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BAKER HUGHES - Drilling Fluids Reference Manual

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Hydraulics<br />

Determination of Flow Regime<br />

The experiments conducted by Reynolds, besides naming the behavior of fluid flow, made the most<br />

celebrated application of dimensional analysis in the history of fluid mechanics by introducing the<br />

Reynolds Number (Re).<br />

Reynolds number takes into consideration the basic factors of pipe flow – pipe diameter, average fluid<br />

= V D ρ<br />

μ<br />

velocity, fluid density, and fluid viscosity. Reynolds number is defined as<br />

Re ( )( )( )<br />

where,<br />

V = average fluid velocity<br />

D = pipe diameter<br />

ρ = fluid density<br />

μ= fluid viscosity<br />

Reynolds showed that for smooth, circular pipes, for all Newtonian fluids, and for all pipe, the<br />

transition from laminar to turbulent flow occurs when the Reynolds number has a value of<br />

approximately 2000. However, turbulent flow throughout the fluid occurs when the Reynolds number<br />

is more than 4000.<br />

Therefore, for Newtonian fluids, laminar flow is defined as a Reynolds number of 2000 or less.<br />

Turbulent flow is defined as a Reynolds number of 4000 or greater. Transitional flow is defined when<br />

the Reynolds number is between 2000 and 4000.<br />

As previously shown, the viscosity of non-Newtonian fluids depends upon the relationship between<br />

shear stress and shear rate. Likewise, the value of the Reynolds number at which the transition from<br />

laminar to turbulent flow occurs depends upon the shear stress/shear rate relationship.<br />

The relationship between shear stress and shear rate for non-Newtonian fluids is developed in the<br />

subsection, Mathematical Fluid Models .<br />

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

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

1-10 Revised 2006

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