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In the title compound, C21H15NO3, which is one of the photoreaction products of N-methyl-1,8-naphthalene­dicar­box­imide with phenyl­acetyl­ene, the cyclo­butene and epoxy rings are trans to each other across the cyclo­hexene ring of the tetralin moiety. The dihedral angle between the mean planes of the cyclo­butene and cyclo­hexene rings is 112.80 (2)°, while the latter makes a dihedral angle of 103.70 (9)° with the epoxy ring. The crystal structure is stabilized by C-H...O intermolecular interactions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270102021650/ob1086sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270102021650/ob1086Isup2.hkl
Contains datablock I

CCDC reference: 204049

Comment top

The photochemistry of imides with alkenes has been extensively studied (Kanaoka, 1978; Mazzocchi, 1981). However, the photochemical reactions of imides with alkynes have not been reported to date. As part of our studies of the photoinduced electron-transfer reactions of aromatic imides with various organic electron donors (Xue et al., 2000), we have investigated the photoinduced reactions of naphthalimides with alkynes. Here, we report the crystal structure of the title compound, (I), which is one of the products of the photoreaction of N-methyl-1,8-naphthalenedicarboximide with phenylacetylene. \sch

The bond lengths and angles in (I) show normal values, except for the geometry of the cyclobutene ring (Table 1). The C7—C10 bond length of 1.569 (2) Å is much longer than the typical Csp3—Csp2 bond distance and is also slightly longer than that of 4-methyl-2-phenylbenzo[de]cyclobut[I]isoquinoline-3,5(2H)-dione (Liu et al., 2002) Please check this name in the light of the systematic name for (I). Such an elongation has also been observed in another cyclobutene derivative (Usman et al., 2001). This is considered to be caused by the steric effect of the bulky substituents attached at positions C7 and C10. The C9—C10 bond length of 1.572 (2) Å and the C9—C14 bond length of 1.485 (3) Å are much longer than the standard average C—C bond length (1.395 Å; Reference?) in a phenyl ring, because the C9—C14 ring is no longer aromatic.

The naphthalimide moiety has lost its coplanarity, due to the sp3 character of atoms C9, C10, C13 and C14. The C7—C10 cyclobutene ring makes a dihedral angle of 112.80 (2)° with the C9—C14 cyclohexadiene ring, while the latter makes dihedral angles of 6.47 (7) and 18.49 (8)°, respectively, with the C11/C12/C15—C18 benzo ring and the C10/C11/C18/C19/N/C20 ring. The dihedral angle between the C10/C11/C18/C19/N/C20 and C11/C12/C15—C18 rings is 15.09 (9)°. The phenyl substituent attached to the C7—C10 cyclobutene ring moiety at C7 is twisted by 150.50 (2)° with respect to the cyclobutene ring. The C13/C14/O1 epoxy ring makes a dihedral angle of 103.70 (9)° with the C9—C14 cyclohexadiene ring.

In the structure of (I), there are intermolecular C4—H4···O1 and C14—H14···O3 close contacts (Table 2).

Experimental top

The title compound was prepared by irradiation (with light of wavelength longer than 300 nm) of a nitrogen-purged benzene solution of N-methyl-1,8-naphthalenedicarboximide with phenylacetylene, and isolated as one of the products of the photoreaction, using flash column chromatography on silica gel (m.p. 447–448.5 K). Single crystals of (I) suitable for X-ray diffraction were obtained by recrystallization from an ethanol-ethyl acetate (Ratio?) solution.

Refinement top

The positions of all H atoms were fixed geometrically and C—H distances were set by the program, in the range 0.93–0.98 Å. Is this added text OK?

Computing details top

Data collection: XSCANS (Siemens, 1994); cell refinement: XSCANS; data reduction: SHELXTL (Sheldrick, 1997); program(s) used to solve structure: SHELXTL; program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. The molecular structure of (I), showing 50% probability displacement ellipsoids and the atom-numbering scheme. H atoms have been omitted for clarity.
[Figure 2] Fig. 2. The molecular packing diagram for the crystal of (I).
4,5,9,10-Tetrahydro-4-methyl-2-phenyl-9,10-epoxy- 3H,10aH-cyclobuta[a]benzo[2,3,4-de]isoquinoline-3,5-dione top
Crystal data top
C21H15NO3F(000) = 688
Mr = 329.34Dx = 1.350 Mg m3
Monoclinic, P21/cMelting point = 447.0–448.5 K
Hall symbol: -P 2ybcMo Kα radiation, λ = 0.71073 Å
a = 14.801 (3) ÅCell parameters from 25 reflections
b = 8.306 (2) Åθ = 3.0–12.6°
c = 14.441 (2) ŵ = 0.09 mm1
β = 114.15 (1)°T = 288 K
V = 1620.0 (6) Å3Prism, colourless
Z = 40.34 × 0.30 × 0.25 mm
Data collection top
Siemens P4
diffractometer
Rint = 0.011
Radiation source: normal-focus sealed tubeθmax = 25.0°, θmin = 1.5°
Graphite monochromatorh = 1716
ω scansk = 90
3306 measured reflectionsl = 017
2852 independent reflections3 standard reflections every 97 reflections
1870 reflections with I > 2σ(I) intensity decay: 4.8%
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)] = 0.041H-atom parameters constrained
wR(F2) = 0.110 w = 1/[σ2(Fo2) + (0.0603P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.97(Δ/σ)max = 0.001
2852 reflectionsΔρmax = 0.19 e Å3
228 parametersΔρmin = 0.12 e Å3
0 restraintsExtinction correction: SHELXTL (Sheldrick, 1997)
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0108 (15)
Crystal data top
C21H15NO3V = 1620.0 (6) Å3
Mr = 329.34Z = 4
Monoclinic, P21/cMo Kα radiation
a = 14.801 (3) ŵ = 0.09 mm1
b = 8.306 (2) ÅT = 288 K
c = 14.441 (2) Å0.34 × 0.30 × 0.25 mm
β = 114.15 (1)°
Data collection top
Siemens P4
diffractometer
Rint = 0.011
3306 measured reflections3 standard reflections every 97 reflections
2852 independent reflections intensity decay: 4.8%
1870 reflections with I > 2σ(I)
Refinement top
R[F2 > 2σ(F2)] = 0.0410 restraints
wR(F2) = 0.110H-atom parameters constrained
S = 0.97Δρmax = 0.19 e Å3
2852 reflectionsΔρmin = 0.12 e Å3
228 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. The structure was solved by direct methods and successive difference Fourier syntheses. 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
O10.35670 (11)0.74281 (17)0.75866 (12)0.0741 (5)
O20.09075 (11)0.10703 (19)0.73214 (12)0.0820 (5)
O30.41892 (10)0.21136 (18)0.85811 (10)0.0682 (4)
N0.25531 (11)0.15509 (18)0.79497 (11)0.0495 (4)
C10.18484 (14)0.1236 (2)0.51476 (13)0.0520 (5)
H10.14610.18450.53860.062*
C20.14094 (16)0.0065 (2)0.44205 (15)0.0635 (6)
H20.07310.01100.41750.076*
C30.1971 (2)0.0838 (3)0.40607 (16)0.0710 (7)
H30.16710.16130.35640.085*
C40.2971 (2)0.0601 (3)0.44305 (17)0.0694 (6)
H40.33510.12300.41930.083*
C50.34211 (15)0.0569 (2)0.51554 (15)0.0572 (5)
H50.41010.07270.53980.069*
C60.28605 (13)0.1513 (2)0.55247 (12)0.0429 (4)
C70.33513 (12)0.2805 (2)0.62437 (13)0.0439 (4)
C80.41512 (13)0.3685 (3)0.64237 (15)0.0565 (5)
H80.46110.36760.61370.068*
C90.40689 (13)0.4707 (2)0.72465 (15)0.0524 (5)
H90.46280.45660.79060.063*
C100.31514 (12)0.3632 (2)0.71184 (12)0.0414 (4)
C110.21737 (12)0.4456 (2)0.68406 (12)0.0410 (4)
C120.20140 (14)0.6046 (2)0.65098 (14)0.0499 (5)
C130.28495 (16)0.7059 (2)0.65566 (16)0.0620 (6)
H130.26940.79300.60580.074*
C140.38572 (15)0.6423 (3)0.69479 (16)0.0610 (6)
H140.42970.69280.66770.073*
C150.10765 (16)0.6708 (3)0.62188 (15)0.0669 (6)
H150.09670.77690.59940.080*
C160.03092 (16)0.5828 (3)0.62561 (17)0.0730 (7)
H160.03160.62870.60460.088*
C170.04622 (14)0.4272 (3)0.66034 (16)0.0626 (6)
H170.00560.36780.66370.075*
C180.13970 (12)0.3585 (2)0.69047 (13)0.0455 (5)
C190.15751 (14)0.1975 (2)0.73739 (15)0.0530 (5)
C200.33582 (14)0.2413 (2)0.79644 (13)0.0465 (5)
C210.27420 (18)0.0144 (3)0.86272 (17)0.0745 (7)
H21A0.24960.03570.91360.089*
H21B0.34410.00580.89490.089*
H21C0.24120.07820.82380.089*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0886 (11)0.0617 (9)0.0829 (11)0.0223 (8)0.0462 (9)0.0217 (8)
O20.0780 (10)0.0791 (11)0.0971 (12)0.0341 (9)0.0441 (9)0.0027 (9)
O30.0545 (8)0.0909 (11)0.0569 (9)0.0177 (8)0.0204 (7)0.0148 (8)
N0.0630 (10)0.0419 (9)0.0497 (9)0.0040 (8)0.0292 (8)0.0013 (7)
C10.0569 (12)0.0506 (12)0.0452 (11)0.0032 (10)0.0177 (9)0.0040 (9)
C20.0735 (14)0.0588 (13)0.0470 (12)0.0068 (11)0.0134 (11)0.0049 (11)
C30.108 (2)0.0537 (13)0.0452 (12)0.0020 (14)0.0256 (13)0.0066 (10)
C40.110 (2)0.0563 (14)0.0580 (14)0.0115 (13)0.0505 (14)0.0040 (11)
C50.0717 (13)0.0584 (12)0.0506 (12)0.0091 (11)0.0344 (10)0.0022 (10)
C60.0535 (11)0.0442 (11)0.0335 (9)0.0053 (9)0.0203 (8)0.0037 (8)
C70.0419 (10)0.0507 (11)0.0421 (10)0.0034 (9)0.0204 (8)0.0007 (9)
C80.0469 (11)0.0725 (14)0.0598 (12)0.0047 (10)0.0318 (10)0.0076 (11)
C90.0406 (10)0.0641 (13)0.0538 (12)0.0125 (9)0.0204 (9)0.0079 (10)
C100.0381 (9)0.0486 (11)0.0390 (10)0.0046 (8)0.0173 (8)0.0033 (8)
C110.0422 (10)0.0460 (11)0.0369 (9)0.0040 (8)0.0183 (8)0.0059 (8)
C120.0584 (12)0.0511 (12)0.0446 (11)0.0028 (10)0.0255 (9)0.0034 (9)
C130.0840 (15)0.0507 (13)0.0619 (13)0.0062 (11)0.0405 (12)0.0049 (10)
C140.0695 (14)0.0583 (13)0.0685 (13)0.0218 (11)0.0418 (11)0.0114 (11)
C150.0751 (15)0.0677 (14)0.0624 (13)0.0233 (12)0.0328 (12)0.0183 (11)
C160.0528 (13)0.0994 (19)0.0667 (15)0.0257 (13)0.0244 (11)0.0164 (14)
C170.0423 (11)0.0914 (17)0.0576 (13)0.0033 (11)0.0240 (10)0.0018 (12)
C180.0432 (10)0.0547 (12)0.0422 (10)0.0045 (9)0.0212 (8)0.0055 (9)
C190.0567 (12)0.0564 (13)0.0553 (12)0.0148 (11)0.0326 (10)0.0106 (10)
C200.0491 (11)0.0509 (11)0.0421 (10)0.0044 (9)0.0214 (9)0.0060 (9)
C210.1095 (18)0.0518 (13)0.0729 (15)0.0046 (12)0.0481 (14)0.0109 (11)
Geometric parameters (Å, º) top
O1—C141.434 (2)C9—C141.485 (3)
O1—C131.464 (2)C9—C101.572 (2)
O2—C191.219 (2)C9—H90.9800
O3—C201.213 (2)C10—C111.500 (2)
N—C201.383 (2)C10—C201.518 (3)
N—C191.388 (2)C11—C121.391 (3)
N—C211.475 (2)C11—C181.393 (2)
C1—C21.383 (3)C12—C151.388 (2)
C1—C61.388 (2)C12—C131.474 (3)
C1—H10.9300C13—C141.460 (3)
C2—C31.370 (3)C13—H130.9800
C2—H20.9300C14—H140.9800
C3—C41.367 (3)C15—C161.370 (3)
C3—H30.9300C15—H150.9300
C4—C51.383 (3)C16—C171.372 (3)
C4—H40.9300C16—H160.9300
C5—C61.397 (2)C17—C181.391 (2)
C5—H50.9300C17—H170.9300
C6—C71.463 (2)C18—C191.474 (3)
C7—C81.324 (2)C21—H21A0.9600
C7—C101.569 (2)C21—H21B0.9600
C8—C91.505 (3)C21—H21C0.9600
C8—H80.9300
C14—O1—C1360.52 (13)C12—C11—C10122.36 (16)
C20—N—C19123.96 (16)C18—C11—C10118.50 (16)
C20—N—C21118.14 (17)C15—C12—C11119.21 (18)
C19—N—C21117.81 (16)C15—C12—C13120.28 (19)
C2—C1—C6120.71 (18)C11—C12—C13120.28 (17)
C2—C1—H1119.6C14—C13—O158.73 (13)
C6—C1—H1119.6C14—C13—C12121.10 (18)
C3—C2—C1120.3 (2)O1—C13—C12114.37 (16)
C3—C2—H2119.9C14—C13—H13116.6
C1—C2—H2119.9O1—C13—H13116.6
C4—C3—C2120.0 (2)C12—C13—H13116.6
C4—C3—H3120.0O1—C14—C1360.74 (13)
C2—C3—H3120.0O1—C14—C9117.07 (17)
C3—C4—C5120.4 (2)C13—C14—C9121.33 (17)
C3—C4—H4119.8O1—C14—H14115.5
C5—C4—H4119.8C13—C14—H14115.5
C4—C5—C6120.4 (2)C9—C14—H14115.5
C4—C5—H5119.8C16—C15—C12121.3 (2)
C6—C5—H5119.8C16—C15—H15119.4
C1—C6—C5118.15 (17)C12—C15—H15119.4
C1—C6—C7122.88 (16)C15—C16—C17120.1 (2)
C5—C6—C7118.87 (16)C15—C16—H16120.0
C8—C7—C6133.57 (16)C17—C16—H16120.0
C8—C7—C1092.76 (14)C16—C17—C18119.67 (19)
C6—C7—C10133.64 (15)C16—C17—H17120.2
C7—C8—C996.42 (15)C18—C17—H17120.2
C7—C8—H8131.8C17—C18—C11120.56 (18)
C9—C8—H8131.8C17—C18—C19118.93 (17)
C14—C9—C8112.80 (17)C11—C18—C19120.31 (16)
C14—C9—C10116.21 (16)O2—C19—N120.07 (19)
C8—C9—C1086.09 (13)O2—C19—C18122.89 (19)
C14—C9—H9113.0N—C19—C18116.91 (16)
C8—C9—H9113.0O3—C20—N120.90 (18)
C10—C9—H9113.0O3—C20—C10122.52 (17)
C11—C10—C20112.00 (14)N—C20—C10116.37 (15)
C11—C10—C7117.64 (13)N—C21—H21A109.5
C20—C10—C7108.29 (14)N—C21—H21B109.5
C11—C10—C9117.68 (15)H21A—C21—H21B109.5
C20—C10—C9113.83 (14)N—C21—H21C109.5
C7—C10—C984.55 (12)H21A—C21—H21C109.5
C12—C11—C18119.14 (17)H21B—C21—H21C109.5
C6—C1—C2—C30.1 (3)C11—C12—C13—C140.0 (3)
C1—C2—C3—C41.0 (3)C15—C12—C13—O1107.5 (2)
C2—C3—C4—C51.2 (3)C11—C12—C13—O166.9 (2)
C3—C4—C5—C60.5 (3)C13—O1—C14—C9112.5 (2)
C2—C1—C6—C50.5 (3)C12—C13—C14—O1101.39 (19)
C2—C1—C6—C7175.89 (17)O1—C13—C14—C9105.6 (2)
C4—C5—C6—C10.3 (3)C12—C13—C14—C94.2 (3)
C4—C5—C6—C7176.23 (17)C8—C9—C14—O1167.69 (16)
C1—C6—C7—C8150.5 (2)C10—C9—C14—O170.5 (2)
C5—C6—C7—C825.9 (3)C8—C9—C14—C1397.0 (2)
C1—C6—C7—C1032.0 (3)C10—C9—C14—C130.1 (3)
C5—C6—C7—C10151.62 (18)C11—C12—C15—C160.3 (3)
C6—C7—C8—C9178.42 (19)C13—C12—C15—C16174.13 (19)
C10—C7—C8—C93.40 (16)C12—C15—C16—C171.2 (3)
C7—C8—C9—C14113.44 (18)C15—C16—C17—C180.8 (3)
C7—C8—C9—C103.40 (16)C16—C17—C18—C111.1 (3)
C8—C7—C10—C11121.73 (17)C16—C17—C18—C19173.75 (19)
C6—C7—C10—C1160.1 (3)C12—C11—C18—C172.6 (3)
C8—C7—C10—C20110.07 (16)C10—C11—C18—C17176.55 (15)
C6—C7—C10—C2068.1 (2)C12—C11—C18—C19172.16 (16)
C8—C7—C10—C93.25 (15)C10—C11—C18—C198.7 (2)
C6—C7—C10—C9178.57 (19)C20—N—C19—O2172.63 (17)
C14—C9—C10—C117.8 (2)C21—N—C19—O210.8 (3)
C8—C9—C10—C11121.30 (15)C20—N—C19—C1811.5 (2)
C14—C9—C10—C20141.72 (17)C21—N—C19—C18165.13 (16)
C8—C9—C10—C20104.74 (16)C17—C18—C19—O216.0 (3)
C14—C9—C10—C7110.68 (17)C11—C18—C19—O2169.19 (17)
C8—C9—C10—C72.86 (13)C17—C18—C19—N159.79 (17)
C20—C10—C11—C12147.24 (17)C11—C18—C19—N15.0 (2)
C7—C10—C11—C1286.4 (2)C19—N—C20—O3169.97 (17)
C9—C10—C11—C1212.5 (2)C21—N—C20—O36.6 (3)
C20—C10—C11—C1833.7 (2)C19—N—C20—C1015.2 (2)
C7—C10—C11—C1892.75 (19)C21—N—C20—C10168.17 (15)
C9—C10—C11—C18168.41 (15)C11—C10—C20—O3148.46 (17)
C18—C11—C12—C152.2 (3)C7—C10—C20—O380.2 (2)
C10—C11—C12—C15176.91 (16)C9—C10—C20—O311.9 (2)
C18—C11—C12—C13172.26 (16)C11—C10—C20—N36.8 (2)
C10—C11—C12—C138.6 (3)C7—C10—C20—N94.50 (17)
C14—O1—C13—C12112.8 (2)C9—C10—C20—N173.40 (14)
C15—C12—C13—C14174.41 (18)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C4—H4···O1i0.932.663.478 (2)147
C14—H14···O3ii0.982.423.329 (2)154
Symmetry codes: (i) x, y+1/2, z1/2; (ii) x+1, y+1/2, z+3/2.

Experimental details

Crystal data
Chemical formulaC21H15NO3
Mr329.34
Crystal system, space groupMonoclinic, P21/c
Temperature (K)288
a, b, c (Å)14.801 (3), 8.306 (2), 14.441 (2)
β (°) 114.15 (1)
V3)1620.0 (6)
Z4
Radiation typeMo Kα
µ (mm1)0.09
Crystal size (mm)0.34 × 0.30 × 0.25
Data collection
DiffractometerSiemens P4
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
3306, 2852, 1870
Rint0.011
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.041, 0.110, 0.97
No. of reflections2852
No. of parameters228
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.19, 0.12

Computer programs: XSCANS (Siemens, 1994), XSCANS, SHELXTL (Sheldrick, 1997), SHELXTL.

Selected geometric parameters (Å, º) top
O1—C141.434 (2)C8—C91.505 (3)
O1—C131.464 (2)C9—C141.485 (3)
C7—C81.324 (2)C9—C101.572 (2)
C7—C101.569 (2)C13—C141.460 (3)
C14—O1—C1360.52 (13)C7—C10—C984.55 (12)
C8—C7—C1092.76 (14)C14—C13—O158.73 (13)
C7—C8—C996.42 (15)O1—C14—C1360.74 (13)
C8—C9—C1086.09 (13)
C1—C6—C7—C8150.5 (2)C6—C7—C10—C2068.1 (2)
C10—C7—C8—C93.40 (16)C11—C18—C19—N15.0 (2)
C8—C7—C10—C11121.73 (17)C11—C10—C20—N36.8 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C4—H4···O1i0.932.663.478 (2)147
C14—H14···O3ii0.982.423.329 (2)154
Symmetry codes: (i) x, y+1/2, z1/2; (ii) x+1, y+1/2, z+3/2.
 

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