| Literature DB >> 21588764 |
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
| C44H60Si | |
| Cu | |
| Tetragonal, | Cell parameters from 25 reflections |
| Hall symbol: -P 4bc | θ = 7.8–35.3° |
| µ = 0.72 mm−1 | |
| Prism, colorless | |
| 0.31 × 0.15 × 0.12 mm | |
| Enraf–Nonius CAD-4 diffractometer | θmax = 67.4°, θmin = 3.6° |
| non–profiled ω/2θ scans | |
| 5204 measured reflections | |
| 1738 independent reflections | |
| 1056 reflections with | 3 standard reflections every 113 reflections |
| intensity decay: 2% |
| Refinement on | H-atom parameters constrained |
| Least-squares matrix: full | |
| (Δ/σ)max < 0.001 | |
| Δρmax = 0.13 e Å−3 | |
| Δρmin = −0.11 e Å−3 | |
| 1738 reflections | Extinction correction: |
| 106 parameters | Extinction 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. |
| Si | 0.25 | 0.25 | 0.25 | 0.0599 (4) | |
| C4 | 0.50538 (12) | 0.30509 (12) | 0.4293 (4) | 0.0780 (7) | |
| H4 | 0.5263 | 0.2856 | 0.5529 | 0.094* | |
| C1 | 0.33661 (10) | 0.25820 (11) | 0.0742 (4) | 0.0674 (7) | |
| H1A | 0.3507 | 0.2069 | 0.0288 | 0.081* | |
| H1B | 0.3217 | 0.2868 | −0.0502 | 0.081* | |
| C5 | 0.54015 (10) | 0.36783 (10) | 0.3360 (3) | 0.0535 (5) | |
| C7 | 0.44050 (11) | 0.35854 (12) | 0.0714 (4) | 0.0668 (6) | |
| H7 | 0.4193 | 0.3779 | −0.0519 | 0.08* | |
| C8 | 0.61357 (11) | 0.40291 (11) | 0.4257 (4) | 0.0624 (6) | |
| C2 | 0.40700 (10) | 0.29575 (10) | 0.1652 (4) | 0.0580 (5) | |
| C6 | 0.50509 (12) | 0.39375 (12) | 0.1556 (4) | 0.0674 (6) | |
| H6 | 0.5255 | 0.4365 | 0.0876 | 0.081* | |
| C3 | 0.44105 (12) | 0.27021 (12) | 0.3468 (4) | 0.0837 (8) | |
| H3 | 0.42 | 0.2281 | 0.4163 | 0.1* | |
| C9 | 0.62982 (15) | 0.48273 (14) | 0.3328 (5) | 0.0951 (9) | |
| H9A | 0.634 | 0.4789 | 0.1827 | 0.143* | |
| H9B | 0.6771 | 0.5023 | 0.3896 | 0.143* | |
| H9C | 0.5885 | 0.517 | 0.3682 | 0.143* | |
| C10 | 0.68066 (12) | 0.35026 (15) | 0.3687 (5) | 0.0992 (9) | |
| H10A | 0.672 | 0.3001 | 0.4269 | 0.149* | |
| H10B | 0.7275 | 0.3711 | 0.4249 | 0.149* | |
| H10C | 0.6848 | 0.3465 | 0.2186 | 0.149* | |
| C11 | 0.60896 (17) | 0.41111 (18) | 0.6619 (5) | 0.1047 (9) | |
| H11A | 0.5674 | 0.445 | 0.6977 | 0.157* | |
| H11B | 0.6564 | 0.432 | 0.714 | 0.157* | |
| H11C | 0.6002 | 0.3616 | 0.7241 | 0.157* |
| Si | 0.0473 (4) | 0.0473 (4) | 0.0852 (9) | 0 | 0 | 0 |
| C4 | 0.0612 (12) | 0.0722 (13) | 0.101 (2) | −0.0089 (11) | −0.0143 (12) | 0.0413 (13) |
| C1 | 0.0543 (11) | 0.0616 (11) | 0.0863 (18) | 0.0010 (9) | 0.0016 (11) | 0.0004 (11) |
| C5 | 0.0496 (10) | 0.0501 (10) | 0.0609 (12) | 0.0033 (8) | 0.0116 (10) | 0.0070 (9) |
| C7 | 0.0658 (12) | 0.0750 (13) | 0.0596 (15) | −0.0063 (10) | 0.0042 (10) | 0.0141 (11) |
| C8 | 0.0584 (11) | 0.0644 (12) | 0.0645 (15) | −0.0057 (9) | 0.0067 (10) | 0.0059 (10) |
| C2 | 0.0477 (10) | 0.0504 (10) | 0.0759 (14) | 0.0042 (8) | 0.0086 (10) | 0.0056 (10) |
| C6 | 0.0688 (12) | 0.0698 (13) | 0.0638 (14) | −0.0169 (10) | 0.0105 (12) | 0.0169 (11) |
| C3 | 0.0617 (12) | 0.0677 (13) | 0.122 (2) | −0.0127 (10) | −0.0093 (14) | 0.0472 (14) |
| C9 | 0.0946 (17) | 0.0790 (15) | 0.112 (2) | −0.0315 (13) | −0.0090 (16) | 0.0155 (15) |
| C10 | 0.0538 (12) | 0.111 (2) | 0.133 (3) | 0.0025 (13) | 0.0030 (14) | −0.0136 (19) |
| C11 | 0.118 (2) | 0.120 (2) | 0.0760 (19) | −0.0328 (17) | 0.0054 (17) | −0.0061 (17) |
| Si—C1i | 1.882 (2) | C8—C11 | 1.512 (3) |
| Si—C1ii | 1.882 (2) | C8—C10 | 1.527 (3) |
| Si—C1iii | 1.882 (2) | C8—C9 | 1.535 (3) |
| Si—C1 | 1.882 (2) | C2—C3 | 1.372 (3) |
| C4—C3 | 1.377 (3) | C6—H6 | 0.93 |
| C4—C5 | 1.382 (3) | C3—H3 | 0.93 |
| C4—H4 | 0.93 | C9—H9A | 0.96 |
| C1—C2 | 1.504 (3) | C9—H9B | 0.96 |
| C1—H1A | 0.97 | C9—H9C | 0.96 |
| C1—H1B | 0.97 | C10—H10A | 0.96 |
| C5—C6 | 1.375 (3) | C10—H10B | 0.96 |
| C5—C8 | 1.526 (3) | C10—H10C | 0.96 |
| C7—C2 | 1.374 (3) | C11—H11A | 0.96 |
| C7—C6 | 1.387 (3) | C11—H11B | 0.96 |
| C7—H7 | 0.93 | C11—H11C | 0.96 |
| C1i—Si—C1ii | 110.68 (7) | C3—C2—C7 | 116.09 (19) |
| C1i—Si—C1iii | 107.08 (14) | C3—C2—C1 | 122.34 (18) |
| C1ii—Si—C1iii | 110.68 (7) | C7—C2—C1 | 121.6 (2) |
| C1i—Si—C1 | 110.68 (7) | C5—C6—C7 | 122.44 (19) |
| C1ii—Si—C1 | 107.08 (14) | C5—C6—H6 | 118.8 |
| C1iii—Si—C1 | 110.68 (7) | C7—C6—H6 | 118.8 |
| C3—C4—C5 | 122.7 (2) | C2—C3—C4 | 121.94 (19) |
| C3—C4—H4 | 118.7 | C2—C3—H3 | 119 |
| C5—C4—H4 | 118.7 | C4—C3—H3 | 119 |
| C2—C1—Si | 117.14 (16) | C8—C9—H9A | 109.5 |
| C2—C1—H1A | 108 | C8—C9—H9B | 109.5 |
| Si—C1—H1A | 108 | H9A—C9—H9B | 109.5 |
| C2—C1—H1B | 108 | C8—C9—H9C | 109.5 |
| Si—C1—H1B | 108 | H9A—C9—H9C | 109.5 |
| H1A—C1—H1B | 107.3 | H9B—C9—H9C | 109.5 |
| C6—C5—C4 | 115.05 (19) | C8—C10—H10A | 109.5 |
| C6—C5—C8 | 123.50 (17) | C8—C10—H10B | 109.5 |
| C4—C5—C8 | 121.4 (2) | H10A—C10—H10B | 109.5 |
| C2—C7—C6 | 121.8 (2) | C8—C10—H10C | 109.5 |
| C2—C7—H7 | 119.1 | H10A—C10—H10C | 109.5 |
| C6—C7—H7 | 119.1 | H10B—C10—H10C | 109.5 |
| C11—C8—C5 | 111.41 (19) | C8—C11—H11A | 109.5 |
| C11—C8—C10 | 109.4 (2) | C8—C11—H11B | 109.5 |
| C5—C8—C10 | 108.13 (17) | H11A—C11—H11B | 109.5 |
| C11—C8—C9 | 107.9 (2) | C8—C11—H11C | 109.5 |
| C5—C8—C9 | 111.83 (18) | H11A—C11—H11C | 109.5 |
| C10—C8—C9 | 108.09 (19) | H11B—C11—H11C | 109.5 |