Literature DB >> 21837110

Phen-yl(2,4,5-triphenyl-cyclo-penta-1,4-dien-1-yl)methanone.

David B Cordes1, Guoxiong Hua, Alexandra M Z Slawin, J Derek Woollins.   

Abstract

The title compound, C(30)H(22)O, does not form face-to-face π-π inter-actions despite the presence of four phenyl rings within the compound. Instead weak C-H⋯π inter-actions occur between adjacent mol-ecules, with CC contact distances in the range 3.633 (4)-3.974 (4) Å. The ketone O atom also takes part in a weak C-H⋯O inter-action. The three pendant phenyl rings are twisted relative to the central cyclopentadiene ring by 17.82 (17), 29.63 (14) and 61.57 (9)°, while the phenylmethanone is nearly orthogonal, the angle between planes being 87.77 (9)°.

Entities:  

Year:  2011        PMID: 21837110      PMCID: PMC3152139          DOI: 10.1107/S1600536811022902

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For a previous preparation of the title compound, see: Lund (2005 ▶). The crystal studied was obtained by reaction of Woollins’ reagent [2,4-bis­(phen­yl)-1,3-diselenadiphosphetane-2,4-disel­en­ide] with quinoxaline-2,3-dithiol. For a review of the chemistry of Woollins’ reagent, see: Hua & Woollins (2009 ▶). There are no structurally closely-related compounds in the literature; however, for some of the closest related, see: Evrard et al. (1971 ▶); Wender et al. (2006 ▶).

Experimental

Crystal data

C30H22O M = 398.48 Monoclinic, a = 25.946 (6) Å b = 6.1573 (14) Å c = 26.602 (6) Å β = 102.236 (7)° V = 4153.3 (16) Å3 Z = 8 Mo Kα radiation μ = 0.08 mm−1 T = 93 K 0.30 × 0.20 × 0.06 mm

Data collection

Rigaku Mercury CCD diffractometer Absorption correction: multi-scan (CrystalClear; Rigaku, 2010 ▶) T min = 0.978, T max = 0.996 13266 measured reflections 4252 independent reflections 2479 reflections with I > 2σ(I) R int = 0.120

Refinement

R[F 2 > 2σ(F 2)] = 0.081 wR(F 2) = 0.225 S = 1.04 4252 reflections 281 parameters H-atom parameters constrained Δρmax = 0.29 e Å−3 Δρmin = −0.39 e Å−3 Data collection: CrystalClear (Rigaku, 2010 ▶); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL. Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811022902/fj2426sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811022902/fj2426Isup2.hkl Supplementary material file. DOI: 10.1107/S1600536811022902/fj2426Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C30H22OF(000) = 1680
Mr = 398.48Dx = 1.275 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 3958 reflections
a = 25.946 (6) Åθ = 6.3–54.9°
b = 6.1573 (14) ŵ = 0.08 mm1
c = 26.602 (6) ÅT = 93 K
β = 102.236 (7)°Prism, colourless
V = 4153.3 (16) Å30.30 × 0.20 × 0.06 mm
Z = 8
Rigaku Mercury CCD diffractometer4252 independent reflections
Radiation source: rotating anode2479 reflections with I > 2σ(I)
confocalRint = 0.120
Detector resolution: 14.7059 pixels mm-1θmax = 27.5°, θmin = 3.1°
ω and φ scansh = −33→26
Absorption correction: multi-scan (CrystalClear; Rigaku, 2010)k = −7→7
Tmin = 0.978, Tmax = 0.996l = −28→33
13266 measured reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.081Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.225H-atom parameters constrained
S = 1.04w = 1/[σ2(Fo2) + (0.1072P)2] where P = (Fo2 + 2Fc2)/3
4252 reflections(Δ/σ)max < 0.001
281 parametersΔρmax = 0.29 e Å3
0 restraintsΔρmin = −0.39 e Å3
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.
xyzUiso*/Ueq
O10.36026 (8)0.0838 (4)0.13591 (8)0.0494 (6)
C10.41982 (10)0.7166 (5)0.21370 (9)0.0300 (7)
H1A0.44800.68660.24430.036*
H1B0.40320.85770.21850.036*
C20.37945 (10)0.5375 (4)0.20539 (9)0.0279 (7)
C30.37812 (10)0.4503 (4)0.15812 (9)0.0289 (7)
C40.41591 (10)0.5655 (4)0.13312 (9)0.0283 (7)
C50.44176 (10)0.7189 (4)0.16562 (9)0.0269 (6)
C60.34825 (10)0.4843 (5)0.24389 (10)0.0304 (7)
C70.34567 (11)0.6341 (5)0.28290 (10)0.0368 (7)
H70.36450.76720.28420.044*
C80.31633 (12)0.5923 (6)0.31959 (11)0.0454 (8)
H80.31530.69640.34570.054*
C90.28875 (12)0.4015 (6)0.31855 (11)0.0452 (8)
H90.26810.37460.34340.054*
C100.29138 (11)0.2480 (5)0.28080 (12)0.0434 (8)
H100.27300.11440.28030.052*
C110.32083 (10)0.2887 (5)0.24366 (11)0.0350 (7)
H110.32230.18280.21800.042*
C120.34422 (11)0.2708 (5)0.13193 (10)0.0315 (7)
C130.29162 (11)0.3222 (5)0.09964 (10)0.0313 (7)
C140.26130 (11)0.1535 (5)0.07379 (10)0.0374 (7)
H140.27460.00930.07650.045*
C150.21138 (11)0.1970 (5)0.04388 (11)0.0416 (8)
H150.19060.08190.02650.050*
C160.19237 (12)0.4045 (6)0.03957 (12)0.0516 (9)
H160.15840.43370.01910.062*
C170.22223 (14)0.5704 (6)0.06479 (16)0.0740 (13)
H170.20900.71480.06150.089*
C180.27205 (12)0.5288 (5)0.09539 (12)0.0522 (10)
H180.29230.64430.11320.063*
C190.42011 (10)0.5280 (5)0.07848 (9)0.0291 (7)
C200.43588 (10)0.3314 (5)0.06182 (10)0.0341 (7)
H200.44370.21320.08520.041*
C210.44040 (11)0.3058 (5)0.01114 (11)0.0397 (8)
H210.45180.17090.00000.048*
C220.42837 (11)0.4765 (5)−0.02322 (11)0.0398 (8)
H220.43150.4583−0.05790.048*
C230.41199 (11)0.6712 (5)−0.00742 (10)0.0380 (8)
H230.40350.7875−0.03120.046*
C240.40768 (11)0.6993 (5)0.04363 (10)0.0358 (7)
H240.39630.83460.05460.043*
C250.48404 (10)0.8684 (4)0.15913 (9)0.0271 (7)
C260.52110 (10)0.8136 (5)0.12983 (10)0.0336 (7)
H260.51840.67750.11270.040*
C270.56144 (11)0.9533 (5)0.12544 (10)0.0381 (8)
H270.58590.91270.10510.046*
C280.56674 (11)1.1516 (5)0.15023 (11)0.0392 (8)
H280.59461.24730.14710.047*
C290.53077 (11)1.2092 (5)0.17984 (11)0.0373 (8)
H290.53411.34470.19730.045*
C300.49004 (11)1.0692 (5)0.18395 (9)0.0317 (7)
H300.46561.11100.20420.038*
U11U22U33U12U13U23
O10.0409 (12)0.0385 (14)0.0614 (14)0.0034 (10)−0.0057 (11)−0.0054 (11)
C10.0278 (15)0.0406 (18)0.0201 (14)0.0017 (12)0.0013 (11)0.0012 (11)
C20.0215 (14)0.0374 (18)0.0244 (15)0.0014 (11)0.0041 (11)0.0016 (11)
C30.0221 (14)0.0344 (17)0.0271 (15)0.0022 (11)−0.0017 (11)0.0006 (12)
C40.0243 (14)0.0341 (17)0.0251 (14)0.0014 (11)0.0019 (11)0.0019 (12)
C50.0227 (14)0.0343 (17)0.0223 (14)0.0008 (11)0.0016 (11)0.0032 (11)
C60.0197 (14)0.0410 (18)0.0280 (15)0.0001 (12)−0.0003 (11)0.0011 (12)
C70.0349 (17)0.048 (2)0.0280 (15)−0.0041 (14)0.0078 (13)−0.0019 (13)
C80.047 (2)0.057 (2)0.0338 (17)−0.0068 (16)0.0134 (14)−0.0049 (15)
C90.0383 (18)0.068 (2)0.0318 (17)−0.0027 (16)0.0139 (14)0.0047 (16)
C100.0355 (18)0.053 (2)0.0419 (18)−0.0084 (15)0.0078 (14)0.0089 (16)
C110.0307 (16)0.0411 (19)0.0337 (16)−0.0035 (13)0.0079 (13)−0.0009 (13)
C120.0314 (16)0.0336 (18)0.0300 (15)0.0018 (13)0.0079 (12)0.0020 (12)
C130.0323 (16)0.0339 (17)0.0270 (15)0.0001 (12)0.0044 (12)−0.0020 (12)
C140.0387 (17)0.0398 (19)0.0317 (16)−0.0051 (14)0.0031 (13)−0.0001 (13)
C150.0395 (18)0.048 (2)0.0330 (17)−0.0103 (15)−0.0032 (13)−0.0044 (14)
C160.0402 (19)0.054 (2)0.050 (2)0.0045 (16)−0.0141 (15)−0.0040 (17)
C170.055 (2)0.047 (2)0.097 (3)0.0130 (18)−0.034 (2)−0.014 (2)
C180.0411 (19)0.040 (2)0.063 (2)0.0018 (15)−0.0173 (16)−0.0145 (16)
C190.0254 (14)0.0352 (18)0.0242 (14)−0.0018 (12)−0.0003 (11)−0.0022 (12)
C200.0331 (16)0.0387 (19)0.0277 (16)0.0003 (13)0.0001 (12)−0.0043 (12)
C210.0349 (17)0.045 (2)0.0384 (18)0.0007 (14)0.0064 (14)−0.0093 (14)
C220.0372 (17)0.054 (2)0.0269 (15)−0.0033 (15)0.0041 (13)−0.0038 (14)
C230.0385 (17)0.049 (2)0.0253 (16)−0.0016 (14)0.0041 (13)0.0006 (13)
C240.0344 (16)0.0428 (19)0.0273 (16)0.0032 (13)0.0000 (12)−0.0018 (13)
C250.0233 (14)0.0365 (17)0.0191 (14)0.0002 (12)−0.0010 (11)0.0034 (11)
C260.0308 (16)0.0416 (19)0.0273 (15)−0.0013 (13)0.0039 (12)−0.0029 (12)
C270.0331 (17)0.050 (2)0.0319 (16)−0.0055 (14)0.0086 (13)0.0022 (14)
C280.0299 (17)0.051 (2)0.0323 (17)−0.0089 (14)−0.0022 (13)0.0075 (14)
C290.0334 (17)0.0406 (19)0.0330 (16)−0.0055 (13)−0.0046 (13)−0.0018 (13)
C300.0335 (16)0.0411 (19)0.0178 (13)0.0022 (13)−0.0005 (11)0.0025 (12)
O1—C121.221 (3)C15—H150.9500
C1—C21.504 (4)C16—C171.369 (5)
C1—C51.506 (4)C16—H160.9500
C1—H1A0.9900C17—C181.398 (4)
C1—H1B0.9900C17—H170.9500
C2—C31.361 (4)C18—H180.9500
C2—C61.471 (4)C19—C201.381 (4)
C3—C41.478 (4)C19—C241.396 (4)
C3—C121.490 (4)C20—C211.387 (4)
C4—C51.358 (3)C20—H200.9500
C4—C191.498 (4)C21—C221.384 (4)
C5—C251.470 (4)C21—H210.9500
C6—C111.398 (4)C22—C231.367 (4)
C6—C71.401 (4)C22—H220.9500
C7—C81.383 (4)C23—C241.397 (4)
C7—H70.9500C23—H230.9500
C8—C91.372 (4)C24—H240.9500
C8—H80.9500C25—C301.395 (4)
C9—C101.392 (4)C25—C261.401 (4)
C9—H90.9500C26—C271.379 (4)
C10—C111.394 (4)C26—H260.9500
C10—H100.9500C27—C281.380 (4)
C11—H110.9500C27—H270.9500
C12—C131.484 (4)C28—C291.389 (4)
C13—C181.366 (4)C28—H280.9500
C13—C141.393 (4)C29—C301.386 (4)
C14—C151.395 (4)C29—H290.9500
C14—H140.9500C30—H300.9500
C15—C161.366 (4)
C2—C1—C5105.0 (2)C14—C15—H15119.9
C2—C1—H1A110.7C15—C16—C17120.0 (3)
C5—C1—H1A110.7C15—C16—H16120.0
C2—C1—H1B110.7C17—C16—H16120.0
C5—C1—H1B110.7C16—C17—C18120.4 (3)
H1A—C1—H1B108.8C16—C17—H17119.8
C3—C2—C6130.2 (3)C18—C17—H17119.8
C3—C2—C1107.8 (2)C13—C18—C17120.1 (3)
C6—C2—C1122.0 (2)C13—C18—H18120.0
C2—C3—C4109.7 (2)C17—C18—H18120.0
C2—C3—C12128.4 (3)C20—C19—C24119.5 (3)
C4—C3—C12121.9 (2)C20—C19—C4122.2 (2)
C5—C4—C3109.4 (2)C24—C19—C4118.3 (2)
C5—C4—C19126.7 (2)C19—C20—C21120.2 (3)
C3—C4—C19123.7 (2)C19—C20—H20119.9
C4—C5—C25129.9 (2)C21—C20—H20119.9
C4—C5—C1108.0 (2)C22—C21—C20120.1 (3)
C25—C5—C1122.1 (2)C22—C21—H21119.9
C11—C6—C7117.8 (3)C20—C21—H21119.9
C11—C6—C2122.9 (3)C23—C22—C21120.3 (3)
C7—C6—C2119.2 (3)C23—C22—H22119.9
C8—C7—C6121.3 (3)C21—C22—H22119.9
C8—C7—H7119.3C22—C23—C24120.1 (3)
C6—C7—H7119.3C22—C23—H23120.0
C9—C8—C7120.5 (3)C24—C23—H23120.0
C9—C8—H8119.7C19—C24—C23119.8 (3)
C7—C8—H8119.7C19—C24—H24120.1
C8—C9—C10119.4 (3)C23—C24—H24120.1
C8—C9—H9120.3C30—C25—C26117.1 (2)
C10—C9—H9120.3C30—C25—C5120.7 (2)
C9—C10—C11120.5 (3)C26—C25—C5122.1 (2)
C9—C10—H10119.8C27—C26—C25121.3 (3)
C11—C10—H10119.8C27—C26—H26119.4
C10—C11—C6120.5 (3)C25—C26—H26119.4
C10—C11—H11119.8C26—C27—C28120.8 (3)
C6—C11—H11119.8C26—C27—H27119.6
O1—C12—C13120.4 (3)C28—C27—H27119.6
O1—C12—C3120.1 (2)C27—C28—C29119.1 (3)
C13—C12—C3119.4 (2)C27—C28—H28120.5
C18—C13—C14119.5 (3)C29—C28—H28120.5
C18—C13—C12121.8 (2)C30—C29—C28120.1 (3)
C14—C13—C12118.7 (3)C30—C29—H29120.0
C13—C14—C15119.8 (3)C28—C29—H29120.0
C13—C14—H14120.1C29—C30—C25121.6 (3)
C15—C14—H14120.1C29—C30—H30119.2
C16—C15—C14120.2 (3)C25—C30—H30119.2
C16—C15—H15119.9
Cg1 and Cg2 are the centroids of the C6–C11 and C25–C30 rings, respectively.
D—H···AD—HH···AD···AD—H···A
C1—H1B···O1i0.992.643.229 (3)118.(2)
C10—H10···Cg1ii0.952.803.527 (3)134 (2)
C20—H20···Cg2iii0.952.803.605 (3)143 (2)
C28—H28···Cg1iv0.952.883.612 (3)134 (2)
C10—H10···C10ii0.953.063.908 (4)150 (2)
C20—H20···C30iii0.952.793.633 (4)148 (2)
C28—H28···C9iv0.953.123.974 (4)151 (2)
Table 1

Hydrogen-bond geometry (Å, °)

Cg1 and Cg2 are the centroids of the C6–C11 and C25–C30 rings, respectively.

D—H⋯AD—HH⋯ADAD—H⋯A
C1—H1B⋯O1i0.992.643.229 (3)118 (2)
C10—H10⋯Cg1ii0.952.803.527 (3)134 (2)
C20—H20⋯Cg2iii0.952.803.605 (3)143 (2)
C28—H28⋯Cg1iv0.952.883.612 (3)134 (2)

Symmetry codes: (i) ; (ii) ; (iii) ; (iv) .

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Authors:  Paul A Wender; Thomas J Paxton; Travis J Williams
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