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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Apr 29;67(Pt 5):o1234. doi: 10.1107/S1600536811014863

2,2,4,4-Tetra­phenyl-1,3-bis­(3,3,5,5-tetra­methyl-1,1-diphenyl-5-vinyl­trisilox­an-1-yl)­cyclo­disilazane

Zhen Lv a, Lina Dai a, Xuezhong Zhang a, Zhijie Zhang a,*, Zemin Xie a
PMCID: PMC3089304  PMID: 21754530

Abstract

The title mol­ecule, C60H70N2O4Si8, lies on an inversion center. In the asymmetric unit, one of the phenyl rings is disordered over two sets of sites with refined occupancies 0.58 (2) and 0.42 (2). In addition, in two substitution sites of the terminal dimeth­yl(vin­yl)silyl unit, a methyl group and the vinyl group are disordered over the same site with refined occupancies 0.523 (13) and 0.477 (13).

Related literature

For similar cyclo­disilaza­nes to the title compound and their synthesis, see: Zhu et al. (2007 ▶).graphic file with name e-67-o1234-scheme1.jpg

Experimental

Crystal data

  • C60H70N2O4Si8

  • M r = 1107.90

  • Triclinic, Inline graphic

  • a = 10.731 (2) Å

  • b = 11.021 (2) Å

  • c = 13.859 (3) Å

  • α = 88.320 (9)°

  • β = 76.120 (6)°

  • γ = 78.860 (8)°

  • V = 1561.0 (6) Å3

  • Z = 1

  • Mo Kα radiation

  • μ = 0.22 mm−1

  • T = 173 K

  • 0.41 × 0.28 × 0.22 mm

Data collection

  • Rigaku Saturn724+ CCD diffractometer

  • Absorption correction: multi-scan (CrystalClear; Rigaku, 2007 ▶) T min = 0.916, T max = 0.954

  • 12950 measured reflections

  • 6338 independent reflections

  • 5389 reflections with I > 2σ(I)

  • R int = 0.040

Refinement

  • R[F 2 > 2σ(F 2)] = 0.072

  • wR(F 2) = 0.169

  • S = 1.11

  • 6338 reflections

  • 390 parameters

  • 74 restraints

  • H-atom parameters constrained

  • Δρmax = 0.55 e Å−3

  • Δρmin = −0.32 e Å−3

Data collection: CrystalClear (Rigaku, 2007 ▶); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811014863/lh5235sup1.cif

e-67-o1234-sup1.cif (40.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811014863/lh5235Isup2.hkl

e-67-o1234-Isup2.hkl (310.2KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Acknowledgments

The authors would like to thank the National Natural Science Foundation of China (grant No. 50803070) for financial support.

supplementary crystallographic information

Comment

Organocyclodisilazanes exhibit high thermal stability, and have been used to enhance the thermal properties of silicone rubbers (Zhu et al., 2007). Different functional groups can be introduced to cyclodisilazanes to improve their reactivity.

The molecular structure of the title compound is shown in Fig. 1. The molecule lies on an inversion center. In the asymmetric unit, one of the phenyl rings is disordered over two sets of sites with refined occupancies 0.58 (2) and 0.42 (2). In addition, in the the terminal dimethyl(vinyl)silyl group one of the methyl groups and the vinyl group are disordered over their respective sites with refined occupancies 0.523 (13) and 0.477 (13).

Experimental

The reaction scheme is shown in Fig. 2. 2 g 1,3-bis-(hydroxydiphenylsilanyl)-2,2,4,4-tetraphenylcyclodisilazane was dissolved in 20 ml tetrahydrofuran and added dropwisely to 2 ml n-butyllithum (2.5 mol/L solution in n-hexane) at 263K, then warmed to room temperature. An excessive amount of 1-vinyl-3-chloro-1,1,3,3-tetramethyldisiloxane was added to the mixture. After stirring for 30 min, solvents and unreacted disiloxane were removed under reduced pressure. The crude product was recrystallized from n-hexane to give colorless crystal.

Refinement

All H atoms were located in difference maps but were constrained in a riding-model approximation with Uiso(H) = 1.2Ueq(Caryl) or Uiso(H) = 1.5Ueq(Cmethyl). C—H distances were constrained to 0.95 and 0.98 Å for aryl and methyl H atoms respectively.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound shown with 30% ellipsoids. H atoms are not shown (symmetry code: (A) -x+1, -y+1, -z+1). The disorder is not shown.

Fig. 2.

Fig. 2.

The synthesis of the title compound.

Crystal data

C60H70N2O4Si8 Z = 1
Mr = 1107.90 F(000) = 588
Triclinic, P1 Dx = 1.179 Mg m−3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 10.731 (2) Å Cell parameters from 4640 reflections
b = 11.021 (2) Å θ = 1.5–26.4°
c = 13.859 (3) Å µ = 0.22 mm−1
α = 88.320 (9)° T = 173 K
β = 76.120 (6)° Block, colorless
γ = 78.860 (8)° 0.41 × 0.28 × 0.22 mm
V = 1561.0 (6) Å3

Data collection

Rigaku Saturn724+ CCD diffractometer 6338 independent reflections
Radiation source: sealed tube 5389 reflections with I > 2σ(I)
graphite Rint = 0.040
ω scans at fixed χ = 45° θmax = 26.4°, θmin = 2.4°
Absorption correction: multi-scan (CrystalClear; Rigaku, 2007) h = −13→13
Tmin = 0.916, Tmax = 0.954 k = −13→13
12950 measured reflections l = −17→17

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.072 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.169 H-atom parameters constrained
S = 1.11 w = 1/[σ2(Fo2) + (0.0572P)2 + 1.4799P] where P = (Fo2 + 2Fc2)/3
6338 reflections (Δ/σ)max = 0.001
390 parameters Δρmax = 0.55 e Å−3
74 restraints Δρmin = −0.32 e Å−3

Special details

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)

x y z Uiso*/Ueq Occ. (<1)
Si1 0.25363 (13) 0.87059 (11) 0.07043 (8) 0.0648 (3)
Si2 0.35367 (9) 0.85862 (8) 0.26534 (7) 0.0431 (2)
Si3 0.44457 (8) 0.58120 (7) 0.30819 (6) 0.0318 (2)
Si4 0.49207 (8) 0.61058 (7) 0.52203 (6) 0.0325 (2)
O1 0.3102 (4) 0.8299 (3) 0.1668 (2) 0.0902 (11)
O2 0.3845 (2) 0.72946 (19) 0.32207 (15) 0.0411 (5)
N1 0.4736 (2) 0.5313 (2) 0.42053 (17) 0.0314 (5)
C4 0.3722 (5) 0.7923 (5) −0.0386 (3) 0.0848 (15)
H4A 0.3830 0.7025 −0.0303 0.127*
H4B 0.4565 0.8174 −0.0451 0.127*
H4C 0.3402 0.8151 −0.0984 0.127*
C5 0.2206 (6) 0.9597 (5) 0.3495 (4) 0.111 (2)
H5A 0.1435 0.9209 0.3658 0.167*
H5B 0.1995 1.0389 0.3175 0.167*
H5C 0.2471 0.9737 0.4105 0.167*
C6 0.5004 (6) 0.9265 (6) 0.2308 (5) 0.125 (3)
H6A 0.5695 0.8703 0.1848 0.187*
H6B 0.5300 0.9400 0.2906 0.187*
H6C 0.4803 1.0058 0.1985 0.187*
C7 0.3206 (3) 0.5015 (3) 0.2770 (2) 0.0361 (6)
C8 0.3566 (3) 0.3802 (3) 0.2406 (2) 0.0452 (8)
H8A 0.4461 0.3409 0.2266 0.054*
C9 0.2644 (4) 0.3153 (4) 0.2242 (3) 0.0568 (9)
H9A 0.2910 0.2322 0.2002 0.068*
C10 0.1356 (4) 0.3712 (4) 0.2427 (3) 0.0636 (11)
H10A 0.0727 0.3266 0.2315 0.076*
C11 0.0964 (4) 0.4913 (4) 0.2774 (3) 0.0625 (11)
H11A 0.0068 0.5301 0.2895 0.075*
C12 0.1883 (3) 0.5556 (4) 0.2945 (3) 0.0500 (8)
H12A 0.1604 0.6386 0.3188 0.060*
C13 0.5940 (3) 0.5541 (3) 0.2047 (2) 0.0390 (7)
C14 0.7229 (9) 0.5085 (12) 0.2155 (7) 0.046 (2) 0.58 (2)
H14 0.7364 0.4915 0.2802 0.055* 0.58 (2)
C15 0.8279 (8) 0.4885 (15) 0.1357 (6) 0.060 (3) 0.58 (2)
H15 0.9133 0.4631 0.1462 0.072* 0.58 (2)
C16 0.8121 (10) 0.5046 (13) 0.0405 (8) 0.054 (2) 0.58 (2)
H16 0.8851 0.4852 −0.0147 0.064* 0.58 (2)
C14' 0.7159 (15) 0.5652 (18) 0.2198 (11) 0.056 (4) 0.42 (2)
H14' 0.7247 0.5753 0.2856 0.067* 0.42 (2)
C15' 0.8242 (12) 0.562 (2) 0.1404 (9) 0.065 (4) 0.42 (2)
H15' 0.9082 0.5607 0.1520 0.078* 0.42 (2)
C16' 0.8082 (16) 0.5605 (18) 0.0437 (12) 0.061 (4) 0.42 (2)
H16' 0.8796 0.5671 −0.0107 0.073* 0.42 (2)
C17 0.6879 (4) 0.5495 (4) 0.0261 (3) 0.0604 (10)
H17A 0.6763 0.5714 −0.0384 0.072*
C18 0.5815 (3) 0.5621 (3) 0.1065 (2) 0.0489 (8)
H18A 0.4963 0.5769 0.0947 0.059*
C19 0.3401 (3) 0.7168 (3) 0.5883 (2) 0.0379 (7)
C20 0.2205 (3) 0.7236 (3) 0.5635 (2) 0.0455 (8)
H20A 0.2164 0.6758 0.5088 0.055*
C21 0.1073 (4) 0.7988 (3) 0.6170 (3) 0.0542 (9)
H21A 0.0269 0.8016 0.5988 0.065*
C22 0.1108 (4) 0.8692 (3) 0.6962 (3) 0.0571 (10)
H22A 0.0331 0.9202 0.7328 0.069*
C23 0.2274 (4) 0.8653 (3) 0.7220 (3) 0.0596 (10)
H23A 0.2301 0.9137 0.7768 0.072*
C24 0.3415 (4) 0.7910 (3) 0.6683 (3) 0.0488 (8)
H24A 0.4218 0.7906 0.6861 0.059*
C25 0.6302 (3) 0.6964 (3) 0.4937 (2) 0.0396 (7)
C26 0.6095 (4) 0.8199 (4) 0.4685 (3) 0.0632 (11)
H26A 0.5233 0.8626 0.4695 0.076*
C27 0.7126 (5) 0.8820 (4) 0.4419 (4) 0.0888 (16)
H27A 0.6965 0.9666 0.4244 0.107*
C28 0.8367 (5) 0.8235 (5) 0.4405 (4) 0.0767 (13)
H28A 0.9069 0.8670 0.4216 0.092*
C29 0.8607 (4) 0.7013 (4) 0.4664 (3) 0.0577 (10)
H29A 0.9470 0.6603 0.4667 0.069*
C30 0.7575 (3) 0.6387 (3) 0.4920 (2) 0.0475 (8)
H30A 0.7745 0.5539 0.5088 0.057*
C1 0.0010 (15) 0.8122 (14) 0.1453 (11) 0.143 (6) 0.523 (13)
H1A 0.0172 0.7954 0.2092 0.172* 0.523 (13)
H1B −0.0805 0.8042 0.1331 0.172* 0.523 (13)
C2 0.0907 (15) 0.8463 (12) 0.0740 (10) 0.088 (4) 0.523 (13)
H2 0.0658 0.8610 0.0127 0.105* 0.523 (13)
C3 0.2438 (10) 1.0414 (7) 0.0555 (6) 0.047 (2) 0.523 (13)
H3A 0.1811 1.0851 0.1130 0.071* 0.523 (13)
H3B 0.2151 1.0672 −0.0053 0.071* 0.523 (13)
H3C 0.3302 1.0613 0.0509 0.071* 0.523 (13)
C1' 0.269 (2) 1.105 (2) 0.0102 (17) 0.202 (11) 0.477 (13)
H1'1 0.3555 1.0657 −0.0206 0.242* 0.477 (13)
H1'2 0.2415 1.1916 0.0029 0.242* 0.477 (13)
C2' 0.187 (2) 1.041 (2) 0.0620 (16) 0.147 (9) 0.477 (13)
H2' 0.0998 1.0778 0.0937 0.177* 0.477 (13)
C3' 0.1027 (19) 0.797 (2) 0.0976 (15) 0.122 (7) 0.477 (13)
H3'1 0.0388 0.8382 0.1558 0.183* 0.477 (13)
H3'2 0.1276 0.7090 0.1111 0.183* 0.477 (13)
H3'3 0.0638 0.8060 0.0400 0.183* 0.477 (13)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Si1 0.0854 (9) 0.0687 (7) 0.0447 (6) −0.0075 (6) −0.0297 (6) 0.0025 (5)
Si2 0.0505 (5) 0.0395 (5) 0.0392 (5) −0.0033 (4) −0.0152 (4) 0.0057 (4)
Si3 0.0321 (4) 0.0377 (4) 0.0253 (4) −0.0043 (3) −0.0083 (3) 0.0021 (3)
Si4 0.0369 (4) 0.0349 (4) 0.0267 (4) −0.0082 (3) −0.0087 (3) 0.0027 (3)
O1 0.164 (3) 0.0658 (19) 0.0599 (19) −0.024 (2) −0.064 (2) 0.0151 (15)
O2 0.0486 (13) 0.0378 (12) 0.0338 (11) −0.0020 (9) −0.0093 (9) 0.0046 (9)
N1 0.0355 (13) 0.0341 (13) 0.0264 (12) −0.0079 (10) −0.0098 (10) 0.0009 (9)
C4 0.109 (4) 0.082 (3) 0.053 (3) 0.007 (3) −0.022 (3) 0.007 (2)
C5 0.144 (5) 0.077 (3) 0.071 (3) 0.053 (3) −0.005 (3) 0.006 (3)
C6 0.106 (4) 0.127 (5) 0.170 (6) −0.065 (4) −0.064 (4) 0.101 (5)
C7 0.0369 (16) 0.0471 (18) 0.0243 (14) −0.0078 (13) −0.0077 (12) 0.0034 (12)
C8 0.051 (2) 0.052 (2) 0.0345 (16) −0.0103 (15) −0.0155 (14) 0.0023 (14)
C9 0.076 (3) 0.053 (2) 0.049 (2) −0.0226 (19) −0.0210 (19) −0.0023 (16)
C10 0.068 (3) 0.089 (3) 0.050 (2) −0.045 (2) −0.0208 (19) 0.007 (2)
C11 0.039 (2) 0.094 (3) 0.058 (2) −0.018 (2) −0.0143 (17) −0.003 (2)
C12 0.0349 (17) 0.062 (2) 0.053 (2) −0.0062 (15) −0.0121 (15) −0.0067 (16)
C13 0.0381 (17) 0.0496 (18) 0.0278 (15) −0.0054 (14) −0.0076 (12) 0.0044 (13)
C14 0.032 (3) 0.067 (6) 0.037 (4) −0.010 (4) −0.009 (3) 0.011 (4)
C15 0.034 (3) 0.095 (7) 0.048 (4) −0.011 (4) −0.007 (3) 0.009 (4)
C16 0.040 (4) 0.071 (6) 0.042 (4) −0.012 (4) 0.005 (3) 0.006 (5)
C14' 0.049 (5) 0.076 (8) 0.035 (5) 0.003 (6) −0.010 (4) −0.003 (6)
C15' 0.045 (5) 0.098 (9) 0.053 (5) −0.019 (6) −0.012 (4) 0.007 (6)
C16' 0.058 (6) 0.072 (8) 0.044 (5) −0.008 (6) −0.002 (4) 0.010 (6)
C17 0.050 (2) 0.101 (3) 0.0295 (17) −0.017 (2) −0.0073 (15) 0.0096 (18)
C18 0.0416 (18) 0.072 (2) 0.0311 (16) −0.0078 (16) −0.0085 (14) 0.0045 (15)
C19 0.0443 (17) 0.0364 (16) 0.0327 (15) −0.0079 (13) −0.0086 (13) 0.0032 (12)
C20 0.0467 (19) 0.0465 (19) 0.0401 (18) −0.0099 (15) −0.0024 (14) −0.0070 (14)
C21 0.0421 (19) 0.060 (2) 0.055 (2) −0.0064 (16) −0.0035 (16) −0.0028 (17)
C22 0.057 (2) 0.047 (2) 0.051 (2) 0.0069 (17) 0.0053 (17) −0.0043 (16)
C23 0.078 (3) 0.047 (2) 0.045 (2) 0.0090 (18) −0.0144 (19) −0.0126 (16)
C24 0.060 (2) 0.0404 (18) 0.0448 (19) 0.0044 (15) −0.0214 (16) −0.0045 (14)
C25 0.0485 (18) 0.0440 (18) 0.0308 (15) −0.0164 (14) −0.0124 (13) 0.0038 (12)
C26 0.066 (3) 0.057 (2) 0.077 (3) −0.0246 (19) −0.029 (2) 0.024 (2)
C27 0.087 (4) 0.066 (3) 0.130 (5) −0.043 (3) −0.041 (3) 0.046 (3)
C28 0.073 (3) 0.082 (3) 0.089 (3) −0.052 (3) −0.019 (2) 0.017 (3)
C29 0.046 (2) 0.076 (3) 0.053 (2) −0.0228 (18) −0.0060 (16) −0.0019 (19)
C30 0.0470 (19) 0.054 (2) 0.0413 (18) −0.0131 (15) −0.0065 (15) −0.0004 (15)
C1 0.144 (10) 0.154 (10) 0.133 (9) −0.024 (8) −0.039 (8) 0.000 (7)
C2 0.099 (7) 0.080 (7) 0.089 (7) −0.026 (6) −0.026 (6) 0.003 (6)
C3 0.063 (5) 0.039 (4) 0.042 (4) −0.001 (3) −0.025 (3) 0.009 (3)
C1' 0.222 (14) 0.194 (13) 0.196 (14) −0.045 (9) −0.055 (9) −0.013 (9)
C2' 0.146 (12) 0.171 (12) 0.129 (11) −0.044 (9) −0.027 (8) −0.016 (8)
C3' 0.118 (10) 0.127 (11) 0.119 (10) −0.028 (8) −0.025 (8) 0.018 (8)

Geometric parameters (Å, °)

Si1—O1 1.613 (3) C16—C17 1.389 (12)
Si1—C2 1.808 (15) C16—H16 0.9500
Si1—C4 1.837 (5) C14'—C15' 1.392 (19)
Si1—C3 1.874 (8) C14'—H14' 0.9500
Si1—C2' 1.89 (2) C15'—C16' 1.39 (2)
Si1—C3' 1.90 (2) C15'—H15' 0.9500
Si2—O1 1.603 (3) C16'—C17 1.398 (18)
Si2—O2 1.622 (2) C16'—H16' 0.9500
Si2—C5 1.817 (5) C17—C18 1.379 (5)
Si2—C6 1.828 (5) C17—H17A 0.9500
Si3—O2 1.635 (2) C18—H18A 0.9500
Si3—N1 1.715 (2) C19—C20 1.394 (5)
Si3—C13 1.859 (3) C19—C24 1.402 (4)
Si3—C7 1.865 (3) C20—C21 1.388 (5)
Si4—N1 1.748 (2) C20—H20A 0.9500
Si4—N1i 1.749 (2) C21—C22 1.374 (5)
Si4—C19 1.865 (3) C21—H21A 0.9500
Si4—C25 1.867 (3) C22—C23 1.374 (6)
Si4—Si4i 2.4940 (17) C22—H22A 0.9500
N1—Si4i 1.749 (2) C23—C24 1.391 (5)
C4—H4A 0.9800 C23—H23A 0.9500
C4—H4B 0.9800 C24—H24A 0.9500
C4—H4C 0.9800 C25—C26 1.385 (5)
C5—H5A 0.9800 C25—C30 1.386 (5)
C5—H5B 0.9800 C26—C27 1.382 (6)
C5—H5C 0.9800 C26—H26A 0.9500
C6—H6A 0.9800 C27—C28 1.360 (6)
C6—H6B 0.9800 C27—H27A 0.9500
C6—H6C 0.9800 C28—C29 1.375 (6)
C7—C8 1.393 (4) C28—H28A 0.9500
C7—C12 1.395 (4) C29—C30 1.386 (5)
C8—C9 1.390 (5) C29—H29A 0.9500
C8—H8A 0.9500 C30—H30A 0.9500
C9—C10 1.367 (6) C1—C2 1.306 (9)
C9—H9A 0.9500 C1—H1A 0.9500
C10—C11 1.373 (6) C1—H1B 0.9500
C10—H10A 0.9500 C2—H2 0.9500
C11—C12 1.388 (5) C3—H3A 0.9800
C11—H11A 0.9500 C3—H3B 0.9800
C12—H12A 0.9500 C3—H3C 0.9800
C13—C18 1.397 (4) C1'—C2' 1.298 (10)
C13—C14' 1.402 (17) C1'—H1'1 0.9500
C13—C14 1.419 (11) C1'—H1'2 0.9500
C14—C15 1.365 (12) C2'—H2' 0.9500
C14—H14 0.9500 C3'—H3'1 0.9800
C15—C16 1.372 (14) C3'—H3'2 0.9800
C15—H15 0.9500 C3'—H3'3 0.9800
O1—Si1—C2 116.9 (5) C13—C14—H14 119.1
O1—Si1—C4 107.6 (2) C14—C15—C16 121.1 (8)
C2—Si1—C4 110.8 (5) C14—C15—H15 119.5
O1—Si1—C3 108.2 (3) C16—C15—H15 119.5
C2—Si1—C3 104.9 (5) C15—C16—C17 119.0 (8)
C4—Si1—C3 108.1 (3) C15—C16—H16 120.5
O1—Si1—C2' 115.7 (7) C17—C16—H16 120.5
C2—Si1—C2' 86.9 (8) C15'—C14'—C13 121.2 (12)
C4—Si1—C2' 118.0 (7) C15'—C14'—H14' 119.4
C3—Si1—C2' 18.1 (7) C13—C14'—H14' 119.4
O1—Si1—C3' 100.8 (6) C14'—C15'—C16' 119.3 (13)
C2—Si1—C3' 19.4 (7) C14'—C15'—H15' 120.4
C4—Si1—C3' 108.9 (7) C16'—C15'—H15' 120.4
C3—Si1—C3' 122.4 (7) C15'—C16'—C17 120.5 (12)
C2'—Si1—C3' 104.3 (8) C15'—C16'—H16' 119.7
O1—Si2—O2 108.31 (14) C17—C16'—H16' 119.7
O1—Si2—C5 110.3 (2) C18—C17—C16 119.3 (5)
O2—Si2—C5 107.30 (19) C18—C17—C16' 117.6 (7)
O1—Si2—C6 109.3 (3) C16—C17—C16' 25.4 (6)
O2—Si2—C6 109.92 (19) C18—C17—H17A 120.4
C5—Si2—C6 111.7 (3) C16—C17—H17A 120.4
O2—Si3—N1 106.34 (11) C16'—C17—H17A 115.8
O2—Si3—C13 109.79 (13) C17—C18—C13 122.6 (3)
N1—Si3—C13 113.21 (13) C17—C18—H18A 118.7
O2—Si3—C7 108.97 (13) C13—C18—H18A 118.7
N1—Si3—C7 109.71 (12) C20—C19—C24 117.1 (3)
C13—Si3—C7 108.74 (14) C20—C19—Si4 122.4 (2)
N1—Si4—N1i 89.00 (11) C24—C19—Si4 120.5 (2)
N1—Si4—C19 114.02 (13) C21—C20—C19 121.4 (3)
N1i—Si4—C19 114.79 (12) C21—C20—H20A 119.3
N1—Si4—C25 114.72 (13) C19—C20—H20A 119.3
N1i—Si4—C25 114.17 (13) C22—C21—C20 120.4 (4)
C19—Si4—C25 109.14 (14) C22—C21—H21A 119.8
N1—Si4—Si4i 44.52 (8) C20—C21—H21A 119.8
N1i—Si4—Si4i 44.48 (8) C23—C22—C21 119.6 (3)
C19—Si4—Si4i 125.40 (11) C23—C22—H22A 120.2
C25—Si4—Si4i 125.46 (11) C21—C22—H22A 120.2
Si2—O1—Si1 153.0 (2) C22—C23—C24 120.4 (3)
Si2—O2—Si3 145.38 (14) C22—C23—H23A 119.8
Si3—N1—Si4 131.82 (15) C24—C23—H23A 119.8
Si3—N1—Si4i 137.03 (14) C23—C24—C19 121.1 (3)
Si4—N1—Si4i 91.00 (11) C23—C24—H24A 119.5
Si1—C4—H4A 109.5 C19—C24—H24A 119.5
Si1—C4—H4B 109.5 C26—C25—C30 117.3 (3)
H4A—C4—H4B 109.5 C26—C25—Si4 120.6 (3)
Si1—C4—H4C 109.5 C30—C25—Si4 122.0 (2)
H4A—C4—H4C 109.5 C27—C26—C25 120.9 (4)
H4B—C4—H4C 109.5 C27—C26—H26A 119.6
Si2—C5—H5A 109.5 C25—C26—H26A 119.6
Si2—C5—H5B 109.5 C28—C27—C26 120.8 (4)
H5A—C5—H5B 109.5 C28—C27—H27A 119.6
Si2—C5—H5C 109.5 C26—C27—H27A 119.6
H5A—C5—H5C 109.5 C27—C28—C29 120.0 (4)
H5B—C5—H5C 109.5 C27—C28—H28A 120.0
Si2—C6—H6A 109.5 C29—C28—H28A 120.0
Si2—C6—H6B 109.5 C28—C29—C30 119.2 (4)
H6A—C6—H6B 109.5 C28—C29—H29A 120.4
Si2—C6—H6C 109.5 C30—C29—H29A 120.4
H6A—C6—H6C 109.5 C29—C30—C25 121.8 (3)
H6B—C6—H6C 109.5 C29—C30—H30A 119.1
C8—C7—C12 117.0 (3) C25—C30—H30A 119.1
C8—C7—Si3 120.2 (2) C2—C1—H1A 120.0
C12—C7—Si3 122.7 (2) C2—C1—H1B 120.0
C9—C8—C7 121.4 (3) H1A—C1—H1B 120.0
C9—C8—H8A 119.3 C1—C2—Si1 131.9 (13)
C7—C8—H8A 119.3 C1—C2—H2 114.1
C10—C9—C8 119.9 (4) Si1—C2—H2 114.1
C10—C9—H9A 120.0 Si1—C3—H3A 109.5
C8—C9—H9A 120.0 Si1—C3—H3B 109.5
C9—C10—C11 120.4 (3) H3A—C3—H3B 109.5
C9—C10—H10A 119.8 Si1—C3—H3C 109.5
C11—C10—H10A 119.8 H3A—C3—H3C 109.5
C10—C11—C12 119.6 (4) H3B—C3—H3C 109.5
C10—C11—H11A 120.2 C2'—C1'—H1'1 120.0
C12—C11—H11A 120.2 C2'—C1'—H1'2 120.0
C11—C12—C7 121.6 (4) H1'1—C1'—H1'2 120.0
C11—C12—H12A 119.2 C1'—C2'—Si1 116 (2)
C7—C12—H12A 119.2 C1'—C2'—H2' 122.1
C18—C13—C14' 116.4 (7) Si1—C2'—H2' 122.1
C18—C13—C14 114.9 (5) Si1—C3'—H3'1 109.5
C14'—C13—C14 25.3 (6) Si1—C3'—H3'2 109.5
C18—C13—Si3 119.4 (2) H3'1—C3'—H3'2 109.5
C14'—C13—Si3 121.1 (6) Si1—C3'—H3'3 109.5
C14—C13—Si3 125.1 (4) H3'1—C3'—H3'3 109.5
C15—C14—C13 121.9 (8) H3'2—C3'—H3'3 109.5
C15—C14—H14 119.1
O2—Si2—O1—Si1 171.8 (6) C14—C13—C14'—C15' 82 (2)
C5—Si2—O1—Si1 54.7 (7) Si3—C13—C14'—C15' −171.0 (9)
C6—Si2—O1—Si1 −68.4 (7) C13—C14'—C15'—C16' 6.8 (19)
C2—Si1—O1—Si2 −108.4 (8) C14'—C15'—C16'—C17 −7(2)
C4—Si1—O1—Si2 126.1 (6) C15—C16—C17—C18 −8.1 (12)
C3—Si1—O1—Si2 9.6 (8) C15—C16—C17—C16' 85 (2)
C2'—Si1—O1—Si2 −8.2 (10) C15'—C16'—C17—C18 11.2 (15)
C3'—Si1—O1—Si2 −119.9 (9) C15'—C16'—C17—C16 −89 (2)
O1—Si2—O2—Si3 36.2 (3) C16—C17—C18—C13 12.4 (9)
C5—Si2—O2—Si3 155.2 (3) C16'—C17—C18—C13 −16.5 (11)
C6—Si2—O2—Si3 −83.2 (4) C14'—C13—C18—C17 16.4 (10)
N1—Si3—O2—Si2 163.1 (2) C14—C13—C18—C17 −11.7 (8)
C13—Si3—O2—Si2 40.3 (3) Si3—C13—C18—C17 176.5 (3)
C7—Si3—O2—Si2 −78.7 (3) N1—Si4—C19—C20 5.1 (3)
O2—Si3—N1—Si4 −19.6 (2) N1i—Si4—C19—C20 −95.6 (3)
C13—Si3—N1—Si4 101.0 (2) C25—Si4—C19—C20 134.8 (3)
C7—Si3—N1—Si4 −137.33 (19) Si4i—Si4—C19—C20 −45.1 (3)
O2—Si3—N1—Si4i 166.09 (19) N1—Si4—C19—C24 −176.9 (2)
C13—Si3—N1—Si4i −73.3 (2) N1i—Si4—C19—C24 82.4 (3)
C7—Si3—N1—Si4i 48.4 (2) C25—Si4—C19—C24 −47.2 (3)
N1i—Si4—N1—Si3 −176.1 (3) Si4i—Si4—C19—C24 132.9 (2)
C19—Si4—N1—Si3 67.1 (2) C24—C19—C20—C21 −1.3 (5)
C25—Si4—N1—Si3 −59.8 (2) Si4—C19—C20—C21 176.8 (3)
Si4i—Si4—N1—Si3 −176.1 (3) C19—C20—C21—C22 0.3 (6)
N1i—Si4—N1—Si4i 0.0 C20—C21—C22—C23 0.3 (6)
C19—Si4—N1—Si4i −116.82 (13) C21—C22—C23—C24 0.2 (6)
C25—Si4—N1—Si4i 116.28 (14) C22—C23—C24—C19 −1.3 (6)
O2—Si3—C7—C8 166.1 (2) C20—C19—C24—C23 1.8 (5)
N1—Si3—C7—C8 −77.9 (3) Si4—C19—C24—C23 −176.3 (3)
C13—Si3—C7—C8 46.4 (3) N1—Si4—C25—C26 93.3 (3)
O2—Si3—C7—C12 −18.2 (3) N1i—Si4—C25—C26 −166.0 (3)
N1—Si3—C7—C12 97.9 (3) C19—Si4—C25—C26 −36.0 (3)
C13—Si3—C7—C12 −137.8 (3) Si4i—Si4—C25—C26 143.9 (3)
C12—C7—C8—C9 −1.2 (5) N1—Si4—C25—C30 −83.4 (3)
Si3—C7—C8—C9 174.8 (3) N1i—Si4—C25—C30 17.3 (3)
C7—C8—C9—C10 0.9 (5) C19—Si4—C25—C30 147.3 (3)
C8—C9—C10—C11 0.0 (6) Si4i—Si4—C25—C30 −32.9 (3)
C9—C10—C11—C12 −0.6 (6) C30—C25—C26—C27 0.6 (6)
C10—C11—C12—C7 0.3 (6) Si4—C25—C26—C27 −176.3 (4)
C8—C7—C12—C11 0.6 (5) C25—C26—C27—C28 −0.5 (8)
Si3—C7—C12—C11 −175.3 (3) C26—C27—C28—C29 −0.4 (8)
O2—Si3—C13—C18 −76.5 (3) C27—C28—C29—C30 1.1 (7)
N1—Si3—C13—C18 164.8 (3) C28—C29—C30—C25 −1.0 (6)
C7—Si3—C13—C18 42.6 (3) C26—C25—C30—C29 0.1 (5)
O2—Si3—C13—C14' 82.7 (10) Si4—C25—C30—C29 176.9 (3)
N1—Si3—C13—C14' −36.0 (10) O1—Si1—C2—C1 8.0 (18)
C7—Si3—C13—C14' −158.2 (10) C4—Si1—C2—C1 131.8 (15)
O2—Si3—C13—C14 112.6 (7) C3—Si1—C2—C1 −111.8 (16)
N1—Si3—C13—C14 −6.0 (7) C2'—Si1—C2—C1 −109.3 (17)
C7—Si3—C13—C14 −128.3 (7) C3'—Si1—C2—C1 44 (3)
C18—C13—C14—C15 7.4 (10) O1—Si1—C2'—C1' 94.4 (19)
C14'—C13—C14—C15 −92 (2) C2—Si1—C2'—C1' −147 (2)
Si3—C13—C14—C15 178.7 (7) C4—Si1—C2'—C1' −35 (2)
C13—C14—C15—C16 −4.1 (14) C3—Si1—C2'—C1' 25.3 (18)
C14—C15—C16—C17 4.2 (14) C3'—Si1—C2'—C1' −155.9 (19)
C18—C13—C14'—C15' −11.2 (15)

Symmetry codes: (i) −x+1, −y+1, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: LH5235).

References

  1. Rigaku (2007). CrystalClear Rigaku Corporation, Tokyo, Japan.
  2. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  3. Zhu, Y. P., Guo, L., Zhang, Z. J., Xie, Z. M. & Xu, C. H. (2007). J. Appl. Polym. Sci. 105, 749–756.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811014863/lh5235sup1.cif

e-67-o1234-sup1.cif (40.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811014863/lh5235Isup2.hkl

e-67-o1234-Isup2.hkl (310.2KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

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