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The title molecule, C17H10N2O2, is a synthetic precursor to the cytotoxic marine alkaloid ascididemin and is also structurally related to cleistopholine, a plant-derived antifungal agent. The molecule was found to be essentially planar with the only significant deviations from planarity being for the quinone O atoms.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270199013578/ja1007sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270199013578/ja1007Isup2.hkl
Contains datablock I

CCDC reference: 140968

Comment top

The search for new human anticancer agents from the marine environment has resulted in the isolation of a large range of polycyclic alkaloids based upon the pyridoacridine framework (Molinski, 1993). Two such examples are the cytotoxic pentacyclic alkaloids ascididemin and its analogue 2-bromoleptoclinidinone (Kobayashi et al., 1988; Bloor & Schmitz, 1987; deGuzman & Schmitz, 1989; Bracher, 1997; Lindsay et al., 1998). Both molecules associate with DNA, probably via base-pair intercalation. In direct contrast to this, previous studies have noted that the tetracyclic synthetic precursor to ascididemin, 11-methylpyrido[2,3-b]acridine-5,12-dione, (I) (NSC 659780), exhibits only modest cytotoxicity (Bracher, 1997), and moderate antibacterial and antifungal properties (Lindsay et al., 1995). As part of our studies directed towards understanding the chemistry (Lindsay et al., 1997, 1998; Copp et al., 1999) and biological activities (Lindsay et al., 1995; Copp et al., 1999) of ascididemin and related marine alkaloids, we now report on the crystal structure of (I).

The title molecule was found to be highly planar, with the greatest deviations from the mean molecular plane being for the quinone atoms O1 [0.125 (4) Å] and O2 [0.195 (4) Å], thus making it a good DNA intercalating chromophore. There are few reported X-ray studies of the quinoline–quinone substructure present in rings AB of (I) although this fragment is present in many biologically active agents, including the antibiotic streptonigrin (Chiu & Lipscomb, 1975) and aza-analogues of the antitumour agent mitoxantrone (Krapcho et al., 1994). Bond lengths observed for rings A and B of (I) are comparable to those reported for other quinoline–quinone-bearing compounds (Chiu & Lipscomb, 1975; Kita et al., 1991; Gieren & Schanda, 1977). However, steric congestion between the quinone O1 and methyl C1' atoms is apparent in (I), as evidenced by bond angles of 118.8 (3) (O1—C12—C12a) and 122.6 (3)° (O1—C12—C11a). This interaction is presumably also responsible for the quinone O atoms bending out of the plane of the rings. Extensive π-π stacking was evident in the crystal of (I), with rings BCD of one molecule overlapping rings ABC of an adjacent molecule. The perpendicular separation between individual chromophores is 3.4 Å.

Experimental top

11-Methylpyrido[2,3-b]acridine-5,12-dione was prepared by a published route and yielded spectroscopic data identical in all respects with that previously reported (Bracher, 1989). Recrystallization from a methanol–dichloromethane solution yielded yellow–brown needles [m.p. 520–525 K, literature 513–521 K (Bracher, 1989)] suitable for X-ray analysis. Full assignment of 1H and 13C NMR data were made by use of standard two-dimensional NMR techniques. 1H NMR (200 MHz, CDCl3): δ 9.16 (1H, dd, J = 4.6, 1.8 Hz, H-2), 8.73 (1H, dd, J = 8.0, 1.8 Hz, H-4), 8.45 (1H, dd, J = 8.5, 0.9 Hz, H-10), 8.38 (dd, J = 8.5, 0.9 Hz, H-7), 7.93 (1H, ddd, J = 8.3, 6.9, 1.4 Hz, H-8), 7.79 (1H, ddd, J = 8.3, 6.9, 1.4 Hz, H-9), 7.77 (1H, dd, J = 7.9, 4.6 Hz, H-3), 3.32 (3H, s, CH3); 13C NMR (100 MHz, CDCl3): δ 183.3 (s), 181.8 (d, J = 4 Hz, C-5), 155.6 (ddd, J = 183, 8, 4 Hz, C-2), 152.7 (dd, J = 6, 3 Hz, C-11), 150.2 (t, J = 5 Hz, C-12a), 148.6 (t, J = 8 Hz, C-6a), 147.5 (s, C-5a), 135.7 (dd, J = 170 Hz, 6, C-4), 132.7 (dd, J = 163 Hz, 9, C-8), 132.3 (dd, J = 165 Hz, 7, C-7), 130.0 (d, J = 7 Hz, C-4a), 125.5 (dd, J = 161 Hz, 8, C-10), 129.8 (dd, J = 163 Hz, 9, C-9), 129.8 (m, C-10a), 127.9 (dd, J = 167 Hz, 9, C-3), 125.5 (m, C-11a), 16.7 (q, J = 130 Hz, CH3).

Computing details top

Data collection: SMART (Siemens, 1994); cell refinement: SAINT (Siemens, 1994); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997a); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997b); molecular graphics: SHELXTL (Siemens, 1994); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1]
[Figure 2]
Fig. 1. The structure of (I) showing 50% probability displacement ellipsoids.
11-Methylpyrido[2,3-b]acridine-5,12-dione top
Crystal data top
C17H10N2O2Dx = 1.479 Mg m3
Mr = 274.27Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, Pca21Cell parameters from 5243 reflections
a = 25.7526 (17) Åθ = 1.5–25.0°
b = 4.2348 (3) ŵ = 0.10 mm1
c = 11.2966 (7) ÅT = 293 K
V = 1231.97 (14) Å3Needle, brown
Z = 40.94 × 0.18 × 0.18 mm
F(000) = 568
Data collection top
Siemens SMART CCD
diffractometer
2040 independent reflections
Radiation source: fine-focus sealed tube1845 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.057
Area–detector ω scansθmax = 25°, θmin = 1.6°
Absorption correction: multi-scan
(Blessing, 1995; Sheldrick, 1998)
h = 2530
Tmin = 0.912, Tmax = 0.982k = 55
6391 measured reflectionsl = 1412
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)] = 0.054Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.141H-atom parameters constrained
S = 1.02Calculated w = 1/[σ2(Fo2) + (0.0608P)2 + 0.3024P]
where P = (Fo2 + 2Fc2)/3
2040 reflections(Δ/σ)max = 0.032
190 parametersΔρmax = 0.16 e Å3
1 restraintΔρmin = 0.18 e Å3
Crystal data top
C17H10N2O2V = 1231.97 (14) Å3
Mr = 274.27Z = 4
Orthorhombic, Pca21Mo Kα radiation
a = 25.7526 (17) ŵ = 0.10 mm1
b = 4.2348 (3) ÅT = 293 K
c = 11.2966 (7) Å0.94 × 0.18 × 0.18 mm
Data collection top
Siemens SMART CCD
diffractometer
2040 independent reflections
Absorption correction: multi-scan
(Blessing, 1995; Sheldrick, 1998)
1845 reflections with I > 2σ(I)
Tmin = 0.912, Tmax = 0.982Rint = 0.057
6391 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0541 restraint
wR(F2) = 0.141H-atom parameters constrained
S = 1.02Δρmax = 0.16 e Å3
2040 reflectionsΔρmin = 0.18 e Å3
190 parameters
Special details top

Refinement. The structure was determined by direct methods and refined by full-matrix least squares on F2. Hydrogen atoms were placed geometrically and refined with a riding model (including free rotation about C—C bonds for the methyl group), and with Uiso constrained to be 1.2 (1.5 for the methyl group) times Ueq of the carrier atom.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.28702 (9)0.3026 (9)0.5575 (3)0.0962 (11)
O20.48874 (8)0.5722 (8)0.5260 (3)0.0817 (9)
N10.34850 (11)0.0947 (7)0.7290 (2)0.0599 (8)
N60.42610 (9)0.8471 (6)0.3681 (2)0.0462 (6)
C1'0.25969 (11)0.6673 (9)0.3689 (3)0.0618 (9)
H1'A0.24740.65260.44990.093*
H1'B0.25150.47350.32710.093*
H1'C0.24290.84380.32980.093*
C20.38132 (16)0.0077 (10)0.8124 (3)0.0675 (10)
H2A0.36780.13440.87330.081*
C30.43368 (16)0.0600 (10)0.8150 (3)0.0646 (10)
H3A0.45460.01450.87720.077*
C4a0.42160 (11)0.3458 (8)0.6366 (3)0.0475 (8)
C40.45459 (13)0.2366 (8)0.7262 (3)0.0566 (9)
H4A0.49030.28380.72510.068*
C5a0.40490 (10)0.6646 (8)0.4488 (3)0.0440 (7)
C50.44264 (11)0.5311 (8)0.5361 (3)0.0506 (8)
C6a0.39462 (11)0.9673 (8)0.2828 (3)0.0434 (7)
C70.41800 (12)1.1609 (8)0.1966 (3)0.0515 (8)
H7A0.45381.20380.20090.062*
C80.38911 (13)1.2867 (9)0.1070 (3)0.0580 (9)
H8A0.40491.41650.04990.070*
C90.33586 (13)1.2215 (8)0.1005 (3)0.0594 (9)
H9A0.31631.30560.03770.071*
C10a0.34025 (11)0.9066 (8)0.2783 (3)0.0453 (7)
C100.31194 (12)1.0397 (8)0.1830 (3)0.0537 (8)
H10A0.27611.00140.17680.064*
C11a0.35069 (11)0.5933 (8)0.4544 (3)0.0434 (7)
C110.31773 (10)0.7174 (7)0.3687 (3)0.0451 (7)
C12a0.36933 (11)0.2704 (8)0.6431 (3)0.0477 (7)
C120.33125 (11)0.3865 (8)0.5514 (3)0.0501 (8)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0360 (12)0.156 (3)0.097 (2)0.0227 (15)0.0073 (13)0.051 (2)
O20.0325 (11)0.131 (3)0.0818 (18)0.0131 (13)0.0113 (12)0.0239 (19)
N10.0532 (16)0.077 (2)0.0491 (16)0.0020 (14)0.0040 (14)0.0017 (15)
N60.0319 (11)0.0553 (15)0.0515 (15)0.0049 (11)0.0003 (11)0.0093 (14)
C1'0.0362 (16)0.082 (2)0.068 (2)0.0032 (15)0.0036 (15)0.002 (2)
C20.068 (2)0.082 (3)0.052 (2)0.005 (2)0.0014 (18)0.002 (2)
C30.067 (2)0.076 (3)0.050 (2)0.0108 (19)0.0119 (17)0.002 (2)
C4a0.0381 (14)0.0543 (19)0.0500 (17)0.0039 (12)0.0026 (13)0.0148 (16)
C40.0472 (16)0.063 (2)0.059 (2)0.0013 (16)0.0111 (16)0.0047 (18)
C5a0.0319 (13)0.0503 (18)0.0498 (17)0.0008 (12)0.0007 (13)0.0121 (15)
C50.0336 (15)0.062 (2)0.057 (2)0.0043 (14)0.0048 (14)0.0100 (17)
C6a0.0317 (15)0.0507 (18)0.0476 (16)0.0016 (13)0.0008 (13)0.0105 (14)
C70.0381 (15)0.0595 (19)0.0569 (19)0.0021 (14)0.0054 (14)0.0062 (17)
C80.0520 (17)0.067 (2)0.055 (2)0.0029 (16)0.0081 (16)0.0009 (18)
C90.0526 (18)0.071 (2)0.055 (2)0.0076 (17)0.0030 (16)0.0008 (19)
C10a0.0340 (15)0.0523 (19)0.0497 (17)0.0007 (13)0.0007 (14)0.0164 (15)
C100.0370 (15)0.067 (2)0.057 (2)0.0044 (14)0.0054 (14)0.0084 (17)
C11a0.0308 (12)0.0510 (18)0.0485 (17)0.0009 (12)0.0008 (13)0.0145 (14)
C110.0295 (13)0.0542 (18)0.0517 (18)0.0001 (12)0.0012 (12)0.0128 (15)
C12a0.0416 (16)0.0538 (18)0.0478 (17)0.0012 (13)0.0020 (14)0.0105 (14)
C120.0332 (15)0.067 (2)0.0496 (18)0.0028 (13)0.0019 (13)0.0021 (17)
Geometric parameters (Å, º) top
O1—C121.195 (4)C5a—C11a1.430 (4)
O2—C51.205 (4)C5a—C51.496 (4)
N1—C12a1.335 (4)C6a—C71.408 (4)
N1—C21.338 (5)C6a—C10a1.424 (4)
N6—C5a1.313 (4)C7—C81.364 (5)
N6—C6a1.358 (4)C8—C91.401 (5)
C1'—C111.510 (4)C9—C101.357 (5)
C2—C31.379 (5)C10a—C101.417 (4)
C3—C41.363 (5)C10a—C111.422 (5)
C4a—C12a1.385 (4)C11a—C111.391 (4)
C4a—C41.400 (5)C11a—C121.489 (4)
C4a—C51.483 (5)C12a—C121.509 (4)
C12a—N1—C2116.0 (3)C7—C8—C9119.7 (3)
C5a—N6—C6a117.7 (2)C10—C9—C8121.3 (3)
N1—C2—C3124.4 (4)C10—C10a—C11124.0 (3)
C4—C3—C2119.0 (3)C10—C10a—C6a117.5 (3)
C12a—C4a—C4118.4 (3)C11—C10a—C6a118.5 (3)
C12a—C4a—C5121.2 (3)C9—C10—C10a120.9 (3)
C4—C4a—C5120.4 (3)C11—C11a—C5a119.0 (3)
C3—C4—C4a118.3 (3)C11—C11a—C12121.9 (2)
N6—C5a—C11a124.1 (3)C5a—C11a—C12119.0 (3)
N6—C5a—C5114.2 (2)C11a—C11—C10a117.6 (2)
C11a—C5a—C5121.7 (3)C11a—C11—C1'123.4 (3)
O2—C5—C4a120.6 (3)C10a—C11—C1'119.0 (3)
O2—C5—C5a121.6 (3)N1—C12a—C4a123.9 (3)
C4a—C5—C5a117.9 (2)N1—C12a—C12114.8 (3)
N6—C6a—C7117.0 (2)C4a—C12a—C12121.3 (3)
N6—C6a—C10a123.0 (3)O1—C12—C11a122.6 (3)
C7—C6a—C10a120.0 (3)O1—C12—C12a118.8 (3)
C8—C7—C6a120.5 (3)C11a—C12—C12a118.6 (2)

Experimental details

Crystal data
Chemical formulaC17H10N2O2
Mr274.27
Crystal system, space groupOrthorhombic, Pca21
Temperature (K)293
a, b, c (Å)25.7526 (17), 4.2348 (3), 11.2966 (7)
V3)1231.97 (14)
Z4
Radiation typeMo Kα
µ (mm1)0.10
Crystal size (mm)0.94 × 0.18 × 0.18
Data collection
DiffractometerSiemens SMART CCD
diffractometer
Absorption correctionMulti-scan
(Blessing, 1995; Sheldrick, 1998)
Tmin, Tmax0.912, 0.982
No. of measured, independent and
observed [I > 2σ(I)] reflections
6391, 2040, 1845
Rint0.057
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.054, 0.141, 1.02
No. of reflections2040
No. of parameters190
No. of restraints1
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.16, 0.18

Computer programs: SMART (Siemens, 1994), SAINT (Siemens, 1994), SAINT, SHELXS97 (Sheldrick, 1997a), SHELXL97 (Sheldrick, 1997b), SHELXTL (Siemens, 1994), SHELXL97.

Selected geometric parameters (Å, º) top
O1—C121.195 (4)C4a—C12a1.385 (4)
O2—C51.205 (4)C4a—C51.483 (5)
N1—C12a1.335 (4)C5a—C11a1.430 (4)
N1—C21.338 (5)C5a—C51.496 (4)
N6—C5a1.313 (4)C11a—C121.489 (4)
N6—C6a1.358 (4)C12a—C121.509 (4)
C1'—C111.510 (4)
O2—C5—C4a120.6 (3)C10a—C11—C1'119.0 (3)
O2—C5—C5a121.6 (3)O1—C12—C11a122.6 (3)
C4a—C5—C5a117.9 (2)O1—C12—C12a118.8 (3)
C11a—C11—C10a117.6 (2)C11a—C12—C12a118.6 (2)
C11a—C11—C1'123.4 (3)
 

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