The crystal structure of syndiotactic 1,2-poly(E-3-methyl-1,3-pentadiene) has been determined by the combination of X-ray diffraction and molecular mechanics. Energy minimizations performed by various potential functions yielded models of crystal structure with calculated X-ray powder profiles similar to the experimental profiles. The best model has been refined in order to fit all the experimental data. The space group is Pcam, and the parameters of the unit cell are a = 15.4 angstrom, b = 7.45 angstrom, and c = 5.15 angstrom. Similarities and differences with the crystal structures of syndiotactic 1;2-poly(1,3-butadiene), syndiotactic 3,4-poly(2-methyl-1;3-butadiene), and syndiotactic 1,2-poly(E-1,3-pentadiene) are discussed

Determination of the Crystal Structure of Syndiotactic 1,2-Poly(E-3-Methyl-1,3-Pentadiene) by X-ray Diffraction and Molecular Mechanics

Ricci G
2007

Abstract

The crystal structure of syndiotactic 1,2-poly(E-3-methyl-1,3-pentadiene) has been determined by the combination of X-ray diffraction and molecular mechanics. Energy minimizations performed by various potential functions yielded models of crystal structure with calculated X-ray powder profiles similar to the experimental profiles. The best model has been refined in order to fit all the experimental data. The space group is Pcam, and the parameters of the unit cell are a = 15.4 angstrom, b = 7.45 angstrom, and c = 5.15 angstrom. Similarities and differences with the crystal structures of syndiotactic 1;2-poly(1,3-butadiene), syndiotactic 3,4-poly(2-methyl-1;3-butadiene), and syndiotactic 1,2-poly(E-1,3-pentadiene) are discussed
2007
Istituto per lo Studio delle Macromolecole - ISMAC - Sede Milano
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/29953
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