The Basis of Bernoulli’s Equation
Energetic interpretation and forms of the relationship
Three equivalent forms
Bernoulli’s equation can be written in three forms, each suited to a particular measurement context:
| Form | Expression | Unit |
|---|---|---|
| Pressure | P + (1/2)ρv² + ρgz = constant | Pa |
| Height (head) | P/(ρg) + v²/(2g) + z = constant | m |
| Volumetric energy | identical to the pressure form | J/m³ |
Physical meaning of the terms
- P: static pressure, associated with the fluid’s pressure energy.
- (1/2)ρv²: dynamic pressure, associated with the kinetic energy of the moving fluid.
- ρgz: positional pressure, associated with gravitational potential energy.
Bernoulli’s equation therefore expresses the conservation of a fluid’s volumetric mechanical energy along a streamline, in the absence of friction and of work exchange with the external environment (no pump, no turbine along the path under consideration).
Practical example
In a horizontal pipe (constant z) that narrows, the continuity equation (conservation of flow rate, S*v = constant for an incompressible fluid) dictates that v must increase at the point where the pipe narrows. Bernoulli’s principle then dictates that P must decrease at this point: this is precisely the principle utilised in the Venturi tube, which is discussed in the following chapter.
Pitfall to avoid
Do not confuse static pressure P, measured perpendicular to the flow, with total pressure P + (1/2)ρv², measured in the direction of the flow (for example, using a Pitot tube). These two quantities do not have the same physical meaning, and confusing them will distort any calculation of velocity.

