Difference between revisions of "Bernoulli's Equation"
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Bernoulli’s theorem is for a frictionless incompressible fluid. However, it can be applied to real incompressible fluids with good results in situations where frictional effects are very small. | Bernoulli’s theorem is for a frictionless incompressible fluid. However, it can be applied to real incompressible fluids with good results in situations where frictional effects are very small. | ||
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| − | + | == References == | |
| + | #ASPE Standard 45 Siphonic Roof Drainage | ||
| + | #FLUID MECHANICS with Engineering Applications p.93 | ||
Revision as of 10:02, 14 February 2017
Common name for the fluid energy equation. An energy balance equation demonstrating the conservation of three major states - static pressure energy, kinetic energy (velocity pressure) and potential energy. Also referred to as Bernoulli’s Principle. Daniel Bernoulli presented the Bernoulli’s theorem in 1738;
(Mathematical Equation to be upload)
Bernoulli’s theorem is for a frictionless incompressible fluid. However, it can be applied to real incompressible fluids with good results in situations where frictional effects are very small.
References
- ASPE Standard 45 Siphonic Roof Drainage
- FLUID MECHANICS with Engineering Applications p.93
