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The title compound, C32H26Si, is a benzosilacyclo­pentene in which the silacyclo­pentene ring assumes an envelope conformation, with the Si atom displaced by 0.953 (2) Å from the mean plane of the four C atoms. The Si atom is bonded to two phenyl rings and to two Csp3 atoms in the silacyclo­pentene ring; one phenyl ring is attached to each of these two Csp3 atoms in the cis configuration.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536806028169/jh2026sup1.cif
Contains datablocks global, 3

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536806028169/jh20263sup2.hkl
Contains datablock 3

CCDC reference: 618251

Key indicators

  • Single-crystal X-ray study
  • T = 295 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.035
  • wR factor = 0.101
  • Data-to-parameter ratio = 15.4

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT230_ALERT_2_C Hirshfeld Test Diff for Si - C16 .. 5.09 su
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 1 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 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 0 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Computing details top

Data collection: CAD-4 EXPRESS (Enraf–Nonius, 1994); cell refinement: CAD-4 EXPRESS; data reduction: XCAD4 (Harms & Wocadlo, 1995); program(s) used to solve structure: SHELXS86 (Sheldrick, 1985); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

cis-1,2,2,3-Tetraphenyl-2,3-dihydro-1H-2-benzosilole top
Crystal data top
C32H26SiZ = 2
Mr = 438.62F(000) = 464
Triclinic, P1Dx = 1.195 Mg m3
Hall symbol: -P 1Cu Kα radiation, λ = 1.54178 Å
a = 9.877 (3) ÅCell parameters from 25 reflections
b = 10.633 (2) Åθ = 3.5–25.2°
c = 13.693 (2) ŵ = 0.96 mm1
α = 67.620 (14)°T = 295 K
β = 84.657 (18)°Prism, colorless
γ = 66.77 (2)°0.50 × 0.30 × 0.25 mm
V = 1219.2 (5) Å3
Data collection top
Enraf–Nonius CAD-4
diffractometer
Rint = 0.013
Radiation source: normal-focus sealed tubeθmax = 69.9°, θmin = 3.5°
Graphite monochromatorh = 1112
non–profiled ω/2θ scansk = 1112
7796 measured reflectionsl = 1216
4604 independent reflections3 standard reflections every 94 reflections
4113 reflections with I > 2σ(I) intensity decay: 3%
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0506P)2 + 0.2363P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.035(Δ/σ)max < 0.001
wR(F2) = 0.101Δρmax = 0.23 e Å3
S = 1.03Δρmin = 0.20 e Å3
4604 reflectionsExtinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
299 parametersExtinction coefficient: 0.0250 (10)
0 restraints
Special details top

Experimental. (1): 1H NMR (300 MHz, CDCl3, δ, p.p.m.): 3.95 (s, 4H), 7.05–7.26 (m, 14H); 13C NMR (75.4 MHz, CDCl3, δ, p.p.m.): 39.0 (CH2), 126.0 (CH), 126.6 (CH), 128.4 (CH), 128.8 (CH), 130.6 (CH), 138.9 (C), 140.8 (C).

(3): 1H NMR (500 MHz, CDCl3, δ, p.p.m.): 4.36 (s, 2H), 6.71 (d, J = 8 Hz, 2H), 6.93 (t, J = 8 Hz, 2H), 7.05 (m, 6H), 7.13 (m, 5H), 7.25 (m, 4H), 7.42 (bt, J = 7 Hz, 2H), 7.47 (bt, J = 7 Hz, 1H), 7.66 (d, J = 8 Hz, 2H); 13C NMR (125.7 MHz, CDCl3, δ, p.p.m.): 41.59 (CH), 124.82 (CH), 126.88 (CH), 127.07 (CH), 128.20(CH), 128.22 (CH), 128.27 (CH), 128.87 (CH), 129.59 (C), 130.03 (C), 130.49(C), 134.38 (C), 135.05 (CH), 136.36 (CH), 141.83 (C), 144.28 (C)

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Si0.43091 (4)0.68959 (4)0.73198 (3)0.04569 (13)
C220.27888 (14)0.86421 (14)0.64767 (10)0.0466 (3)
C270.16428 (16)0.95296 (16)0.69054 (12)0.0558 (3)
H270.16060.92310.76370.067*
C160.56546 (14)0.60922 (14)0.64593 (11)0.0485 (3)
C230.27846 (16)0.91449 (15)0.53762 (11)0.0528 (3)
H230.35260.85850.50640.063*
C240.17074 (18)1.04549 (17)0.47352 (12)0.0627 (4)
H240.17351.07670.40030.075*
C280.25036 (16)0.50845 (16)0.80844 (11)0.0555 (3)
C330.10765 (18)0.60581 (18)0.76522 (13)0.0658 (4)
H330.07680.70490.75490.079*
C50.38919 (17)0.72624 (16)0.91117 (11)0.0571 (4)
C100.57759 (16)0.83369 (16)0.81243 (11)0.0535 (3)
C210.58560 (19)0.47552 (16)0.63999 (14)0.0641 (4)
H210.5350.42010.68380.077*
C260.05716 (16)1.08338 (16)0.62663 (13)0.0609 (4)
H260.01721.14070.65690.073*
C40.30808 (17)0.64298 (16)0.91202 (11)0.0572 (4)
C170.64621 (17)0.68624 (18)0.57996 (14)0.0625 (4)
H170.6370.77520.58280.075*
C150.50363 (18)0.97942 (17)0.74465 (14)0.0643 (4)
H150.41261.00660.71190.077*
C190.7551 (2)0.50218 (19)0.50561 (15)0.0725 (5)
H190.81720.4670.45830.087*
C10.51491 (16)0.71737 (15)0.83767 (11)0.0537 (3)
H10.59590.62280.87450.064*
C110.71408 (19)0.7988 (2)0.85753 (15)0.0740 (5)
H110.76750.70230.90290.089*
C140.5618 (2)1.08499 (18)0.72472 (14)0.0679 (4)
H140.50951.18180.67950.081*
C250.05989 (18)1.12922 (16)0.51803 (13)0.0639 (4)
H250.01321.21670.47510.077*
C320.0112 (2)0.5578 (2)0.73738 (14)0.0742 (5)
H320.08380.62450.70950.089*
C30.35802 (16)0.55839 (15)0.83785 (11)0.0536 (3)
H30.44440.46880.87420.064*
C60.3457 (2)0.8162 (2)0.96970 (13)0.0744 (5)
H60.39880.87160.96950.089*
C290.2910 (2)0.36132 (18)0.82231 (14)0.0687 (4)
H290.38480.29320.85190.082*
C200.6792 (2)0.42314 (19)0.57040 (16)0.0767 (5)
H20C0.69060.33350.56770.092*
C80.1448 (3)0.7397 (3)1.03046 (15)0.0917 (6)
H80.06320.74421.07090.11*
C310.0547 (2)0.4124 (2)0.75065 (15)0.0798 (5)
H310.010.38060.73110.096*
C180.73960 (19)0.6336 (2)0.51045 (15)0.0730 (5)
H180.7920.68730.46690.088*
C130.6960 (2)1.0475 (2)0.77119 (15)0.0733 (5)
H130.73481.11860.75850.088*
C300.1947 (2)0.3142 (2)0.79299 (17)0.0824 (5)
H300.2250.21560.8020.099*
C90.1865 (2)0.6493 (2)0.97282 (12)0.0727 (5)
H90.13340.59310.97480.087*
C70.2225 (3)0.8226 (3)1.02838 (15)0.0930 (6)
H70.19240.88381.06670.112*
C120.7723 (2)0.9049 (2)0.83637 (18)0.0869 (6)
H120.86460.87850.8670.104*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Si0.0453 (2)0.03789 (19)0.0459 (2)0.01026 (14)0.00127 (14)0.01339 (15)
C220.0462 (7)0.0397 (6)0.0490 (7)0.0149 (5)0.0004 (5)0.0130 (5)
C270.0520 (8)0.0495 (7)0.0523 (8)0.0120 (6)0.0039 (6)0.0132 (6)
C160.0445 (7)0.0428 (7)0.0528 (7)0.0119 (5)0.0008 (5)0.0173 (6)
C230.0577 (8)0.0456 (7)0.0508 (7)0.0173 (6)0.0006 (6)0.0160 (6)
C240.0740 (10)0.0521 (8)0.0490 (8)0.0209 (7)0.0066 (7)0.0071 (6)
C280.0589 (8)0.0478 (7)0.0495 (7)0.0209 (6)0.0080 (6)0.0083 (6)
C330.0634 (9)0.0542 (8)0.0664 (10)0.0218 (7)0.0009 (7)0.0094 (7)
C50.0621 (8)0.0528 (8)0.0394 (7)0.0102 (7)0.0067 (6)0.0103 (6)
C100.0553 (8)0.0491 (7)0.0534 (8)0.0125 (6)0.0025 (6)0.0231 (6)
C210.0721 (10)0.0463 (8)0.0734 (10)0.0240 (7)0.0204 (8)0.0245 (7)
C260.0496 (8)0.0469 (8)0.0709 (10)0.0087 (6)0.0039 (7)0.0169 (7)
C40.0621 (8)0.0489 (7)0.0380 (7)0.0109 (6)0.0014 (6)0.0033 (6)
C170.0601 (9)0.0571 (8)0.0800 (11)0.0285 (7)0.0159 (7)0.0325 (8)
C150.0613 (9)0.0514 (8)0.0739 (10)0.0149 (7)0.0124 (7)0.0207 (7)
C190.0688 (10)0.0645 (10)0.0729 (11)0.0131 (8)0.0205 (8)0.0311 (8)
C10.0531 (8)0.0428 (7)0.0522 (8)0.0072 (6)0.0077 (6)0.0139 (6)
C110.0662 (10)0.0605 (9)0.0825 (12)0.0148 (8)0.0191 (9)0.0186 (9)
C140.0777 (11)0.0515 (8)0.0735 (10)0.0219 (8)0.0017 (8)0.0243 (8)
C250.0596 (9)0.0432 (7)0.0673 (10)0.0107 (6)0.0102 (7)0.0048 (7)
C320.0652 (10)0.0791 (12)0.0695 (10)0.0348 (9)0.0038 (8)0.0119 (9)
C30.0532 (8)0.0402 (7)0.0506 (7)0.0106 (6)0.0010 (6)0.0067 (6)
C60.0884 (12)0.0791 (11)0.0508 (9)0.0220 (9)0.0030 (8)0.0287 (8)
C290.0684 (10)0.0523 (8)0.0768 (11)0.0241 (8)0.0115 (8)0.0163 (8)
C200.0919 (13)0.0531 (9)0.0872 (12)0.0236 (9)0.0245 (10)0.0376 (9)
C80.0977 (15)0.1110 (16)0.0519 (10)0.0323 (13)0.0255 (10)0.0292 (10)
C310.0863 (13)0.0937 (14)0.0761 (12)0.0587 (12)0.0197 (10)0.0279 (10)
C180.0650 (10)0.0756 (11)0.0819 (12)0.0335 (9)0.0257 (9)0.0316 (9)
C130.0786 (11)0.0726 (11)0.0808 (12)0.0364 (9)0.0038 (9)0.0339 (9)
C300.0940 (14)0.0662 (11)0.0966 (14)0.0450 (10)0.0232 (11)0.0300 (10)
C90.0802 (11)0.0723 (10)0.0468 (8)0.0263 (9)0.0101 (8)0.0080 (7)
C70.1103 (16)0.1108 (17)0.0582 (11)0.0319 (14)0.0175 (10)0.0462 (11)
C120.0707 (11)0.0850 (13)0.1071 (16)0.0319 (10)0.0177 (11)0.0311 (12)
Geometric parameters (Å, º) top
Si—C161.8611 (15)C17—H170.93
Si—C221.8777 (15)C15—C141.383 (2)
Si—C11.9007 (15)C15—H150.93
Si—C31.9038 (15)C19—C201.364 (3)
C22—C231.3938 (19)C19—C181.372 (2)
C22—C271.404 (2)C19—H190.93
C27—C261.378 (2)C1—H10.98
C27—H270.93C11—C121.386 (3)
C16—C211.389 (2)C11—H110.93
C16—C171.393 (2)C14—C131.366 (2)
C23—C241.384 (2)C14—H140.93
C23—H230.93C25—H250.93
C24—C251.372 (2)C32—C311.373 (3)
C24—H240.93C32—H320.93
C28—C291.392 (2)C3—H30.98
C28—C331.395 (2)C6—C71.388 (3)
C28—C31.504 (2)C6—H60.93
C33—C321.383 (2)C29—C301.384 (3)
C33—H330.93C29—H290.93
C5—C61.392 (2)C20—H20C0.93
C5—C41.406 (2)C8—C71.370 (3)
C5—C11.520 (2)C8—C91.386 (3)
C10—C111.387 (2)C8—H80.93
C10—C151.391 (2)C31—C301.374 (3)
C10—C11.507 (2)C31—H310.93
C21—C201.381 (2)C18—H180.93
C21—H210.93C13—C121.363 (3)
C26—C251.379 (2)C13—H130.93
C26—H260.93C30—H300.93
C4—C91.390 (2)C9—H90.93
C4—C31.528 (2)C7—H70.93
C17—C181.380 (2)C12—H120.93
C16—Si—C22109.70 (6)C10—C1—H1105.9
C16—Si—C1115.01 (7)C5—C1—H1105.9
C22—Si—C1111.95 (6)Si—C1—H1105.9
C16—Si—C3115.92 (7)C12—C11—C10121.27 (16)
C22—Si—C3112.55 (6)C12—C11—H11119.4
C1—Si—C390.68 (7)C10—C11—H11119.4
C23—C22—C27116.69 (12)C13—C14—C15120.22 (16)
C23—C22—Si120.54 (10)C13—C14—H14119.9
C27—C22—Si122.74 (10)C15—C14—H14119.9
C26—C27—C22121.44 (14)C24—C25—C26119.82 (14)
C26—C27—H27119.3C24—C25—H25120.1
C22—C27—H27119.3C26—C25—H25120.1
C21—C16—C17116.86 (13)C31—C32—C33120.45 (18)
C21—C16—Si122.66 (11)C31—C32—H32119.8
C17—C16—Si120.40 (11)C33—C32—H32119.8
C24—C23—C22121.81 (14)C28—C3—C4117.49 (13)
C24—C23—H23119.1C28—C3—Si120.72 (10)
C22—C23—H23119.1C4—C3—Si98.12 (9)
C25—C24—C23120.00 (14)C28—C3—H3106.4
C25—C24—H24120C4—C3—H3106.4
C23—C24—H24120Si—C3—H3106.4
C29—C28—C33117.05 (16)C7—C6—C5119.5 (2)
C29—C28—C3120.66 (14)C7—C6—H6120.2
C33—C28—C3122.28 (14)C5—C6—H6120.2
C32—C33—C28121.30 (16)C30—C29—C28121.43 (17)
C32—C33—H33119.4C30—C29—H29119.3
C28—C33—H33119.4C28—C29—H29119.3
C6—C5—C4119.79 (16)C19—C20—C21120.38 (16)
C6—C5—C1124.81 (16)C19—C20—H20C119.8
C4—C5—C1115.26 (13)C21—C20—H20C119.8
C11—C10—C15116.65 (15)C7—C8—C9120.65 (19)
C11—C10—C1120.53 (14)C7—C8—H8119.7
C15—C10—C1122.82 (13)C9—C8—H8119.7
C20—C21—C16121.40 (15)C32—C31—C30119.43 (18)
C20—C21—H21119.3C32—C31—H31120.3
C16—C21—H21119.3C30—C31—H31120.3
C27—C26—C25120.24 (14)C19—C18—C17119.97 (16)
C27—C26—H26119.9C19—C18—H18120
C25—C26—H26119.9C17—C18—H18120
C9—C4—C5119.66 (16)C12—C13—C14119.35 (17)
C9—C4—C3124.98 (16)C12—C13—H13120.3
C5—C4—C3115.24 (13)C14—C13—H13120.3
C18—C17—C16121.58 (15)C31—C30—C29120.33 (18)
C18—C17—H17119.2C31—C30—H30119.8
C16—C17—H17119.2C29—C30—H30119.8
C14—C15—C10121.75 (15)C8—C9—C4119.7 (2)
C14—C15—H15119.1C8—C9—H9120.2
C10—C15—H15119.1C4—C9—H9120.2
C20—C19—C18119.79 (16)C8—C7—C6120.68 (19)
C20—C19—H19120.1C8—C7—H7119.7
C18—C19—H19120.1C6—C7—H7119.7
C10—C1—C5116.53 (12)C13—C12—C11120.75 (17)
C10—C1—Si122.88 (10)C13—C12—H12119.6
C5—C1—Si98.27 (10)C11—C12—H12119.6
 

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