PM10 


Polymer Melts: From Molecular Rheology to Processing


Mobility of polymer-tethered nanoparticles in unentangled polymer melts


October 16, 2018 (Tuesday) 3:45


Track 2 / Plaza I

(Click on name to view author profile)

  1. Ge, Ting (Duke University, Mechanical Engineering and Materials Science)
  2. Rubinstein, Michael (Duke University, Mechanical Engineering and Materials Science)

(in printed abstract book)
Ting Ge and Michael Rubinstein
Mechanical Engineering and Materials Science, Duke University, Durham, NC 27710


Ge, Ting


A scaling theory is developed for the motion of a polymer-tethered NP in an unentangled polymer melt. Both NPs tethered with a single polymer chain (tail) and with multiple chains (tails) are studied. For a single-tail NP in a polymer melt, we identify two types of scaling regimes, particle-dominated and tail-dominated regimes, depending on the NP diameter d and the size of the tail R_tail. In a particle-dominated regime, the single-tail NP motion is dominated by the bare NP, as the friction coefficient of the tail is lower than that of the less mobile particle. In a tail-dominated regime, the single-tail NP motion is dominated by the tail when the tail friction coefficient surpasses that of the particle at time scales above a crossover time. A multi-tail NP in an unentangled polymer melt is studied by considering a corresponding star polymer in the same melt. For loosely grafted tails, the boundary separating the tail-dominated and particle-dominated regions in the (d, R_tail) parameter space is similar to but shifted with respect to that for a single-tail NP. In each tail-dominated regime, the crossover time is smaller than its counterpart for a single-tail NP, resulting from enhanced effects of the multiple tails. For densely grafted tails, a multi-tail NP diffuses through the polymer melt with the hydrodynamic radius equal to the radius of the corresponding star polymer.