Fluid mechanics Foundations and kinematics of flow Concept
Reynolds number
Summary
The Reynolds number is the dimensionless number that compares inertial forces with viscous forces in a flow. At small Reynolds number viscosity dominates and flows are smooth and orderly. At large Reynolds number inertia dominates and flows tend to become unstable and turbulent. It is the main parameter of the incompressible Navier–Stokes equations after they are made dimensionless.
Where this leads
21 pages build on this one.
- Orr–Sommerfeld equation
- Dittus–Boelter equation
- Stanton number
- Knudsen number
- Thermal boundary layer
- Turbulence
- Drag coefficient
- Squire's theorem
- Chilton–Colburn J-factor analogy
- Taylor–Couette instability
- Aerodynamics
- Dynamic similarity
- Kármán vortex street
- Lubrication theory
- Laminar–turbulent transition
- Reynolds analogy
- Tollmien–Schlichting wave
- Taylor microscale
- Kolmogorov microscales
- Forced convection
- Péclet number
Further reading
About this page
| Tag | JH9EJ0HA0R |
|---|---|
| URI | m2://JH9EJ0HA0R |
| Kind | concept |
| Writing | W0 stub |
| MSC | 76M55, 76D05, 76F06 |
| Specializes | Dimensionless numbers in fluid mechanics |
| Same as | |
| Changed | 3 November 2026 |
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Used by
- Orr–Sommerfeld equation
- Dittus–Boelter equation
- Stanton number
- Knudsen number
- Thermal boundary layer
- Turbulence
- Drag coefficient
- Squire's theorem
- Taylor–Couette instability
- Aerodynamics
- Dynamic similarity
- Kármán vortex street
- Lubrication theory
- Laminar–turbulent transition
- Reynolds analogy
- Tollmien–Schlichting wave
- Taylor microscale
- Kolmogorov microscales
- Forced convection
- Péclet number