TY - JOUR
T1 - Determining the Dilution Exponent for Entangled 1,4-Polybutadienes Using Blends of Near-Monodisperse Star with Unentangled, Low Molecular Weight Linear Polymers
AU - Hall, Ryan
AU - Kang, Beom Goo
AU - Lee, Sanghoon
AU - Chang, Taihyun
AU - Venerus, David C.
AU - Hadjichristidis, Nikos
AU - Mays, Jimmy
AU - Larson, Ronald G.
N1 - Publisher Copyright:
© 2019 American Chemical Society.
PY - 2019/2/26
Y1 - 2019/2/26
N2 - We determine experimentally the "dilution exponent" α for entangled polymers from the scaling of terminal crossover frequency with entanglement density from the linear rheology of three 1,4-polybutadiene star polymers that are blended with low-molecular-weight, unentangled linear 1,4-polybutadiene at various star volume fractions, η s . Assuming that the rheology of monodisperse stars depends solely on the plateau modulus G N (η s ) ≈ ηs1+α, the number of entanglements per chain M e (η s ) ≈ ηs-α, and the tube-segment frictional Rouse time τ e (η s ) ≈ ηs-2α, we show that only an α = 1 scaling superposes the M e (η s ) dependence of the terminal crossover frequency ω x,t of the blends with those of pure stars, not α = 4/3. This is the first determination of α for star polymers that does not rely on any particular tube model implementation. We also show that a generalized tube model, the "Hierarchical model", using the "Das" parameter set with α = 1 reasonably predicts the rheological data of the melts and blends featured in this paper.
AB - We determine experimentally the "dilution exponent" α for entangled polymers from the scaling of terminal crossover frequency with entanglement density from the linear rheology of three 1,4-polybutadiene star polymers that are blended with low-molecular-weight, unentangled linear 1,4-polybutadiene at various star volume fractions, η s . Assuming that the rheology of monodisperse stars depends solely on the plateau modulus G N (η s ) ≈ ηs1+α, the number of entanglements per chain M e (η s ) ≈ ηs-α, and the tube-segment frictional Rouse time τ e (η s ) ≈ ηs-2α, we show that only an α = 1 scaling superposes the M e (η s ) dependence of the terminal crossover frequency ω x,t of the blends with those of pure stars, not α = 4/3. This is the first determination of α for star polymers that does not rely on any particular tube model implementation. We also show that a generalized tube model, the "Hierarchical model", using the "Das" parameter set with α = 1 reasonably predicts the rheological data of the melts and blends featured in this paper.
UR - http://www.scopus.com/inward/record.url?scp=85061894337&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85061894337&partnerID=8YFLogxK
U2 - 10.1021/acs.macromol.8b01828
DO - 10.1021/acs.macromol.8b01828
M3 - Article
AN - SCOPUS:85061894337
SN - 0024-9297
VL - 52
SP - 1757
EP - 1771
JO - Macromolecules
JF - Macromolecules
IS - 4
ER -