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BAKER HUGHES - Drilling Fluids Reference Manual

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Hydraulics<br />

Newtonian Fluid Model<br />

The Newtonian Fluid Model is the basis from which other fluid models are developed. The flow<br />

behavior of Newtonian fluids has been discussed and it can be seen from this equation that the shear<br />

stress-shear rate relationship is given by:<br />

where,<br />

τ<br />

=<br />

( μ) ( γ)<br />

τ = shear stress<br />

μ = viscosity<br />

γ = shear rate<br />

At a constant temperature, the shear stress and shear rate are directly proportional. The<br />

proportionality constant is the viscosity (μ).<br />

Figure 1-7 illustrates the flow curve of a Newtonian fluid. Note that the flow curve is a straight line<br />

which passes through the origin (0, 0) and the slope of the line is the viscosity (μ).<br />

Figure 1-7<br />

Bingham Plastic Model<br />

Flow Curve for a Newtonian Fluid<br />

In the early 1900s, E.C. Bingham first recognized that some fluids exhibited a plastic behavior,<br />

distinguished from Newtonian fluids, in that they require a yield stress to initiate flow. No bulk<br />

movement of the fluid occurs until the applied force exceeds the yield stress. The yield stress is<br />

commonly referred to as the Yield Point. The shear stress / shear rate relationship for the Bingham<br />

Plastic Model is given by:<br />

where,<br />

τ = τ o<br />

+ ( μ<br />

∞ )γ) (<br />

τ = shear stress<br />

τ o = yield point<br />

μ ∞ = Plastic viscosity<br />

γ = shear rate.<br />

<strong>Reference</strong> <strong>Manual</strong><br />

Baker Hughes <strong>Drilling</strong> <strong>Fluids</strong><br />

1-12 Revised 2006

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