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In the title compound, C24H17Cl2NO, the oxazine ring adopts a half-chair conformation. The dihedral angle between the phenyl ring and the naphthyl ring system is 78.56 (9)°. Intra­molecular C—H...Cl hydrogen bonding is observed in the crystal structure.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S160053680705787X/xu2366sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S160053680705787X/xu2366Isup2.hkl
Contains datablock I

CCDC reference: 672995

Key indicators

  • Single-crystal X-ray study
  • T = 291 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.047
  • wR factor = 0.104
  • Data-to-parameter ratio = 14.8

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT420_ALERT_2_C D-H Without Acceptor N1 - H1A ... ?
Alert level G PLAT793_ALERT_1_G Check the Absolute Configuration of C11 = ... S PLAT793_ALERT_1_G Check the Absolute Configuration of C18 = ... S
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 1 ALERT level C = Check and explain 2 ALERT level G = General alerts; check 2 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 0 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

The class of oxazine derivatives is useful heterocyclic compound which is widely used as antimalarial agent (Ren et al., 2001) and a versatile intermediate for the synthesis of carbapenems (Fuganti et al., 1994). Here we present the synthesis and crystal structure of the title compound.

In the molecule (Fig. 1), the oxazine ring is distorted and adopts a half chair conformation, O1 and N1 atoms deviate from the O1—C18—N1—C11—C1—C2 mean plane by 0.168 (1) and 0.282 (2)%A, respectively. The dihedral angle between the C12-phenyl ring and naphthyl system is 78.56 (9)°. Intra-molecular C—H···Cl hydrogen bond is observed in the crystal structure (Table 1), but no inter-molecular hydrogen bonding occurs in the crystal structure.

Related literature top

For general background, see: Fuganti et al. (1994); Ren et al. (2001).

Experimental top

1-(Amino(phenyl)methyl)naphthalen-2-ol (1 mmol, 0.249 g) was dissolved in anhydrous methanol, the solution was stirred for several min. and then 2,4-dichlorobenzyaldehyde (1 mmol 0.175 g) in methanol (8 ml) was added dropwise and the mixture was stirred at room temperature for 2 h. The product was isolated and recrystallized in a methanol solution, colourless single crystals were obtained after 2 d.

Refinement top

Amine H atom was located in a difference Fourier map and positional parameters were refined, Uiso(H) = 1.2Ueq(N). Other H atoms were placed in calculated positions with C—H = 0.93 Å (aromatic) and 0.97 Å (methine) and refined in riding mode with Uiso(H) = 1.2Ueq(C).

Computing details top

Data collection: SMART (Bruker, 2000); cell refinement: SAINT (Bruker, 2000); data reduction: SAINT (Bruker, 2000); program(s) used to solve structure: SHELXTL (Bruker, 2000); program(s) used to refine structure: SHELXTL (Bruker, 2000; molecular graphics: SHELXTL (Bruker, 2000; software used to prepare material for publication: SHELXTL (Bruker, 2000.

Figures top
[Figure 1] Fig. 1. the ORTEP plot of (I). Displacement ellipsoids are drawn at the 30% probability level. H atoms are presented as small spheres of arbitrary radii.
3-(2,4-Dichlorophenyl)-1-phenyl-2,3-dihydro-1H-naphtho[1,2-e][1,3]oxazine top
Crystal data top
C24H17Cl2NOZ = 2
Mr = 406.29F(000) = 420
Triclinic, P1Dx = 1.397 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 6.664 (3) ÅCell parameters from 816 reflections
b = 8.224 (3) Åθ = 2.3–20.1°
c = 18.106 (7) ŵ = 0.35 mm1
α = 92.269 (6)°T = 291 K
β = 99.420 (5)°Block, colourless
γ = 98.624 (6)°0.30 × 0.26 × 0.24 mm
V = 965.8 (7) Å3
Data collection top
Bruker SMART Apex CCD area-detector
diffractometer
3386 reflections with I > 2σ(I)
Radiation source: sealed tubeRint = 0.034
Graphite monochromatorθmax = 26.0°, θmin = 1.1°
ϕ and ω scansh = 88
7267 measured reflectionsk = 1010
3783 independent reflectionsl = 2222
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)] = 0.047Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.104H atoms treated by a mixture of independent and constrained refinement
S = 1.02 w = 1/[σ2(Fo2) + (0.04P)2 + 0.66P]
where P = (Fo2 + 2Fc2)/3
3783 reflections(Δ/σ)max < 0.001
256 parametersΔρmax = 0.16 e Å3
0 restraintsΔρmin = 0.21 e Å3
Crystal data top
C24H17Cl2NOγ = 98.624 (6)°
Mr = 406.29V = 965.8 (7) Å3
Triclinic, P1Z = 2
a = 6.664 (3) ÅMo Kα radiation
b = 8.224 (3) ŵ = 0.35 mm1
c = 18.106 (7) ÅT = 291 K
α = 92.269 (6)°0.30 × 0.26 × 0.24 mm
β = 99.420 (5)°
Data collection top
Bruker SMART Apex CCD area-detector
diffractometer
3386 reflections with I > 2σ(I)
7267 measured reflectionsRint = 0.034
3783 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0470 restraints
wR(F2) = 0.104H atoms treated by a mixture of independent and constrained refinement
S = 1.02Δρmax = 0.16 e Å3
3783 reflectionsΔρmin = 0.21 e Å3
256 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. 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
C10.0160 (3)0.4644 (2)0.26512 (12)0.0363 (4)
C20.1740 (3)0.5189 (2)0.21512 (10)0.0317 (4)
C30.3762 (3)0.4255 (3)0.19891 (12)0.0378 (5)
H30.47890.46540.16690.045*
C40.4207 (3)0.2810 (3)0.22920 (13)0.0437 (5)
H40.55380.22220.21920.052*
C50.2576 (3)0.2171 (3)0.27800 (12)0.0381 (5)
C60.0633 (3)0.3062 (2)0.29281 (11)0.0350 (4)
C70.1011 (4)0.2367 (3)0.33856 (12)0.0440 (5)
H70.23380.29580.35060.053*
C80.0552 (3)0.0841 (3)0.36297 (12)0.0395 (5)
H80.15980.03750.39060.047*
C90.1457 (4)0.0061 (3)0.34780 (14)0.0481 (6)
H90.17140.10900.36690.058*
C100.3037 (4)0.0551 (3)0.30547 (13)0.0465 (6)
H100.43590.00530.29470.056*
C110.1908 (3)0.5714 (3)0.28337 (11)0.0341 (4)
H110.29410.51280.26630.041*
C120.2558 (3)0.6199 (3)0.36802 (12)0.0388 (5)
C130.1190 (3)0.6381 (3)0.41515 (11)0.0408 (5)
H130.02170.61140.39750.049*
C140.1890 (4)0.6959 (3)0.48886 (13)0.0470 (5)
H140.09350.70790.52000.056*
C150.3972 (4)0.7365 (3)0.51786 (13)0.0481 (6)
H150.44170.77560.56760.058*
C160.5396 (4)0.7171 (3)0.46977 (14)0.0554 (7)
H160.68010.74590.48740.066*
C170.4700 (3)0.6547 (3)0.39579 (12)0.0391 (5)
H170.56380.63600.36480.047*
C180.0708 (3)0.7100 (2)0.17348 (11)0.0332 (4)
H180.11950.62850.14270.040*
C190.0854 (3)0.8725 (2)0.13725 (11)0.0356 (4)
C200.2413 (3)0.9202 (3)0.09702 (12)0.0409 (5)
C210.2598 (4)1.0652 (3)0.06420 (12)0.0419 (5)
H210.36351.09250.03610.050*
C220.1272 (3)1.1695 (2)0.07259 (11)0.0333 (4)
C230.0264 (3)1.1347 (3)0.11365 (13)0.0419 (5)
H230.11311.21060.12070.050*
C240.0500 (3)0.9809 (3)0.14506 (12)0.0410 (5)
H240.15760.95200.17130.049*
Cl10.41832 (9)0.78745 (8)0.08509 (4)0.05364 (18)
Cl20.15778 (9)1.36256 (7)0.03317 (3)0.04927 (17)
N10.1937 (3)0.7299 (2)0.24802 (10)0.0359 (4)
H1A0.138 (4)0.797 (3)0.2759 (14)0.043*
O10.1441 (2)0.65590 (19)0.17832 (8)0.0403 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0295 (10)0.0336 (10)0.0448 (12)0.0019 (8)0.0074 (8)0.0025 (9)
C20.0261 (9)0.0415 (11)0.0264 (9)0.0008 (8)0.0073 (7)0.0010 (8)
C30.0324 (10)0.0398 (11)0.0389 (11)0.0012 (9)0.0066 (8)0.0008 (9)
C40.0298 (10)0.0464 (12)0.0520 (13)0.0084 (9)0.0130 (9)0.0001 (10)
C50.0294 (10)0.0428 (11)0.0399 (11)0.0066 (8)0.0131 (8)0.0070 (9)
C60.0372 (11)0.0364 (10)0.0286 (10)0.0029 (8)0.0072 (8)0.0038 (8)
C70.0546 (14)0.0467 (12)0.0306 (10)0.0130 (10)0.0027 (9)0.0034 (9)
C80.0362 (11)0.0452 (12)0.0384 (11)0.0061 (9)0.0113 (9)0.0015 (9)
C90.0502 (14)0.0424 (12)0.0492 (13)0.0049 (10)0.0120 (11)0.0029 (10)
C100.0428 (13)0.0446 (12)0.0473 (13)0.0130 (10)0.0128 (10)0.0017 (10)
C110.0282 (10)0.0416 (11)0.0278 (9)0.0028 (8)0.0031 (7)0.0114 (8)
C120.0349 (11)0.0468 (12)0.0351 (11)0.0109 (9)0.0012 (8)0.0087 (9)
C130.0397 (11)0.0541 (13)0.0303 (10)0.0138 (10)0.0047 (9)0.0020 (9)
C140.0559 (14)0.0395 (12)0.0411 (12)0.0034 (10)0.0054 (10)0.0003 (9)
C150.0543 (14)0.0510 (13)0.0362 (11)0.0067 (11)0.0030 (10)0.0071 (10)
C160.0403 (13)0.0630 (16)0.0516 (14)0.0134 (11)0.0005 (11)0.0193 (12)
C170.0329 (11)0.0475 (12)0.0421 (12)0.0208 (9)0.0076 (9)0.0070 (9)
C180.0310 (10)0.0354 (10)0.0316 (10)0.0033 (8)0.0008 (8)0.0064 (8)
C190.0369 (11)0.0313 (10)0.0360 (10)0.0015 (8)0.0027 (8)0.0005 (8)
C200.0409 (12)0.0381 (11)0.0424 (12)0.0029 (9)0.0059 (9)0.0060 (9)
C210.0537 (13)0.0375 (11)0.0325 (11)0.0102 (10)0.0021 (9)0.0046 (9)
C220.0375 (10)0.0315 (10)0.0260 (9)0.0023 (8)0.0057 (8)0.0001 (7)
C230.0423 (12)0.0381 (11)0.0477 (13)0.0094 (9)0.0119 (10)0.0037 (9)
C240.0427 (12)0.0519 (13)0.0314 (10)0.0115 (10)0.0109 (9)0.0054 (9)
Cl10.0490 (3)0.0618 (4)0.0551 (4)0.0125 (3)0.0175 (3)0.0144 (3)
Cl20.0547 (3)0.0395 (3)0.0520 (3)0.0126 (2)0.0025 (3)0.0124 (2)
N10.0295 (9)0.0434 (10)0.0324 (9)0.0014 (7)0.0026 (7)0.0111 (7)
O10.0280 (7)0.0484 (9)0.0420 (8)0.0047 (6)0.0019 (6)0.0125 (7)
Geometric parameters (Å, º) top
C1—C21.411 (3)C13—H130.9300
C1—C61.422 (3)C14—C151.386 (3)
C1—C111.499 (3)C14—H140.9300
C2—O11.337 (2)C15—C161.411 (4)
C2—C31.426 (3)C15—H150.9300
C3—C41.342 (3)C16—C171.394 (3)
C3—H30.9300C16—H160.9300
C4—C51.460 (3)C17—H170.9300
C4—H40.9300C18—N11.449 (3)
C5—C61.368 (3)C18—O11.453 (2)
C5—C101.448 (3)C18—C191.509 (3)
C6—C71.463 (3)C18—H180.9800
C7—C81.355 (3)C19—C241.379 (3)
C7—H70.9300C19—C201.383 (3)
C8—C91.409 (3)C20—C211.351 (3)
C8—H80.9300C20—Cl11.756 (2)
C9—C101.369 (4)C21—C221.342 (3)
C9—H90.9300C21—H210.9300
C10—H100.9300C22—C231.364 (3)
C11—N11.474 (3)C22—Cl21.764 (2)
C11—C121.542 (3)C23—C241.405 (3)
C11—H110.9800C23—H230.9300
C12—C131.366 (3)C24—H240.9300
C12—C171.416 (3)N1—H1A0.89 (2)
C13—C141.380 (3)
C2—C1—C6116.83 (18)C14—C13—H13119.9
C2—C1—C11118.91 (18)C13—C14—C15122.0 (2)
C6—C1—C11124.21 (19)C13—C14—H14119.0
O1—C2—C1123.06 (17)C15—C14—H14119.0
O1—C2—C3115.88 (18)C14—C15—C16118.2 (2)
C1—C2—C3121.02 (19)C14—C15—H15120.9
C4—C3—C2121.0 (2)C16—C15—H15120.9
C4—C3—H3119.5C17—C16—C15120.1 (2)
C2—C3—H3119.5C17—C16—H16120.0
C3—C4—C5119.18 (19)C15—C16—H16120.0
C3—C4—H4120.4C16—C17—C12119.6 (2)
C5—C4—H4120.4C16—C17—H17120.2
C6—C5—C10121.7 (2)C12—C17—H17120.2
C6—C5—C4119.6 (2)N1—C18—O1109.70 (16)
C10—C5—C4118.57 (18)N1—C18—C19110.19 (16)
C5—C6—C1122.0 (2)O1—C18—C19107.78 (16)
C5—C6—C7119.0 (2)N1—C18—H18109.7
C1—C6—C7118.94 (19)O1—C18—H18109.7
C8—C7—C6118.3 (2)C19—C18—H18109.7
C8—C7—H7120.8C24—C19—C20117.6 (2)
C6—C7—H7120.8C24—C19—C18121.76 (19)
C7—C8—C9122.1 (2)C20—C19—C18120.58 (19)
C7—C8—H8118.9C21—C20—C19122.2 (2)
C9—C8—H8118.9C21—C20—Cl1118.04 (18)
C10—C9—C8121.2 (2)C19—C20—Cl1119.74 (17)
C10—C9—H9119.4C22—C21—C20119.4 (2)
C8—C9—H9119.4C22—C21—H21120.3
C9—C10—C5117.6 (2)C20—C21—H21120.3
C9—C10—H10121.2C21—C22—C23122.2 (2)
C5—C10—H10121.2C21—C22—Cl2119.43 (17)
N1—C11—C1112.31 (16)C23—C22—Cl2118.29 (16)
N1—C11—C12104.43 (17)C22—C23—C24118.1 (2)
C1—C11—C12112.58 (17)C22—C23—H23121.0
N1—C11—H11109.1C24—C23—H23121.0
C1—C11—H11109.1C19—C24—C23120.4 (2)
C12—C11—H11109.1C19—C24—H24119.8
C13—C12—C17119.7 (2)C23—C24—H24119.8
C13—C12—C11123.50 (19)C18—N1—C11111.41 (16)
C17—C12—C11116.68 (19)C18—N1—H1A107.6 (16)
C12—C13—C14120.2 (2)C11—N1—H1A108.0 (16)
C12—C13—H13119.9C2—O1—C18113.20 (15)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C18—H18···Cl10.982.603.030 (3)107

Experimental details

Crystal data
Chemical formulaC24H17Cl2NO
Mr406.29
Crystal system, space groupTriclinic, P1
Temperature (K)291
a, b, c (Å)6.664 (3), 8.224 (3), 18.106 (7)
α, β, γ (°)92.269 (6), 99.420 (5), 98.624 (6)
V3)965.8 (7)
Z2
Radiation typeMo Kα
µ (mm1)0.35
Crystal size (mm)0.30 × 0.26 × 0.24
Data collection
DiffractometerBruker SMART Apex CCD area-detector
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
7267, 3783, 3386
Rint0.034
(sin θ/λ)max1)0.617
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.047, 0.104, 1.02
No. of reflections3783
No. of parameters256
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.16, 0.21

Computer programs: SMART (Bruker, 2000), SAINT (Bruker, 2000), SHELXTL (Bruker, 2000), SHELXTL (Bruker, 2000.

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C18—H18···Cl10.982.603.030 (3)107
 

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