The effect of elasticity on the meniscus shape and film thickness for
the free boundary creeping flow created by injecting air to a Hele-Sha
w cell initially filled with a viscoelastic fluid is studied theoretic
ally. The theory is developed with the assumptions that the displaced
viscoelastic fluid wets the walls and that capillary number Ca and the
local Weissenberg number We are both small. The transition region bet
ween the advancing meniscus and the entrained film is where the fluid
theology has its greatest effect. The Oldroyd-B constitutive equation
is used to model the viscoelastic fluid. The theory is formulated as a
double expansion in Ca-1/3 and We/Ca-1/3. According to our asymptotic
analysis, as the fluid becomes more viscoelastic, the film thickness
decreases and the pressure drop at the meniscus tip increases. A detai
led analysis shows that the dominant mechanisms are the resistance to
stream-wise strain, tending to lower the film thickness, and the build
up of shear stress, tending to raise the film thickness, with the form
er being the numerically larger of the two. Our theory leads to the pr
ediction that as viscoelasticity comes to dominate the shear resistanc
e, the film thickness will scale with U-4/3. The effects of shear thin
ning and normal stress thinning are analyzed by adapting an approximat
e model obtained by retaining only the dominant terms in the force bal
ance. Our Hele-Shaw cell theory is extended to dip coating and soap fi
lm forming flows. Our theoretical results pertaining to the effects of
viscoelasticity on the thickness of the film are in qualitative agree
ment with recent experimental data.