This paper explores rheological characteristics of and molecular
mechanism for a superfluid-like stick−slip transition occurring under controlled pressure in
capillary flow of a series of highly
entangled linear polyethylene (PE) melts and establishes its connection
with the spurt flow phenomenon.
The transition is signified by a large discontinuity in the flow
rate at a critical stress, resulting in a
double value within the flow curve. The magnitude of the
transition can be quantified in terms of an
extrapolation length, b. In particular, the
superfluid-like flow transition occurs throughout a range
of
temperatures from T = 180 to 260 °C as long as a
critical stress, σc, is exceeded. It is found that
σc
increases linearly with T, and b
c at
the transition remains around 1.7 mm at all the temperatures for
the
PE (MH20) of weight-average molecular weight M
w
= 316 600. Thus the observed remarkably large
interfacial slip is believed to be due to complete disentanglement of
the adsorbed chains from free chains
at the melt/wall interface at and beyond the transition. The
amount of wall slip, as described by b,
diminishes quickly with decreasing M
w, in
qualitative agreement with a simple scaling relation for
noninteracting interfaces. The flow transition depends on the
surface condition of the die wall and occurs
at a considerably lower critical stress when the wall is treated by
depositing a fluorocarbon elastomer to
weaken the PE adsorption. Application of both controlled-pressure
and controlled-piston speed conditions
demonstrates that spurt flow instability originates from indeterminacy
of the hydrodynamic boundary
condition at the PE/die wall interfaces.