A number of processes for fabricating dense, solid materials begin with a solid powder that is to be fashioned--without melting--into an article with a particular geometric shape. Moreover, it is often the case that the small, discrete particles are dispersed in a continuous liquid phase, such as in ceramic slips, filled molten polymers, as well as suspensions used in some powder metallurgy and composite fabrication processes. Further, in these cases it is often the flow behavior or deformability of the solid-liquid suspension that is of central importance in a particular materials fabrication process, since such operations as mold-filling, pressing, extrusion, transport through pipes and channels, and even some mixing and separation processes, must take advantage of certain of the rheological characteristics of the suspension. In particular, it is the fact that such suspensions possess distinctly fluid-like properties (that is, even though they may contain a significant amount of a non-fluid-like solid phase) which allows them to be deformed. Difficulties arise, of course, as the volume fraction of the dispersed solid phase is increased, since in this case the suspension behaves like a fluid with a viscosity that is significantly higher than that of the liquid alone. For a variety of reasons, of course, it is desirable to use a suspension with a high volume fraction of solids (φs)--such as in shape-forming operations where the goal is to prepare a shaped article with a high solids volume fraction--even though the suspension’s high “viscosity” makes that shape-forming operation more difficult. What is needed, of course, is a detailed, quantitative knowledge of the relationship between φs and the “viscosity” of a given suspension, for a variety of flow conditions, in order to design a shape-forming process, or perhaps to improve an existing one.
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