A new concept, named ''molecular curvature friction'', is presented as
a tool to describe the collective dynamic interaction of a dense visc
oelastic medium (polymer melt or network) with a reference flexible li
near chain. The reptation-in-a-tube model is used as a platform to int
roduce the new effect. The corrected molecular friction coefficient an
d the longest relaxation time increase exponentially with the chain le
ngth. In the short-to-intermediate range of lengths of entangled chain
s (which seems to comprise the longest tested chains reported in the l
iterature) the interplay of the new contribution with chain end effect
s (exemplified here by the contour length fluctuation), gives an appar
ent power law scaling of the longest relaxation time as a 3.3 to 3.6 p
ower of the chain length. In the same range the two effects result in
an apparent power law scaling of the self-diffusion coefficient as a -
2.1 to -2.3 power of the chain length. Three sets of experimental data
on longest relaxation time, self-diffusion coefficient and zero shear
-rate viscosity were very well fitted by the respective new expression
s.