Summarizing Bernoulli’s Equation
Summary
- Bernoulli’s equation states that the sum on each side of the following equation is constant, or the same at any two points in an incompressible frictionless fluid:
\({P}_{1}+\cfrac{1}{2}{\mathrm{\rho v}}_{1}^{2}+\rho {\mathrm{gh}}_{1}={P}_{2}+\cfrac{1}{2}{\mathrm{\rho v}}_{2}^{2}+\rho {\text{gh}}_{2}.\)
- Bernoulli’s principle is Bernoulli’s equation applied to situations in which depth is constant. The terms involving depth (or height h ) subtract out, yielding
\({P}_{1}+\cfrac{1}{2}{\mathrm{\rho v}}_{1}^{2}={P}_{2}+\cfrac{1}{2}{\mathrm{\rho v}}_{2}^{2}.\)
- Bernoulli’s principle has many applications, including entrainment, wings and sails, and velocity measurement.
Glossary
Bernoulli’s equation
the equation resulting from applying conservation of energy to an incompressible frictionless fluid: P + 1/2pv2 + pgh = constant , through the fluid
Bernoulli’s principle
Bernoulli’s equation applied at constant depth: P1 + 1/2pv12 = P2 + 1/2pv22
This lesson is part of:
Fluid Dynamics and Applications
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