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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2014 Apr 16;70(Pt 5):o554. doi: 10.1107/S1600536814006746

N-Benzyl-2-chloro­quinazolin-4-amine

Tarek Mohamed a,b, Abdeljalil Assoud a, Praveen P N Rao b,*
PMCID: PMC4011242  PMID: 24860362

Abstract

The asymmetric unit of the title compound, C15H12ClN3, contains two independent mol­ecules. The quinazoline ring system in each is essentially planar, with maximum deviations of 0.025 (16) and 0.0171 (16) Å. The dihedral angles between quinazoline ring systems and the phenyl rings are 88.25 (8) and 85.28 (16)° in the two independent mol­ecules. In the crystal, alternating independent mol­ecules are linked by N—H⋯N hydrogen bonds, forming chains along [001].

Related literature  

For the biological activity of some quinazoline and related derivatives, see: Deng & Mani (2006); Lee et al. (1995); Lopez et al. (2011); Mohamed et al. (2011); Wynne et al. (2009); Yoshida & Taguchi (1992); Zhang et al. (2009); Zhou et al. (2011).graphic file with name e-70-0o554-scheme1.jpg

Experimental  

Crystal data  

  • C15H12ClN3

  • M r = 269.73

  • Triclinic, Inline graphic

  • a = 9.4018 (1) Å

  • b = 13.0108 (1) Å

  • c = 13.3035 (1) Å

  • α = 113.968 (1)°

  • β = 105.377 (1)°

  • γ = 100.213 (1)°

  • V = 1356.69 (2) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.27 mm−1

  • T = 296 K

  • 0.35 × 0.26 × 0.10 mm

Data collection  

  • Bruker Kappa APEXII diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2008) T min = 0.911, T max = 0.974

  • 22349 measured reflections

  • 6531 independent reflections

  • 5274 reflections with I > 2σ(I)

  • R int = 0.024

  • 3 standard reflections every 15 min intensity decay: none

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.039

  • wR(F 2) = 0.086

  • S = 1.13

  • 6531 reflections

  • 344 parameters

  • H-atom parameters constrained

  • Δρmax = 0.33 e Å−3

  • Δρmin = −0.49 e Å−3

Data collection: APEX2 (Bruker, 2008); cell refinement: SAINT (Bruker, 2008); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2013 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 1999); software used to prepare material for publication: publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) I. DOI: 10.1107/S1600536814006746/lh5690sup1.cif

e-70-0o554-sup1.cif (834.6KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814006746/lh5690Isup2.hkl

e-70-0o554-Isup2.hkl (319.6KB, hkl)

Supporting information file. DOI: 10.1107/S1600536814006746/lh5690Isup3.cml

CCDC reference: 993912

Additional supporting information: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
N3A—H3AA⋯N1B i 0.86 2.21 2.9954 (17) 152
N3B—H3BA⋯N1A 0.86 2.18 2.9482 (16) 149

Symmetry code: (i) Inline graphic.

Acknowledgments

The authors would like to thank Faculty of Science, Office of Research, and the School of Pharmacy at the University of Waterloo and Ontario Mental Health Foundation (TM) for financial support of this research project.

supplementary crystallographic information

1. Introduction

Quinazolines represent an important class of nitro­gen containing heterocycles that are present in a number of therapeutically useful small molecules such as tyrosine kinase inhibitors (Zhang et al., 2009; Lopez et al., 2011) and adrenergic antagonists (Zhou et al., 2011). In our study, we have used 2,4-di­chloro­quinazolines to explore the selectivity of nucleophilic displacement of halogens (Mohamed et al., 2011). It is known that the monocyclic compound 2,4-di­chloro­pyrimidine, generally favours C-4 substitution selectively or as the major regioisomer during simple SNAr reactions with amine nucleophiles (Deng et al., 2006). A similar effect is seen with the bicyclic 2,4-di­chloro­quinazoline (Yoshida et al., 1992). Reaction of 2,4-di­chloro­quinazoline with benzyl­amine provided selective substitution at C-4 position. The chemical structure was confirmed by determining the crystal structure of N-benzyl-2-chloro­quinazoline-4-amine (I).

2. Experimental

The title compound was prepared by slowly adding 0.75 mL of benzyl­amine (6.53mmol) to a mixture of 2,4-di­chloro­quinazoline (1g, 5.02 mmol) in 20 mL of methanol on ice-bath while stirring. The solution was allowed to stir on ice for 5 minutes before drop wise addition of DIPEA (1.75 mL, 10.04 mmol). The reaction was allowed to stir on the ice-bath for an additional 5 minutes and then refluxed at 348–353K for 3 hours. After cooling to 298 K, the solvent was evaporated in vacuo and the residue was re-dissolved in EtOAc, washed with saturated NaHCO3 and NaCl solution (2 x 15 mL) respectively. Aqueous layer (pH 7.5-8.0) was washed with EtOAc (1 x 15 mL) and the combined organic layer was dried over anhydrous MgSO4, then filtered. The organic layer was evaporated in vacuo and the resulting yellowish solid was further purified by silica gel column chromatography using EtOAc:MeOH (5:1) as eluent to afford the desired product as a white solid (1.02 g, 75% yield). Mp: 442–444K. 1H-NMR (300MHz, DMSO-d6) d 9.24 (t, 6.0Hz 1H), d 8.27 (d, J = 6.0, 1H), d 7.75 (t, J = 9.0Hz, 1H), d 7.59 (d, J = 6.0, 1H), d 7.49 (t, J = 9.0Hz, 1H), d 7.20-7.34 (m, 5H), d 4.72 (d, J = 6.0, 2H). ESI-MS m/z: 270 [M+1]+ (Lee et al., 1995; Wynne et al., 2009). Crystal growth was carried out by dissolving 5mg of the product in 20mL of ethanol at room temperature and heating the solution to 353K to form a concentrated solution with a reduced volume of 10mL. The hot solution was transferred to a scintillation vial, capped and stored at 275-279K undisturbed for four days at which needle-like crystals were obtained which were suitable for X-ray diffraction.

2.1. Refinement

All H-atoms were positioned in geometrically idealized positions and refined using a riding model with C—H = 0.93–1.00 Å and N—H = 0.86 Å and isotropic displacement parameters of Uiso(H) = 1.2Ueq(C).

3. Results and discussion

The asymmetric unit of (I) is shown in Fig. 1. The quinazoline ring system [N1/N2/C1–8] in each independent molecule is essentially planar with maximum deviations of 0.025 (16) and 0.0171 (16) Å for C4A and C4B, repectively. The dihedral angles between quinazoline ring systems and the phenyl rings [C10–C15 ] are 88.25 (8)° and 85.28 (16) ° for molecules A and B, respectively. In the crystal, alternating independent molecules are linked by N—H···N hydrogen bonds forming chains along [001] (Fig .2).

Figures

Fig. 1.

Fig. 1.

The asymmetric unit of (I) with displacement ellipsoids drawn at the 50% probability level.

Fig. 2.

Fig. 2.

Part of the crystal structure showing hydrogen bonds (dashed lines) which connect molecules along [001].

Crystal data

C15H12ClN3 Z = 4
Mr = 269.73 F(000) = 560
Triclinic, P1 Dx = 1.321 Mg m3
a = 9.4018 (1) Å Mo Kα radiation, λ = 0.71073 Å
b = 13.0108 (1) Å Cell parameters from 407 reflections
c = 13.3035 (1) Å θ = 1.5–30°
α = 113.968 (1)° µ = 0.27 mm1
β = 105.377 (1)° T = 296 K
γ = 100.213 (1)° Block, colourless
V = 1356.69 (2) Å3 0.35 × 0.26 × 0.10 mm

Data collection

Bruker Kappa APEXII diffractometer 5274 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.024
Graphite monochromator θmax = 28.0°, θmin = 2.4°
ω and φ scans h = −12→12
Absorption correction: multi-scan (SADABS; Bruker, 2008) k = −17→17
Tmin = 0.911, Tmax = 0.974 l = −17→17
22349 measured reflections 3 standard reflections every 15 min
6531 independent reflections intensity decay: none

Refinement

Refinement on F2 Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: full H-atom parameters constrained
R[F2 > 2σ(F2)] = 0.039 w = 1/[σ2(Fo2) + (0.0141P)2 + 0.4615P] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.086 (Δ/σ)max < 0.001
S = 1.13 Δρmax = 0.33 e Å3
6531 reflections Δρmin = −0.49 e Å3
344 parameters Extinction correction: SHELXL2013 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraints Extinction coefficient: 0.0041 (6)

Special details

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq
Cl1A 0.80906 (7) 0.05252 (4) 0.09218 (4) 0.07177 (16)
N1A 0.75236 (15) 0.23972 (11) 0.09405 (10) 0.0431 (3)
N2A 0.81249 (15) 0.11531 (11) −0.06785 (10) 0.0437 (3)
N3A 0.81842 (15) 0.15522 (12) −0.21892 (11) 0.0461 (3)
H3AA 0.8049 0.1991 −0.2522 0.055*
C1A 0.78763 (18) 0.14847 (13) 0.03282 (13) 0.0432 (3)
C2A 0.74116 (16) 0.31670 (12) 0.04724 (12) 0.0381 (3)
C3A 0.76545 (16) 0.29524 (13) −0.05817 (12) 0.0373 (3)
C4A 0.79930 (16) 0.18703 (13) −0.11613 (12) 0.0375 (3)
C5A 0.7048 (2) 0.41884 (15) 0.10729 (14) 0.0515 (4)
H5AA 0.6880 0.4334 0.1769 0.062*
C6A 0.6941 (2) 0.49701 (16) 0.06391 (16) 0.0617 (5)
H6AA 0.6697 0.5645 0.1042 0.074*
C7A 0.7193 (2) 0.47677 (16) −0.04001 (17) 0.0648 (5)
H7AA 0.7121 0.5309 −0.0685 0.078*
C8A 0.7548 (2) 0.37788 (15) −0.10035 (15) 0.0532 (4)
H8AA 0.7718 0.3651 −0.1696 0.064*
C9A 0.86081 (18) 0.05090 (14) −0.27836 (13) 0.0485 (4)
H9AA 0.8007 0.0127 −0.3629 0.058*
H9AB 0.8337 −0.0050 −0.2502 0.058*
C10A 1.03177 (17) 0.07992 (12) −0.25780 (12) 0.0387 (3)
C11A 1.14458 (19) 0.16829 (14) −0.15033 (14) 0.0472 (4)
H11A 1.1148 0.2127 −0.0895 0.057*
C12A 1.3005 (2) 0.19105 (16) −0.13271 (17) 0.0594 (4)
H12A 1.3753 0.2502 −0.0600 0.071*
C13A 1.3458 (2) 0.12649 (18) −0.2225 (2) 0.0670 (5)
H13A 1.4510 0.1419 −0.2106 0.080*
C14A 1.2353 (2) 0.03958 (16) −0.32935 (19) 0.0638 (5)
H14A 1.2656 −0.0037 −0.3903 0.077*
C15A 1.0797 (2) 0.01593 (14) −0.34694 (15) 0.0499 (4)
H15A 1.0057 −0.0438 −0.4197 0.060*
Cl1B 0.49469 (5) 0.17163 (4) 0.57865 (4) 0.06102 (13)
N1B 0.78003 (14) 0.23433 (11) 0.59600 (10) 0.0413 (3)
N2B 0.58069 (14) 0.20758 (11) 0.42357 (10) 0.0416 (3)
N3B 0.63353 (14) 0.23214 (12) 0.27581 (10) 0.0442 (3)
H3BA 0.7001 0.2522 0.2480 0.053*
C1B 0.63823 (17) 0.20955 (13) 0.52713 (13) 0.0402 (3)
C2B 0.89177 (16) 0.26517 (12) 0.55393 (12) 0.0378 (3)
C3B 0.85120 (16) 0.26871 (12) 0.44613 (12) 0.0369 (3)
C4B 0.68648 (16) 0.23599 (12) 0.38078 (12) 0.0375 (3)
C5B 1.04922 (18) 0.29186 (14) 0.62032 (14) 0.0487 (4)
H5BA 1.0771 0.2897 0.6918 0.058*
C6B 1.16159 (19) 0.32102 (16) 0.58031 (15) 0.0569 (4)
H6BA 1.2657 0.3381 0.6246 0.068*
C7B 1.12207 (19) 0.32550 (17) 0.47386 (16) 0.0593 (4)
H7BA 1.1997 0.3457 0.4477 0.071*
C8B 0.96948 (18) 0.30032 (15) 0.40786 (14) 0.0497 (4)
H8BA 0.9438 0.3041 0.3372 0.060*
C9B 0.46910 (17) 0.19581 (14) 0.20594 (13) 0.0460 (3)
H9BA 0.4136 0.1313 0.2143 0.055*
H9BB 0.4553 0.1652 0.1230 0.055*
C10B 0.39638 (16) 0.29301 (13) 0.23906 (12) 0.0404 (3)
C11B 0.48004 (19) 0.40835 (15) 0.32662 (15) 0.0537 (4)
H11B 0.5860 0.4282 0.3680 0.064*
C12B 0.4087 (2) 0.49486 (16) 0.35374 (17) 0.0625 (5)
H12B 0.4667 0.5721 0.4134 0.075*
C13B 0.2534 (2) 0.46736 (18) 0.29325 (18) 0.0626 (5)
H13B 0.2054 0.5255 0.3112 0.075*
C14B 0.1692 (2) 0.35318 (19) 0.20577 (19) 0.0679 (5)
H14B 0.0635 0.3341 0.1641 0.081*
C15B 0.23929 (19) 0.26642 (16) 0.17885 (15) 0.0558 (4)
H15B 0.1803 0.1892 0.1196 0.067*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cl1A 0.1269 (4) 0.0514 (3) 0.0519 (3) 0.0322 (3) 0.0343 (3) 0.0364 (2)
N1A 0.0559 (7) 0.0427 (7) 0.0340 (6) 0.0137 (6) 0.0193 (6) 0.0209 (5)
N2A 0.0582 (8) 0.0414 (7) 0.0353 (6) 0.0188 (6) 0.0178 (6) 0.0205 (5)
N3A 0.0578 (8) 0.0574 (8) 0.0391 (7) 0.0293 (6) 0.0251 (6) 0.0288 (6)
C1A 0.0559 (9) 0.0386 (8) 0.0358 (7) 0.0107 (7) 0.0141 (7) 0.0222 (6)
C2A 0.0399 (7) 0.0396 (7) 0.0334 (7) 0.0112 (6) 0.0126 (6) 0.0177 (6)
C3A 0.0387 (7) 0.0416 (8) 0.0347 (7) 0.0133 (6) 0.0131 (6) 0.0214 (6)
C4A 0.0373 (7) 0.0440 (8) 0.0330 (7) 0.0132 (6) 0.0127 (6) 0.0202 (6)
C5A 0.0650 (10) 0.0511 (9) 0.0413 (8) 0.0237 (8) 0.0250 (8) 0.0198 (7)
C6A 0.0832 (13) 0.0488 (10) 0.0561 (10) 0.0336 (9) 0.0268 (9) 0.0224 (8)
C7A 0.0954 (14) 0.0545 (10) 0.0622 (11) 0.0365 (10) 0.0306 (10) 0.0382 (9)
C8A 0.0746 (11) 0.0542 (10) 0.0464 (9) 0.0274 (9) 0.0275 (8) 0.0325 (8)
C9A 0.0537 (9) 0.0500 (9) 0.0367 (8) 0.0168 (7) 0.0194 (7) 0.0144 (7)
C10A 0.0517 (8) 0.0360 (7) 0.0358 (7) 0.0169 (6) 0.0196 (6) 0.0207 (6)
C11A 0.0579 (9) 0.0452 (9) 0.0392 (8) 0.0178 (7) 0.0177 (7) 0.0205 (7)
C12A 0.0550 (10) 0.0531 (10) 0.0601 (11) 0.0078 (8) 0.0105 (8) 0.0289 (9)
C13A 0.0535 (10) 0.0669 (12) 0.0961 (15) 0.0193 (9) 0.0366 (11) 0.0475 (12)
C14A 0.0730 (12) 0.0543 (10) 0.0812 (13) 0.0246 (9) 0.0521 (11) 0.0317 (10)
C15A 0.0645 (10) 0.0394 (8) 0.0473 (9) 0.0147 (7) 0.0300 (8) 0.0172 (7)
Cl1B 0.0539 (2) 0.0861 (3) 0.0579 (3) 0.0173 (2) 0.0323 (2) 0.0430 (2)
N1B 0.0468 (7) 0.0482 (7) 0.0335 (6) 0.0145 (6) 0.0176 (5) 0.0224 (6)
N2B 0.0424 (6) 0.0507 (7) 0.0378 (6) 0.0165 (6) 0.0186 (5) 0.0238 (6)
N3B 0.0442 (7) 0.0593 (8) 0.0366 (6) 0.0178 (6) 0.0175 (5) 0.0279 (6)
C1B 0.0465 (8) 0.0433 (8) 0.0391 (7) 0.0146 (6) 0.0240 (6) 0.0222 (6)
C2B 0.0445 (8) 0.0363 (7) 0.0333 (7) 0.0129 (6) 0.0161 (6) 0.0164 (6)
C3B 0.0410 (7) 0.0376 (7) 0.0328 (7) 0.0117 (6) 0.0158 (6) 0.0167 (6)
C4B 0.0455 (8) 0.0381 (7) 0.0334 (7) 0.0160 (6) 0.0176 (6) 0.0183 (6)
C5B 0.0473 (8) 0.0550 (9) 0.0383 (8) 0.0116 (7) 0.0094 (7) 0.0235 (7)
C6B 0.0391 (8) 0.0670 (11) 0.0533 (10) 0.0079 (8) 0.0096 (7) 0.0271 (9)
C7B 0.0439 (9) 0.0745 (12) 0.0571 (10) 0.0067 (8) 0.0222 (8) 0.0324 (9)
C8B 0.0483 (9) 0.0615 (10) 0.0413 (8) 0.0104 (7) 0.0189 (7) 0.0280 (8)
C9B 0.0469 (8) 0.0510 (9) 0.0336 (7) 0.0127 (7) 0.0099 (6) 0.0188 (7)
C10B 0.0418 (7) 0.0489 (8) 0.0320 (7) 0.0108 (6) 0.0131 (6) 0.0228 (6)
C11B 0.0460 (9) 0.0503 (9) 0.0505 (9) 0.0099 (7) 0.0080 (7) 0.0198 (8)
C12B 0.0681 (12) 0.0483 (10) 0.0621 (11) 0.0160 (9) 0.0205 (9) 0.0219 (9)
C13B 0.0703 (12) 0.0638 (12) 0.0747 (12) 0.0340 (10) 0.0371 (10) 0.0409 (10)
C14B 0.0452 (9) 0.0793 (14) 0.0774 (13) 0.0228 (9) 0.0166 (9) 0.0387 (11)
C15B 0.0447 (9) 0.0570 (10) 0.0501 (9) 0.0092 (7) 0.0088 (7) 0.0199 (8)

Geometric parameters (Å, º)

Cl1A—C1A 1.7403 (14) Cl1B—C1B 1.7503 (14)
N1A—C1A 1.2962 (19) N1B—C1B 1.2964 (19)
N1A—C2A 1.3826 (18) N1B—C2B 1.3866 (17)
N2A—C1A 1.3291 (18) N2B—C1B 1.3275 (18)
N2A—C4A 1.3359 (18) N2B—C4B 1.3383 (17)
N3A—C4A 1.3305 (17) N3B—C4B 1.3289 (17)
N3A—C9A 1.4537 (19) N3B—C9B 1.4489 (18)
N3A—H3AA 0.8600 N3B—H3BA 0.8600
C2A—C5A 1.401 (2) C2B—C5B 1.403 (2)
C2A—C3A 1.4040 (18) C2B—C3B 1.4051 (19)
C3A—C8A 1.407 (2) C3B—C8B 1.4047 (19)
C3A—C4A 1.444 (2) C3B—C4B 1.4446 (19)
C5A—C6A 1.364 (2) C5B—C6B 1.365 (2)
C5A—H5AA 0.9300 C5B—H5BA 0.9300
C6A—C7A 1.392 (3) C6B—C7B 1.394 (2)
C6A—H6AA 0.9300 C6B—H6BA 0.9300
C7A—C8A 1.366 (2) C7B—C8B 1.367 (2)
C7A—H7AA 0.9300 C7B—H7BA 0.9300
C8A—H8AA 0.9300 C8B—H8BA 0.9300
C9A—C10A 1.506 (2) C9B—C10B 1.508 (2)
C9A—H9AA 0.9700 C9B—H9BA 0.9700
C9A—H9AB 0.9700 C9B—H9BB 0.9700
C10A—C15A 1.384 (2) C10B—C11B 1.379 (2)
C10A—C11A 1.385 (2) C10B—C15B 1.382 (2)
C11A—C12A 1.378 (2) C11B—C12B 1.383 (2)
C11A—H11A 0.9300 C11B—H11B 0.9300
C12A—C13A 1.377 (3) C12B—C13B 1.365 (3)
C12A—H12A 0.9300 C12B—H12B 0.9300
C13A—C14A 1.368 (3) C13B—C14B 1.370 (3)
C13A—H13A 0.9300 C13B—H13B 0.9300
C14A—C15A 1.375 (2) C14B—C15B 1.378 (3)
C14A—H14A 0.9300 C14B—H14B 0.9300
C15A—H15A 0.9300 C15B—H15B 0.9300
C1A—N1A—C2A 114.20 (12) C1B—N1B—C2B 113.92 (12)
C1A—N2A—C4A 115.75 (12) C1B—N2B—C4B 115.30 (12)
C4A—N3A—C9A 124.03 (13) C4B—N3B—C9B 123.18 (12)
C4A—N3A—H3AA 118.0 C4B—N3B—H3BA 118.4
C9A—N3A—H3AA 118.0 C9B—N3B—H3BA 118.4
N1A—C1A—N2A 131.20 (13) N1B—C1B—N2B 131.77 (13)
N1A—C1A—Cl1A 115.28 (11) N1B—C1B—Cl1B 114.95 (10)
N2A—C1A—Cl1A 113.52 (11) N2B—C1B—Cl1B 113.29 (11)
N1A—C2A—C5A 118.76 (13) N1B—C2B—C5B 118.87 (13)
N1A—C2A—C3A 121.78 (13) N1B—C2B—C3B 121.78 (13)
C5A—C2A—C3A 119.46 (13) C5B—C2B—C3B 119.35 (13)
C2A—C3A—C8A 119.10 (13) C8B—C3B—C2B 119.24 (13)
C2A—C3A—C4A 116.21 (12) C8B—C3B—C4B 124.64 (13)
C8A—C3A—C4A 124.69 (13) C2B—C3B—C4B 116.11 (12)
N3A—C4A—N2A 117.73 (13) N3B—C4B—N2B 117.24 (13)
N3A—C4A—C3A 121.47 (13) N3B—C4B—C3B 121.66 (12)
N2A—C4A—C3A 120.80 (12) N2B—C4B—C3B 121.10 (12)
C6A—C5A—C2A 120.19 (15) C6B—C5B—C2B 120.14 (14)
C6A—C5A—H5AA 119.9 C6B—C5B—H5BA 119.9
C2A—C5A—H5AA 119.9 C2B—C5B—H5BA 119.9
C5A—C6A—C7A 120.63 (16) C5B—C6B—C7B 120.74 (15)
C5A—C6A—H6AA 119.7 C5B—C6B—H6BA 119.6
C7A—C6A—H6AA 119.7 C7B—C6B—H6BA 119.6
C8A—C7A—C6A 120.38 (16) C8B—C7B—C6B 120.19 (15)
C8A—C7A—H7AA 119.8 C8B—C7B—H7BA 119.9
C6A—C7A—H7AA 119.8 C6B—C7B—H7BA 119.9
C7A—C8A—C3A 120.23 (15) C7B—C8B—C3B 120.34 (14)
C7A—C8A—H8AA 119.9 C7B—C8B—H8BA 119.8
C3A—C8A—H8AA 119.9 C3B—C8B—H8BA 119.8
N3A—C9A—C10A 112.90 (13) N3B—C9B—C10B 114.71 (12)
N3A—C9A—H9AA 109.0 N3B—C9B—H9BA 108.6
C10A—C9A—H9AA 109.0 C10B—C9B—H9BA 108.6
N3A—C9A—H9AB 109.0 N3B—C9B—H9BB 108.6
C10A—C9A—H9AB 109.0 C10B—C9B—H9BB 108.6
H9AA—C9A—H9AB 107.8 H9BA—C9B—H9BB 107.6
C15A—C10A—C11A 118.33 (14) C11B—C10B—C15B 118.09 (15)
C15A—C10A—C9A 119.91 (14) C11B—C10B—C9B 122.94 (14)
C11A—C10A—C9A 121.75 (13) C15B—C10B—C9B 118.97 (14)
C12A—C11A—C10A 120.64 (15) C10B—C11B—C12B 120.99 (16)
C12A—C11A—H11A 119.7 C10B—C11B—H11B 119.5
C10A—C11A—H11A 119.7 C12B—C11B—H11B 119.5
C13A—C12A—C11A 120.16 (17) C13B—C12B—C11B 120.26 (17)
C13A—C12A—H12A 119.9 C13B—C12B—H12B 119.9
C11A—C12A—H12A 119.9 C11B—C12B—H12B 119.9
C14A—C13A—C12A 119.70 (17) C12B—C13B—C14B 119.29 (17)
C14A—C13A—H13A 120.1 C12B—C13B—H13B 120.4
C12A—C13A—H13A 120.1 C14B—C13B—H13B 120.4
C13A—C14A—C15A 120.30 (17) C13B—C14B—C15B 120.74 (17)
C13A—C14A—H14A 119.9 C13B—C14B—H14B 119.6
C15A—C14A—H14A 119.8 C15B—C14B—H14B 119.6
C14A—C15A—C10A 120.86 (16) C14B—C15B—C10B 120.61 (17)
C14A—C15A—H15A 119.6 C14B—C15B—H15B 119.7
C10A—C15A—H15A 119.6 C10B—C15B—H15B 119.7
C2A—N1A—C1A—N2A −1.2 (2) C2B—N1B—C1B—N2B 0.5 (2)
C2A—N1A—C1A—Cl1A 177.92 (10) C2B—N1B—C1B—Cl1B −179.43 (10)
C4A—N2A—C1A—N1A −0.1 (3) C4B—N2B—C1B—N1B 0.1 (2)
C4A—N2A—C1A—Cl1A −179.20 (11) C4B—N2B—C1B—Cl1B −179.97 (10)
C1A—N1A—C2A—C5A −179.46 (14) C1B—N1B—C2B—C5B −178.94 (14)
C1A—N1A—C2A—C3A 0.4 (2) C1B—N1B—C2B—C3B 0.2 (2)
N1A—C2A—C3A—C8A −179.03 (14) N1B—C2B—C3B—C8B −179.85 (14)
C5A—C2A—C3A—C8A 0.8 (2) C5B—C2B—C3B—C8B −0.8 (2)
N1A—C2A—C3A—C4A 1.3 (2) N1B—C2B—C3B—C4B −1.2 (2)
C5A—C2A—C3A—C4A −178.80 (13) C5B—C2B—C3B—C4B 177.84 (13)
C9A—N3A—C4A—N2A −3.4 (2) C9B—N3B—C4B—N2B −1.8 (2)
C9A—N3A—C4A—C3A 176.58 (13) C9B—N3B—C4B—C3B 177.81 (13)
C1A—N2A—C4A—N3A −177.93 (13) C1B—N2B—C4B—N3B 178.31 (13)
C1A—N2A—C4A—C3A 2.1 (2) C1B—N2B—C4B—C3B −1.3 (2)
C2A—C3A—C4A—N3A 177.36 (13) C8B—C3B—C4B—N3B 0.8 (2)
C8A—C3A—C4A—N3A −2.3 (2) C2B—C3B—C4B—N3B −177.75 (13)
C2A—C3A—C4A—N2A −2.6 (2) C8B—C3B—C4B—N2B −179.62 (14)
C8A—C3A—C4A—N2A 177.74 (15) C2B—C3B—C4B—N2B 1.9 (2)
N1A—C2A—C5A—C6A 179.50 (15) N1B—C2B—C5B—C6B 179.16 (15)
C3A—C2A—C5A—C6A −0.4 (2) C3B—C2B—C5B—C6B 0.0 (2)
C2A—C5A—C6A—C7A −0.2 (3) C2B—C5B—C6B—C7B 0.4 (3)
C5A—C6A—C7A—C8A 0.2 (3) C5B—C6B—C7B—C8B −0.2 (3)
C6A—C7A—C8A—C3A 0.2 (3) C6B—C7B—C8B—C3B −0.6 (3)
C2A—C3A—C8A—C7A −0.8 (2) C2B—C3B—C8B—C7B 1.0 (2)
C4A—C3A—C8A—C7A 178.83 (16) C4B—C3B—C8B—C7B −177.45 (16)
C4A—N3A—C9A—C10A −99.54 (17) C4B—N3B—C9B—C10B 83.98 (18)
N3A—C9A—C10A—C15A −145.39 (14) N3B—C9B—C10B—C11B 1.7 (2)
N3A—C9A—C10A—C11A 35.9 (2) N3B—C9B—C10B—C15B −178.82 (14)
C15A—C10A—C11A—C12A −0.5 (2) C15B—C10B—C11B—C12B 0.2 (2)
C9A—C10A—C11A—C12A 178.29 (15) C9B—C10B—C11B—C12B 179.71 (15)
C10A—C11A—C12A—C13A 0.5 (3) C10B—C11B—C12B—C13B −0.4 (3)
C11A—C12A—C13A—C14A 0.0 (3) C11B—C12B—C13B—C14B 0.2 (3)
C12A—C13A—C14A—C15A −0.5 (3) C12B—C13B—C14B—C15B 0.2 (3)
C13A—C14A—C15A—C10A 0.6 (3) C13B—C14B—C15B—C10B −0.4 (3)
C11A—C10A—C15A—C14A −0.1 (2) C11B—C10B—C15B—C14B 0.2 (2)
C9A—C10A—C15A—C14A −178.87 (15) C9B—C10B—C15B—C14B −179.30 (16)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
N3A—H3AA···N1Bi 0.86 2.21 2.9954 (17) 152
N3B—H3BA···N1A 0.86 2.18 2.9482 (16) 149

Symmetry code: (i) x, y, z−1.

Footnotes

Supporting information for this paper is available from the IUCr electronic archives (Reference: LH5690).

References

  1. Brandenburg, K. (1999). DIAMOND Crystal Impact GbR, Bonn, Germany.
  2. Bruker (2008). APEX2 and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  3. Deng, X. & Mani, N. S. (2006). Org. Lett. 8, 269–272. [DOI] [PubMed]
  4. Lee, S. J., Konishi, Y., Yu, D. T., Miskowski, T. A., Riviello, C. M., Macina, O. T., Frierson, M. R., Kondo, K., Sugitani, M., Sircar, J. C. & Balzejewski, K. M. (1995). J. Med. Chem. 38, 3547–3557. [DOI] [PubMed]
  5. Lopez, C. O., Garcia, C. A., Nunez, M. C., Kimatrai, M., Rubino, G. M. E., Morales, F., Perez, G. V. & Campos, J. M. (2011). Curr. Med. Chem. 18, 943–963. [DOI] [PubMed]
  6. Mohamed, T., Zhao, X., Habib, L. K., Yang, J. & Rao, P. P. N. (2011). Bioorg. Med. Chem. 19, 2269–2281. [DOI] [PMC free article] [PubMed]
  7. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  8. Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.
  9. Wynne, G. M., De Moor, O., Johnson, P. D. & Vickers, R. (2009). World Patent WO 2009/001060 A2.
  10. Yoshida, K. & Taguchi, M. (1992). J. Chem. Soc. Perkin Trans. 1, pp. 919–922.
  11. Zhang, J., Yang, P. L. & Gray, N. S. (2009). Nat. Rev. Cancer, 9, 28–39. [DOI] [PMC free article] [PubMed]
  12. Zhou, G., Wang, L., Ma, Y., Wang, L., Zhang, Y. & Jiang, W. (2011). Bioorg. Med. Chem. Lett. 21, 5905–5909. [DOI] [PubMed]

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) I. DOI: 10.1107/S1600536814006746/lh5690sup1.cif

e-70-0o554-sup1.cif (834.6KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814006746/lh5690Isup2.hkl

e-70-0o554-Isup2.hkl (319.6KB, hkl)

Supporting information file. DOI: 10.1107/S1600536814006746/lh5690Isup3.cml

CCDC reference: 993912

Additional supporting information: crystallographic information; 3D view; checkCIF report


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