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In the roof-shaped molecule of the title compound, C15H11NO2, a planar cyclic imide and a phenyl ring are tethered by a methyl­ene group. In the crystal structure, parallel layers of phthalimides stack along the a axis with inter­planar distances of 3.394 (2) and 3.495 (2)Å.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536806017971/ac2023sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536806017971/ac2023Isup2.hkl
Contains datablock I

CCDC reference: 610680

Key indicators

  • Single-crystal X-ray study
  • T = 100 K
  • Mean [sigma](C-C)= 0.002 Å
  • R factor = 0.043
  • wR factor = 0.108
  • Data-to-parameter ratio = 11.7

checkCIF/PLATON results

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Computing details top

Data collection: COLLECT (Hooft, 1999); cell refinement: DENZO (Otwinowski & Minor, 1997); data reduction: DENZO; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SCHAKAL99 (Keller, 1999); software used to prepare material for publication: SHELXL97, PLATON (Spek, 2003) and enCIFer (Allen et al., 2004).

2-Benzylisoindoline-1,3-dione top
Crystal data top
C15H11NO2Z = 2
Mr = 237.25F(000) = 248
Triclinic, P1Dx = 1.390 Mg m3
Hall symbol: -P 1Melting point = 384–385 K
a = 7.1159 (3) ÅMo Kα radiation, λ = 0.71073 Å
b = 8.4691 (3) ÅCell parameters from 3760 reflections
c = 10.1461 (5) Åθ = 2.1–27.0°
α = 99.480 (2)°µ = 0.09 mm1
β = 97.648 (2)°T = 100 K
γ = 106.745 (2)°Platelet, colourless
V = 566.88 (4) Å30.45 × 0.45 × 0.30 mm
Data collection top
Nonius KappaCCD
diffractometer
1709 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.057
Graphite monochromatorθmax = 27.0°, θmin = 2.1°
φ and ω scansh = 99
3760 measured reflectionsk = 107
2441 independent reflectionsl = 1212
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)] = 0.043All H-atom parameters refined
wR(F2) = 0.108 w = 1/[σ2(Fo2) + (0.045P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.00(Δ/σ)max = 0.014
2441 reflectionsΔρmax = 0.23 e Å3
209 parametersΔρmin = 0.21 e Å3
0 restraintsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.061 (8)
Special details top

Experimental. IR (neat): 1708, 1432, 1391, 1332, 1063, 938, 716, 696 cm-1.

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
C10.2687 (2)0.33335 (18)0.06927 (16)0.0177 (4)
C20.3703 (2)0.56852 (18)0.24614 (17)0.0175 (4)
C30.3183 (2)0.62295 (17)0.11800 (16)0.0161 (4)
C40.3222 (2)0.77985 (19)0.09640 (18)0.0219 (4)
H40.364 (2)0.8801 (19)0.1748 (17)0.023 (4)*
C50.2628 (2)0.7928 (2)0.03761 (18)0.0239 (4)
H50.264 (3)0.900 (2)0.0549 (19)0.042 (5)*
C60.2040 (2)0.6521 (2)0.14419 (18)0.0230 (4)
H60.159 (2)0.6662 (19)0.2384 (18)0.022 (4)*
C70.2002 (2)0.4939 (2)0.12103 (18)0.0207 (4)
H70.155 (2)0.3944 (19)0.1967 (17)0.023 (4)*
C80.2577 (2)0.48172 (17)0.01130 (16)0.0169 (4)
C90.3558 (2)0.2873 (2)0.30685 (18)0.0197 (4)
H9A0.464 (2)0.3598 (19)0.3860 (17)0.026 (5)*
H9B0.394 (2)0.1932 (19)0.2585 (16)0.026 (4)*
C100.1609 (2)0.21752 (18)0.35308 (16)0.0181 (4)
C110.0233 (2)0.06337 (19)0.28379 (17)0.0218 (4)
H110.053 (2)0.0045 (19)0.2047 (18)0.030 (5)*
C120.1583 (3)0.0027 (2)0.32373 (19)0.0265 (4)
H120.255 (2)0.106 (2)0.2750 (17)0.029 (5)*
C130.2046 (3)0.0959 (2)0.43241 (18)0.0282 (4)
H130.337 (3)0.054 (2)0.4600 (18)0.041 (5)*
C140.0688 (3)0.2502 (2)0.50149 (18)0.0270 (4)
H140.101 (3)0.3177 (19)0.5754 (18)0.032 (5)*
C150.1133 (2)0.3103 (2)0.46305 (17)0.0215 (4)
H150.213 (2)0.419 (2)0.5109 (17)0.027 (4)*
N10.33554 (18)0.39477 (14)0.20934 (13)0.0169 (3)
O10.22971 (16)0.18756 (12)0.01184 (11)0.0247 (3)
O20.43030 (16)0.65272 (13)0.36125 (12)0.0243 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0132 (8)0.0207 (8)0.0189 (9)0.0056 (6)0.0040 (7)0.0021 (7)
C20.0124 (8)0.0178 (8)0.0217 (10)0.0038 (6)0.0048 (7)0.0030 (7)
C30.0100 (8)0.0192 (8)0.0199 (9)0.0048 (6)0.0035 (7)0.0050 (7)
C40.0171 (9)0.0209 (8)0.0267 (10)0.0052 (7)0.0029 (7)0.0048 (8)
C50.0186 (9)0.0245 (9)0.0327 (11)0.0094 (7)0.0054 (8)0.0128 (8)
C60.0170 (9)0.0314 (9)0.0245 (11)0.0093 (7)0.0044 (8)0.0138 (8)
C70.0165 (9)0.0255 (9)0.0198 (10)0.0073 (7)0.0031 (7)0.0037 (7)
C80.0108 (8)0.0209 (8)0.0198 (9)0.0047 (6)0.0040 (7)0.0066 (7)
C90.0183 (9)0.0208 (8)0.0213 (10)0.0066 (7)0.0029 (7)0.0082 (7)
C100.0186 (9)0.0205 (8)0.0179 (9)0.0083 (6)0.0006 (7)0.0101 (7)
C110.0235 (10)0.0216 (8)0.0217 (10)0.0090 (7)0.0016 (8)0.0077 (7)
C120.0202 (10)0.0239 (9)0.0335 (11)0.0029 (7)0.0003 (8)0.0130 (8)
C130.0190 (10)0.0395 (10)0.0306 (11)0.0088 (8)0.0057 (8)0.0200 (9)
C140.0264 (10)0.0388 (10)0.0205 (10)0.0147 (8)0.0061 (8)0.0106 (8)
C150.0215 (9)0.0245 (9)0.0181 (10)0.0073 (7)0.0005 (7)0.0063 (7)
N10.0174 (7)0.0168 (7)0.0164 (8)0.0053 (5)0.0026 (6)0.0041 (6)
O10.0285 (7)0.0195 (6)0.0246 (7)0.0079 (5)0.0039 (5)0.0008 (5)
O20.0255 (7)0.0244 (6)0.0184 (7)0.0049 (5)0.0003 (5)0.0001 (5)
Geometric parameters (Å, º) top
C1—O11.2098 (17)C9—N11.4704 (19)
C1—N11.397 (2)C9—C101.511 (2)
C1—C81.489 (2)C9—H9A1.009 (17)
C2—O21.2134 (18)C9—H9B0.990 (15)
C2—N11.3966 (19)C10—C111.391 (2)
C2—C31.486 (2)C10—C151.394 (2)
C3—C41.375 (2)C11—C121.387 (2)
C3—C81.393 (2)C11—H110.991 (16)
C4—C51.401 (2)C12—C131.381 (2)
C4—H41.006 (16)C12—H120.978 (16)
C5—C61.390 (2)C13—C141.387 (2)
C5—H50.95 (2)C13—H131.000 (18)
C6—C71.391 (2)C14—C151.382 (2)
C6—H61.005 (17)C14—H140.961 (16)
C7—C81.380 (2)C15—H150.989 (16)
C7—H70.984 (16)
O1—C1—N1124.75 (14)C10—C9—H9A111.2 (9)
O1—C1—C8129.30 (15)N1—C9—H9B106.5 (9)
N1—C1—C8105.95 (12)C10—C9—H9B109.5 (9)
O2—C2—N1125.02 (15)H9A—C9—H9B111.6 (13)
O2—C2—C3128.94 (13)C11—C10—C15118.98 (15)
N1—C2—C3106.04 (13)C11—C10—C9120.76 (14)
C4—C3—C8121.63 (15)C15—C10—C9120.22 (14)
C4—C3—C2130.27 (15)C12—C11—C10120.53 (15)
C8—C3—C2108.11 (13)C12—C11—H11118.9 (10)
C3—C4—C5117.44 (15)C10—C11—H11120.6 (10)
C3—C4—H4120.6 (9)C13—C12—C11120.07 (16)
C5—C4—H4121.9 (9)C13—C12—H12119.3 (9)
C6—C5—C4120.90 (15)C11—C12—H12120.7 (9)
C6—C5—H5120.2 (11)C12—C13—C14119.76 (17)
C4—C5—H5118.9 (11)C12—C13—H13120.4 (10)
C7—C6—C5121.14 (16)C14—C13—H13119.8 (10)
C7—C6—H6120.4 (9)C15—C14—C13120.37 (16)
C5—C6—H6118.4 (9)C15—C14—H14119.2 (10)
C8—C7—C6117.69 (15)C13—C14—H14120.4 (10)
C8—C7—H7121.6 (9)C14—C15—C10120.28 (15)
C6—C7—H7120.7 (9)C14—C15—H15122.1 (9)
C7—C8—C3121.20 (14)C10—C15—H15117.6 (9)
C7—C8—C1130.82 (14)C2—N1—C1111.92 (13)
C3—C8—C1107.98 (13)C2—N1—C9124.19 (13)
N1—C9—C10111.20 (13)C1—N1—C9123.81 (12)
N1—C9—H9A106.7 (9)
 

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