Fluid · Experiment

Viscosity & Turbulence

Watch fluid stream past a cylinder. Turn viscosity up and the flow glides past in smooth laminar sheets; turn it down and the wake breaks into a marching street of vortices, then full turbulence.

Controls

Reynolds number Re204
Re = ρ·v·D / μ
Shedding (Strouhal)
Laminar vortex street.
About this experiment

What you are looking at

A steady stream of fluid flows from left to right past a fixed circular cylinder. The drifting dots are tracer particles carried along by the flow — their trails reveal the streamlines. Whether the flow stays smooth or breaks up depends on a tug-of-war between two effects: the fluid's inertia (which wants to keep moving and tumble) and its viscosity (internal friction, which wants to smooth everything out).

Viscosity

Viscosity is a fluid's resistance to flowing — honey is very viscous, water much less so, air less still. It arises because neighbouring layers of fluid moving at different speeds drag on one another. Newton's law of viscosity captures this shear stress:
τ = μ (dv/dy)
where μ is the viscosity and dv/dy is the velocity gradient between layers. Turn the viscosity up in the simulation and the fluid moves in orderly, parallel sheets — laminar flow.

The Reynolds number

The single number that decides the character of the flow is the dimensionless Reynolds number:
Re = ρ v D / μ = (inertial forces) / (viscous forces)
with ρ the density, v the speed, D the cylinder diameter and μ the viscosity. Low Re (thick fluid, slow flow, small body) means viscosity dominates and the flow is smooth and laminar. High Re means inertia wins and the flow becomes unsteady and chaotic — turbulent. Because v and D are on top and μ is on the bottom, you can reach the same Re by speeding up the flow, shrinking the viscosity, or growing the cylinder.

The story as Re climbs

Re < 5: creeping (Stokes) flow — the streamlines slip around the cylinder almost symmetrically. Re ≈ 5–40: two steady eddies sit attached behind the cylinder. Re ≈ 40–1000: those eddies peel off alternately, top then bottom, forming the beautiful von Kármán vortex street — the same effect that makes flags flutter and power lines hum. The shedding frequency follows the Strouhal relation f = St·v/D with St ≈ 0.2. Re > ~2000: the wake becomes fully turbulent, a churning mess of eddies on every scale.

Things to try

Start with high viscosity and watch the smooth laminar flow, then lower it step by step to trigger the vortex street and finally turbulence — the Reynolds readout and regime label track the transition. Speed the flow up for the same effect, or grow the cylinder. Use the slow-motion button to watch individual vortices peel away from the cylinder one at a time.