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The racemic form of the title compound, C14H15Cl2NO, was prepared by the base-catalyzed reaction of 2,4-dichloro­benzaldehyde with 1-aza­bicyclo­[2.2.2]octan-3-one and subsequent reduction to the corresponding secondary alcohol. In the mol­ecule, the olefinic bond connecting the 2,4-dichloro­phenyl ring and 1-aza­bicyclo­[2.2.2]octan-3-ol group has Z geometry. The C=C—CH=C torsion angle [45.3 (3)°] indicates deviation of the 2,4-dichloro­phenyl ring from the plane of the double bond connected to the aza­bicyclic ring. The hydroxyl group is disordered over two sites, the ratio of occupancies being approximately 0.67:0.33. The crystal structure contains intermolecular O—H...N hydrogen bonds.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807041128/lh2483sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807041128/lh2483Isup2.hkl
Contains datablock I

CCDC reference: 660366

Key indicators

  • Single-crystal X-ray study
  • T = 90 K
  • Mean [sigma](C-C) = 0.003 Å
  • Disorder in main residue
  • R factor = 0.034
  • wR factor = 0.089
  • Data-to-parameter ratio = 16.4

checkCIF/PLATON results

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Alert level C PLAT154_ALERT_1_C The su's on the Cell Angles are Equal (x 10000) 100 Deg. PLAT180_ALERT_3_C Check Cell Rounding: # of Values Ending with 0 = 5 PLAT220_ALERT_2_C Large Non-Solvent C Ueq(max)/Ueq(min) ... 2.54 Ratio PLAT250_ALERT_2_C Large U3/U1 Ratio for Average U(i,j) Tensor .... 2.20 PLAT301_ALERT_3_C Main Residue Disorder ......................... 5.00 Perc. PLAT432_ALERT_2_C Short Inter X...Y Contact O16 .. C2 .. 2.99 Ang.
Alert level G PLAT860_ALERT_3_G Note: Number of Least-Squares Restraints ....... 21
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 6 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 3 ALERT type 2 Indicator that the structure model may be wrong or deficient 3 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

Radio-sensitizers are drugs that make cancer cells more sensitive to radiation therapy. Radiation therapy prevents cancer cells from growing and dividing. Radiation therapy, however, can also damage normal cells. Consequently, researchers are looking for substances that can either make a tumor more sensitive to radiation without affecting healthy tissues, or that can shield normal cells from radiation. Recently, we have reported (Sekhar et al., 2007) on the radio-sensitizing activity of N-arylsubstituted rac-(Z)-2-(1H-indol-3-ylmethylene)-1-azabicyclo[2.2.2]octan -3-ols. In addition to these indole analogues, we also synthesized 1-azabicyclo[2.2.2]octan-3-ols linked to non-indolic systems to compare their radio-sensitizing activities with those of the indole analogs.

In order to confirm the double-bond geometry, and to determine the molecular conformation in the crystal structure, the X-ray analysis of the title compound has been carried out. The molecular structure and atom-numbering scheme for the title molecule is shown in Fig. 1. The title molecule comprises a 1-azabicyclo[2.2.2]octan-3-ol moiety and a 2,4-dichlorophenyl group linked via a C7C8 bond that has the Z geometry. The bond angles around the C7 and C8 atoms deviate from the ideal value [120°]; the angles for N9—C8—C13, and C7=C8—C1 [114.16 (14), and 128.31 (15)°, respectively] are distorted, as a consequence of the strain induced by the double bond linkage at C7C8. These deviations contribute to the release of the intramolecular nonbonded interactions. The C2C1—C7C8 torsion angle [45.3 (3)°] indicates a deviation of the 2,4-dichlorophenyl ring from the plane of the double bond connected to the azabicyclic ring. Also, the C1—C7 bond length [1.472 (2) Å], in comparison with the standard value for a Car—Csp2 single bond [1.470 (15) Å; Wilson, 1992], suggests a lack of conjugation to the 2,4-dichlorophenyl ring.

Related literature top

For related literature, see: Sekhar et al. (2007); Sonar et al. (2004); Wilson (1992).

Experimental top

The title compound was prepared according to the previously reported procedure of Sonar et al. (2004). Crystallization from ethyl acetate afforded colorless crystals. 1H NMR (CDCl3, p.p.m.): δ 1.42–1.61 (m, 2H), 1.69–1.78 (m, 1H), 1.79–1.99 (m, 2H), 2.07 (p, 1H), 2.68–2.78 (m, 1H), 2.91–3.01 (m, 3H), 4.34 (p, 1H), 6.60 (d, 1H), 7.17 (dt, 1H), 7.35 (d, 1H), 8.21 (d, 1H). 13C NMR (CDCl3, p.p.m.): δ 19.17, 25.28, 31.05, 47.36, 48.38, 71.35, 117.51, 126.88, 128.90, 132.13, 132.30, 132.83, 133.82, 155.06.

Refinement top

H atoms were found in difference Fourier maps and subsequently placed in idealized positions with constrained C—H distances of 1.00 Å (R3CH), 0.99 Å (R2CH2), 0.95 Å (CArH) and 0.84 Å (OH). Uiso(H) values were set to either 1.2Ueq(C) or 1.5Ueq(O). The hydroxyl group is disordered over two sites with occupancy factors 0.67:0.33, and the hydroxyl hydrogen is also disordered. The major component was placed the position of maximum electron density as calculated in a torus beyond the oxygen atom labelled O16, while the minor component was placed in the most reasonable hydrogen bonding position, as dictated by the SHELXL (Sheldrick, 1997) commands "HFIX 147" and "HFIX 87" respectively.

Structure description top

Radio-sensitizers are drugs that make cancer cells more sensitive to radiation therapy. Radiation therapy prevents cancer cells from growing and dividing. Radiation therapy, however, can also damage normal cells. Consequently, researchers are looking for substances that can either make a tumor more sensitive to radiation without affecting healthy tissues, or that can shield normal cells from radiation. Recently, we have reported (Sekhar et al., 2007) on the radio-sensitizing activity of N-arylsubstituted rac-(Z)-2-(1H-indol-3-ylmethylene)-1-azabicyclo[2.2.2]octan -3-ols. In addition to these indole analogues, we also synthesized 1-azabicyclo[2.2.2]octan-3-ols linked to non-indolic systems to compare their radio-sensitizing activities with those of the indole analogs.

In order to confirm the double-bond geometry, and to determine the molecular conformation in the crystal structure, the X-ray analysis of the title compound has been carried out. The molecular structure and atom-numbering scheme for the title molecule is shown in Fig. 1. The title molecule comprises a 1-azabicyclo[2.2.2]octan-3-ol moiety and a 2,4-dichlorophenyl group linked via a C7C8 bond that has the Z geometry. The bond angles around the C7 and C8 atoms deviate from the ideal value [120°]; the angles for N9—C8—C13, and C7=C8—C1 [114.16 (14), and 128.31 (15)°, respectively] are distorted, as a consequence of the strain induced by the double bond linkage at C7C8. These deviations contribute to the release of the intramolecular nonbonded interactions. The C2C1—C7C8 torsion angle [45.3 (3)°] indicates a deviation of the 2,4-dichlorophenyl ring from the plane of the double bond connected to the azabicyclic ring. Also, the C1—C7 bond length [1.472 (2) Å], in comparison with the standard value for a Car—Csp2 single bond [1.470 (15) Å; Wilson, 1992], suggests a lack of conjugation to the 2,4-dichlorophenyl ring.

For related literature, see: Sekhar et al. (2007); Sonar et al. (2004); Wilson (1992).

Computing details top

Data collection: COLLECT (Nonius, 1999); cell refinement: SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO-SMN (Otwinowski & Minor, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: XP in SHELXTL (Sheldrick, 1995); software used to prepare material for publication: SHELX97 and local procedures.

Figures top
[Figure 1] Fig. 1. A view of the title molecule, with the atom numbering scheme. Displacement ellipsoids are drawn at the 50% probability level and H atoms are shown as small spheres of arbitrary radii. The hydroxyl group is disordered.
rac-(Z)-2-(2,4-Dichlorobenzylidene)-1-azabicyclo[2.2.2]octan-3-ol top
Crystal data top
C14H15Cl2NOZ = 2
Mr = 284.17F(000) = 296
Triclinic, P1Dx = 1.500 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 6.1374 (1) ÅCell parameters from 2861 reflections
b = 10.3379 (2) Åθ = 1.0–27.5°
c = 10.6340 (2) ŵ = 0.50 mm1
α = 107.269 (1)°T = 90 K
β = 98.391 (1)°Block, colourless
γ = 96.098 (1)°0.40 × 0.30 × 0.25 mm
V = 629.36 (2) Å3
Data collection top
Nonius KappaCCD area-detector
diffractometer
2873 independent reflections
Radiation source: fine-focus sealed tube2459 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.022
Detector resolution: 18 pixels mm-1θmax = 27.5°, θmin = 2.0°
ω scans at fixed χ = 55°h = 77
Absorption correction: multi-scan
(SCALEPACK; Otwinowski & Minor, 1997)
k = 1313
Tmin = 0.825, Tmax = 0.885l = 1313
5704 measured reflections
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)] = 0.034Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.089H-atom parameters constrained
S = 1.07 w = 1/[σ2(Fo2) + (0.0373P)2 + 0.4377P]
where P = (Fo2 + 2Fc2)/3
2873 reflections(Δ/σ)max < 0.001
175 parametersΔρmax = 0.38 e Å3
21 restraintsΔρmin = 0.59 e Å3
Crystal data top
C14H15Cl2NOγ = 96.098 (1)°
Mr = 284.17V = 629.36 (2) Å3
Triclinic, P1Z = 2
a = 6.1374 (1) ÅMo Kα radiation
b = 10.3379 (2) ŵ = 0.50 mm1
c = 10.6340 (2) ÅT = 90 K
α = 107.269 (1)°0.40 × 0.30 × 0.25 mm
β = 98.391 (1)°
Data collection top
Nonius KappaCCD area-detector
diffractometer
2873 independent reflections
Absorption correction: multi-scan
(SCALEPACK; Otwinowski & Minor, 1997)
2459 reflections with I > 2σ(I)
Tmin = 0.825, Tmax = 0.885Rint = 0.022
5704 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.03421 restraints
wR(F2) = 0.089H-atom parameters constrained
S = 1.07Δρmax = 0.38 e Å3
2873 reflectionsΔρmin = 0.59 e Å3
175 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 > 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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Cl10.98623 (7)0.11120 (4)0.35241 (4)0.02142 (12)
Cl20.21149 (7)0.13519 (4)0.05932 (4)0.01986 (12)
C10.4485 (3)0.35709 (16)0.25998 (16)0.0140 (3)
C20.6331 (3)0.41588 (17)0.36374 (17)0.0172 (3)
H20.64570.50960.41560.021*
C30.7983 (3)0.34190 (17)0.39344 (17)0.0178 (3)
H30.92090.38380.46510.021*
C40.7811 (3)0.20619 (16)0.31682 (16)0.0152 (3)
C50.6030 (3)0.14248 (16)0.21268 (15)0.0154 (3)
H50.59330.04930.16010.018*
C60.4387 (3)0.21898 (16)0.18738 (15)0.0142 (3)
C70.2664 (3)0.43339 (16)0.23489 (16)0.0162 (3)
H70.11950.38500.21960.019*
C80.2812 (3)0.56122 (18)0.2309 (2)0.0234 (4)
N90.4903 (2)0.64743 (15)0.24100 (18)0.0263 (4)
C100.5113 (3)0.77456 (19)0.3572 (2)0.0276 (4)
H10A0.65430.83400.36650.033*
H10B0.51350.74970.44030.033*
C110.3171 (3)0.85452 (18)0.33952 (17)0.0210 (4)
H11A0.24080.86850.41730.025*
H11B0.37510.94570.33460.025*
C120.1525 (3)0.77320 (16)0.21067 (17)0.0173 (3)
H120.02170.82150.19940.021*
C130.0756 (3)0.63001 (19)0.2150 (3)0.0355 (5)
H130.01580.57730.12470.043*0.666 (4)
H13'0.04860.65430.30910.043*0.334 (4)
C140.4787 (3)0.68899 (19)0.1179 (2)0.0284 (4)
H14A0.47680.60720.04000.034*
H14B0.61420.75490.12730.034*
C150.2710 (3)0.75526 (19)0.09092 (18)0.0236 (4)
H15A0.31550.84550.07970.028*
H15B0.16980.69590.00780.028*
O160.0490 (3)0.6203 (2)0.30373 (19)0.0229 (5)0.666 (4)
H160.18300.61920.27180.034*0.666 (4)
O16'0.0997 (5)0.5521 (3)0.1570 (4)0.0174 (10)0.334 (4)
H16'0.11070.53510.07380.026*0.334 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.0206 (2)0.0230 (2)0.0238 (2)0.01253 (16)0.00340 (16)0.00927 (17)
Cl20.0184 (2)0.0187 (2)0.0192 (2)0.00315 (15)0.00177 (15)0.00352 (15)
C10.0128 (7)0.0147 (7)0.0177 (7)0.0034 (6)0.0062 (6)0.0080 (6)
C20.0161 (8)0.0126 (8)0.0215 (8)0.0025 (6)0.0038 (6)0.0033 (6)
C30.0148 (8)0.0177 (8)0.0196 (8)0.0019 (6)0.0006 (6)0.0055 (6)
C40.0138 (7)0.0180 (8)0.0182 (7)0.0077 (6)0.0051 (6)0.0095 (6)
C50.0183 (8)0.0137 (8)0.0156 (7)0.0037 (6)0.0059 (6)0.0050 (6)
C60.0138 (7)0.0155 (8)0.0140 (7)0.0012 (6)0.0030 (6)0.0057 (6)
C70.0107 (7)0.0156 (8)0.0230 (8)0.0025 (6)0.0043 (6)0.0066 (6)
C80.0100 (8)0.0181 (9)0.0450 (11)0.0036 (6)0.0056 (7)0.0134 (8)
N90.0095 (7)0.0184 (7)0.0562 (11)0.0027 (6)0.0050 (7)0.0200 (7)
C100.0166 (8)0.0241 (9)0.0429 (11)0.0015 (7)0.0058 (8)0.0186 (8)
C110.0168 (8)0.0254 (9)0.0209 (8)0.0047 (7)0.0031 (6)0.0073 (7)
C120.0117 (7)0.0133 (8)0.0268 (9)0.0041 (6)0.0011 (6)0.0067 (6)
C130.0113 (8)0.0195 (9)0.0826 (17)0.0043 (7)0.0093 (9)0.0255 (10)
C140.0220 (9)0.0206 (9)0.0488 (12)0.0087 (7)0.0158 (8)0.0139 (8)
C150.0197 (9)0.0247 (9)0.0227 (9)0.0063 (7)0.0012 (7)0.0022 (7)
O160.0126 (9)0.0333 (12)0.0320 (11)0.0090 (8)0.0086 (8)0.0202 (9)
O16'0.0111 (17)0.0147 (18)0.0239 (19)0.0009 (13)0.0002 (13)0.0043 (14)
Geometric parameters (Å, º) top
Cl1—C41.7425 (16)C10—H10A0.9900
Cl2—C61.7430 (16)C10—H10B0.9900
C1—C61.397 (2)C11—C121.529 (2)
C1—C21.401 (2)C11—H11A0.9900
C1—C71.472 (2)C11—H11B0.9900
C2—C31.388 (2)C12—C131.521 (2)
C2—H20.9500C12—C151.531 (2)
C3—C41.381 (2)C12—H121.0000
C3—H30.9500C13—O16'1.231 (4)
C4—C51.384 (2)C13—O161.318 (3)
C5—C61.390 (2)C13—H131.0000
C5—H50.9500C13—H13'1.0000
C7—C81.329 (2)C14—C151.540 (2)
C7—H70.9500C14—H14A0.9900
C8—N91.453 (2)C14—H14B0.9900
C8—C131.525 (2)C15—H15A0.9900
N9—C141.489 (3)C15—H15B0.9900
N9—C101.491 (3)O16—H160.8400
C10—C111.542 (2)O16'—H16'0.8400
C6—C1—C2116.32 (14)C12—C11—H11B109.9
C6—C1—C7121.62 (14)C10—C11—H11B109.9
C2—C1—C7121.92 (14)H11A—C11—H11B108.3
C3—C2—C1122.23 (15)C13—C12—C11109.58 (15)
C3—C2—H2118.9C13—C12—C15106.75 (15)
C1—C2—H2118.9C11—C12—C15109.35 (13)
C4—C3—C2118.79 (15)C13—C12—H12110.4
C4—C3—H3120.6C11—C12—H12110.4
C2—C3—H3120.6C15—C12—H12110.4
C3—C4—C5121.66 (14)O16'—C13—O1670.8 (2)
C3—C4—Cl1119.60 (12)O16'—C13—C12128.5 (2)
C5—C4—Cl1118.73 (12)O16—C13—C12117.11 (19)
C4—C5—C6117.97 (14)O16'—C13—C8115.7 (2)
C4—C5—H5121.0O16—C13—C8111.26 (18)
C6—C5—H5121.0C12—C13—C8107.96 (14)
C5—C6—C1123.01 (14)O16—C13—H13106.6
C5—C6—Cl2117.20 (12)C12—C13—H13106.6
C1—C6—Cl2119.79 (12)C8—C13—H13106.6
C8—C7—C1128.31 (15)O16'—C13—H13'99.3
C8—C7—H7115.8C12—C13—H13'99.3
C1—C7—H7115.8C8—C13—H13'99.3
C7—C8—N9123.90 (15)H13—C13—H13'134.9
C7—C8—C13121.94 (15)N9—C14—C15112.54 (15)
N9—C8—C13114.16 (14)N9—C14—H14A109.1
C8—N9—C14108.26 (15)C15—C14—H14A109.1
C8—N9—C10108.20 (15)N9—C14—H14B109.1
C14—N9—C10107.50 (14)C15—C14—H14B109.1
N9—C10—C11111.53 (14)H14A—C14—H14B107.8
N9—C10—H10A109.3C12—C15—C14108.05 (15)
C11—C10—H10A109.3C12—C15—H15A110.1
N9—C10—H10B109.3C14—C15—H15A110.1
C11—C10—H10B109.3C12—C15—H15B110.1
H10A—C10—H10B108.0C14—C15—H15B110.1
C12—C11—C10109.14 (14)H15A—C15—H15B108.4
C12—C11—H11A109.9C13—O16—H16109.5
C10—C11—H11A109.9C13—O16'—H16'109.5
C6—C1—C2—C30.1 (2)C14—N9—C10—C1156.80 (18)
C7—C1—C2—C3175.79 (15)N9—C10—C11—C123.6 (2)
C1—C2—C3—C40.9 (2)C10—C11—C12—C1355.83 (19)
C2—C3—C4—C50.6 (2)C10—C11—C12—C1560.86 (18)
C2—C3—C4—Cl1179.89 (12)C11—C12—C13—O16'154.0 (3)
C3—C4—C5—C60.5 (2)C15—C12—C13—O16'87.6 (3)
Cl1—C4—C5—C6178.75 (12)C11—C12—C13—O1667.7 (2)
C4—C5—C6—C11.5 (2)C15—C12—C13—O16174.01 (17)
C4—C5—C6—Cl2177.99 (12)C11—C12—C13—C858.8 (2)
C2—C1—C6—C51.3 (2)C15—C12—C13—C859.5 (2)
C7—C1—C6—C5177.03 (14)C7—C8—C13—O16'26.6 (4)
C2—C1—C6—Cl2178.20 (12)N9—C8—C13—O16'153.4 (3)
C7—C1—C6—Cl22.5 (2)C7—C8—C13—O1651.6 (3)
C6—C1—C7—C8139.20 (19)N9—C8—C13—O16128.34 (19)
C2—C1—C7—C845.3 (3)C7—C8—C13—C12178.55 (18)
C1—C7—C8—N95.1 (3)N9—C8—C13—C121.5 (2)
C1—C7—C8—C13174.83 (18)C8—N9—C14—C1553.4 (2)
C7—C8—N9—C14121.4 (2)C10—N9—C14—C1563.25 (18)
C13—C8—N9—C1458.6 (2)C13—C12—C15—C1463.62 (18)
C7—C8—N9—C10122.3 (2)C11—C12—C15—C1454.84 (18)
C13—C8—N9—C1057.6 (2)N9—C14—C15—C126.6 (2)
C8—N9—C10—C1159.91 (19)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O16—H16···N9i0.842.052.872 (2)166
Symmetry code: (i) x1, y, z.

Experimental details

Crystal data
Chemical formulaC14H15Cl2NO
Mr284.17
Crystal system, space groupTriclinic, P1
Temperature (K)90
a, b, c (Å)6.1374 (1), 10.3379 (2), 10.6340 (2)
α, β, γ (°)107.269 (1), 98.391 (1), 96.098 (1)
V3)629.36 (2)
Z2
Radiation typeMo Kα
µ (mm1)0.50
Crystal size (mm)0.40 × 0.30 × 0.25
Data collection
DiffractometerNonius KappaCCD area-detector
Absorption correctionMulti-scan
(SCALEPACK; Otwinowski & Minor, 1997)
Tmin, Tmax0.825, 0.885
No. of measured, independent and
observed [I > 2σ(I)] reflections
5704, 2873, 2459
Rint0.022
(sin θ/λ)max1)0.649
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.034, 0.089, 1.07
No. of reflections2873
No. of parameters175
No. of restraints21
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.38, 0.59

Computer programs: COLLECT (Nonius, 1999), SCALEPACK (Otwinowski & Minor, 1997), DENZO-SMN (Otwinowski & Minor, 1997), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), XP in SHELXTL (Sheldrick, 1995), SHELX97 and local procedures.

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O16—H16···N9i0.842.052.872 (2)165.8
Symmetry code: (i) x1, y, z.
 

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