The turning effect (or moment) of a force is how much that force tends to rotate an object about a pivot point. It depends on two things:
Mathematically, the moment is \$M = F \times d\$. The larger the moment, the stronger the tendency to rotate.
When a rigid body is in rotational equilibrium (i.e. it does not rotate), the sum of all clockwise moments equals the sum of all counter‑clockwise moments:
\$\sum M{\text{clockwise}} = \sum M{\text{counter‑clockwise}}\$
This is the same idea as balancing a seesaw: the heavier side must be farther from the pivot to stay level.
In many IGCSE problems you’ll see a simple beam with a single force on each side of a pivot. The beam is balanced when:
\$F1 \times d1 = F2 \times d2\$
where \$F1\$ and \$F2\$ are the forces, and \$d1\$ and \$d2\$ are their distances from the pivot.
Imagine a playground seesaw. If you sit 1 m from the centre and your friend sits 2 m away, you need to be twice as light as your friend to stay level. That’s exactly the principle of moments in action!
Suppose a beam has a 5 kg weight hanging 0.4 m to the left of the pivot and a 3 kg weight hanging 0.6 m to the right. Does the beam balance?
To balance, you could move the 3 kg weight further right or add a small weight on the left.
A beam is balanced with a 4 kg weight 0.5 m to the left of the pivot. An unknown weight \$x\$ is 0.3 m to the right. What is \$x\$?
| Side | Mass (kg) | Distance (m) | Moment (N·m) |
|---|---|---|---|
| Left | 4 | 0.5 | \$4 \times 9.8 \times 0.5 = 19.6\$ |
| Right | \$x\$ | 0.3 | \$x \times 9.8 \times 0.3\$ |
| Set moments equal | \$19.6 = 2.94x\$ | ||
| Solve for \$x\$ | \$x = \dfrac{19.6}{2.94} \approx 6.67\$ kg | ||
Keep practising, and soon you’ll be able to solve any moment problem with confidence! 🚀