Sh. Spiegelberg et al., THE ROLE OF END-EFFECTS ON MEASUREMENTS OF EXTENSIONAL VISCOSITY IN FILAMENT STRETCHING RHEOMETERS, Journal of non-Newtonian fluid mechanics, 64(2-3), 1996, pp. 229-267
The transient extensional viscosity function of two semi-dilute polyis
obutylene polymer solutions is investigated in a filament stretching r
heometer of the type developed by Tirtaatmadja and Sridhar (J. Rheol.,
37 (1993) 1081). A velocity compensation algorithm which yields a con
stant deformation rate at a single point in both Newtonian and non-New
tonian fluid samples is detailed. Good experimental reproducibility is
obtained in the device and measurements with a viscous Newtonian oil
yield steady-state Trouton ratios of <(eta)over bar>/mu = 3 +/- 0.5. B
oth viscoelastic fluids show the onset of significant strain-hardening
for Hencky strains greater than two, and transient extensional viscos
ities that increase by three orders of magnitude. Good agreement betwe
en the results for the two different fluids is obtained when tests are
performed at identical values of the Deborah number. The maximum Henc
ky strain achievable in the device is epsilon = 5 and steady-state val
ues of the extensional viscosity are never achieved over the range of
strain rates attainable. Measurements show that the evolution of the t
ensile force exerted by the deforming filament is a strong function of
the initial aspect ratio of the cylindrical test sample. A lubricatio
n analysis for small sample aspect ratios demonstrates that this varia
tion results from large radial pressure gradients arising from the non
-homogeneous shear flow near the rigid disks. This simplified analysis
provides a good description of the experimental observations, and tes
ts conducted with the Newtonian oil suggest that only at Hencky strain
s epsilon > 2 does the extensional deformation of the filament dominat
e the shearing flow. In the case of viscoelastic fluid filaments, the
initial shearing motion near the fixed endplates significantly affects
the measured tensile stress in the filament at all later times in the
extension. Careful attention is focused on the non-homogeneous deform
ation induced at the endplates that constrain the fluid sample at each
end of the test apparatus. Measurements of the filament profile and s
urface curvature with a video-imaging system show distinct differences
in the evolution of Newtonian and non-Newtonian samples. In both case
s, different strain histories are experienced by fluid elements at dif
ferent axial positions in the filament, and a spatially homogenous def
ormation is not achieved in the viscoelastic filaments until Hencky st
rains epsilon > 4 are attained. Observations at larger strains and hig
h Deborah numbers, De > 3, indicate the onset of an elastic instabilit
y near the stationary endplate which results in the deforming fluid co
lumn partially decohering from the endplate.