The motional behavior of complex phthalates and structurally
related liquids has been investigated in order
to study the structural effect of molecular framework on the
macroscopic and microscopic dynamic properties.
13C NMR spin−lattice relaxation times and nuclear
Overhauser enhancements (NOE) of individual carbon
nuclei of bis(2-ethylhexyl) cyclohexane-1,2-dicarboxylate (DEHHP),
bis(2-ethylhexyl) isophthalate (DEHIP),
bis(2-ethylhexyl) terephthalate (DEHTP), and
tris(2-ethylhexyl) trimellitate (TOTM) have been measured
as
a function of temperature from −40 to 90 °C. Individual
13C peaks were unambiguously assigned by using
2D hydrogen−carbon chemical shift correlation spectra. In
addition, the density and viscosity of these
compounds as a function of temperature have been measured. The
results were also compared with those of
2-ethylhexyl benzoate (EHB), 2-ethylhexyl cyclohexanecarboxylate (EHC),
and bis(2-ethylhexyl) phthalate
(DEHP), complex liquids studied earlier in our laboratory. Both
the macroscopic and microscopic dynamic
properties were significantly affected by the structure of the
molecular framework. The conjugation between
a phenyl ring and carboxyl groups was found to make the structural
framework stiffer and resulted in an
enhanced viscosity. The 13C NMR relaxation data were
interpreted in terms of a theoretical model assuming
a Cole−Davidson distribution of correlation times. The internal
motions of the common 2-ethylhexyl side
chains were found to be independent of the nature of the molecular
framework of the compounds. The
parameter β in the Cole−Davidson model, representing the
distribution width of the involved correlation
times of the molecular motions, contained useful information on the
detailed motional features of individual
carbon nuclei. The β values for the rigid phenyl ring carbons
reflected the reorientational anisotropy resulting
from the molecular shape of the structural framework and could be
successfully correlated with the parameter
κ introduced by McClung and Kivelson in the modified
Stokes−Einstein−Debye (SED) equation. On the
other hand, the β values for the flexible cyclohexane ring carbons
were affected by both the internal motion
of the cyclohexane ring and the anisotropy of the molecular
reorientation.