The size and conformation of a series
of poly(α-olefin) homopolymers
in good solvent conditions were measured by a combination of small-angle
neutron scattering (SANS), triple detector size exclusion chromatography
(SEC), and MD simulations. The bottlebrush samples were prepared via
organometallic coordinative insertion polymerization of 1-alkenes,
with carbon numbers ranging from 6 to 18 carbons. A linear polyolefin,
that is, polypropylene, is included in this study for comparison.
SANS data for all the solutions are well described by the flexible
cylinder model, from which the cylinder radius (R) and the Kuhn length (l
k) are determined.
These two quantities, also calculated by MD simulations, are monotonic
increasing functions of the bottlebrush side chain length (N
sc). The dependences of the hydrodynamic radius
(R
h) and the radius of gyration (R
g) with the molecular weight (M), measured by SEC and MD simulations, are well described by the
power laws, R
h ∼ M
υh
and R
g ∼ M
υg
, respectively.
Intriguingly, υh is a nonmonotonic function of N
sc, whereas υg increases monotonically
with N
sc. We postulate that this is due
to weakening of the intermolecular hydrodynamic interactions as N
sc increases, which also marks a transition
from linear-like (for N
sc < 9) to brush-like
chain architecture (for N
sc > 9). Taking
the R
g data for all the bottlebrush polymers
together, they cannot be described by the Kratky–Porod wormlike
chain model. We propose an empirical parabolic function of the backbone
molecular weight (N
bb) and N
sc that predicts the R
g values
for all the bottlebrushes adequately.