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An introduction to Electricity and Strength of Materials with Peter Eyland

Poiseuille's Law Derivation


Consider a solid cylinder of fluid, of radius r inside a hollow cylindrical pipe of radius R.

The driving force on the cylinder due to the pressure difference is:

driving force on the cylinder due to the pressure difference

The viscous drag force opposing motion depends on the surface area of the cylinder (length L and radius r):

viscous drag force opposing motion

In an equilibrium condition of constant speed, where the net force goes to zero.


We know empirically that the velocity gradient should look like this:

velocity gradient graph

At the centre
r=0
dv/dr
v is at its maximum.

At the edge
r=R
v=0


From the velocity gradient equation above, and using the empirical velocity gradient limits, an integration can be made to get an expression for the velocity.

velocity equation from integration

Which has a parabolic form as expected.


Now the equation of continuity giving the volume flux for a variable speed is:

equation of continuity for a variable speed

Substituting the velocity profile equation and the surface area of the moving cylinder:

volume flux for a variable speed

Poiseuille's equation

Poiseuille's equation



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