An introduction to the mechanics of fluids - download pdf or read online

By Edwin Henry Barton

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20, which is expressed in terms of the kinematic viscosity, where both absolute viscosity and density are a function of temperature. 21). For additional data, Reid also provides an extensive list of most available experimental data for the viscosity of various fluids, along with techniques to approximate viscosity for different conditions or materials if only one value of density or viscosity is available. 42) where μL (centipoise) is the required liquid viscosity at TL (°F), and μK is a known viscosity at TK.

In particular, changes in density and viscosity affect the Reynold’s number and predicted pressure drops in pipes. 12. Fig. 13 provide more detailed data on water, where the specific gravity of water varies slightly depending on the reference temperature. Additional density data on petroleum products is available in the work of Crane [21], and both Reid [47] and Perry [48] provide techniques for estimating unknown densities for many fluids. 14). 6 Aluminum tube (ASTM B429/B 429M-06 [42], reprinted with permission of ASTM International, 100 Bar Harbor Drive, West Conshohocken, Pa, 19428) in Fig.

3 Laminar Flow in Newtonian and NonNewtonian Fluids Darby [35] provides derivations for numerous closed form laminar and turbulent flow equations for different fluids with detailed examples. Of these fluids, Newtonian fluids are the most common and will be the focus of most of this text, but water hammer equations are just as valid for these other fluids, and non-Newtonian fluids are also briefly considered in this text. For various fluids in laminar flow, flow rates are related to shear stresses, t, and strain rates, g� ¢, which are described using Figs.

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An introduction to the mechanics of fluids by Edwin Henry Barton


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