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In the title compound, C30H18, the fluorene moiety displays normal dimensions, such as a narrow ring angle of 105.3 (3)° at the 9-position, the atom bearing the exocyclic double bond. The phen­yl rings subtend angles of 14.8 (2) and 3.9 (2)° to the fluorene plane. Mol­ecules are stacked parallel to the short c axis of 4.001 (1) Å.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805005623/bt6610sup1.cif
Contains datablocks 3, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536805005623/bt66103sup2.hkl
Contains datablock 3

CCDC reference: 270231

Key indicators

  • Single-crystal X-ray study
  • T = 173 K
  • Mean [sigma](C-C) = 0.005 Å
  • R factor = 0.045
  • wR factor = 0.126
  • Data-to-parameter ratio = 7.4

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT063_ALERT_3_C Crystal Probably too Large for Beam Size ....... 0.64 mm PLAT089_ALERT_3_C Poor Data / Parameter Ratio (Zmax .LT. 18) ..... 7.39 PLAT125_ALERT_4_C No _symmetry_space_group_name_Hall Given ....... ? PLAT340_ALERT_3_C Low Bond Precision on C-C bonds (x 1000) Ang ... 5 PLAT371_ALERT_2_C Long C(sp2)-C(sp1) Bond C10 - C11 ... 1.44 Ang. PLAT371_ALERT_2_C Long C(sp2)-C(sp1) Bond C10 - C11' ... 1.43 Ang. PLAT371_ALERT_2_C Long C(sp2)-C(sp1) Bond C12 - C13 ... 1.44 Ang. PLAT371_ALERT_2_C Long C(sp2)-C(sp1) Bond C12' - C13' ... 1.44 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 25.06 From the CIF: _reflns_number_total 2004 Count of symmetry unique reflns 2011 Completeness (_total/calc) 99.65% 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 0 ALERT level B = Potentially serious problem 8 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 4 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 2 ALERT type 4 Improvement, methodology, query or suggestion

Computing details top

Data collection: P3 (Nicolet, 1987); cell refinement: P3; data reduction: XDISK (Nicolet, 1987); program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: XP (Siemens, 1994); software used to prepare material for publication: SHELXL97.

9-Methylene-10,10-bis(phenylethynyl)fluorene top
Crystal data top
C30H18Dx = 1.284 Mg m3
Mr = 378.44Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, Pna21Cell parameters from 50 reflections
a = 25.824 (9) Åθ = 10–11.5°
b = 18.944 (8) ŵ = 0.07 mm1
c = 4.001 (1) ÅT = 173 K
V = 1957.3 (12) Å3Prism, yellow
Z = 40.64 × 0.22 × 0.18 mm
F(000) = 792
Data collection top
Siemens R3
diffractometer
Rint = 0.066
Radiation source: fine-focus sealed tubeθmax = 25.1°, θmin = 3.2°
Graphite monochromatorh = 3030
ω scansk = 2222
6350 measured reflectionsl = 04
2004 independent reflections3 standard reflections every 147 reflections
1320 reflections with I > 2σ(I) intensity decay: none
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)] = 0.045Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.127H-atom parameters constrained
S = 1.10 w = 1/[σ2(Fo2) + (0.0598P)2]
where P = (Fo2 + 2Fc2)/3
2004 reflections(Δ/σ)max = 0.001
271 parametersΔρmax = 0.21 e Å3
285 restraintsΔρmin = 0.22 e Å3
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.

Least-squares planes (x,y,z in crystal coordinates) and deviations from them (* indicates atom used to define plane)

8.4000 (0.0440) x - 5.9065 (0.0319) y + 3.5718 (0.0036) z = 0.8779 (0.0230)

* -0.0044 (0.0030) C13 * 0.0036 (0.0030) C14 * 0.0024 (0.0029) C15 * -0.0075 (0.0031) C16 * 0.0066 (0.0032) C17 * -0.0007 (0.0031) C18

Rms deviation of fitted atoms = 0.0048

12.3509 (0.0215) x - 1.9894 (0.0121) y + 3.4885 (0.0024) z = 5.0351 (0.0089)

Angle to previous plane (with approximate e.s.d.) = 14.83 (0.15)

* 0.0435 (0.0036) C1 * -0.0178 (0.0034) C1A * 0.0521 (0.0036) C2 * 0.0222 (0.0035) C3 * -0.0166 (0.0037) C4 * -0.0473 (0.0038) C4A * -0.0280 (0.0038) C5 * -0.0477 (0.0038) C5A * 0.0314 (0.0035) C6 * 0.0636 (0.0036) C7 * 0.0315 (0.0035) C8 * -0.0329 (0.0037) C8A * -0.0539 (0.0032) C9

Rms deviation of fitted atoms = 0.0402

11.8786 (0.0398) x - 0.7654 (0.0321) y + 3.5489 (0.0035) z = 5.4197 (0.0348)

Angle to previous plane (with approximate e.s.d.) = 3.94 (0.17)

* 0.0123 (0.0030) C13' * -0.0081 (0.0032) C14' * -0.0013 (0.0033) C15' * 0.0064 (0.0031) C16' * -0.0020 (0.0030) C17' * -0.0074 (0.0030) C18'

Rms deviation of fitted atoms = 0.0073

=============================================================================

Pseudo-torsion angles:

10.04 (0.44) C9 - C10 - C13 - C14 - 4.73 (0.44) C9 - C10 - C13' - C14'

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
C1A0.34117 (12)0.80376 (18)0.6887 (10)0.0324 (9)
C10.37149 (14)0.86291 (18)0.6327 (12)0.0408 (10)
H10.40410.85880.52490.049*
C20.35326 (15)0.92867 (18)0.7372 (11)0.0451 (10)
H20.37350.96960.69650.054*
C30.30595 (15)0.9351 (2)0.8998 (11)0.0464 (10)
H30.29430.98040.96870.056*
C40.27568 (15)0.8764 (2)0.9624 (11)0.0453 (11)
H40.24360.88071.07680.054*
C4A0.29324 (13)0.81047 (18)0.8538 (10)0.0364 (9)
C5A0.27044 (13)0.73986 (18)0.8941 (10)0.0366 (9)
C50.22494 (14)0.7190 (2)1.0490 (12)0.0445 (10)
H50.20200.75291.14180.053*
C60.21344 (14)0.6473 (2)1.0658 (11)0.0471 (11)
H60.18250.63191.17180.057*
C70.24712 (14)0.5984 (2)0.9279 (11)0.0447 (10)
H70.23890.54960.94230.054*
C80.29272 (13)0.61867 (19)0.7688 (11)0.0390 (9)
H80.31540.58440.67530.047*
C8A0.30433 (13)0.69047 (18)0.7502 (10)0.0334 (8)
C90.34942 (12)0.72813 (17)0.6060 (10)0.0325 (8)
C100.38960 (12)0.70004 (17)0.4275 (10)0.0328 (9)
C110.39264 (12)0.62645 (18)0.3437 (11)0.0337 (9)
C120.39649 (13)0.56679 (18)0.2479 (11)0.0369 (9)
C130.39706 (13)0.49517 (18)0.1296 (11)0.0368 (9)
C140.35269 (14)0.45300 (18)0.1664 (11)0.0402 (10)
H140.32250.47170.26990.048*
C150.35315 (15)0.38410 (19)0.0511 (11)0.0428 (10)
H150.32310.35560.07620.051*
C160.39677 (15)0.35634 (19)0.1002 (11)0.0455 (10)
H160.39640.30920.18170.055*
C170.44102 (15)0.39708 (19)0.1329 (12)0.0472 (11)
H170.47120.37750.23210.057*
C180.44129 (14)0.46677 (19)0.0203 (11)0.0416 (10)
H180.47150.49490.04550.050*
C11'0.43049 (13)0.74157 (18)0.2900 (11)0.0344 (9)
C12'0.46466 (13)0.77370 (18)0.1565 (11)0.0341 (9)
C13'0.50500 (12)0.81704 (18)0.0165 (10)0.0337 (8)
C14'0.50166 (14)0.89057 (18)0.0378 (12)0.0425 (10)
H14'0.47210.91200.13620.051*
C15'0.54127 (15)0.9320 (2)0.0839 (12)0.0510 (11)
H15'0.53910.98190.06590.061*
C16'0.58392 (15)0.9018 (2)0.2310 (12)0.0479 (11)
H16'0.61110.93090.31250.057*
C17'0.58760 (14)0.8292 (2)0.2614 (11)0.0447 (10)
H17'0.61700.80840.36480.054*
C18'0.54805 (12)0.78719 (19)0.1395 (11)0.0385 (9)
H18'0.55020.73740.16250.046*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C1A0.0333 (19)0.0322 (18)0.032 (2)0.0012 (15)0.0068 (17)0.0014 (18)
C10.045 (2)0.035 (2)0.043 (2)0.0008 (17)0.000 (2)0.002 (2)
C20.058 (2)0.032 (2)0.046 (3)0.0006 (18)0.004 (2)0.001 (2)
C30.058 (2)0.039 (2)0.042 (2)0.0138 (18)0.002 (2)0.003 (2)
C40.044 (2)0.048 (2)0.044 (3)0.0114 (17)0.002 (2)0.003 (2)
C4A0.0387 (19)0.0378 (19)0.033 (2)0.0033 (16)0.0050 (18)0.002 (2)
C5A0.0339 (18)0.044 (2)0.032 (2)0.0021 (16)0.0038 (18)0.002 (2)
C50.040 (2)0.055 (2)0.038 (2)0.0010 (18)0.001 (2)0.001 (2)
C60.038 (2)0.066 (3)0.038 (3)0.0073 (19)0.001 (2)0.004 (2)
C70.047 (2)0.049 (2)0.038 (2)0.0116 (18)0.006 (2)0.003 (2)
C80.040 (2)0.042 (2)0.035 (2)0.0036 (16)0.006 (2)0.003 (2)
C8A0.0346 (18)0.036 (2)0.030 (2)0.0002 (15)0.0049 (17)0.0014 (19)
C90.0326 (18)0.0335 (19)0.031 (2)0.0011 (15)0.0037 (17)0.0028 (18)
C100.0330 (18)0.0282 (19)0.037 (2)0.0006 (15)0.0063 (18)0.0013 (18)
C110.0299 (17)0.0308 (19)0.041 (2)0.0012 (14)0.0015 (18)0.0007 (19)
C120.0333 (18)0.035 (2)0.042 (2)0.0004 (15)0.005 (2)0.002 (2)
C130.0438 (19)0.0289 (18)0.038 (2)0.0021 (16)0.002 (2)0.0033 (19)
C140.039 (2)0.0331 (19)0.048 (3)0.0014 (16)0.005 (2)0.006 (2)
C150.052 (2)0.035 (2)0.041 (2)0.0013 (18)0.002 (2)0.003 (2)
C160.063 (2)0.032 (2)0.042 (2)0.0043 (18)0.006 (2)0.004 (2)
C170.047 (2)0.047 (2)0.047 (3)0.0132 (18)0.001 (2)0.009 (2)
C180.042 (2)0.041 (2)0.042 (3)0.0018 (17)0.002 (2)0.005 (2)
C11'0.0340 (19)0.0302 (19)0.039 (2)0.0027 (15)0.0036 (18)0.0011 (19)
C12'0.0353 (19)0.033 (2)0.034 (2)0.0009 (16)0.0032 (18)0.0044 (19)
C13'0.0331 (18)0.034 (2)0.034 (2)0.0031 (15)0.0057 (18)0.0018 (18)
C14'0.0372 (19)0.032 (2)0.058 (3)0.0001 (16)0.004 (2)0.002 (2)
C15'0.054 (2)0.039 (2)0.060 (3)0.0062 (18)0.007 (2)0.010 (2)
C16'0.043 (2)0.051 (2)0.050 (3)0.0136 (19)0.005 (2)0.013 (2)
C17'0.040 (2)0.053 (2)0.041 (3)0.0045 (18)0.001 (2)0.002 (2)
C18'0.0382 (19)0.034 (2)0.043 (2)0.0001 (15)0.004 (2)0.002 (2)
Geometric parameters (Å, º) top
C1A—C11.385 (4)C11'—C12'1.198 (5)
C1A—C4A1.409 (5)C12'—C13'1.440 (5)
C1A—C91.486 (5)C13'—C18'1.395 (5)
C1—C21.396 (5)C13'—C14'1.398 (4)
C2—C31.389 (5)C14'—C15'1.378 (5)
C3—C41.383 (5)C15'—C16'1.374 (5)
C4—C4A1.398 (5)C16'—C17'1.385 (5)
C4A—C5A1.470 (5)C17'—C18'1.383 (5)
C5A—C51.386 (5)C1—H10.9500
C5A—C8A1.405 (5)C2—H20.9500
C5—C61.392 (5)C3—H30.9500
C6—C71.385 (5)C4—H40.9500
C7—C81.392 (5)C5—H50.9500
C8—C8A1.395 (5)C6—H60.9500
C8A—C91.482 (5)C7—H70.9500
C9—C101.367 (5)C8—H80.9500
C10—C11'1.427 (5)C14—H140.9500
C10—C111.436 (5)C15—H150.9500
C11—C121.197 (4)C16—H160.9500
C12—C131.437 (5)C17—H170.9500
C13—C181.398 (5)C18—H180.9500
C13—C141.405 (4)C14'—H14'0.9500
C14—C151.384 (5)C15'—H15'0.9500
C15—C161.383 (5)C16'—H16'0.9500
C16—C171.385 (5)C17'—H17'0.9500
C17—C181.395 (5)C18'—H18'0.9500
C1—C1A—C4A120.0 (3)C15'—C14'—C13'120.0 (4)
C1—C1A—C9131.5 (3)C16'—C15'—C14'120.6 (4)
C4A—C1A—C9108.5 (3)C15'—C16'—C17'120.5 (4)
C1A—C1—C2118.9 (4)C18'—C17'—C16'119.3 (4)
C3—C2—C1121.0 (4)C17'—C18'—C13'120.9 (3)
C4—C3—C2120.7 (4)C1A—C1—H1120.6
C3—C4—C4A118.6 (4)C2—C1—H1120.6
C4—C4A—C1A120.8 (3)C3—C2—H2119.5
C4—C4A—C5A130.4 (3)C1—C2—H2119.5
C1A—C4A—C5A108.7 (3)C4—C3—H3119.6
C5—C5A—C8A121.4 (3)C2—C3—H3119.6
C5—C5A—C4A130.4 (3)C3—C4—H4120.7
C8A—C5A—C4A108.2 (3)C4A—C4—H4120.7
C5A—C5—C6118.8 (4)C5A—C5—H5120.6
C7—C6—C5119.9 (4)C6—C5—H5120.6
C6—C7—C8121.9 (3)C7—C6—H6120.0
C7—C8—C8A118.4 (4)C5—C6—H6120.0
C8—C8A—C5A119.6 (3)C6—C7—H7119.0
C8—C8A—C9131.2 (3)C8—C7—H7119.0
C5A—C8A—C9109.2 (3)C7—C8—H8120.8
C10—C9—C8A127.7 (3)C8A—C8—H8120.8
C10—C9—C1A126.9 (3)C15—C14—H14120.2
C8A—C9—C1A105.3 (3)C13—C14—H14120.2
C9—C10—C11'123.3 (3)C16—C15—H15119.6
C9—C10—C11122.8 (3)C14—C15—H15119.6
C11'—C10—C11113.9 (3)C15—C16—H16120.0
C12—C11—C10174.6 (4)C17—C16—H16120.0
C11—C12—C13175.8 (4)C16—C17—H17120.0
C18—C13—C14119.5 (3)C18—C17—H17120.0
C18—C13—C12120.9 (3)C17—C18—H18120.0
C14—C13—C12119.6 (3)C13—C18—H18120.0
C15—C14—C13119.6 (4)C15'—C14'—H14'120.0
C16—C15—C14120.8 (4)C13'—C14'—H14'120.0
C15—C16—C17120.1 (4)C16'—C15'—H15'119.7
C16—C17—C18120.1 (4)C14'—C15'—H15'119.7
C17—C18—C13119.9 (4)C15'—C16'—H16'119.8
C12'—C11'—C10175.8 (4)C17'—C16'—H16'119.8
C11'—C12'—C13'175.1 (4)C18'—C17'—H17'120.3
C18'—C13'—C14'118.7 (3)C16'—C17'—H17'120.3
C18'—C13'—C12'121.3 (3)C17'—C18'—H18'119.6
C14'—C13'—C12'120.0 (3)C13'—C18'—H18'119.6
C4A—C1A—C1—C21.1 (6)C5A—C8A—C9—C10176.0 (4)
C9—C1A—C1—C2179.4 (4)C8—C8A—C9—C1A175.5 (4)
C1A—C1—C2—C31.1 (6)C5A—C8A—C9—C1A2.6 (4)
C1—C2—C3—C40.0 (6)C1—C1A—C9—C104.8 (7)
C2—C3—C4—C4A1.0 (6)C4A—C1A—C9—C10175.6 (4)
C3—C4—C4A—C1A1.0 (6)C1—C1A—C9—C8A176.6 (4)
C3—C4—C4A—C5A177.8 (4)C4A—C1A—C9—C8A3.0 (4)
C1—C1A—C4A—C40.1 (6)C8A—C9—C10—C11'177.9 (4)
C9—C1A—C4A—C4179.7 (4)C1A—C9—C10—C11'0.4 (6)
C1—C1A—C4A—C5A177.4 (4)C8A—C9—C10—C112.0 (6)
C9—C1A—C4A—C5A2.3 (4)C1A—C9—C10—C11176.3 (4)
C4—C4A—C5A—C50.6 (7)C12—C13—C14—C15179.7 (4)
C1A—C4A—C5A—C5177.7 (4)C13—C14—C15—C160.0 (6)
C4—C4A—C5A—C8A177.7 (4)C14—C15—C16—C171.1 (6)
C1A—C4A—C5A—C8A0.6 (4)C15—C16—C17—C181.5 (7)
C8A—C5A—C5—C61.1 (6)C16—C17—C18—C130.8 (7)
C4A—C5A—C5—C6176.9 (4)C14—C13—C18—C170.2 (6)
C5A—C5—C6—C70.3 (6)C12—C13—C18—C17179.9 (4)
C5—C6—C7—C80.3 (7)C18'—C13'—C14'—C15'2.2 (7)
C6—C7—C8—C8A0.1 (6)C12'—C13'—C14'—C15'177.3 (4)
C7—C8—C8A—C5A0.7 (6)C13'—C14'—C15'—C16'0.9 (7)
C7—C8—C8A—C9178.7 (4)C14'—C15'—C16'—C17'0.5 (7)
C5—C5A—C8A—C81.4 (6)C15'—C16'—C17'—C18'0.5 (7)
C4A—C5A—C8A—C8177.1 (4)C16'—C17'—C18'—C13'0.8 (6)
C5—C5A—C8A—C9179.7 (4)C14'—C13'—C18'—C17'2.1 (6)
C4A—C5A—C8A—C91.3 (4)C12'—C13'—C18'—C17'177.4 (4)
C8—C8A—C9—C105.9 (7)
 

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