Internal dynamics of flexible polymer
chains is one of the most
important fundamental problems in polymer physics. Although numerous
efforts have been devoted to the understanding of internal dynamics
for linear polymers, little attention was paid to branched systems.
This work aims to elucidate how the branching effect quantitatively
influences the internal motions of long-subchain hyperbranched polymers
in dilute solution. By light scattering study of four hyperbranched
polystyrene samples with controlled branching patterns and low polydispersities
(M
w/M
n <
1.40 and M
w ∼ 107 g/mol),
we quantified and analyzed the asymptotic behavior of the reduced
first cumulant [Γ* = Γ(q)/(q
3
k
B
T/η0)], the value of Γ* at high q-regime
[the approximate values of Γ*(∞)], the scattering vector
(q) dependence of linewidth [Γ(q)], the number of relaxation modes in Γ(q)-distribution
curves, the characteristic relaxation time (τ1) of
the first internal mode, and the q-dependent relative
strength of internal motions. Our results reveal: (i) Γ*(∞)
is not sensitive to the branching density, but more related to the
fractal dimension of a given system; (ii) the asymptotic power law
in the intermediate qR
h regime (1.5 < qR
h < 3.0), compared to Γ*(∞),
is a better indicator, which could reflect the structural details
of different branched systems; (iii) the branching effect could lead
to the suppression of overall internal motions, but the introduction
of moderate branching could enhance the contribution of some energetically
favorable internal modes in linewidth distribution; (iv) by comparing
the experimentally determined and theoretically calculated τ1, the result provides direct experimental evidence supporting
that the classical theory is not applicable to hyperbranched polymer
systems. The present work not only helps clarify some long-standing
controversial issues existed in previous studies, but also provides
useful experimental data for further theoretical calculations of internal
dynamics for branched systems.