Fosbury's technique may have looked radical at the time, but it had the benefit of squaring nicely with some fundamental scientific principles.
John Barrow, a mathematician at Cambridge University, explains that the genius of the Fosbury Flop is that the jumper's centre of gravity, or centre of mass, stays low to the ground, which means that less energy is needed to clear the bar.
The centre of mass of an object is defined as the "average location of all the mass in an object".
What makes the Fosbury Flop revolutionary is that it enables a jumper's centre of gravity to travel underneath the bar while the jumper clears the bar.
Barrow points out that if an object has a bendy or irregular shape, the centre of gravity for that object can be positioned outside of itself.
Because a high jumper leaps into a semi-circular position at the top of his flight, with his back facing the ground, the centre of mass will be positioned somewhere between the jumper's feet and head. That is, lower than the athlete's back as it crosses over
the bar for a successful jump.
To achieve this, a high jumper has to launch with as much vertical speed as possible.
Dr Jesus Dapena, a biomechanicist at the University of Indiana, estimates the point of take-off for a high jumper lasts between 0.16 and 0.20 seconds.
In that time, the athlete must make a substantial "vertical impulse" on the ground.
That requires jumpers to swing their arms and front legs hard to create the maximum amount of upward forces.
The high jump world record was achieved using the Fosbury Flop. In 1993, Cuba's Javier Sotomayer jumped a staggering 2.45m in Salamanca.
That record is 10cm higher than the best straddle-technique jump, which was achieved by Ukraine's Vladimir Yashchenko in 1978.