Structural Characterization of POSS Siloxane Dimer and Trimer

Ion mobility and molecular modeling methods were used to examine the gas-phase conformational properties of POSS (polyhedral oligomeric silsesquioxanes) siloxane oligomers. MALDI generated the sodiated dimers (Cy7T8)2O·Na+ and (Cp7T8)2O·Na+ and the trimer ion [Cy7T8O−Cy8Si8O11−OCy7T8] Na+ (T = SiO1....

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Bibliographic Details
Published inChemistry of materials Vol. 18; no. 6; pp. 1490 - 1497
Main Authors Anderson, Stanley E, Mitchell, Connie, Haddad, Timothy S, Vij, Ashwani, Schwab, Joseph J, Bowers, Michael T
Format Journal Article
LanguageEnglish
Published American Chemical Society 21.03.2006
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Summary:Ion mobility and molecular modeling methods were used to examine the gas-phase conformational properties of POSS (polyhedral oligomeric silsesquioxanes) siloxane oligomers. MALDI generated the sodiated dimers (Cy7T8)2O·Na+ and (Cp7T8)2O·Na+ and the trimer ion [Cy7T8O−Cy8Si8O11−OCy7T8] Na+ (T = SiO1.5, Cy = cyclohexyl, and Cp = cyclopentyl); their collision cross sections were measured in helium using ion mobility based methods. Experimental results are consistent with one observed conformer for each of the dimers and the exo-exo isomer for the trimer (formed by retention of configuration at silicon during synthesis). For the cyclopentyl dimer, theory predicts two separate conformer families based on whether the substituents on the POSS cages are staggered (σcalc = 357 Å2) or eclipsed (σcalc = 365 Å2); experiment fits the staggered conformation best (σexpt = 355 Å2). For the cyclohexyl dimer, on the other hand, folding of the Cy groups seems to be important:  (σexpt = 402 Å2 vs unfolded σcalc = 421 Å2 or partially folded σcalc = 407 Å2). Similar to the Cy dimer, for the trimer theory indicates that a low-energy exo-exo family of structures fits the experimental cross section (σexpt = 557 Å2) only if several Cy groups are folded (σcalc = 557 Å2) as compared to unfolded structures (average σcalc = 570 Å2). Modeling shows the nonbonded interactions of the capping Cp and Cy groups stabilize POSS cage packing leading to compact structures being lowest in energy. Modeling also suggests that two POSS cages bonded together by a single oxygen atom gives a benchmark 8.3−8.5 Å cage−cage center distance which may be used to evaluate cage packing in other POSS oligomers. X-ray crystal structures at 100 and 298 K for (Cy7T8)2O were carried out which show that solid state cage−cage intermolecular distances are perfectly consistent with the modeled POSS−PMA dimer and trimer structures. At room temperature there is considerable unresolved disorder of the cyclohexyl R groups in the X-ray structure due to rapid boat−chair interconversion.
Bibliography:ark:/67375/TPS-DVJN5TJ7-Q
istex:68042A81E0AC5E7D87C53E1B4A5FC1EEEC27E1E7
ISSN:0897-4756
1520-5002
DOI:10.1021/cm052589c