By Raymond Mulley

ISBN-10: 0849327679

ISBN-13: 9780849327674

ISBN-10: 1420038281

ISBN-13: 9781420038286

Presents perception to the elemental conception and equations of fluid move. Emphasizes sensible difficulties and comprises precious appendices.

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**Extra resources for flow of industrial fluids**

**Example text**

It should be noticed that the profile is uniformly smooth. Distortion of the profile will give numbers that cannot easily be used in a correlation. 14 Flow of Industrial Fluids-Theory and Equations Flow of Incompressible Fluids C H A P T E R O N E Figure 1-8. Average, maximum and point velocities U Developing profile U Developed profile Figure 1-9. Developing profile Figure 1-9 shows a profile that may not be fully developed for about thirty pipe diameters. Devices such as orifice plates, which infer flow rates from differential pressure, are subject to profile limitations.

Conservation o f energy The first law of thermodynamics deals with the conservation of energy. It cannot be bypassed. It applies to all systems, reversible and irreversible. For open (flowing), steady state systems, 18 Flow of Industrial Fluids-Theory and Equations Flow o f Incompressible Fluids C H A P T E R O N E the first law is expressed in two forms. The second form is the integrated form that is more useful when relationships already developed have to be applied in practice. Both forms will be put on a per-unit-mass basis.

The irreversibility is generally the unavoidable flow of heat energy generated by turbulence to a lower temperature sink, either in the environment or in the same flowing fluid-There is no practical way of recovering this incremental internal energy as mechanical energy. Flow of a fluid through a horizontal duct of constant cross section is always associated with a pressure drop. "Ideal" flow would not require adding energy to maintain itself. Once established, flow would continue without external help.

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