Galileo: Throwing cannonballs off The Leaning Tower of Pisa
This post is inspired by the excellent book by Robert Banks – Towing Icebergs. This book would make a great investment if you want some novel ideas for a maths investigation.
Galileo Galilei was an Italian mathematician and astronomer who (reputedly) conducted experiments from the top of the Tower of Pisa. He dropped various objects from in order to measure how long it took for them to reach the bottom, coming to the remarkable conclusion that the objects’ weight did not affect the speed at which it fell. But does that really mean that a feather and a cannonball would fall at the same speed? Well, yes – as long as they were dropped in a vacuum. Let’s have a look at how we can prove that.
For an object falling through the air we have:
psgV – pagV – FD = psVa
ps = The density of the falling object
pa = The density of the air it’s falling in
FD = The drag force
g = The gravitational force
V = The volume of the falling object
a = The acceleration of the falling object
To understand where this equation comes from we note that Newton second law (Force = mass x acceleration) is
F = ma
The LHS of our equation (psgV – pagV – FD) represents the forces acting on the object and the RHS (psVa) represents mass x acceleration.
Time to simplify things
Things look a little complicated at the moment – luckily we can make our lives easier through a little simplification. pa will be many magnitudes smaller than than ps – as the density of air is much smaller than the density of objects like cannonballs. Therefore we ignore this part of the equation, giving an approximate equation:
psgV – FD ≈ psVa
Next, we can note that in a vacuum FD (the drag force) will be 0 – as there is no air resistance. Therefore this can also be ignored to get:
psgV ≈ psVa
g ≈ a
But we have a = dU/dt where U = velocity, therefore,
g ≈ a
g ≈ dU/dt
g dt ≈ dU
and integrating both sides will give:
gt ≈ U
Therefore the velocity (U) of the falling object in a vacuum is only dependent on time and the gravitational force. In other words it is independent of the object’s mass. Amazing!
This might be difficult to believe – as it is quite unintuitive. So if you’re not convinced you can watch the video below in which Brian Cox tests this out in the world’s largest vacuum chamber.
If you liked this post you might also like:
War maths – how modeling projectiles plays an essential part in waging wars.