Notifications

Log in to see your notifications.

Fluid Dynamics

13 min read

Streamline and turbulent flow

A moving fluid is described by flow lines. In streamline (laminar) flow each part of the fluid follows a smooth path without crossing others. When the speed is too high or the passage too rough, the flow becomes turbulent and swirls in eddies. An ideal fluid is incompressible and has no viscosity.

The equation of continuity and Bernoulli’s principle

If an ideal fluid flows through a pipe, the volume passing each section every second is the same. So where the pipe is narrower the fluid moves faster.

Continuity (left) and Bernoulli’s equation (right). Where the speed of a fluid is higher, its pressure is lower. ρ = density, h = height.
Bernoulli and the venturi tubeA fluid flows through a tube that narrows. In the narrow part the fluid moves faster, so by the principle of continuity and Bernoulli’s principle the pressure there is lower. The vertical tubes show it: the liquid column is lower above the narrow section, where the pressure is less.slow, high pressurefast, low pressureslow againA₁v₁ = A₂v₂ P + ½ρv² = constant
Try itA narrowing pipe

Choose the speed of the water in the wide pipe and the pipe areas. Find the speed in the narrow section and the drop in pressure there. (ρ = 1 000 kg/m³)

ApplicationBernoulli idea
Aeroplane wingAir moves faster over the curved top, so the pressure there is lower: lift
Spray gun and carburettorFast air in a narrow section has low pressure and draws up liquid
Bunsen burnerFast gas jet draws in air
Two ships close togetherFast water between them has lower pressure and pushes the ships together
Curved ballA spinning ball drags air round and curves

Viscosity and Stokes’ law

Viscosity is the internal friction of a fluid that resists the relative motion of its layers. Honey is more viscous than water. The viscosity η (eta) falls as a liquid is heated and rises for gases. A small sphere moving slowly through a viscous fluid experiences a drag force given by Stokes’ law.

η = viscosity (Pa s), r = radius of the sphere, v = speed. The drag increases with speed.

A sphere falling through a fluid is acted on by weight (down), upthrust (up) and viscous drag (up). The drag grows with speed until the forces balance and the sphere falls at a constant terminal velocity.

Terminal velocity of a sphere of density ρₛ in a fluid of density ρ_f. It depends on the square of the radius, so bigger drops fall much faster.
The speed rises, then levels off at the terminal velocity when drag balances weight minus upthrust.
Try itTerminal velocity

Choose the radius of a steel ball and the viscosity of the oil it falls through. (Steel ρ = 7 800 kg/m³, oil ρ = 900 kg/m³, g = 9.8 m/s²)

Laminar flow in pipes

The flow of a viscous fluid through a narrow tube depends strongly on the radius of the tube. Poiseuille’s equation: the volume flow rate is Q = πPr⁴ ÷ (8ηL), where P is the pressure difference and L the length. Halving the radius reduces the flow sixteen times. This is why narrowed arteries seriously reduce blood flow.

Check yourself When the speed of a fluid increases, the pressure in it…
Check yourself Water flows at 2 m/s in a pipe of area 10 cm². It enters a section of area 5 cm². The speed there is…
Check yourself A sphere falling at terminal velocity has…

Key terms

Streamline flow
Smooth flow in which fluid layers do not mix.
Viscosity
The internal friction of a fluid, resisting relative motion of its layers.
Terminal velocity
The constant velocity reached when drag balances the driving force.
Bernoulli's principle
In a steady flow, an increase in speed is accompanied by a decrease in pressure.

Summary

  • Continuity: A₁v₁ = A₂v₂; Bernoulli: P + ½ρv² + ρgh = constant.
  • Faster fluid, lower pressure: lift, spray guns.
  • Stokes' law F = 6πηrv; terminal velocity v = 2r²(ρₛ − ρ_f)g ÷ 9η.
  • Poiseuille: flow in a tube ∝ r⁴.