)
C220.0304 (6)0.0330 (7)0.0378 (7)0.0005 (5)0.0006 (5)0.0032 (5)
C320.0369 (7)0.0563 (9)0.0413 (8)0.0039 (7)0.0099 (6)0.0035 (7)
C420.0470 (8)0.0450 (8)0.0351 (7)0.0028 (7)0.0062 (6)0.0023 (6)
C520.0390 (8)0.0360 (7)0.0379 (7)0.0004 (6)0.0010 (6)0.0028 (6)
Geometric parameters (Å, º) top
O21—C211.2050 (18)C11—H11B0.9500
O51—C511.209 (2)C31—H31B0.9500
O22—C221.2042 (18)C31—H31A0.9500
O52—C521.2102 (19)C41—H41B0.9500
N1—C211.3889 (18)C41—H41A0.9500
N1—C511.3841 (19)C12—C12ii1.515 (2)
N1—C111.4514 (18)C22—C321.507 (2)
N2—C121.4539 (18)C32—C421.514 (2)
N2—C521.3833 (18)C42—C521.504 (2)
N2—C221.3866 (17)C12—H12A0.9500
C11—C11i1.516 (2)C12—H12B0.9500
C21—C311.505 (2)C32—H32A0.9500
C31—C411.518 (2)C32—H32B0.9500
C41—C511.503 (2)C42—H42A0.9500
C11—H11A0.9500C42—H42B0.9500
O21···O22iii3.1861 (17)C21···O51x3.091 (2)
O21···C22iii3.3449 (18)C22···O21v3.3449 (18)
O21···C31iv3.280 (2)C22···O52viii3.1057 (19)
O22···C11v3.3734 (18)C31···O21xii3.280 (2)
O22···C32v3.263 (2)C31···O51x3.330 (2)
O22···C42v3.325 (2)C32···O22iii3.263 (2)
O22···C413.358 (2)C41···O223.358 (2)
O22···O21v3.1861 (17)C42···O22iii3.325 (2)
O51···C31vi3.330 (2)C21···H11Ai3.0300
O51···C21vi3.091 (2)C32···H41Biii3.0900
O52···N2vii3.1249 (19)C52···H12Bii3.0300
O52···C22vii3.1057 (19)H11A···O512.5700
O52···C12vii3.332 (2)H11A···C21i3.0300
O21···H11B2.6300H11A···H41Avi2.5400
O21···H12Aviii2.6700H11B···O212.6300
O21···H31Aiv2.5600H11B···O22iii2.6200
O21···H42Aix2.5000H12A···O522.6200
O22···H12B2.5400H12A···O21vii2.6700
O22···H41B2.5100H12B···C52ii3.0300
O22···H11Bv2.6200H12B···O222.5400
O22···H32Bv2.5100H31A···O21xii2.5600
O22···H42Bv2.6200H31B···O52viii2.5800
O51···H11A2.5700H32A···O51vi2.8000
O51···H32Ax2.8000H32B···O22iii2.5100
O52···H12A2.6200H41A···H11Ax2.5400
O52···H42Bxi2.7800H41B···C32v3.0900
O52···H31Bvii2.5800H41B···O222.5100
N2···O52viii3.1249 (19)H42A···O21xiii2.5000
C11···O22iii3.3734 (18)H42B···O52xi2.7800
C12···O52viii3.332 (2)H42B···O22iii2.6200
C11—N1—C21123.21 (11)C51—C41—H41A111.00
C11—N1—C51123.64 (12)C51—C41—H41B111.00
C21—N1—C51113.07 (11)C31—C41—H41A110.00
C12—N2—C52123.29 (11)N2—C12—C12ii110.79 (12)
C22—N2—C52113.26 (11)O22—C22—N2124.18 (13)
C12—N2—C22123.33 (11)O22—C22—C32128.18 (12)
N1—C11—C11i111.16 (11)N2—C22—C32107.64 (11)
O21—C21—N1123.79 (13)C22—C32—C42105.73 (12)
O21—C21—C31128.33 (13)C32—C42—C52105.05 (12)
N1—C21—C31107.87 (12)O52—C52—N2123.45 (13)
C21—C31—C41105.40 (12)O52—C52—C42128.24 (14)
C31—C41—C51105.25 (12)N2—C52—C42108.31 (12)
O51—C51—N1123.87 (14)N2—C12—H12A109.00
O51—C51—C41127.87 (14)N2—C12—H12B109.00
N1—C51—C41108.26 (12)H12A—C12—H12B109.00
C11i—C11—H11A106.00C12ii—C12—H12A111.00
C11i—C11—H11B112.00C12ii—C12—H12B107.00
N1—C11—H11A109.00C22—C32—H32A110.00
N1—C11—H11B109.00C22—C32—H32B110.00
H11A—C11—H11B109.00C42—C32—H32A110.00
C21—C31—H31A110.00C42—C32—H32B110.00
C21—C31—H31B110.00H32A—C32—H32B109.00
C41—C31—H31A111.00C32—C42—H42A111.00
C41—C31—H31B111.00C32—C42—H42B111.00
H31A—C31—H31B109.00C52—C42—H42A111.00
C31—C41—H41B110.00C52—C42—H42B111.00
H41A—C41—H41B109.00H42A—C42—H42B109.00
C21—N1—C11—C11i87.24 (15)C22—N2—C52—O52178.74 (14)
C51—N1—C11—C11i89.34 (16)C22—N2—C52—C420.89 (16)
C11—N1—C21—O210.0 (2)C52—N2—C22—C320.64 (16)
C11—N1—C21—C31179.10 (12)C12—N2—C52—O522.6 (2)
C51—N1—C21—O21176.87 (14)N1—C11—C11i—N1i180.00 (11)
C51—N1—C21—C314.00 (16)O21—C21—C31—C41177.28 (15)
C11—N1—C51—O510.4 (2)N1—C21—C31—C413.64 (16)
C11—N1—C51—C41179.50 (12)C21—C31—C41—C512.09 (16)
C21—N1—C51—O51177.30 (15)C31—C41—C51—O51179.77 (17)
C21—N1—C51—C412.62 (17)C31—C41—C51—N10.14 (17)
C52—N2—C12—C12ii87.17 (16)N2—C12—C12ii—N2ii179.98 (14)
C12—N2—C22—O223.0 (2)O22—C22—C32—C42179.64 (15)
C22—N2—C12—C12ii97.03 (15)N2—C22—C32—C420.12 (15)
C12—N2—C52—C42177.08 (12)C22—C32—C42—C520.37 (16)
C12—N2—C22—C32176.83 (12)C32—C42—C52—O52178.86 (16)
C52—N2—C22—O22179.13 (14)C32—C42—C52—N20.75 (16)
Symmetry codes: (i) x+1, y, z+1; (ii) x, y+1, z; (iii) x, y+1/2, z+1/2; (iv) x, y1/2, z+1/2; (v) x, y+1/2, z1/2; (vi) x+1, y+1/2, z+1/2; (vii) x, y+1/2, z+1/2; (viii) x, y1/2, z+1/2; (ix) x, y1, z; (x) x+1, y1/2, z+1/2; (xi) x, y+1, z+1; (xii) x, y1/2, z1/2; (xiii) x, y+1, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C12—H12B···O220.952.542.8709 (18)100
C31—H31A···O21xii0.952.563.280 (2)132
C31—H31B···O52viii0.952.583.511 (2)167
C32—H32B···O22iii0.952.513.263 (2)136
C41—H41B···O220.952.513.358 (2)149
C42—H42A···O21xiii0.952.503.437 (2)167
Symmetry codes: (iii) x, y+1/2, z+1/2; (viii) x, y1/2, z+1/2; (xii) x, y1/2, z1/2; (xiii) x, y+1, z.
 

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