Bernoulli's principle
Along a streamline in an incompressible, inviscid fluid, p + ½ρv² + ρgh is conserved.
Definition
Bernoulli's principle is the statement, for steady incompressible inviscid flow, that along any single streamline the sum of static pressure, dynamic pressure, and hydrostatic pressure is constant: p + ½ρv² + ρgh = const. It is an energy-conservation argument for fluids: the three terms are pressure energy, kinetic energy, and gravitational potential energy per unit volume.
The practical consequence is counter-intuitive: faster-moving fluid has lower static pressure than slower-moving fluid at the same height. Blow across the top of a piece of paper and the paper lifts because the moving air has lower pressure than the still air underneath. Water through a narrowed pipe speeds up and drops in pressure — the Venturi effect. The principle contributes to airplane lift (alongside Newton's third law via downwash), to the spin of thrown baseballs, and to the suction of a perfume atomiser.
History
Daniel Bernoulli published the principle in 1738 in Hydrodynamica; Euler derived it rigorously from his equations of motion in 1757.