Concept · Fluid Mechanics — laminar vs turbulent

The Reynolds Number

Every flow is a tug-of-war: inertia wants to tumble, viscosity wants to smooth. One dimensionless ratio — the Reynolds number — predicts the winner. Osborne Reynolds settled it in 1883 with a thread of dye in a glass tube.

Re= ρ·V·Dμ = V·Dν
Re dimensionless  ·  ρ density  ·  V mean velocity  ·  D pipe diameter  ·  μ dynamic viscosity  ·  ν = μ/ρ kinematic viscosity
what one number decides
Laminar Transition Turbulent

What did we learn?

1Re = ρVD/μ = VD/ν. A single dimensionless ratio of inertia to viscosity. Because it's dimensionless, the same number governs flow in a pipe, over a wing, and through an artery.
2Three regimes. Below ~2300 the dye holds a razor line — laminar, ordered layers. Above ~4000 it shatters into eddies — turbulent, chaotic mixing. Between them lies the unstable transition.
3It's a competition. Faster flow or a wider pipe (more inertia) pushes toward chaos; a stickier fluid (more viscosity) pulls back to order. That's why glycerin stays glassy even wide open — viscosity wins.
4Why it matters. Reynolds read the regime straight off a dye filament — exactly what you just did. The same number sizes pipelines, predicts drag, and lets a small wind-tunnel model stand in for a full-size aircraft.
Interactive Explainer · Fluid Mechanics

When Does Smooth Flow Turn Turbulent?

Inject a fine thread of dye into water gliding down a glass tube — exactly as Osborne Reynolds did in 1883. Open the valve and watch a single number, Re = ρVD/μ, decide whether the dye holds a razor-straight line or shatters into churning eddies. Change the speed, the pipe, the fluid — and feel where order gives way to chaos.

Re= V·Dν =
V= D= ν=
Trickle (laminar) → wide open (turbulent). Mean velocity V of the water in the tube.
A wider tube carries more inertia at the same speed — so Re climbs with D.

The dye filament is the real observable — exactly what Reynolds watched. Re below 2300 → one clean thread. Above 4000 → it bursts into eddies and the whole tube clouds with dye. The wavering grows downstream because the instability amplifies as it travels.

Live Reading
Open the valve
Press play, then nudge the velocity up and watch the dye thread.
Reynolds numberRe = VD/ν
Flow regime scale
2300
4000
Mean velocity V
set by the valve
Diameter D
bore of the tube
Kinematic ν
water · 20°C
Inertia : viscosity
which force is winning

One number, three behaviours.

Reynolds discovered that flow doesn't care about speed, size, or stickiness separately — only about their combination Re = ρVD/μ. Push it up and ordered layers lose their grip.

The lever you control: velocity and diameter raise inertia (numerator); viscosity (denominator) resists. The dye thread is just Re made visible.