MOLECULAR-DYNAMICS SIMULATIONS COMBINED WITH LARGE-ANGLE X-RAY-SCATTERING TECHNIQUE FOR THE DETERMINATION OF THE STRUCTURE, CONFORMATION, AND CONFORMATIONAL DYNAMICS OF POLYPHOSPHAZENES IN AMORPHOUS PHASE - STUDY OF POLY[DI(4-METHYLPHENOXY)PHOSPHAZENE]
R. Caminiti et al., MOLECULAR-DYNAMICS SIMULATIONS COMBINED WITH LARGE-ANGLE X-RAY-SCATTERING TECHNIQUE FOR THE DETERMINATION OF THE STRUCTURE, CONFORMATION, AND CONFORMATIONAL DYNAMICS OF POLYPHOSPHAZENES IN AMORPHOUS PHASE - STUDY OF POLY[DI(4-METHYLPHENOXY)PHOSPHAZENE], Journal of the American Chemical Society, 119(9), 1997, pp. 2196-2204
Suitable parameter sets for the CHARMm force field were derived using
the Dinur-Hagler energy second-derivative procedure, on the basis of S
CF calculations at the 6-31G level, for the uncommon structural units
in poly(phenoxyphosphazenes) [P=N, P-N, P-X (X=aryloxy)]. It is shown
that application of molecular dynamics (MD) simulations, in combinati
on with experimental energy dispersive X-ray diffraction (EDXD) measur
ements, provide unambiguous structural and conformational information
on amorphous polymers. The procedure for the analysis of the EDXD data
involves comparison of computed atom-atom radial distribution functio
n (RDF) curve from MD simulations for the various polymer backbone con
formations, with the RDF obtained from experimental X-ray scattering d
ata. The applicability of this combined experimental/computational met
hodology is illustrated on the amorphous poly[di(4-methylphenoxy)phosp
hazene] (PMPP). The results showed that (i) the backbone conformation
is safely [TC](n) rather than [T3C](n) and (ii) the computed RDFs are
best assessed by using a MD simulation technique that avoids assumptio
n of static chain conformation and the needed best fit of the distance
dependent parameters s(jk). In this method of analysis, the RDF that
to be compared with the experimental one is directly calculated from a
ll microstates collected during the entire simulation period. Validati
on of the polymer model provides a complete picture, otherwise experim
entally inaccessible, of the internal fluctuations of the polymeric ha
ins. The computational protocol delineated for analysis of EDXD data i
s general and its application specifically necessary when highly flexi
ble amorphous polymers are involved.