The Reynolds number (Re) is the single most important dimensionless quantity in fluid mechanics. Named after Osborne Reynolds, who published his landmark pipe-flow experiments in 1883, it predicts whether a flow will be smooth and orderly (laminar) or chaotic and mixing (turbulent). Engineers and scientists rely on it to design pipelines, aircraft wings, heat exchangers, blood-flow models, chemical reactors, and virtually any system where a fluid moves past a surface.
The formula
Re = ρ · v · L / μ
| Symbol | Quantity | SI unit |
|---|---|---|
| ρ (rho) | Fluid density | kg/m³ |
| v | Flow velocity | m/s |
| L | Characteristic length | m |
| μ (mu) | Dynamic viscosity | Pa·s |
| Re | Reynolds number | — (dimensionless) |
Because μ / ρ = ν (kinematic viscosity, m²/s), the formula is often written Re = v · L / ν. Both forms are identical; this calculator accepts density and dynamic viscosity separately so you can use standard tabulated values.
What the number tells you
The Reynolds number is a ratio of inertial forces (which tend to sustain motion and create turbulence) to viscous forces (which damp disturbances and keep flow laminar). Three regimes are recognised for pipe flow:
- Re < 2 300 — Laminar. Fluid moves in parallel layers with no mixing between them. Velocity profile is parabolic (Poiseuille flow). Friction factor follows the exact analytical result f = 64/Re.
- 2 300 ≤ Re < 4 000 — Transitional. The flow is unstable; small perturbations can trigger turbulent bursts. Difficult to predict analytically.
- Re ≥ 4 000 — Turbulent. Rapid, irregular fluctuations mix momentum and energy across the flow cross-section. Engineering correlations (Moody chart, Colebrook equation) describe friction.
For external flow over a flat plate the critical Re is approximately 5 × 10⁵ at the leading edge. For flow around a sphere it is around 2 × 10⁵ (drag crisis). The calculator uses the pipe-flow thresholds by default; enter your measured Re and compare against the geometry-specific value for other cases.
How it works
The calculator implements the exact Navier–Stokes dimensional analysis result. No approximations are introduced. You can solve for any of the four primary variables:
- Reynolds number — standard forward calculation.
- Flow velocity — rearranges to v = Re · μ / (ρ · L); useful for sizing pumps or fans.
- Characteristic length — rearranges to L = Re · μ / (ρ · v); useful for pipe diameter selection.
- Kinematic viscosity — rearranges to ν = v · L / Re; useful for identifying an unknown fluid from flow measurements.
Eight built-in fluid presets (Air 20 °C, Water 20 °C, Water 60 °C, Seawater, SAE 30
oil, Blood, Glycerol, Custom) cover the most common engineering and biomedical scenarios.
Dynamic viscosity accepts scientific notation (e.g. 1.002e-3 Pa·s for water at 20 °C).
Worked example — water in a 50 mm pipe
A domestic pump circulates water at 20 °C through a 50 mm internal-diameter pipe at 1 m/s. Is the flow laminar or turbulent?
- ρ = 998.2 kg/m³, μ = 1.002 × 10⁻³ Pa·s
- L = 0.05 m (pipe diameter), v = 1 m/s
Re = 998.2 × 1 × 0.05 / 1.002 × 10⁻³ ≈ 49 821
Re = 49 821 is far above 4 000 — the flow is firmly turbulent. To achieve laminar flow in that pipe you would need to reduce velocity to below about 46 mm/s (Re ≈ 2 300 threshold), which is impractically slow for domestic heating circuits. Select “Flow velocity” in the calculator, enter Re = 2300, and it will confirm this exactly.
| Fluid | v (m/s) | L (m) | Re | Regime |
|---|---|---|---|---|
| Water 20 °C | 1.0 | 0.05 | 49 821 | Turbulent |
| Water 20 °C | 0.046 | 0.05 | 2 297 | Laminar |
| Air 20 °C | 5.0 | 0.1 | 33 024 | Turbulent |
| Engine oil SAE 30 | 1.0 | 0.05 | 555 | Laminar |
| Blood (37 °C) | 0.3 | 0.004 | 363 | Laminar |
Blood in the aorta (diameter ~25 mm, velocity ~0.3 m/s) gives Re ≈ 2 700 — right in the transitional zone, explaining the systolic murmurs cardiologists listen for.
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