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Bernoulli's Equation

Reference from the original Physics I textbook.

Bernoulli's Equation

For steady, incompressible, inviscid flow along a streamline: P₁ + ½ρv₁² + ρgH₁ = P₂ + ½ρv₂² + ρgH₂. All terms have units Pa = J/m³.

 

P₁, P₂ = pressures (Pa); ρ = fluid density (kg/m³); v₁, v₂ = mean flow speeds (m/s); H₁, H₂ = heights relative to a common datum (m); g = gravitational-acceleration magnitude (m/s²).

Figure8.2.2 1 — details in the accompanying text.

 

Related Glossary Terms

Continuity Equation↗, Continuity Theory, Kinetic Energy of the Fluid, Potential Energy of a Fluid

Index

Chapter 8 - Bernoulli’s Equation

Chapter 8 - Bernoulli’s Equation

Chapter 8 - FFR - More on Fluids

Reviewed physics notes (2)

These corrections keep the original lesson’s purpose while fixing errors in the source edition.

  • Bernoulli needs conditions and scalar speeds. — Reference 1
  • Definitions must match scalar speeds in Bernoulli equation. — Reference 1

About this edition and its source ↗

Glossary and deeper reading · 2 refreshers

These editorial refreshers supplement the reading. Definitions and examples are added guidance; original source wording and recorded answers remain in their original context.

  • Bernoulli’s equation

    Bernoulli’s equation relates pressure, fluid speed, and elevation along a streamline in steady ideal flow. Its usual form assumes an incompressible, nonviscous fluid and no added or removed mechanical energy along the path. For example, in a horizontal pipe narrowing under those assumptions, higher flow speed accompanies lower pressure.

    Read more: Bernoulli’s equation →

  • Continuity equation

    The continuity equation expresses conservation of mass in fluid flow. For steady incompressible flow through one unbranched channel, cross-sectional area times average flow speed is constant. For example, water moves faster through a narrower part of a pipe when the same volume passes each second.

    Read more: Continuity equation →

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