PM9 


Polymer Melts: From Molecular Rheology to Processing


Determining the dilution exponent for 1,4-polybutadienes using blends of entangled monodispersed star with unentangled, low molecular weight linear polymers


October 16, 2018 (Tuesday) 2:45


Track 2 / Plaza I

(Click on name to view author profile)

  1. Hall, Ryan (University of Michigan, Macromolecular Science and Engineering Program)
  2. Kang, Beomgoo (Princeston University, Department of Chemical and Biological Engineering)
  3. Lee, Sanghoon (Pohang University of Science and Technology, Chemistry)
  4. Chang, Taihyun (Pohang University of Science and Technology, Chemistry)
  5. Venerus, David (Illinois Institute of Science and Technology, Chemical and Biological Engineering)
  6. Hadjichristidis, Nikos (King Abdullah University of science and Technology, KAUST, Physical Sciences and Engineering Division)
  7. Mays, Jimmy (University of Tennessee)
  8. Larson, Ronald G. (University of Michigan, Department of Chemical Engineering)

(in printed abstract book)
Ryan Hall1, Beomgoo Kang2, Sanghoon Lee3, Taihyun Chang3, David Venerus4, Nikos Hadjichristidis5, Jimmy Mays2, and Ronald G. Larson6
1Macromolecular Science and Engineering Program, University of Michigan, Ann Arbor, MI 48197; 2University of Tennessee, Knoxville, TN; 3Chemistry, Pohang University of Science and Technology, Pohang, Republic of Korea; 4Chemical and Biological Engineering, Illinois Institute of Science and Technology, Chicago, IL; 5Physical Sciences and Engineering Division, King Abdullah University of science and Technology, KAUST, Thuwal, Saudi Arabia; 6Department of Chemical Engineering, University of Michigan, Ann Arbor, MI


Larson, Ronald G.


We determine experimentally the “dilution exponent” α for entangled polymers from the scaling of terminal time with entanglement density from the linear rheology of three well characterized 1,4-polybutadiene 4-arm star polymers. These stars are blended with low-molecular-weight, unentangled linear 1,4-polybutadiene at various star volume fractions, φs. Assuming only that the rheology of monodisperse stars depends solely on the plateau modulus G0Ns)∝φs1+α; the number of entanglements per chain Mes)∝ φs−α; and the tube-segment frictional Rouse time τes)∝−2α, we show that only an α=1 scaling superposes the Mes)-dependence of the terminal cross-over frequency ωx,t of the blends with those of pure stars, while an order-of-magnitude deviation between these dependencies is found if one takes α=4⁄3. The nearly exponential dependence of ωx,t on Mes) is strong enough to clearly distinguish the value of the dilution exponent α , which is not possible from the weaker dependence of the low-frequency cross-over modulus Gx,t on Mes). We show that this conclusion holds when accounting for experimental uncertainties in arm molecular weights. This is the first clear rheological determination of α that does not rely on the use of any particular tube model, but only on the dependence of rheology on the above three parameters. We also show that a generalized tube model, the “Hierarchical model”, using the “Das” parameter set with α=1 performs reasonably in predicting the terminal and plateau regions of the melts and blends featured here.