P + 1/2ρv2 + ρgh = constant
The fundamental energy conservation equation for incompressible, inviscid flow along a streamline. Sum of pressure, kinetic, and potential energy per unit volume remains constant.
| Term | Description |
|---|---|
| Static Pressure (P) | Thermodynamic pressure of fluid |
| Dynamic Pressure (1/2ρv2) | Kinetic energy per unit volume |
| Hydrostatic (ρgh) | Gravitational potential energy |
P/γ + v2/2g + h = h_total
Bernoulli equation expressed as head (length units). Commonly used in hydraulics and pipe flow analysis. Each term represents energy per unit weight of fluid.
| Term | Description |
|---|---|
| Pressure Head | Height of fluid column for given pressure |
| Velocity Head | Height fluid would fall to reach velocity v |
| Elevation Head | Geometric height above datum |
P1 + 1/2ρv12 = P2 + 1/2ρv22
Practical applications where elevation change is negligible. Pressure difference relates directly to velocity change. Foundation for flow measurement and aerodynamic lift.
| Term | Description |
|---|---|
| Venturi Effect | Pressure drop in constricted flow |
| Pitot Tube | Velocity measurement from stagnation pressure |
| Airfoil Lift | Pressure difference from velocity difference |
Assumptions must hold
Bernoulli equation applies only under specific conditions. Real flows with viscosity, turbulence, or compressibility require modifications or alternative approaches.
| Term | Description |
|---|---|
| No Pumps/Turbines | No external work addition/extraction |
| No Friction Losses | Negligible viscous dissipation |
| Single Phase | No cavitation or phase change |