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The title compound, C15H17FO, was synthesized directly from the condensation of cyclo­octanone with 2-fluorobenzaldehyde, catalysed effectively by palladium in the presence of tri­methyl­silyl chloride (TMSCl). The structure contains a boat–chair eight-membered ring and a benzene ring. The packing of the mol­ecules in the crystal structure is mainly due to C—H...π interactions and C—H...O hydrogen bonds.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536804011079/ci6365sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536804011079/ci6365Isup2.hkl
Contains datablock I

CCDC reference: 242326

Key indicators

  • Single-crystal X-ray study
  • T = 287 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.032
  • wR factor = 0.073
  • Data-to-parameter ratio = 10.1

checkCIF/PLATON results

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Alert level B PLAT480_ALERT_4_B Long H...A H-Bond Reported H4A .. CGP .. 2.85 Ang. PLAT480_ALERT_4_B Long H...A H-Bond Reported H4B .. CGP .. 2.90 Ang.
Alert level C PLAT481_ALERT_4_C Long D...A H-Bond Reported C4 .. CGP .. 3.74 Ang. PLAT481_ALERT_4_C Long D...A H-Bond Reported C4 .. CGP .. 3.83 Ang.
Alert level G REFLT03_ALERT_4_G Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF. From the CIF: _diffrn_reflns_theta_max 27.85 From the CIF: _reflns_number_total 1560 Count of symmetry unique reflns 1560 Completeness (_total/calc) 100.00% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 0 Fraction of Friedel pairs measured 0.000 Are heavy atom types Z>Si present no
0 ALERT level A = In general: serious problem 2 ALERT level B = Potentially serious problem 2 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 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 5 ALERT type 4 Improvement, methodology, query or suggestion

Computing details top

Data collection: XSCANS (Siemens, 1994); cell refinement: XSCANS; data reduction: SHELXTL (Siemens, 1991); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

(I) top
Crystal data top
C15H17FODx = 1.233 Mg m3
Mr = 232.29Melting point: 465–466 K K
Orthorhombic, Pna21Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2c -2nCell parameters from 39 reflections
a = 12.291 (1) Åθ = 3.0–14.6°
b = 8.294 (1) ŵ = 0.09 mm1
c = 12.273 (1) ÅT = 287 K
V = 1251.2 (2) Å3Block, colorless
Z = 40.50 × 0.50 × 0.46 mm
F(000) = 496
Data collection top
Siemens P4
diffractometer
Rint = 0.009
Radiation source: normal-focus sealed tubeθmax = 27.9°, θmin = 3.0°
Graphite monochromatorh = 116
ω scansk = 010
1904 measured reflectionsl = 016
1560 independent reflections3 standard reflections every 97 reflections
1207 reflections with I > 2σ(I) intensity decay: 2.7%
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.032H-atom parameters constrained
wR(F2) = 0.073 w = 1/[σ2(Fo2) + (0.0429P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.94(Δ/σ)max < 0.001
1560 reflectionsΔρmax = 0.11 e Å3
154 parametersΔρmin = 0.10 e Å3
0 restraintsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.033 (3)
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
F10.74470 (11)0.76983 (16)0.40459 (10)0.0722 (4)
O10.46008 (14)0.37243 (18)0.41115 (12)0.0684 (5)
C10.52979 (17)0.3016 (2)0.35914 (16)0.0461 (4)
C20.5466 (2)0.1227 (2)0.37770 (17)0.0573 (6)
H2A0.54060.10030.45500.069*
H2B0.61960.09380.35490.069*
C30.4650 (2)0.0181 (3)0.31624 (19)0.0621 (6)
H3A0.47080.09130.34370.075*
H3B0.39240.05620.33340.075*
C40.47646 (18)0.0126 (2)0.19302 (18)0.0546 (5)
H4A0.42450.06460.16460.066*
H4B0.54870.02680.17550.066*
C50.45920 (16)0.1737 (2)0.13445 (16)0.0485 (5)
H5A0.41260.15500.07200.058*
H5B0.42060.24560.18340.058*
C60.56082 (18)0.2586 (2)0.09556 (16)0.0498 (5)
H6A0.53950.35850.06050.060*
H6B0.59550.19170.04080.060*
C70.64514 (13)0.2979 (2)0.18409 (17)0.0451 (4)
H7A0.67630.19790.21070.054*
H7B0.70340.36060.15190.054*
C80.59863 (13)0.3901 (2)0.27899 (14)0.0382 (4)
C90.61667 (15)0.5459 (2)0.30104 (15)0.0428 (4)
H90.58370.58540.36380.051*
C100.68198 (15)0.6627 (2)0.23886 (15)0.0407 (4)
C110.68246 (16)0.6746 (2)0.12592 (16)0.0475 (5)
H110.64000.60410.08520.057*
C120.74456 (19)0.7889 (3)0.0728 (2)0.0563 (6)
H120.74310.79490.00280.068*
C130.8086 (2)0.8937 (3)0.1311 (2)0.0644 (6)
H130.85130.96900.09480.077*
C140.80958 (18)0.8877 (3)0.2435 (2)0.0595 (6)
H140.85230.95850.28380.071*
C150.74594 (17)0.7745 (2)0.29407 (17)0.0492 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
F10.0863 (9)0.0736 (9)0.0568 (8)0.0067 (7)0.0207 (7)0.0137 (7)
O10.0921 (11)0.0618 (9)0.0514 (9)0.0018 (8)0.0305 (9)0.0017 (8)
C10.0590 (11)0.0454 (10)0.0341 (9)0.0037 (10)0.0048 (10)0.0026 (8)
C20.0797 (14)0.0466 (11)0.0456 (12)0.0055 (11)0.0047 (11)0.0126 (9)
C30.0805 (16)0.0475 (11)0.0583 (14)0.0167 (11)0.0069 (13)0.0081 (10)
C40.0589 (12)0.0474 (11)0.0576 (13)0.0115 (9)0.0052 (11)0.0044 (10)
C50.0484 (10)0.0531 (11)0.0441 (9)0.0033 (10)0.0037 (9)0.0068 (9)
C60.0616 (12)0.0496 (10)0.0383 (9)0.0050 (9)0.0111 (9)0.0057 (9)
C70.0390 (8)0.0396 (9)0.0568 (11)0.0008 (8)0.0117 (10)0.0020 (10)
C80.0365 (9)0.0391 (9)0.0389 (9)0.0032 (7)0.0060 (8)0.0015 (8)
C90.0486 (10)0.0433 (9)0.0364 (9)0.0030 (9)0.0056 (8)0.0005 (8)
C100.0405 (11)0.0335 (10)0.0482 (11)0.0041 (8)0.0065 (9)0.0017 (8)
C110.0477 (11)0.0432 (11)0.0516 (12)0.0031 (10)0.0063 (10)0.0019 (9)
C120.0577 (14)0.0516 (13)0.0595 (13)0.0006 (11)0.0043 (11)0.0084 (10)
C130.0563 (13)0.0446 (12)0.0923 (19)0.0061 (11)0.0123 (13)0.0042 (13)
C140.0488 (12)0.0428 (12)0.0870 (19)0.0074 (10)0.0085 (12)0.0107 (13)
C150.0484 (11)0.0417 (11)0.0575 (13)0.0043 (9)0.0120 (10)0.0069 (10)
Geometric parameters (Å, º) top
F1—C151.357 (2)C6—H6B0.97
O1—C11.219 (2)C7—C81.506 (3)
C1—C81.491 (3)C7—H7A0.97
C1—C21.515 (3)C7—H7B0.97
C2—C31.526 (3)C8—C91.339 (2)
C2—H2A0.97C9—C101.472 (3)
C2—H2B0.97C9—H90.93
C3—C41.520 (3)C10—C111.390 (2)
C3—H3A0.97C10—C151.391 (3)
C3—H3B0.97C11—C121.380 (3)
C4—C51.532 (3)C11—H110.93
C4—H4A0.97C12—C131.374 (3)
C4—H4B0.97C12—H120.93
C5—C61.511 (3)C13—C141.380 (3)
C5—H5A0.97C13—H130.93
C5—H5B0.97C14—C151.370 (3)
C6—C71.537 (3)C14—H140.93
C6—H6A0.97
O1—C1—C8120.46 (17)H6A—C6—H6B107.4
O1—C1—C2119.27 (19)C8—C7—C6113.48 (14)
C8—C1—C2120.27 (18)C8—C7—H7A108.9
C1—C2—C3113.17 (18)C6—C7—H7A108.9
C1—C2—H2A108.9C8—C7—H7B108.9
C3—C2—H2A108.9C6—C7—H7B108.9
C1—C2—H2B108.9H7A—C7—H7B107.7
C3—C2—H2B108.9C9—C8—C1115.84 (17)
H2A—C2—H2B107.8C9—C8—C7125.70 (17)
C4—C3—C2116.59 (19)C1—C8—C7118.41 (15)
C4—C3—H3A108.1C8—C9—C10128.40 (17)
C2—C3—H3A108.1C8—C9—H9115.8
C4—C3—H3B108.1C10—C9—H9115.8
C2—C3—H3B108.1C11—C10—C15115.85 (19)
H3A—C3—H3B107.3C11—C10—C9124.50 (18)
C3—C4—C5115.37 (17)C15—C10—C9119.62 (17)
C3—C4—H4A108.4C12—C11—C10121.5 (2)
C5—C4—H4A108.4C12—C11—H11119.3
C3—C4—H4B108.4C10—C11—H11119.3
C5—C4—H4B108.4C13—C12—C11120.4 (2)
H4A—C4—H4B107.5C13—C12—H12119.8
C6—C5—C4116.11 (18)C11—C12—H12119.8
C6—C5—H5A108.3C12—C13—C14120.2 (2)
C4—C5—H5A108.3C12—C13—H13119.9
C6—C5—H5B108.3C14—C13—H13119.9
C4—C5—H5B108.3C15—C14—C13118.2 (2)
H5A—C5—H5B107.4C15—C14—H14120.9
C5—C6—C7115.65 (16)C13—C14—H14120.9
C5—C6—H6A108.4F1—C15—C14118.6 (2)
C7—C6—H6A108.4F1—C15—C10117.48 (19)
C5—C6—H6B108.4C14—C15—C10123.9 (2)
C7—C6—H6B108.4
O1—C1—C2—C381.3 (2)C7—C8—C9—C101.6 (3)
C8—C1—C2—C399.3 (2)C8—C9—C10—C1141.5 (3)
C1—C2—C3—C469.8 (3)C8—C9—C10—C15140.8 (2)
C2—C3—C4—C563.1 (3)C15—C10—C11—C121.2 (3)
C3—C4—C5—C6103.5 (2)C9—C10—C11—C12179.01 (17)
C4—C5—C6—C757.8 (2)C10—C11—C12—C130.5 (3)
C5—C6—C7—C853.3 (2)C11—C12—C13—C141.3 (4)
O1—C1—C8—C929.4 (3)C12—C13—C14—C150.4 (4)
C2—C1—C8—C9149.91 (18)C13—C14—C15—F1178.7 (2)
O1—C1—C8—C7152.93 (19)C13—C14—C15—C101.4 (4)
C2—C1—C8—C727.7 (2)C11—C10—C15—F1177.92 (18)
C6—C7—C8—C9107.7 (2)C9—C10—C15—F10.0 (3)
C6—C7—C8—C174.9 (2)C11—C10—C15—C142.2 (3)
C1—C8—C9—C10179.00 (17)C9—C10—C15—C14179.88 (19)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C11—H11···O1i0.932.473.189 (3)134
C14—H14···O1ii0.932.483.408 (3)173
C4—H4A···CgPiii0.972.853.738 (3)153
C4—H4B···CgPiv0.972.903.829 (2)160
Symmetry codes: (i) x+1, y+1, z1/2; (ii) x+1/2, y+3/2, z; (iii) x1/2, y+3/2, z; (iv) x, y1, z.
 

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