Flow Visualization
P1P2P3P + 1/2ρv2 + ρgh

Standard Bernoulli Equation

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.

P
Static Pressure
Pa (Pascals)
ρ
Fluid Density
kg/m3
v
Flow Velocity
m/s
g
Gravity
9.81 m/s2

Energy Terms

Conservation
TermDescription
Static Pressure (P)Thermodynamic pressure of fluid
Dynamic Pressure (1/2ρv2)Kinetic energy per unit volume
Hydrostatic (ρgh)Gravitational potential energy

Practical Examples

  • Pipe flow analysis: Calculate pressure drop from velocity change
  • Tank discharge: Torricelli's theorem (v = √2gh)
  • Siphon design: Maximum height limited by vapor pressure
Flow Visualization
WideNarrowWidev↑ → P↓

Engineering Applications

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.

ΔP
Pressure Difference
Pa
v1, v2
Velocities at points 1, 2
m/s
ρ
Fluid Density
kg/m3

Energy Terms

Conservation
TermDescription
Venturi EffectPressure drop in constricted flow
Pitot TubeVelocity measurement from stagnation pressure
Airfoil LiftPressure difference from velocity difference

Practical Examples

  • Venturi meter: Q = A2√[2(P1-P2)/ρ(1-(A2/A1)2)]
  • Pitot-static tube: Aircraft airspeed measurement
  • Atomizers/spray bottles: Low pressure draws fluid upward
  • Baseball curveball: Magnus effect pressure differential
Flow Visualization
VALIDREGIONSteadyInviscidIncompressibleStreamlineAssumptions

Limitations & Assumptions

Assumptions must hold

Bernoulli equation applies only under specific conditions. Real flows with viscosity, turbulence, or compressibility require modifications or alternative approaches.

Steady Flow
∂/∂t = 0
-
Incompressible
ρ = constant
-
Inviscid
μ ≈ 0
-
Along Streamline
Same streamline
-

Energy Terms

Conservation
TermDescription
No Pumps/TurbinesNo external work addition/extraction
No Friction LossesNegligible viscous dissipation
Single PhaseNo cavitation or phase change

Practical Examples

  • Boundary layers: Viscous effects near solid surfaces
  • Turbulent flow: Energy losses require Darcy-Weisbach
  • Compressible flow: Use isentropic relations (M > 0.3)
  • Pumps/turbines: Add head terms (h_pump, h_turbine)