organic compounds
5,7-Dibromo-3-trifluoromethyl-3,4-dihydroacridin-1(2H)-one
aDepartment of Chemistry, Boswell Science Complex, Tennessee State University, Nashville, 3500 John A Merritt Blvd, Nashville, TN 37209, USA
*Correspondence e-mail: tsiddiqu@tnstate.edu
In the title compound, C14H8Br2F3NO, the molecule is disordered across an approximate non-crystallographic mirror plane, which is in the plane of the fused ring system [The tetrahedral C atom bearing the trifluormethyl substituent is disordered with site occupancy factors of 0.80 (2) and 0.20 (2)]. In the crystal, a one-dimensional stacking of molecules involves interactions between the pyridine ring and symmetry-related Br and O atoms of adjacent molecules. The stacking distance between the mean planes of adjacent molecules is 3.395 (4) Å.
Related literature
For the anticancer activity of the title compound, see: Fadeyi et al. (2008). For fluorinated acridones, see: Fadeyi et al. (2008); Mayur et al. (2009); Svyatkina et al. (1988). For a related structure, see: Martinez et al. (1995).
Experimental
Crystal data
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Data collection: CrystalClear (Rigaku, 1999; Pflugrath, 1999); cell CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SIR2004 (Burla et al., 2005); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997) as included in WinGX (Farrugia, 1999); software used to prepare material for publication: WinGX and publCIF (Westrip, 2010).
Supporting information
10.1107/S1600536811027516/pk2334sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536811027516/pk2334Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536811027516/pk2334Isup3.cml
To a mixture of 3,5-dibromo-2-aminobenzaldehyde (1.0 mmol) and 5-trifluoromethyl-cyclohexanedione (1.0 mmol) was added 1 mL of 1N HCl. The reaction mixture was stirred at 60–75°C for 30 minutes. After this period the reaction mixture was neutralized with 1 mL of 1N NaOH. The solid was filtered and washed with water (3 × 6 mL) and air dried. Colorless single crystals suitable for X-ray diffraction studies were harvested after recrystallization from aqueous ethanol. M.p. = 140–143°C. IR (nujol): 2925, 1600, 1465, 964 and 787 cm-1. 1HNMR (CDCl3): δ 2.4–2.49 (dd, 2H), 2.88–2.93 (dd, 2H), 3.22 (m, 1H), 8.32 (d, 1H), 8.91 (s, 1H).
H atoms (except those of the minor disorder component) were found in difference Fourier maps and subsequently placed in idealized positions with constrained distances of 0.97 Å (R2CH2), 0.98 Å (R3CH), 0.93 Å (Csp2H), and with Uiso(H) values set to 1.2Ueq of the attached atom.
To ensure satisfactory
of the disordered parts of the structure, a combination of constraints and restraints were needed. The constraints (SHELXL97 command EADP) were used to make the displacement parameters of closely proximate disordered atoms equal. The restraints (SHELXL97 commands SAME, SIMU & DELU) were used to ensure similar geometries and displacement parameters of closely proximate, chemically identical groups.Data collection: CrystalClear (Rigaku, 1999; Pflugrath, 1999); cell
CrystalClear (Rigaku, 1999; Pflugrath, 1999); data reduction: CrystalClear (Rigaku, 1999; Pflugrath, 1999); program(s) used to solve structure: SIR2004 (Burla et al., 2005); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997) as included in WinGX (Farrugia, 1999); software used to prepare material for publication: WinGX (Farrugia, 1999) and publCIF (Westrip, 2010).Fig. 1. Thermal ellipsoid plot (50% probability) of 5,7-dibromo-3-(trifluoromethyl)-3,4-dihydroacridin-1(2H)-one. In the interest of clarity, only the major component of disorder is shown. |
C14H8Br2F3NO | Z = 2 |
Mr = 423.03 | F(000) = 408 |
Triclinic, P1 | Dx = 1.977 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 5.3303 (10) Å | Cell parameters from 3749 reflections |
b = 10.926 (2) Å | θ = 3.3–27.6° |
c = 12.354 (2) Å | µ = 5.74 mm−1 |
α = 83.349 (6)° | T = 293 K |
β = 85.741 (6)° | Prism, colorless |
γ = 85.051 (6)° | 0.21 × 0.13 × 0.06 mm |
V = 710.5 (2) Å3 |
Rigaku XtaLAB mini diffractometer | 2188 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.050 |
ω scans | θmax = 27.5°, θmin = 3.3° |
Absorption correction: multi-scan (CrystalClear; Rigaku, 1999; Pflugrath, 1999) | h = −3→6 |
Tmin = 0.379, Tmax = 0.725 | k = −14→14 |
4444 measured reflections | l = −15→15 |
3153 independent reflections |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.055 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.134 | H-atom parameters constrained |
S = 0.97 | w = 1/[σ2(Fo2) + (0.0643P)2] where P = (Fo2 + 2Fc2)/3 |
3153 reflections | (Δ/σ)max = 0.001 |
217 parameters | Δρmax = 0.80 e Å−3 |
34 restraints | Δρmin = −0.67 e Å−3 |
C14H8Br2F3NO | γ = 85.051 (6)° |
Mr = 423.03 | V = 710.5 (2) Å3 |
Triclinic, P1 | Z = 2 |
a = 5.3303 (10) Å | Mo Kα radiation |
b = 10.926 (2) Å | µ = 5.74 mm−1 |
c = 12.354 (2) Å | T = 293 K |
α = 83.349 (6)° | 0.21 × 0.13 × 0.06 mm |
β = 85.741 (6)° |
Rigaku XtaLAB mini diffractometer | 3153 independent reflections |
Absorption correction: multi-scan (CrystalClear; Rigaku, 1999; Pflugrath, 1999) | 2188 reflections with I > 2σ(I) |
Tmin = 0.379, Tmax = 0.725 | Rint = 0.050 |
4444 measured reflections |
R[F2 > 2σ(F2)] = 0.055 | 34 restraints |
wR(F2) = 0.134 | H-atom parameters constrained |
S = 0.97 | Δρmax = 0.80 e Å−3 |
3153 reflections | Δρmin = −0.67 e Å−3 |
217 parameters |
Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
Br1 | −0.08381 (9) | 0.38272 (5) | 0.91649 (4) | 0.05150 (19) | |
Br2 | 0.25701 (14) | 0.07810 (5) | 0.58890 (5) | 0.0731 (2) | |
N1 | 0.3349 (7) | 0.5389 (3) | 0.8099 (3) | 0.0420 (9) | |
O1 | 1.0453 (7) | 0.6599 (4) | 0.5769 (3) | 0.0583 (10) | |
C1 | 0.8841 (9) | 0.6822 (5) | 0.6495 (4) | 0.0455 (11) | |
C2 | 0.875 (2) | 0.7995 (11) | 0.7024 (11) | 0.051 (3) | 0.796 (6) |
H2A | 0.7635 | 0.8621 | 0.6642 | 0.061* | 0.796 (6) |
H2B | 1.0423 | 0.8292 | 0.6969 | 0.061* | 0.796 (6) |
C3 | 0.7812 (11) | 0.7788 (5) | 0.8223 (5) | 0.0418 (14) | 0.796 (6) |
H3 | 0.8977 | 0.7168 | 0.8602 | 0.05* | 0.796 (6) |
C11 | 0.770 (2) | 0.8972 (8) | 0.8778 (9) | 0.056 (2) | 0.796 (6) |
F1 | 0.6920 (9) | 0.8785 (4) | 0.9826 (3) | 0.0747 (14) | 0.796 (6) |
F2 | 1.0046 (8) | 0.9352 (4) | 0.8774 (4) | 0.0779 (15) | 0.796 (6) |
F3 | 0.6313 (10) | 0.9893 (4) | 0.8297 (4) | 0.0829 (18) | 0.796 (6) |
C4 | 0.519 (3) | 0.7294 (10) | 0.8318 (9) | 0.048 (3) | 0.796 (6) |
H4A | 0.4667 | 0.7103 | 0.9084 | 0.058* | 0.796 (6) |
H4B | 0.3987 | 0.7933 | 0.8007 | 0.058* | 0.796 (6) |
C2' | 0.897 (9) | 0.779 (5) | 0.718 (5) | 0.051 (3) | 0.204 (6) |
H2'1 | 0.9643 | 0.8496 | 0.6739 | 0.061* | 0.204 (6) |
H2'2 | 1.0123 | 0.7504 | 0.7741 | 0.061* | 0.204 (6) |
C3' | 0.641 (4) | 0.8190 (18) | 0.7713 (17) | 0.044 (5)* | 0.204 (6) |
H3' | 0.5204 | 0.8398 | 0.7148 | 0.053* | 0.204 (6) |
C11' | 0.661 (4) | 0.933 (2) | 0.831 (2) | 0.058 (7)* | 0.204 (6) |
F1' | 0.442 (3) | 0.9642 (17) | 0.8836 (14) | 0.084 (6)* | 0.204 (6) |
F2' | 0.828 (6) | 0.897 (3) | 0.910 (2) | 0.095 (12)* | 0.204 (6) |
F3' | 0.754 (4) | 1.0247 (17) | 0.7699 (17) | 0.093 (7)* | 0.204 (6) |
C4' | 0.546 (13) | 0.714 (4) | 0.853 (5) | 0.048 (3) | 0.204 (6) |
H4'1 | 0.3875 | 0.7386 | 0.8911 | 0.058* | 0.204 (6) |
H4'2 | 0.6692 | 0.6838 | 0.9059 | 0.058* | 0.204 (6) |
C4A | 0.5120 (8) | 0.6143 (4) | 0.7741 (4) | 0.0421 (11) | |
C5 | 0.1374 (9) | 0.3514 (4) | 0.7950 (4) | 0.0426 (10) | |
C6 | 0.1224 (9) | 0.2471 (4) | 0.7460 (4) | 0.0489 (12) | |
H6 | 0.0023 | 0.1921 | 0.7718 | 0.059* | |
C7 | 0.2894 (10) | 0.2233 (4) | 0.6562 (4) | 0.0506 (12) | |
C8 | 0.4680 (10) | 0.3008 (4) | 0.6163 (4) | 0.0498 (12) | |
H8 | 0.5753 | 0.2832 | 0.5563 | 0.06* | |
C8A | 0.4892 (9) | 0.4080 (4) | 0.6668 (3) | 0.0410 (10) | |
C9 | 0.6745 (9) | 0.4917 (4) | 0.6312 (4) | 0.0436 (11) | |
H9 | 0.7869 | 0.4772 | 0.5719 | 0.052* | |
C9A | 0.6878 (9) | 0.5944 (4) | 0.6845 (3) | 0.0410 (10) | |
C10A | 0.3249 (8) | 0.4357 (4) | 0.7576 (4) | 0.0408 (10) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Br1 | 0.0544 (3) | 0.0519 (3) | 0.0473 (3) | −0.0081 (2) | 0.0128 (2) | −0.0092 (2) |
Br2 | 0.1173 (6) | 0.0430 (3) | 0.0626 (4) | −0.0170 (3) | 0.0078 (3) | −0.0210 (3) |
N1 | 0.042 (2) | 0.043 (2) | 0.042 (2) | −0.0072 (18) | 0.0037 (17) | −0.0121 (17) |
O1 | 0.058 (2) | 0.060 (2) | 0.056 (2) | −0.0144 (18) | 0.0230 (18) | −0.0146 (18) |
C1 | 0.043 (2) | 0.044 (3) | 0.048 (3) | −0.002 (2) | 0.002 (2) | −0.005 (2) |
C2 | 0.053 (4) | 0.047 (5) | 0.053 (5) | −0.008 (3) | 0.011 (4) | −0.011 (4) |
C3 | 0.048 (3) | 0.034 (3) | 0.044 (3) | −0.009 (3) | 0.007 (3) | −0.010 (2) |
C11 | 0.057 (5) | 0.044 (4) | 0.069 (5) | −0.007 (3) | 0.007 (5) | −0.018 (4) |
F1 | 0.104 (3) | 0.064 (3) | 0.061 (2) | −0.014 (2) | 0.013 (2) | −0.035 (2) |
F2 | 0.070 (3) | 0.073 (3) | 0.099 (3) | −0.021 (2) | 0.009 (2) | −0.046 (3) |
F3 | 0.107 (4) | 0.046 (3) | 0.097 (4) | 0.017 (3) | −0.016 (3) | −0.026 (3) |
C4 | 0.042 (4) | 0.060 (4) | 0.049 (6) | −0.009 (4) | 0.005 (4) | −0.026 (4) |
C2' | 0.053 (4) | 0.047 (5) | 0.053 (5) | −0.008 (3) | 0.011 (4) | −0.011 (4) |
C4' | 0.042 (4) | 0.060 (4) | 0.049 (6) | −0.009 (4) | 0.005 (4) | −0.026 (4) |
C4A | 0.042 (2) | 0.042 (3) | 0.043 (2) | −0.003 (2) | −0.001 (2) | −0.013 (2) |
C5 | 0.046 (2) | 0.045 (3) | 0.037 (2) | −0.002 (2) | −0.0009 (19) | −0.008 (2) |
C6 | 0.058 (3) | 0.042 (3) | 0.046 (3) | −0.009 (2) | 0.002 (2) | −0.001 (2) |
C7 | 0.072 (3) | 0.034 (3) | 0.047 (3) | −0.002 (2) | 0.000 (2) | −0.011 (2) |
C8 | 0.061 (3) | 0.046 (3) | 0.042 (3) | −0.001 (2) | 0.006 (2) | −0.011 (2) |
C8A | 0.050 (3) | 0.042 (3) | 0.032 (2) | −0.003 (2) | 0.0028 (19) | −0.0085 (19) |
C9 | 0.048 (3) | 0.044 (3) | 0.036 (2) | 0.002 (2) | 0.011 (2) | −0.007 (2) |
C9A | 0.045 (2) | 0.040 (3) | 0.038 (2) | −0.002 (2) | 0.001 (2) | −0.009 (2) |
C10A | 0.045 (3) | 0.038 (2) | 0.038 (2) | 0.000 (2) | 0.001 (2) | −0.0072 (19) |
Br1—C5 | 1.884 (4) | C2'—H2'2 | 0.97 |
Br2—C7 | 1.901 (5) | C3'—C4' | 1.54 (2) |
N1—C4A | 1.325 (6) | C3'—C11' | 1.538 (19) |
N1—C10A | 1.369 (5) | C3'—H3' | 0.98 |
O1—C1 | 1.226 (5) | C11'—F3' | 1.29 (2) |
C1—C2' | 1.43 (5) | C11'—F1' | 1.33 (2) |
C1—C9A | 1.487 (7) | C11'—F2' | 1.37 (2) |
C1—C2 | 1.499 (13) | C4'—C4A | 1.57 (6) |
C2—C3 | 1.526 (11) | C4'—H4'1 | 0.97 |
C2—H2A | 0.97 | C4'—H4'2 | 0.97 |
C2—H2B | 0.97 | C4A—C9A | 1.420 (6) |
C3—C11 | 1.527 (9) | C5—C6 | 1.361 (6) |
C3—C4 | 1.535 (13) | C5—C10A | 1.433 (6) |
C3—H3 | 0.98 | C6—C7 | 1.403 (6) |
C11—F3 | 1.307 (12) | C6—H6 | 0.93 |
C11—F1 | 1.327 (11) | C7—C8 | 1.356 (7) |
C11—F2 | 1.353 (11) | C8—C8A | 1.406 (6) |
C4—C4A | 1.519 (13) | C8—H8 | 0.93 |
C4—H4A | 0.97 | C8A—C9 | 1.415 (7) |
C4—H4B | 0.97 | C8A—C10A | 1.416 (6) |
C2'—C3' | 1.52 (2) | C9—C9A | 1.375 (6) |
C2'—H2'1 | 0.97 | C9—H9 | 0.93 |
C4A—N1—C10A | 117.5 (4) | F3'—C11'—F1' | 113 (2) |
O1—C1—C2' | 123.2 (16) | F3'—C11'—F2' | 106 (2) |
O1—C1—C9A | 120.2 (5) | F1'—C11'—F2' | 106 (2) |
C2'—C1—C9A | 115.7 (16) | F3'—C11'—C3' | 113.6 (19) |
O1—C1—C2 | 121.1 (5) | F1'—C11'—C3' | 110.7 (17) |
C9A—C1—C2 | 118.6 (5) | F2'—C11'—C3' | 106 (2) |
C1—C2—C3 | 111.0 (8) | C3'—C4'—C4A | 101 (3) |
C1—C2—H2A | 109.4 | C3'—C4'—H4'1 | 111.6 |
C3—C2—H2A | 109.4 | C4A—C4'—H4'1 | 111.6 |
C1—C2—H2B | 109.4 | C3'—C4'—H4'2 | 111.6 |
C3—C2—H2B | 109.4 | C4A—C4'—H4'2 | 111.6 |
H2A—C2—H2B | 108 | H4'1—C4'—H4'2 | 109.4 |
C2—C3—C11 | 112.0 (7) | N1—C4A—C9A | 123.6 (4) |
C2—C3—C4 | 109.8 (8) | N1—C4A—C4 | 116.9 (5) |
C11—C3—C4 | 109.5 (6) | C9A—C4A—C4 | 119.5 (5) |
C2—C3—H3 | 108.5 | N1—C4A—C4' | 113.6 (13) |
C11—C3—H3 | 108.5 | C9A—C4A—C4' | 121.7 (16) |
C4—C3—H3 | 108.5 | C6—C5—C10A | 120.9 (4) |
F3—C11—F1 | 109.6 (7) | C6—C5—Br1 | 119.7 (4) |
F3—C11—F2 | 106.5 (7) | C10A—C5—Br1 | 119.4 (3) |
F1—C11—F2 | 104.9 (10) | C5—C6—C7 | 119.6 (5) |
F3—C11—C3 | 113.9 (9) | C5—C6—H6 | 120.2 |
F1—C11—C3 | 111.9 (6) | C7—C6—H6 | 120.2 |
F2—C11—C3 | 109.5 (6) | C8—C7—C6 | 122.1 (4) |
C4A—C4—C3 | 112.7 (8) | C8—C7—Br2 | 119.9 (4) |
C4A—C4—H4A | 109.1 | C6—C7—Br2 | 118.0 (4) |
C3—C4—H4A | 109.1 | C7—C8—C8A | 119.2 (4) |
C4A—C4—H4B | 109.1 | C7—C8—H8 | 120.4 |
C3—C4—H4B | 109.1 | C8A—C8—H8 | 120.4 |
H4A—C4—H4B | 107.8 | C8—C8A—C9 | 122.4 (4) |
C1—C2'—C3' | 113 (4) | C8—C8A—C10A | 120.6 (4) |
C1—C2'—H2'1 | 109 | C9—C8A—C10A | 117.0 (4) |
C3'—C2'—H2'1 | 109 | C9A—C9—C8A | 119.8 (4) |
C1—C2'—H2'2 | 109 | C9A—C9—H9 | 120.1 |
C3'—C2'—H2'2 | 109 | C8A—C9—H9 | 120.1 |
H2'1—C2'—H2'2 | 107.8 | C9—C9A—C4A | 118.7 (4) |
C2'—C3'—C4' | 110 (2) | C9—C9A—C1 | 120.6 (4) |
C2'—C3'—C11' | 110 (2) | C4A—C9A—C1 | 120.7 (4) |
C4'—C3'—C11' | 109 (2) | N1—C10A—C8A | 123.4 (4) |
C2'—C3'—H3' | 108.9 | N1—C10A—C5 | 119.0 (4) |
C4'—C3'—H3' | 108.9 | C8A—C10A—C5 | 117.6 (4) |
C11'—C3'—H3' | 108.9 | ||
O1—C1—C2—C3 | −147.1 (7) | C10A—C5—C6—C7 | −1.3 (7) |
C2'—C1—C2—C3 | −43 (9) | Br1—C5—C6—C7 | −179.3 (4) |
C9A—C1—C2—C3 | 34.9 (12) | C5—C6—C7—C8 | 0.3 (8) |
C1—C2—C3—C11 | −179.8 (8) | C5—C6—C7—Br2 | −178.9 (4) |
C1—C2—C3—C4 | −58.0 (11) | C6—C7—C8—C8A | 0.6 (8) |
C2—C3—C11—F3 | 56.1 (10) | Br2—C7—C8—C8A | 179.8 (4) |
C4—C3—C11—F3 | −65.8 (9) | C7—C8—C8A—C9 | 178.6 (5) |
C2—C3—C11—F1 | −178.9 (10) | C7—C8—C8A—C10A | −0.6 (7) |
C4—C3—C11—F1 | 59.1 (11) | C8—C8A—C9—C9A | −179.3 (4) |
C2—C3—C11—F2 | −63.0 (11) | C10A—C8A—C9—C9A | −0.2 (7) |
C4—C3—C11—F2 | 175.0 (8) | C8A—C9—C9A—C4A | −0.5 (7) |
C2—C3—C4—C4A | 54.2 (10) | C8A—C9—C9A—C1 | 178.9 (4) |
C11—C3—C4—C4A | 177.5 (7) | N1—C4A—C9A—C9 | 0.2 (7) |
O1—C1—C2'—C3' | 159 (2) | C4—C4A—C9A—C9 | −178.2 (7) |
C9A—C1—C2'—C3' | −32 (5) | C4'—C4A—C9A—C9 | 168 (3) |
C2—C1—C2'—C3' | 76 (10) | N1—C4A—C9A—C1 | −179.1 (4) |
C1—C2'—C3'—C4' | 66 (5) | C4—C4A—C9A—C1 | 2.5 (9) |
C1—C2'—C3'—C11' | −173 (3) | C4'—C4A—C9A—C1 | −12 (3) |
C2'—C3'—C11'—F3' | 55 (4) | O1—C1—C9A—C9 | −4.2 (7) |
C4'—C3'—C11'—F3' | 176 (3) | C2'—C1—C9A—C9 | −174 (3) |
C2'—C3'—C11'—F1' | −176 (3) | C2—C1—C9A—C9 | 173.8 (7) |
C4'—C3'—C11'—F1' | −55 (4) | O1—C1—C9A—C4A | 175.2 (4) |
C2'—C3'—C11'—F2' | −61 (4) | C2'—C1—C9A—C4A | 6 (3) |
C4'—C3'—C11'—F2' | 60 (4) | C2—C1—C9A—C4A | −6.8 (9) |
C2'—C3'—C4'—C4A | −64 (5) | C4A—N1—C10A—C8A | −1.5 (7) |
C11'—C3'—C4'—C4A | 174 (3) | C4A—N1—C10A—C5 | 179.4 (4) |
C10A—N1—C4A—C9A | 0.7 (7) | C8—C8A—C10A—N1 | −179.6 (4) |
C10A—N1—C4A—C4 | 179.2 (7) | C9—C8A—C10A—N1 | 1.2 (7) |
C10A—N1—C4A—C4' | −168 (3) | C8—C8A—C10A—C5 | −0.4 (7) |
C3—C4—C4A—N1 | 154.8 (6) | C9—C8A—C10A—C5 | −179.6 (4) |
C3—C4—C4A—C9A | −26.7 (11) | C6—C5—C10A—N1 | −179.4 (4) |
C3—C4—C4A—C4' | 77 (10) | Br1—C5—C10A—N1 | −1.5 (6) |
C3'—C4'—C4A—N1 | −152 (2) | C6—C5—C10A—C8A | 1.4 (7) |
C3'—C4'—C4A—C9A | 40 (5) | Br1—C5—C10A—C8A | 179.3 (3) |
C3'—C4'—C4A—C4 | −43 (7) |
Experimental details
Crystal data | |
Chemical formula | C14H8Br2F3NO |
Mr | 423.03 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 293 |
a, b, c (Å) | 5.3303 (10), 10.926 (2), 12.354 (2) |
α, β, γ (°) | 83.349 (6), 85.741 (6), 85.051 (6) |
V (Å3) | 710.5 (2) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 5.74 |
Crystal size (mm) | 0.21 × 0.13 × 0.06 |
Data collection | |
Diffractometer | Rigaku XtaLAB mini diffractometer |
Absorption correction | Multi-scan (CrystalClear; Rigaku, 1999; Pflugrath, 1999) |
Tmin, Tmax | 0.379, 0.725 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 4444, 3153, 2188 |
Rint | 0.050 |
(sin θ/λ)max (Å−1) | 0.649 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.055, 0.134, 0.97 |
No. of reflections | 3153 |
No. of parameters | 217 |
No. of restraints | 34 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.80, −0.67 |
Computer programs: CrystalClear (Rigaku, 1999; Pflugrath, 1999), SIR2004 (Burla et al., 2005), SHELXL97 (Sheldrick, 2008), ORTEP-3 for Windows (Farrugia, 1997) as included in WinGX (Farrugia, 1999), WinGX (Farrugia, 1999) and publCIF (Westrip, 2010).
Acknowledgements
COO and TAS acknowledge the US Department of Education Title III Grant, Tennessee State University, for the purchase of the diffractometer.
References
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The compound, 5,7-dibromo-3-trifluoromethyl-3,4-dihydroacridin-1(2H)-one exhibited anticancer activity in several cell lines (Fadeyi et al., 2008). The molecule is disordered across an approximate non-crystallographic mirror plane, which is in the plane of the fused ring system. A one dimensional stacking of molecules involves interactions between the pyridine ring and symmetry related Br (via 1+x, y, z) and O (via (1-x, y, z) on adjacent molecules. The stacking distance between the mean planes of adjacent molecules is 3.395 (4) Å. The molecule is disordered in the crystal with site occupancy factors of 0.796 (6) and 0.204 (6) for the major and minor components, respectively.