PIE plo = mole fraction of component I = characteristic time of flow process = characteristic or natural time of fluid = viscosity at zero shear rate = final or equilibrium mass density of solvent in = initial mass density of solvent in sample sample In this paper an analysis is made of the hydrodynamic stability of a Boussinesq viscoelastic fluid undergoing plane Couette flow with a superposed temperature gradient. Of special interest is the effect of including the dissipation term in the energy equation. This term is shown to destabilize the fluid for most values of disturbance wave number and material parameters and to cause overstability for all values of the Brinkman number.At a critical Weissenberg number of 1, a rheological instability is developed which is essentially independent of the Reynolds, Prandtl, and Brinkman numbers.
SCOPEOne of the most common and important processing operations in the polymer industry is fiber spinning. This operation is depicted schematically in Figure 1 and consists of many sequential flows, each of which is important in the production of an end product of satisfactory material properties. For the purposes of the research described, the process will be divided heuristically into four regimes:Correspondence concerning this paper should be addressed to Larry V. McIntire.
1.The die entry. Here the polymer melt is forced (by an extruder or other pressure source) from the reservoir into a capillary of very small diameter (relative to reservoir dimensions). The entry flow is very complicated and combines aspects of a complicated shear flow with an accelerated elongational flow.
The capillary.Here an approximation to simple shear flow is developed. Viscous dissipation induced temperature effects may be important.3. Die exit. The complex phenomenon of die swell is encountered in this region.