The
viscosity can be calculated by allowing small spherical objects of known weight to fall through a fluid until they reach
terminal velocity.
The masses of the balls are measured using a balance and the diameters of the balls are measured using Vernier callipers
The density of the balls is calculated using
Three rubber bands around the tube to make three positions. The highest is placed below the surface of the liquid to ensure the ball is travelling at terminal velocity when it reaches this band.
The remaining two bands are placed 10 – 15 cm apart so that time can be measured accurately

Release the ball and start the timer when it reaches the first band, then find the time to fall the distances d
1 between the highest and middle rubber band and d
2 between the highest and lowest bands.
Repeat three times for balls of same diameter at different temperatures.

At terminal velocity, the vector sum of the forces on the ball is zero so
weight – drag – upthrust = 0
From this it can be shown that
, where η is the viscosity of the liquid
r is the radius of the ball
ρ is the density of the ball
σ is the density of the liquid
v is the terminal velocity.