We have simulated the motion of a bead subjected to a constant force while
embedded in a network of semiflexible polymers which can represent actin
filaments. We find that the bead displacement obeys the power law x ~ t^alfa.
After the initial stage characterized by the exponent alfa=0.75 we find a new
regime with alfa=0.5. The response in this regime is linear in force and scales
with the polymer concentration as c^(-1.4). We find that the polymers pile up
ahead of the moving bead, while behind it the polymer density is reduced. We
show that the force resisting the bead motion is due to steric repulsion
exerted by the polymers on the front hemisphere of the bead.Comment: 35 pages with 10 figure