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The title compound, C22H18N2, displays some release of the usual strain in [2.2]­para­cyclo­phanes (e.g. the bridge bonds are no longer lengthened), associated with the lengthening of the bridgehead contact C3...C14. However, the effect is not uniform; the basketene ring system introduces strain of its own (e.g. lengthened single bonds, wide angles at the corresponding bridge atoms).

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536802009480/na6168sup1.cif
Contains datablocks 2, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536802009480/na61682sup2.hkl
Contains datablock 2

CCDC reference: 189889

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.002 Å
  • R factor = 0.040
  • wR factor = 0.117
  • Data-to-parameter ratio = 12.7

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Yellow Alert Alert Level C:
PLAT_320 Alert C Check Hybridisation of C(18) in main residue ? PLAT_320 Alert C Check Hybridisation of C(19) in main residue ? PLAT_320 Alert C Check Hybridisation of C(20) in main residue ?
0 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
3 Alert Level C = Please check

Computing details top

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

[2.2]basketenoparacyclophane 18,20-dicarbonitrile top
Crystal data top
C22H18N2F(000) = 656
Mr = 310.38Dx = 1.310 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 6.6094 (14) ÅCell parameters from 50 reflections
b = 17.251 (3) Åθ = 10–11.5°
c = 13.910 (3) ŵ = 0.08 mm1
β = 97.272 (16)°T = 293 K
V = 1573.3 (5) Å3Plate, colourless
Z = 40.6 × 0.6 × 0.08 mm
Data collection top
Nicolet R3
diffractometer
Rint = 0.024
Radiation source: fine-focus sealed tubeθmax = 25.0°, θmin = 3.1°
Graphite monochromatorh = 77
ω scansk = 2020
5639 measured reflectionsl = 160
2760 independent reflections3 standard reflections every 147 reflections
2175 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)] = 0.040Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.117H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.0592P)2 + 0.3931P]
where P = (Fo2 + 2Fc2)/3
2760 reflections(Δ/σ)max < 0.001
217 parametersΔρmax = 0.22 e Å3
0 restraintsΔρmin = 0.21 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)

- 1.1042 (0.0051) x + 16.8350 (0.0064) y + 2.2328 (0.0164) z = 11.9081 (0.0050)

* -0.0045 (0.0008) C12 * 0.0045 (0.0008) C13 * -0.0045 (0.0008) C15 * 0.0045 (0.0008) C16 - 0.1541 (0.0025) C11 - 0.1420 (0.0025) C14

Rms deviation of fitted atoms = 0.0045

Non-bonded distances: 3.0227 (0.0023) C3 - C14 2.7980 (0.0022) C6 - C11

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
C10.4122 (3)0.64203 (11)0.40469 (14)0.0524 (5)
H1A0.30240.66670.43340.065*
H1B0.53330.64310.45200.065*
C20.3542 (3)0.55730 (10)0.38012 (13)0.0438 (4)
H2A0.36050.52900.44070.055*
H2B0.21290.55670.35090.055*
C30.4785 (2)0.51175 (9)0.31326 (11)0.0352 (4)
C40.3869 (2)0.49151 (9)0.20535 (12)0.0368 (4)
H40.23930.48310.19980.045*
C50.4425 (2)0.54168 (9)0.12594 (11)0.0382 (4)
H50.34410.56060.07800.045*
C60.6389 (2)0.55832 (9)0.12644 (11)0.0360 (4)
C70.7718 (2)0.52073 (9)0.20871 (11)0.0341 (4)
H70.91610.53320.20730.040*
C80.7110 (2)0.52785 (9)0.31314 (11)0.0340 (4)
H80.77850.56670.35750.040*
C90.7301 (3)0.61092 (10)0.05539 (13)0.0472 (4)
H9A0.72360.58420.00630.055*
H9B0.87300.61900.07900.055*
C100.6266 (3)0.69141 (11)0.03779 (13)0.0565 (5)
H10A0.72280.72850.01730.067*
H10B0.51130.68760.01260.067*
C110.5563 (3)0.71725 (9)0.13142 (13)0.0459 (4)
C120.3532 (3)0.71087 (10)0.14603 (15)0.0534 (5)
H120.25110.71670.09400.065*
C130.3017 (3)0.69586 (10)0.23777 (15)0.0523 (5)
H130.16510.69190.24690.065*
C140.4521 (3)0.68664 (9)0.31608 (13)0.0445 (4)
C150.6482 (3)0.70927 (9)0.30399 (13)0.0438 (4)
H150.74640.71380.35780.050*
C160.6994 (3)0.72524 (9)0.21295 (13)0.0441 (4)
H160.83090.74150.20610.050*
C170.5057 (2)0.41391 (9)0.21873 (12)0.0374 (4)
H170.44610.36650.18830.045*
C180.7378 (2)0.43105 (9)0.21861 (11)0.0358 (4)
C190.5277 (3)0.42301 (9)0.33029 (12)0.0393 (4)
H190.46640.38900.37510.047*
C200.7591 (2)0.43934 (9)0.33238 (11)0.0374 (4)
C210.8551 (3)0.37897 (10)0.16549 (13)0.0438 (4)
C220.9261 (3)0.40857 (10)0.39827 (13)0.0469 (4)
N10.9479 (3)0.33944 (11)0.12212 (14)0.0675 (5)
N21.0577 (3)0.38472 (11)0.45089 (14)0.0715 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0646 (12)0.0466 (11)0.0491 (10)0.0010 (9)0.0194 (9)0.0102 (8)
C20.0477 (10)0.0419 (9)0.0438 (9)0.0006 (7)0.0140 (8)0.0025 (7)
C30.0389 (9)0.0310 (8)0.0362 (8)0.0003 (6)0.0060 (7)0.0006 (6)
C40.0330 (8)0.0332 (8)0.0432 (9)0.0015 (6)0.0014 (7)0.0038 (7)
C50.0467 (10)0.0295 (8)0.0357 (8)0.0036 (6)0.0051 (7)0.0022 (6)
C60.0483 (10)0.0275 (8)0.0320 (8)0.0024 (7)0.0040 (7)0.0022 (6)
C70.0352 (8)0.0288 (8)0.0386 (8)0.0006 (6)0.0061 (6)0.0014 (6)
C80.0381 (8)0.0297 (8)0.0334 (8)0.0001 (6)0.0009 (6)0.0006 (6)
C90.0678 (12)0.0375 (9)0.0380 (9)0.0000 (8)0.0130 (8)0.0051 (7)
C100.0854 (15)0.0409 (10)0.0428 (10)0.0014 (9)0.0069 (9)0.0111 (8)
C110.0664 (12)0.0238 (8)0.0464 (10)0.0041 (7)0.0032 (8)0.0056 (7)
C120.0587 (12)0.0363 (9)0.0602 (12)0.0119 (8)0.0117 (9)0.0032 (8)
C130.0444 (10)0.0404 (10)0.0726 (13)0.0088 (8)0.0094 (9)0.0047 (9)
C140.0572 (11)0.0295 (8)0.0480 (10)0.0068 (7)0.0108 (8)0.0093 (7)
C150.0554 (11)0.0296 (8)0.0446 (9)0.0013 (7)0.0012 (8)0.0082 (7)
C160.0510 (10)0.0274 (8)0.0538 (10)0.0021 (7)0.0065 (8)0.0026 (7)
C170.0437 (9)0.0267 (8)0.0416 (9)0.0034 (6)0.0048 (7)0.0025 (6)
C180.0433 (9)0.0279 (8)0.0368 (8)0.0039 (6)0.0067 (7)0.0016 (6)
C190.0478 (10)0.0313 (8)0.0401 (9)0.0011 (7)0.0102 (7)0.0041 (7)
C200.0433 (9)0.0324 (8)0.0364 (8)0.0044 (7)0.0045 (7)0.0039 (7)
C210.0497 (10)0.0338 (9)0.0492 (10)0.0044 (7)0.0116 (8)0.0024 (7)
C220.0491 (10)0.0438 (10)0.0469 (10)0.0054 (8)0.0023 (8)0.0085 (8)
N10.0761 (12)0.0546 (10)0.0775 (12)0.0146 (9)0.0317 (10)0.0060 (9)
N20.0664 (11)0.0720 (12)0.0715 (12)0.0135 (9)0.0087 (10)0.0198 (10)
Geometric parameters (Å, º) top
C1—C141.505 (3)C9—H9B0.9700
C1—C21.539 (2)C10—C111.505 (3)
C1—H1A0.9700C10—H10A0.9700
C1—H1B0.9700C10—H10B0.9700
C2—C31.534 (2)C11—C121.388 (3)
C2—H2A0.9700C11—C161.388 (3)
C2—H2B0.9700C12—C131.386 (3)
C3—C81.562 (2)C12—H120.9300
C3—C191.577 (2)C13—C141.388 (3)
C3—C41.585 (2)C13—H130.9300
C4—C51.485 (2)C14—C151.384 (3)
C4—C171.551 (2)C15—C161.379 (3)
C4—H40.9800C15—H150.9300
C5—C61.329 (2)C16—H160.9300
C5—H50.9300C17—C191.548 (2)
C6—C71.499 (2)C17—C181.562 (2)
C6—C91.521 (2)C17—H170.9800
C7—C81.560 (2)C18—C211.449 (2)
C7—C181.572 (2)C18—C201.578 (2)
C7—H70.9800C19—C201.552 (2)
C8—C201.576 (2)C19—H190.9800
C8—H80.9800C20—C221.444 (2)
C9—C101.554 (2)C21—N11.140 (2)
C9—H9A0.9700C22—N21.140 (2)
C14—C1—C2111.63 (14)C11—C10—H10A110.1
C14—C1—H1A109.3C9—C10—H10A110.1
C2—C1—H1A109.3C11—C10—H10B110.1
C14—C1—H1B109.3C9—C10—H10B110.1
C2—C1—H1B109.3H10A—C10—H10B108.5
H1A—C1—H1B108.0C12—C11—C16117.37 (17)
C3—C2—C1118.93 (14)C12—C11—C10120.91 (17)
C3—C2—H2A107.6C16—C11—C10118.93 (18)
C1—C2—H2A107.6C13—C12—C11120.30 (17)
C3—C2—H2B107.6C13—C12—H12119.8
C1—C2—H2B107.6C11—C12—H12119.8
H2A—C2—H2B107.0C12—C13—C14120.60 (18)
C2—C3—C8120.83 (13)C12—C13—H13119.7
C2—C3—C19121.49 (13)C14—C13—H13119.7
C8—C3—C1989.36 (11)C15—C14—C13117.46 (17)
C2—C3—C4121.15 (14)C15—C14—C1120.52 (17)
C8—C3—C4107.23 (12)C13—C14—C1121.28 (17)
C19—C3—C488.58 (11)C16—C15—C14120.67 (16)
C5—C4—C17115.02 (13)C16—C15—H15119.7
C5—C4—C3118.37 (13)C14—C15—H15119.7
C17—C4—C387.10 (11)C15—C16—C11120.63 (17)
C5—C4—H4111.4C15—C16—H16119.7
C17—C4—H4111.4C11—C16—H16119.7
C3—C4—H4111.4C19—C17—C490.84 (12)
C6—C5—C4117.09 (14)C19—C17—C1890.82 (12)
C6—C5—H5121.5C4—C17—C18108.58 (12)
C4—C5—H5121.5C19—C17—H17119.9
C5—C6—C7112.85 (14)C4—C17—H17119.9
C5—C6—C9126.36 (15)C18—C17—H17119.9
C7—C6—C9120.78 (14)C21—C18—C17118.16 (14)
C6—C7—C8118.79 (13)C21—C18—C7118.29 (14)
C6—C7—C18114.59 (13)C17—C18—C7109.73 (12)
C8—C7—C1886.52 (11)C21—C18—C20125.62 (14)
C6—C7—H7111.6C17—C18—C2088.79 (12)
C8—C7—H7111.6C7—C18—C2090.18 (11)
C18—C7—H7111.6C17—C19—C2090.25 (12)
C7—C8—C3110.88 (12)C17—C19—C387.50 (11)
C7—C8—C2090.68 (11)C20—C19—C390.59 (12)
C3—C8—C2090.27 (11)C17—C19—H19125.6
C7—C8—H8119.4C20—C19—H19125.6
C3—C8—H8119.4C3—C19—H19125.6
C20—C8—H8119.4C22—C20—C19128.15 (14)
C6—C9—C10115.64 (15)C22—C20—C8125.85 (14)
C6—C9—H9A108.4C19—C20—C889.76 (11)
C10—C9—H9A108.4C22—C20—C18124.57 (14)
C6—C9—H9B108.4C19—C20—C1890.13 (12)
C10—C9—H9B108.4C8—C20—C1885.81 (11)
H9A—C9—H9B107.4N1—C21—C18178.31 (19)
C11—C10—C9107.84 (14)N2—C22—C20179.4 (2)
C14—C1—C2—C344.9 (2)C3—C4—C17—C1918.48 (12)
C1—C2—C3—C832.4 (2)C5—C4—C17—C1847.44 (17)
C1—C2—C3—C19142.94 (16)C3—C4—C17—C1872.66 (13)
C1—C2—C3—C4107.40 (19)C19—C17—C18—C21131.05 (14)
C2—C3—C4—C598.29 (18)C4—C17—C18—C21137.79 (15)
C8—C3—C4—C546.26 (18)C19—C17—C18—C789.20 (13)
C19—C3—C4—C5135.15 (15)C4—C17—C18—C71.96 (17)
C2—C3—C4—C17144.70 (14)C19—C17—C18—C200.55 (11)
C8—C3—C4—C1770.75 (13)C4—C17—C18—C2091.71 (13)
C19—C3—C4—C1718.14 (11)C6—C7—C18—C2188.66 (18)
C17—C4—C5—C652.95 (19)C8—C7—C18—C21151.15 (14)
C3—C4—C5—C647.9 (2)C6—C7—C18—C1751.03 (17)
C4—C5—C6—C71.2 (2)C8—C7—C18—C1769.16 (13)
C4—C5—C6—C9177.29 (14)C6—C7—C18—C20139.80 (13)
C5—C6—C7—C848.82 (19)C8—C7—C18—C2019.61 (11)
C9—C6—C7—C8129.74 (15)C4—C17—C19—C20109.16 (12)
C5—C6—C7—C1851.28 (18)C18—C17—C19—C200.56 (11)
C9—C6—C7—C18130.16 (15)C4—C17—C19—C318.58 (12)
C6—C7—C8—C345.34 (18)C18—C17—C19—C390.02 (12)
C18—C7—C8—C370.90 (13)C2—C3—C19—C17144.45 (15)
C6—C7—C8—C20135.89 (14)C8—C3—C19—C1789.08 (12)
C18—C7—C8—C2019.64 (11)C4—C3—C19—C1718.17 (12)
C2—C3—C8—C7143.30 (14)C2—C3—C19—C20125.32 (15)
C19—C3—C8—C789.70 (13)C8—C3—C19—C201.14 (11)
C4—C3—C8—C71.38 (16)C4—C3—C19—C20108.40 (12)
C2—C3—C8—C20125.87 (15)C17—C19—C20—C22135.78 (17)
C19—C3—C8—C201.13 (11)C3—C19—C20—C22136.72 (17)
C4—C3—C8—C2089.45 (12)C17—C19—C20—C886.36 (11)
C5—C6—C9—C1049.2 (2)C3—C19—C20—C81.13 (11)
C7—C6—C9—C10129.17 (17)C17—C19—C20—C180.55 (11)
C6—C9—C10—C1134.3 (2)C3—C19—C20—C1886.94 (11)
C9—C10—C11—C12101.56 (19)C7—C8—C20—C22110.88 (17)
C9—C10—C11—C1659.0 (2)C3—C8—C20—C22138.24 (17)
C16—C11—C12—C1313.9 (2)C7—C8—C20—C19109.74 (12)
C10—C11—C12—C13146.98 (18)C3—C8—C20—C191.14 (11)
C11—C12—C13—C140.3 (3)C7—C8—C20—C1819.59 (11)
C12—C13—C14—C1513.7 (2)C3—C8—C20—C1891.29 (11)
C12—C13—C14—C1156.48 (17)C21—C18—C20—C2213.8 (3)
C2—C1—C14—C15109.31 (19)C17—C18—C20—C22138.20 (16)
C2—C1—C14—C1360.6 (2)C7—C18—C20—C22112.07 (17)
C13—C14—C15—C1612.8 (2)C21—C18—C20—C19124.99 (17)
C1—C14—C15—C16157.42 (16)C17—C18—C20—C190.55 (11)
C14—C15—C16—C111.5 (2)C7—C18—C20—C19109.18 (11)
C12—C11—C16—C1514.8 (2)C21—C18—C20—C8145.26 (16)
C10—C11—C16—C15146.44 (16)C17—C18—C20—C890.30 (11)
C5—C4—C17—C19138.58 (14)C7—C18—C20—C819.43 (11)
 

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