organic compounds
4-Nitro-1-[(trimethylsilyl)ethynyl]benzene: low-temperature polymorph at 100 K†
aDepartment of Chemistry, Louisiana State University, Baton Rouge, LA 70803-1804, USA
*Correspondence e-mail: ffroncz@lsu.edu
The title compound, C11H13NO2Si, is a low-temperature form of the previously reported room-temperature structure [Garcia et al. (1998). Acta Cryst. C54, 489–491]. At 298 K, the material crystallizes in the Pnma and occupies a crystallographic mirror plane, but at 100 K the changes to P212121, the volume decreases by 5% and the molecule distorts. The greatest molecular distortions from Cs symmetry are rotations of the trimethylsilyl and nitro groups by 10.56 (8) and 11.47 (9)°, respectively, to the benzene mean plane. At low temperature, the crystal also becomes an the refined ratio of the twin components being 0.35 (15):0.65 (15).
Related literature
For the synthesis of the title compound, see: Takahashi et al. (1980). For the of the room temperature form of the title compound, see: Garcia et al. (1998). For a description of the Cambridge Structural Database, see: Allen (2002). For Hooft analysis of Bijvoet pairs, see: Hooft et al. (2008).
Experimental
Crystal data
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Data collection: COLLECT (Nonius, 2000); cell DENZO and SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO and SCALEPACK; program(s) used to solve structure: SIR2002 (Burla et al., 2003); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).
Supporting information
10.1107/S1600536812034034/su2491sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536812034034/su2491Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536812034034/su2491Isup3.cml
The compound was prepared by palladium(II) coupling of trimethylsilylacetylene with 4-nitroiodobenzene as described by (Takahashi et al., 1980).
Analysis of 1953 Bijvoet pairs yields a Hooft (Hooft et al., 2008) parameter y = 0.42 (6) and P3(rac-twin) = 1.000. The model was therefore refined as an
(SHELXL commands TWIN and BASF) giving the refined ratio 0.35 (15):0.65 (15) for the twin components. The C-bound H atoms were placed in calculated positions, guided by difference maps, and treated as riding atoms: C—H = 0.95 and 0.98 Å for CH(aromatic) and CH3 H atoms, respectively, with Uiso = k × Ueq(C), where k = 1.5 for CH3 H atoms and = 1.2 for other H atoms. A torsional parameter was refined for each methyl group.Data collection: COLLECT (Nonius, 2000); cell
DENZO and SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO and SCALEPACK (Otwinowski & Minor, 1997); program(s) used to solve structure: SIR2002 (Burla et al., 2003); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).Fig. 1. View of the molecular structure of the title compound, with atom numbering. The displacement ellipsoids are drawn at the 50% probability level. |
C11H13NO2Si | F(000) = 464 |
Mr = 219.31 | Dx = 1.209 Mg m−3 |
Orthorhombic, P212121 | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: P 2ac 2ab | Cell parameters from 2709 reflections |
a = 10.222 (2) Å | θ = 2.5–34.3° |
b = 7.128 (2) Å | µ = 0.18 mm−1 |
c = 16.537 (4) Å | T = 100 K |
V = 1204.9 (5) Å3 | Needle fragment, yellow |
Z = 4 | 0.20 × 0.15 × 0.12 mm |
Nonius KappaCCD diffractometer | 4690 independent reflections |
Radiation source: sealed tube | 3538 reflections with I > 2σ(I) |
Horizonally mounted graphite crystal monochromator | Rint = 0.032 |
Detector resolution: 9 pixels mm-1 | θmax = 33.8°, θmin = 3.1° |
ω and ϕ scans | h = −15→15 |
Absorption correction: multi-scan (SCALEPACK; Otwinowski & Minor, 1997) | k = −11→11 |
Tmin = 0.966, Tmax = 0.979 | l = −25→25 |
17805 measured reflections |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.051 | H-atom parameters constrained |
wR(F2) = 0.123 | w = 1/[σ2(Fo2) + (0.046P)2 + 0.4973P] where P = (Fo2 + 2Fc2)/3 |
S = 1.02 | (Δ/σ)max < 0.001 |
4690 reflections | Δρmax = 0.36 e Å−3 |
139 parameters | Δρmin = −0.32 e Å−3 |
0 restraints | Absolute structure: Flack (1983), 1953 Bijvoet pairs |
0 constraints | Absolute structure parameter: 0.35 (15) |
Primary atom site location: structure-invariant direct methods |
C11H13NO2Si | V = 1204.9 (5) Å3 |
Mr = 219.31 | Z = 4 |
Orthorhombic, P212121 | Mo Kα radiation |
a = 10.222 (2) Å | µ = 0.18 mm−1 |
b = 7.128 (2) Å | T = 100 K |
c = 16.537 (4) Å | 0.20 × 0.15 × 0.12 mm |
Nonius KappaCCD diffractometer | 4690 independent reflections |
Absorption correction: multi-scan (SCALEPACK; Otwinowski & Minor, 1997) | 3538 reflections with I > 2σ(I) |
Tmin = 0.966, Tmax = 0.979 | Rint = 0.032 |
17805 measured reflections |
R[F2 > 2σ(F2)] = 0.051 | H-atom parameters constrained |
wR(F2) = 0.123 | Δρmax = 0.36 e Å−3 |
S = 1.02 | Δρmin = −0.32 e Å−3 |
4690 reflections | Absolute structure: Flack (1983), 1953 Bijvoet pairs |
139 parameters | Absolute structure parameter: 0.35 (15) |
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. |
x | y | z | Uiso*/Ueq | ||
C1 | 0.67962 (16) | 0.2773 (3) | 0.66604 (9) | 0.0270 (3) | |
C2 | 0.77829 (16) | 0.2789 (3) | 0.70632 (9) | 0.0252 (3) | |
C3 | 0.89002 (14) | 0.2769 (3) | 0.75911 (9) | 0.0218 (3) | |
C4 | 1.01780 (16) | 0.2851 (3) | 0.72849 (9) | 0.0262 (3) | |
H4 | 1.0316 | 0.2956 | 0.6719 | 0.031* | |
C5 | 1.12430 (15) | 0.2779 (3) | 0.78050 (10) | 0.0265 (3) | |
H5 | 1.2111 | 0.2842 | 0.7602 | 0.032* | |
C6 | 1.10107 (14) | 0.2614 (3) | 0.86239 (9) | 0.0234 (3) | |
C7 | 0.97590 (14) | 0.2541 (3) | 0.89480 (9) | 0.0242 (3) | |
H7 | 0.9629 | 0.2433 | 0.9515 | 0.029* | |
C8 | 0.87080 (14) | 0.2629 (3) | 0.84253 (9) | 0.0225 (3) | |
H8 | 0.7843 | 0.2594 | 0.8635 | 0.027* | |
C9 | 0.5612 (2) | 0.2384 (5) | 0.50094 (10) | 0.0415 (5) | |
H9A | 0.6112 | 0.1226 | 0.4926 | 0.062* | |
H9B | 0.6129 | 0.3459 | 0.4825 | 0.062* | |
H9C | 0.4794 | 0.2322 | 0.4702 | 0.062* | |
C10 | 0.4263 (2) | 0.0658 (3) | 0.64911 (14) | 0.0376 (5) | |
H10A | 0.4097 | 0.0836 | 0.707 | 0.056* | |
H10B | 0.475 | −0.0512 | 0.6409 | 0.056* | |
H10C | 0.3429 | 0.0593 | 0.6201 | 0.056* | |
C10B | 0.4280 (2) | 0.4829 (3) | 0.62787 (15) | 0.0394 (5) | |
H10D | 0.477 | 0.5912 | 0.6075 | 0.059* | |
H10E | 0.4124 | 0.4982 | 0.686 | 0.059* | |
H10F | 0.3439 | 0.4742 | 0.5996 | 0.059* | |
N1 | 1.21298 (13) | 0.2499 (3) | 0.91772 (9) | 0.0345 (3) | |
O1 | 1.32160 (13) | 0.2830 (3) | 0.89090 (11) | 0.0531 (4) | |
O2 | 1.19270 (16) | 0.2043 (4) | 0.98780 (9) | 0.0670 (7) | |
Si1 | 0.52365 (4) | 0.26554 (7) | 0.61012 (3) | 0.02349 (11) |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.0248 (7) | 0.0341 (10) | 0.0221 (7) | 0.0007 (8) | −0.0007 (6) | −0.0014 (7) |
C2 | 0.0248 (7) | 0.0291 (9) | 0.0219 (6) | 0.0008 (7) | −0.0009 (5) | −0.0006 (7) |
C3 | 0.0208 (6) | 0.0240 (8) | 0.0207 (6) | 0.0008 (7) | −0.0020 (5) | 0.0005 (6) |
C4 | 0.0247 (7) | 0.0345 (9) | 0.0194 (6) | 0.0007 (8) | 0.0022 (6) | 0.0026 (6) |
C5 | 0.0189 (6) | 0.0334 (10) | 0.0270 (7) | −0.0001 (7) | 0.0027 (5) | 0.0008 (8) |
C6 | 0.0183 (6) | 0.0274 (9) | 0.0245 (6) | 0.0001 (8) | −0.0048 (5) | −0.0022 (8) |
C7 | 0.0223 (6) | 0.0311 (8) | 0.0192 (5) | 0.0013 (8) | −0.0001 (5) | −0.0013 (7) |
C8 | 0.0177 (6) | 0.0285 (9) | 0.0212 (6) | −0.0005 (7) | 0.0001 (5) | −0.0016 (7) |
C9 | 0.0392 (9) | 0.0626 (15) | 0.0228 (7) | −0.0031 (12) | −0.0018 (7) | −0.0023 (10) |
C10 | 0.0296 (10) | 0.0364 (12) | 0.0467 (12) | 0.0002 (8) | 0.0011 (9) | 0.0090 (9) |
C10B | 0.0310 (10) | 0.0343 (11) | 0.0530 (13) | 0.0074 (8) | −0.0112 (10) | −0.0091 (9) |
N1 | 0.0235 (6) | 0.0442 (10) | 0.0357 (7) | 0.0034 (8) | −0.0094 (6) | −0.0075 (9) |
O1 | 0.0217 (6) | 0.0733 (12) | 0.0641 (10) | −0.0078 (7) | −0.0111 (7) | 0.0065 (11) |
O2 | 0.0388 (8) | 0.136 (2) | 0.0264 (7) | 0.0166 (12) | −0.0122 (6) | −0.0023 (10) |
Si1 | 0.02129 (18) | 0.0293 (2) | 0.01984 (18) | 0.00030 (19) | −0.00383 (15) | −0.00043 (19) |
C1—C2 | 1.209 (2) | C9—Si1 | 1.8560 (18) |
C1—Si1 | 1.8450 (17) | C9—H9A | 0.98 |
C2—C3 | 1.438 (2) | C9—H9B | 0.98 |
C3—C8 | 1.397 (2) | C9—H9C | 0.98 |
C3—C4 | 1.402 (2) | C10—Si1 | 1.853 (2) |
C4—C5 | 1.388 (2) | C10—H10A | 0.98 |
C4—H4 | 0.95 | C10—H10B | 0.98 |
C5—C6 | 1.380 (2) | C10—H10C | 0.98 |
C5—H5 | 0.95 | C10B—Si1 | 1.856 (2) |
C6—C7 | 1.388 (2) | C10B—H10D | 0.98 |
C6—N1 | 1.4671 (19) | C10B—H10E | 0.98 |
C7—C8 | 1.380 (2) | C10B—H10F | 0.98 |
C7—H7 | 0.95 | N1—O1 | 1.219 (2) |
C8—H8 | 0.95 | N1—O2 | 1.221 (2) |
C2—C1—Si1 | 176.09 (16) | H9A—C9—H9C | 109.5 |
C1—C2—C3 | 175.90 (18) | H9B—C9—H9C | 109.5 |
C8—C3—C4 | 119.38 (13) | Si1—C10—H10A | 109.5 |
C8—C3—C2 | 119.25 (14) | Si1—C10—H10B | 109.5 |
C4—C3—C2 | 121.36 (14) | H10A—C10—H10B | 109.5 |
C5—C4—C3 | 120.35 (14) | Si1—C10—H10C | 109.5 |
C5—C4—H4 | 119.8 | H10A—C10—H10C | 109.5 |
C3—C4—H4 | 119.8 | H10B—C10—H10C | 109.5 |
C6—C5—C4 | 118.44 (14) | Si1—C10B—H10D | 109.5 |
C6—C5—H5 | 120.8 | Si1—C10B—H10E | 109.5 |
C4—C5—H5 | 120.8 | H10D—C10B—H10E | 109.5 |
C5—C6—C7 | 122.73 (14) | Si1—C10B—H10F | 109.5 |
C5—C6—N1 | 118.86 (13) | H10D—C10B—H10F | 109.5 |
C7—C6—N1 | 118.42 (14) | H10E—C10B—H10F | 109.5 |
C8—C7—C6 | 118.29 (13) | O1—N1—O2 | 123.47 (16) |
C8—C7—H7 | 120.9 | O1—N1—C6 | 118.21 (16) |
C6—C7—H7 | 120.9 | O2—N1—C6 | 118.31 (15) |
C7—C8—C3 | 120.81 (13) | C1—Si1—C10 | 108.92 (10) |
C7—C8—H8 | 119.6 | C1—Si1—C10B | 109.77 (10) |
C3—C8—H8 | 119.6 | C10—Si1—C10B | 107.68 (10) |
Si1—C9—H9A | 109.5 | C1—Si1—C9 | 108.27 (8) |
Si1—C9—H9B | 109.5 | C10—Si1—C9 | 111.68 (12) |
H9A—C9—H9B | 109.5 | C10B—Si1—C9 | 110.51 (12) |
Si1—C9—H9C | 109.5 | ||
C8—C3—C4—C5 | 0.5 (3) | C6—C7—C8—C3 | 0.6 (3) |
C2—C3—C4—C5 | −178.28 (19) | C4—C3—C8—C7 | −1.0 (3) |
C3—C4—C5—C6 | 0.4 (3) | C2—C3—C8—C7 | 177.76 (18) |
C4—C5—C6—C7 | −0.9 (3) | C5—C6—N1—O1 | 10.6 (3) |
C4—C5—C6—N1 | 178.80 (18) | C7—C6—N1—O1 | −169.7 (2) |
C5—C6—C7—C8 | 0.3 (3) | C5—C6—N1—O2 | −168.0 (2) |
N1—C6—C7—C8 | −179.33 (18) | C7—C6—N1—O2 | 11.7 (3) |
Experimental details
Crystal data | |
Chemical formula | C11H13NO2Si |
Mr | 219.31 |
Crystal system, space group | Orthorhombic, P212121 |
Temperature (K) | 100 |
a, b, c (Å) | 10.222 (2), 7.128 (2), 16.537 (4) |
V (Å3) | 1204.9 (5) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.18 |
Crystal size (mm) | 0.20 × 0.15 × 0.12 |
Data collection | |
Diffractometer | Nonius KappaCCD diffractometer |
Absorption correction | Multi-scan (SCALEPACK; Otwinowski & Minor, 1997) |
Tmin, Tmax | 0.966, 0.979 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 17805, 4690, 3538 |
Rint | 0.032 |
(sin θ/λ)max (Å−1) | 0.782 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.051, 0.123, 1.02 |
No. of reflections | 4690 |
No. of parameters | 139 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.36, −0.32 |
Absolute structure | Flack (1983), 1953 Bijvoet pairs |
Absolute structure parameter | 0.35 (15) |
Computer programs: COLLECT (Nonius, 2000), DENZO and SCALEPACK (Otwinowski & Minor, 1997), SIR2002 (Burla et al., 2003), SHELXL97 (Sheldrick, 2008), ORTEP-3 for Windows (Farrugia, 1997), WinGX (Farrugia, 1999).
Footnotes
†CAS 75867-38-8.
Acknowledgements
Purchase of the diffractometer was made possible by grant No. LEQSF(1999–2000)-ESH-TR-13, administered by the Louisiana Board of Regents.
References
Allen, F. H. (2002). Acta Cryst. B58, 380–388. Web of Science CrossRef CAS IUCr Journals Google Scholar
Burla, M. C., Camalli, M., Carrozzini, B., Cascarano, G. L., Giacovazzo, C., Polidori, G. & Spagna, R. (2003). J. Appl. Cryst. 36, 1103. CrossRef IUCr Journals Google Scholar
Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565. CrossRef IUCr Journals Google Scholar
Farrugia, L. J. (1999). J. Appl. Cryst. 32, 837–838. CrossRef CAS IUCr Journals Google Scholar
Flack, H. D. (1983). Acta Cryst. A39, 876–881. CrossRef CAS Web of Science IUCr Journals Google Scholar
Garcia, J. G., Asfaw, B., Rodriguez, A. & Fronczek, F. R. (1998). Acta Cryst. C54, 489–491. Web of Science CSD CrossRef CAS IUCr Journals Google Scholar
Hooft, R. W. W., Straver, L. H. & Spek, A. L. (2008). J. Appl. Cryst. 41, 96–103. Web of Science CrossRef CAS IUCr Journals Google Scholar
Nonius (2000). COLLECT. Nonius BV, Delft, The Netherlands. Google Scholar
Otwinowski, Z. & Minor, W. (1997). Methods in Enzymology, Vol. 276, Macromolecular Crystallography, Part A, edited by C. W. Carter Jr & R. M. Sweet, pp. 307–326. New York: Academic Press. Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Takahashi, S., Kuroyama, Y., Sonogashira, K. & Hagihara, N. (1980). Synthesis, 8, 627–630. CrossRef Google Scholar
This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
At 298 K title molecule has Cs symmetry (Garcia et al., 1998; CSD refcode NILWIO; Allen, 2002), with all but two methyl groups lying in the mirror plane. When the temperature is reduced to 100 K, the inversion center vanishes and the space group changes from Pnma to P212121, the unit cell volume is reduced from 1261.8 (3) to 1204.9 (5) Å3, and the molecular symmetry is reduced to C1. The mean plane of the six benzene C atoms, (mean deviation δr.m.s. = 0.004 Å), is normal to the b axis at 298 K but inclines +4.51 (8)° from normal at 100 K, while the C1—Si1—C9 plane is rotated off-normal by -6.05 (8)° and the NO2 group is rotated off-normal by +15.78 (9)°.
Other geometrical parameters in the two polymorphs are similar, for example [those at 298 K are in parentheses] : C1≡C2 = 1.209 (2) [1.199 (4)] Å, Si1—C1 = 1.845 (2) [1.839 (3)] Å, Si1—C9 = 1.856 (2) [1.831 (4)] Å, Si1—C10 = 1.853 (2) [1.838 (3)] Å, Si1—C10B = 1.856 (2)[1.838 (3)] Å, N1—O1 = 1.219 (2) [1.201 (4)] Å, N1—O2 = 1.221 (2) [1.175 (4)] Å, Si1—C1≡C2 = 176.1 (2) [177.9 (3)]°, C1≡C2—C3 = 175.9 (2) [178.0 (3)]°, O1—N1—O2 = 123.5 (2) [122.9 (3)]°.