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Continuity Theory

Reference from the original Physics I textbook.

Continuity Theory

The same amount of fluid coming in through one area must be the same amount coming out from another area.

For steady incompressible flow, A₁v₁ = A₂v₂, where the v values are mean speeds normal to the sections.

A₁, A₂ = cross-sectional areas (m²); v₁, v₂ = mean flow speeds normal to those sections (m/s).

Figure8.2.1 1 — details in the accompanying text.

 

Related Glossary Terms

Bernoulli's Equation↗, Continuity Equation

Index

Chapter 8 - Bernoulli’s Equation

Chapter 8 - Bernoulli’s Equation

Chapter 8 - Bernoulli’s Equation

 

Reviewed physics notes (2)

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

  • Continuity conserves scalar volume flow, not vector velocity. — Reference 1
  • Definitions must agree with scalar continuity law. — Reference 1

About this edition and its source ↗

Glossary and deeper reading · 1 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 →

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