Literature DB >> 24764976

2,3-Di-phenyl-male-imide 1-methyl-pyrrol-idin-2-one monosolvate.

Evgeny Bulatov1, Dina Boyarskaya2, Tatiana Chulkova2, Matti Haukka3.   

Abstract

In the title compound, C16H11NO2·C5H9NO, the dihedral angles between the male-imide and phenyl rings are 34.7 (2) and 64.8 (2)°. In the crystal, the 2,3-di-phenyl-male-imide and 1-methyl-pyrrolidin-2-one mol-ecules form centrosymmetrical dimers via pairs of strong N-H⋯O hydrogen bonds and π-π stacking inter-actions between the two neighboring male-imide rings [centroid-centroid distance = 3.495 (2) Å]. The dimers are further linked by weak C-H⋯O and C-H⋯π hydrogen bonds into a three-dimensional framework.

Entities:  

Year:  2014        PMID: 24764976      PMCID: PMC3998429          DOI: 10.1107/S1600536814002372

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For general background to male­imides, see: Yeh et al. (2004 ▶); Billiet et al. (2011 ▶); Zhu et al. (2012 ▶); Parsons & Du Bois (2013 ▶). For the crystal structures of related compounds, see: Zhang et al. (2004 ▶); Mitzi & Afzali (2007 ▶).

Experimental

Crystal data

C16H11NO2·C5H9NO M = 348.39 Monoclinic, a = 13.1962 (3) Å b = 10.0002 (2) Å c = 13.5600 (3) Å β = 100.469 (3)° V = 1759.65 (7) Å3 Z = 4 Mo Kα radiation μ = 0.09 mm−1 T = 170 K 0.54 × 0.40 × 0.24 mm

Data collection

Agilent SuperNova (Single source at offset, Eos) diffractometer Absorption correction: multi-scan (CrysAlis PRO, Agilent, 2013 ▶) T min = 0.815, T max = 1.000 22206 measured reflections 8818 independent reflections 5708 reflections with I > 2σ(I) R int = 0.028

Refinement

R[F 2 > 2σ(F 2)] = 0.064 wR(F 2) = 0.204 S = 1.03 8818 reflections 236 parameters H-atom parameters constrained Δρmax = 0.63 e Å−3 Δρmin = −0.30 e Å−3 Data collection: CrysAlis PRO (Agilent, 2013 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: CrystalMaker (CrystalMaker, 2011 ▶); software used to prepare material for publication: OLEX2 (Dolomanov et al., 2009 ▶) and SHELXLE (Hübschle et al., 2011 ▶). Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536814002372/kq2011sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814002372/kq2011Isup2.hkl Click here for additional data file. Supporting information file. DOI: 10.1107/S1600536814002372/kq2011Isup3.cml CCDC reference: 978501 Additional supporting information: crystallographic information; 3D view; checkCIF report
C16H11NO2·C5H9NOF(000) = 736
Mr = 348.39Dx = 1.315 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 13.1962 (3) ÅCell parameters from 5604 reflections
b = 10.0002 (2) Åθ = 3.7–36.7°
c = 13.5600 (3) ŵ = 0.09 mm1
β = 100.469 (3)°T = 170 K
V = 1759.65 (7) Å3Block, colourless
Z = 40.54 × 0.40 × 0.24 mm
Agilent SuperNova (Single source at offset, Eos) diffractometer8818 independent reflections
Radiation source: SuperNova (Mo) X-ray Source5708 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.028
Detector resolution: 16.0107 pixels mm-1θmax = 37.5°, θmin = 3.1°
φ scans and ω scans with κ offseth = −22→22
Absorption correction: multi-scan (CrysAlis PRO, Agilent, 2013)k = −13→16
Tmin = 0.815, Tmax = 1.000l = −22→23
22206 measured reflections
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.064H-atom parameters constrained
wR(F2) = 0.204w = 1/[σ2(Fo2) + (0.0916P)2 + 0.4242P] where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max < 0.001
8818 reflectionsΔρmax = 0.63 e Å3
236 parametersΔρmin = −0.30 e Å3
Experimental. Absorption correction: CrysAlis PRO (Agilent, 2013); Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
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.
xyzUiso*/Ueq
O10.06128 (8)0.79304 (9)0.09092 (7)0.0333 (2)
O20.16449 (8)0.38928 (10)−0.01022 (8)0.0365 (2)
N10.10893 (8)0.60420 (10)0.01257 (7)0.0272 (2)
H10.11270.6383−0.04650.033*
C10.13055 (9)0.47257 (12)0.04002 (9)0.0260 (2)
C20.10664 (8)0.45632 (11)0.14421 (8)0.0230 (2)
C30.12077 (8)0.33036 (11)0.20052 (9)0.0240 (2)
C40.09962 (10)0.20708 (12)0.15227 (10)0.0300 (2)
H40.07640.20420.08180.036*
C50.11244 (11)0.08926 (13)0.20683 (12)0.0366 (3)
H50.09820.00590.17360.044*
C60.14610 (11)0.09271 (14)0.31006 (12)0.0370 (3)
H60.15400.01180.34730.044*
C70.16818 (10)0.21392 (14)0.35876 (11)0.0334 (3)
H70.19180.21600.42920.040*
C80.15569 (9)0.33222 (13)0.30448 (9)0.0275 (2)
H80.17090.41520.33810.033*
C90.07716 (8)0.57673 (11)0.17357 (8)0.02304 (19)
C100.04640 (8)0.61711 (11)0.26815 (8)0.0232 (2)
C11−0.04123 (10)0.56355 (15)0.29686 (10)0.0324 (3)
H11−0.08290.50130.25470.039*
C12−0.06732 (11)0.60162 (19)0.38744 (12)0.0418 (3)
H12−0.12760.56620.40670.050*
C13−0.00602 (12)0.69086 (17)0.44990 (11)0.0406 (3)
H13−0.02410.71580.51210.049*
C140.08136 (12)0.74379 (15)0.42201 (10)0.0362 (3)
H140.12370.80420.46530.043*
C150.10711 (10)0.70841 (13)0.33056 (9)0.0290 (2)
H150.16610.74650.31050.035*
C160.08056 (9)0.67456 (12)0.09100 (9)0.0254 (2)
O30.67483 (9)0.76077 (11)0.35649 (9)0.0429 (3)
N20.65279 (9)0.53588 (12)0.32844 (9)0.0348 (2)
C170.66039 (10)0.66246 (14)0.30065 (11)0.0333 (3)
C180.64860 (19)0.66600 (18)0.18720 (12)0.0554 (5)
H18A0.59150.72630.15800.066*
H18B0.71290.69830.16720.066*
C190.62610 (16)0.52685 (18)0.15209 (12)0.0483 (4)
H19A0.67670.49660.11120.058*
H19B0.55620.52080.11090.058*
C200.63358 (14)0.44090 (16)0.24659 (13)0.0447 (4)
H20A0.56850.39170.24670.054*
H20B0.69080.37580.25140.054*
C210.65804 (14)0.4951 (2)0.43134 (12)0.0479 (4)
H21A0.59060.46130.44040.072*
H21B0.67730.57190.47570.072*
H21C0.70980.42440.44780.072*
U11U22U33U12U13U23
O10.0447 (5)0.0228 (4)0.0320 (4)0.0014 (4)0.0059 (4)0.0003 (3)
O20.0443 (5)0.0350 (5)0.0337 (5)0.0028 (4)0.0161 (4)−0.0076 (4)
N10.0337 (5)0.0265 (5)0.0219 (4)−0.0021 (4)0.0062 (4)−0.0016 (4)
C10.0263 (5)0.0271 (5)0.0247 (5)−0.0012 (4)0.0050 (4)−0.0041 (4)
C20.0235 (4)0.0221 (5)0.0232 (4)−0.0005 (3)0.0039 (4)−0.0028 (4)
C30.0219 (4)0.0218 (4)0.0283 (5)0.0014 (4)0.0046 (4)−0.0026 (4)
C40.0304 (5)0.0230 (5)0.0355 (6)0.0006 (4)0.0028 (5)−0.0054 (4)
C50.0329 (6)0.0221 (5)0.0536 (8)0.0002 (4)0.0049 (6)−0.0022 (5)
C60.0316 (6)0.0278 (6)0.0515 (8)0.0042 (5)0.0074 (6)0.0094 (6)
C70.0300 (5)0.0358 (6)0.0341 (6)0.0071 (5)0.0047 (5)0.0060 (5)
C80.0277 (5)0.0254 (5)0.0292 (5)0.0035 (4)0.0040 (4)−0.0002 (4)
C90.0242 (4)0.0219 (4)0.0230 (4)−0.0008 (4)0.0043 (4)−0.0018 (4)
C100.0249 (4)0.0219 (4)0.0234 (4)0.0016 (4)0.0054 (4)−0.0007 (4)
C110.0268 (5)0.0382 (7)0.0331 (6)−0.0036 (5)0.0077 (4)−0.0008 (5)
C120.0332 (6)0.0589 (10)0.0371 (7)−0.0004 (6)0.0163 (5)0.0034 (7)
C130.0460 (8)0.0513 (9)0.0275 (6)0.0078 (6)0.0148 (6)−0.0004 (6)
C140.0479 (7)0.0354 (7)0.0258 (5)−0.0018 (6)0.0083 (5)−0.0061 (5)
C150.0345 (6)0.0270 (5)0.0264 (5)−0.0047 (4)0.0081 (4)−0.0038 (4)
C160.0275 (5)0.0244 (5)0.0239 (5)−0.0018 (4)0.0036 (4)−0.0020 (4)
O30.0568 (6)0.0368 (5)0.0397 (5)−0.0118 (5)0.0214 (5)−0.0127 (4)
N20.0366 (5)0.0342 (6)0.0347 (6)−0.0033 (4)0.0091 (4)−0.0007 (5)
C170.0317 (5)0.0324 (6)0.0368 (6)−0.0018 (5)0.0085 (5)−0.0040 (5)
C180.0896 (14)0.0413 (9)0.0326 (7)−0.0106 (9)0.0043 (8)0.0021 (6)
C190.0630 (10)0.0473 (9)0.0359 (7)−0.0088 (8)0.0126 (7)−0.0103 (7)
C200.0566 (9)0.0310 (7)0.0478 (8)−0.0027 (6)0.0134 (7)−0.0093 (6)
C210.0487 (8)0.0598 (10)0.0359 (7)−0.0088 (8)0.0098 (6)0.0105 (7)
O1—C161.2118 (15)C11—H110.9500
O2—C11.2121 (15)C12—C131.385 (2)
N1—C161.3824 (15)C12—H120.9500
N1—C11.3835 (16)C13—C141.383 (2)
N1—H10.8800C13—H130.9500
C1—C21.5113 (16)C14—C151.3898 (18)
C2—C91.3476 (16)C14—H140.9500
C2—C31.4672 (16)C15—H150.9500
C3—C41.3998 (16)O3—C171.2344 (17)
C3—C81.4013 (17)N2—C171.3296 (19)
C4—C51.3851 (19)N2—C211.4433 (19)
C4—H40.9500N2—C201.448 (2)
C5—C61.390 (2)C17—C181.518 (2)
C5—H50.9500C18—C191.483 (2)
C6—C71.386 (2)C18—H18A0.9900
C6—H60.9500C18—H18B0.9900
C7—C81.3872 (18)C19—C201.531 (2)
C7—H70.9500C19—H19A0.9900
C8—H80.9500C19—H19B0.9900
C9—C101.4703 (15)C20—H20A0.9900
C9—C161.4936 (16)C20—H20B0.9900
C10—C111.3926 (17)C21—H21A0.9800
C10—C151.3947 (16)C21—H21B0.9800
C11—C121.388 (2)C21—H21C0.9800
C16—N1—C1110.41 (10)C12—C13—H13119.9
C16—N1—H1124.8C13—C14—C15119.86 (13)
C1—N1—H1124.8C13—C14—H14120.1
O2—C1—N1125.57 (12)C15—C14—H14120.1
O2—C1—C2127.79 (12)C14—C15—C10120.10 (12)
N1—C1—C2106.62 (10)C14—C15—H15120.0
C9—C2—C3129.02 (11)C10—C15—H15120.0
C9—C2—C1107.49 (10)O1—C16—N1125.67 (12)
C3—C2—C1123.40 (10)O1—C16—C9127.31 (11)
C4—C3—C8118.88 (11)N1—C16—C9107.01 (10)
C4—C3—C2121.14 (11)C17—N2—C21123.38 (14)
C8—C3—C2119.97 (10)C17—N2—C20114.78 (13)
C5—C4—C3120.32 (13)C21—N2—C20121.78 (14)
C5—C4—H4119.8O3—C17—N2126.55 (14)
C3—C4—H4119.8O3—C17—C18125.38 (14)
C4—C5—C6120.16 (13)N2—C17—C18108.07 (13)
C4—C5—H5119.9C19—C18—C17106.32 (14)
C6—C5—H5119.9C19—C18—H18A110.5
C7—C6—C5120.18 (13)C17—C18—H18A110.5
C7—C6—H6119.9C19—C18—H18B110.5
C5—C6—H6119.9C17—C18—H18B110.5
C6—C7—C8119.91 (13)H18A—C18—H18B108.7
C6—C7—H7120.0C18—C19—C20106.22 (13)
C8—C7—H7120.0C18—C19—H19A110.5
C7—C8—C3120.54 (12)C20—C19—H19A110.5
C7—C8—H8119.7C18—C19—H19B110.5
C3—C8—H8119.7C20—C19—H19B110.5
C2—C9—C10130.04 (11)H19A—C19—H19B108.7
C2—C9—C16108.31 (10)N2—C20—C19104.41 (13)
C10—C9—C16121.64 (10)N2—C20—H20A110.9
C11—C10—C15119.78 (11)C19—C20—H20A110.9
C11—C10—C9120.87 (11)N2—C20—H20B110.9
C15—C10—C9119.33 (10)C19—C20—H20B110.9
C12—C11—C10119.61 (13)H20A—C20—H20B108.9
C12—C11—H11120.2N2—C21—H21A109.5
C10—C11—H11120.2N2—C21—H21B109.5
C13—C12—C11120.44 (13)H21A—C21—H21B109.5
C13—C12—H12119.8N2—C21—H21C109.5
C11—C12—H12119.8H21A—C21—H21C109.5
C14—C13—C12120.19 (13)H21B—C21—H21C109.5
C14—C13—H13119.9
D—H···AD—HH···AD···AD—H···A
N1—H1···O3i0.881.952.7800 (15)156
C5—H5···O1ii0.952.413.3639 (17)179
C21—H21A···O1iii0.982.593.498 (2)154
C21—H21B···O1iv0.982.733.436 (2)129
C15—H15···Cg2v0.952.963.8081 (14)149
C20—H20A···Cg3iii0.992.913.6508 (18)133
Table 1

Hydrogen-bond geometry (Å, °)

Cg2 and Cg3 are the centroids of the C3–C8 and C10–C15 rings, respectively.

D—H⋯A D—HH⋯A DA D—H⋯A
N1—H1⋯O3i 0.881.952.7800 (15)156
C5—H5⋯O1ii 0.952.413.3639 (17)179
C21—H21A⋯O1iii 0.982.593.498 (2)154
C21—H21B⋯O1iv 0.982.733.436 (2)129
C15—H15⋯Cg2v 0.952.963.8081 (14)149
C20—H20ACg3iii 0.992.913.6508 (18)133

Symmetry codes: (i) ; (ii) ; (iii) ; (iv) ; (v) .

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