Literature DB >> 21588764

Tetra-kis(4-tert-butyl-benz-yl)silane.

Lauren E Burnham1, Rulla M Kachlan, Andy A Thomas, Craig A Ogle, Daniel S Jones.   

Abstract

The title compound, C(44)H(60)Si, was prepared as an inter-nal standard for diffusion-ordered NMR spectroscopy. The Si atom lies on a special position with site symmetry.

Entities:  

Year:  2010        PMID: 21588764      PMCID: PMC3007930          DOI: 10.1107/S1600536810034173

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


Related literature

For applications of the title compound in NMR spectroscopy, see: Li et al. (2009 ▶). For similar structures in the same space group, see: Liao et al. (2002 ▶); Laliberté et al. (2004 ▶). For a previously reported NMR standard, see: Monroe et al. (2010 ▶). For a description of the Cambridge Structural Database, see: Allen (2002 ▶).

Experimental

Crystal data

C44H60Si M = 617.01 Tetragonal, a = 17.394 (2) Å c = 6.3613 (6) Å V = 1924.7 (4) Å3 Z = 2 Cu Kα radiation μ = 0.72 mm−1 T = 295 K 0.31 × 0.15 × 0.12 mm

Data collection

Enraf–Nonius CAD-4 diffractometer 5204 measured reflections 1738 independent reflections 1056 reflections with I > 2σ(I) R int = 0.036 3 standard reflections every 113 reflections intensity decay: 2%

Refinement

R[F 2 > 2σ(F 2)] = 0.041 wR(F 2) = 0.135 S = 1.02 1738 reflections 106 parameters H-atom parameters constrained Δρmax = 0.13 e Å−3 Δρmin = −0.11 e Å−3 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: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶) and Mercury (Macrae et al., 2006 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶). Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810034173/su2206sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536810034173/su2206Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C44H60SiDx = 1.065 Mg m3
Mr = 617.01Cu Kα radiation, λ = 1.54184 Å
Tetragonal, P42/nCell parameters from 25 reflections
Hall symbol: -P 4bcθ = 7.8–35.3°
a = 17.394 (2) ŵ = 0.72 mm1
c = 6.3613 (6) ÅT = 295 K
V = 1924.7 (4) Å3Prism, colorless
Z = 20.31 × 0.15 × 0.12 mm
F(000) = 676
Enraf–Nonius CAD-4 diffractometerθmax = 67.4°, θmin = 3.6°
non–profiled ω/2θ scansh = −20→20
5204 measured reflectionsk = −20→15
1738 independent reflectionsl = −7→0
1056 reflections with I > 2σ(I)3 standard reflections every 113 reflections
Rint = 0.036 intensity decay: 2%
Refinement on F2H-atom parameters constrained
Least-squares matrix: fullw = 1/[σ2(Fo2) + (0.0761P)2 + 0.1124P] where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.041(Δ/σ)max < 0.001
wR(F2) = 0.135Δρmax = 0.13 e Å3
S = 1.02Δρmin = −0.11 e Å3
1738 reflectionsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
106 parametersExtinction coefficient: 0.0033 (6)
0 restraints
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.
xyzUiso*/Ueq
Si0.250.250.250.0599 (4)
C40.50538 (12)0.30509 (12)0.4293 (4)0.0780 (7)
H40.52630.28560.55290.094*
C10.33661 (10)0.25820 (11)0.0742 (4)0.0674 (7)
H1A0.35070.20690.02880.081*
H1B0.32170.2868−0.05020.081*
C50.54015 (10)0.36783 (10)0.3360 (3)0.0535 (5)
C70.44050 (11)0.35854 (12)0.0714 (4)0.0668 (6)
H70.41930.3779−0.05190.08*
C80.61357 (11)0.40291 (11)0.4257 (4)0.0624 (6)
C20.40700 (10)0.29575 (10)0.1652 (4)0.0580 (5)
C60.50509 (12)0.39375 (12)0.1556 (4)0.0674 (6)
H60.52550.43650.08760.081*
C30.44105 (12)0.27021 (12)0.3468 (4)0.0837 (8)
H30.420.22810.41630.1*
C90.62982 (15)0.48273 (14)0.3328 (5)0.0951 (9)
H9A0.6340.47890.18270.143*
H9B0.67710.50230.38960.143*
H9C0.58850.5170.36820.143*
C100.68066 (12)0.35026 (15)0.3687 (5)0.0992 (9)
H10A0.6720.30010.42690.149*
H10B0.72750.37110.42490.149*
H10C0.68480.34650.21860.149*
C110.60896 (17)0.41111 (18)0.6619 (5)0.1047 (9)
H11A0.56740.4450.69770.157*
H11B0.65640.4320.7140.157*
H11C0.60020.36160.72410.157*
U11U22U33U12U13U23
Si0.0473 (4)0.0473 (4)0.0852 (9)000
C40.0612 (12)0.0722 (13)0.101 (2)−0.0089 (11)−0.0143 (12)0.0413 (13)
C10.0543 (11)0.0616 (11)0.0863 (18)0.0010 (9)0.0016 (11)0.0004 (11)
C50.0496 (10)0.0501 (10)0.0609 (12)0.0033 (8)0.0116 (10)0.0070 (9)
C70.0658 (12)0.0750 (13)0.0596 (15)−0.0063 (10)0.0042 (10)0.0141 (11)
C80.0584 (11)0.0644 (12)0.0645 (15)−0.0057 (9)0.0067 (10)0.0059 (10)
C20.0477 (10)0.0504 (10)0.0759 (14)0.0042 (8)0.0086 (10)0.0056 (10)
C60.0688 (12)0.0698 (13)0.0638 (14)−0.0169 (10)0.0105 (12)0.0169 (11)
C30.0617 (12)0.0677 (13)0.122 (2)−0.0127 (10)−0.0093 (14)0.0472 (14)
C90.0946 (17)0.0790 (15)0.112 (2)−0.0315 (13)−0.0090 (16)0.0155 (15)
C100.0538 (12)0.111 (2)0.133 (3)0.0025 (13)0.0030 (14)−0.0136 (19)
C110.118 (2)0.120 (2)0.0760 (19)−0.0328 (17)0.0054 (17)−0.0061 (17)
Si—C1i1.882 (2)C8—C111.512 (3)
Si—C1ii1.882 (2)C8—C101.527 (3)
Si—C1iii1.882 (2)C8—C91.535 (3)
Si—C11.882 (2)C2—C31.372 (3)
C4—C31.377 (3)C6—H60.93
C4—C51.382 (3)C3—H30.93
C4—H40.93C9—H9A0.96
C1—C21.504 (3)C9—H9B0.96
C1—H1A0.97C9—H9C0.96
C1—H1B0.97C10—H10A0.96
C5—C61.375 (3)C10—H10B0.96
C5—C81.526 (3)C10—H10C0.96
C7—C21.374 (3)C11—H11A0.96
C7—C61.387 (3)C11—H11B0.96
C7—H70.93C11—H11C0.96
C1i—Si—C1ii110.68 (7)C3—C2—C7116.09 (19)
C1i—Si—C1iii107.08 (14)C3—C2—C1122.34 (18)
C1ii—Si—C1iii110.68 (7)C7—C2—C1121.6 (2)
C1i—Si—C1110.68 (7)C5—C6—C7122.44 (19)
C1ii—Si—C1107.08 (14)C5—C6—H6118.8
C1iii—Si—C1110.68 (7)C7—C6—H6118.8
C3—C4—C5122.7 (2)C2—C3—C4121.94 (19)
C3—C4—H4118.7C2—C3—H3119
C5—C4—H4118.7C4—C3—H3119
C2—C1—Si117.14 (16)C8—C9—H9A109.5
C2—C1—H1A108C8—C9—H9B109.5
Si—C1—H1A108H9A—C9—H9B109.5
C2—C1—H1B108C8—C9—H9C109.5
Si—C1—H1B108H9A—C9—H9C109.5
H1A—C1—H1B107.3H9B—C9—H9C109.5
C6—C5—C4115.05 (19)C8—C10—H10A109.5
C6—C5—C8123.50 (17)C8—C10—H10B109.5
C4—C5—C8121.4 (2)H10A—C10—H10B109.5
C2—C7—C6121.8 (2)C8—C10—H10C109.5
C2—C7—H7119.1H10A—C10—H10C109.5
C6—C7—H7119.1H10B—C10—H10C109.5
C11—C8—C5111.41 (19)C8—C11—H11A109.5
C11—C8—C10109.4 (2)C8—C11—H11B109.5
C5—C8—C10108.13 (17)H11A—C11—H11B109.5
C11—C8—C9107.9 (2)C8—C11—H11C109.5
C5—C8—C9111.83 (18)H11A—C11—H11C109.5
C10—C8—C9108.09 (19)H11B—C11—H11C109.5
  5 in total

1.  The Cambridge Structural Database: a quarter of a million crystal structures and rising.

Authors:  Frank H Allen
Journal:  Acta Crystallogr B       Date:  2002-05-29

2.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

3.  Structure and exchange in silicon-linked tetraradicals.

Authors:  Yi Liao; Martha Baskett; Paul M Lahti; Fernando Palacio
Journal:  Chem Commun (Camb)       Date:  2002-02-07       Impact factor: 6.222

4.  Formula weight prediction by internal reference diffusion-ordered NMR spectroscopy (DOSY).

Authors:  Deyu Li; Gerald Kagan; Russell Hopson; Paul G Williard
Journal:  J Am Chem Soc       Date:  2009-04-22       Impact factor: 15.419

5.  Bis(2-naphthyl-meth-yl)diphenyl-silane.

Authors:  Thomas Blake Monroe; Andy A Thomas; Daniel S Jones; Craig A Ogle
Journal:  Acta Crystallogr Sect E Struct Rep Online       Date:  2009-12-12
  5 in total

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