Cambridge IGCSE Physics 0625 – Turning Effect of Forces
1.5.2 Turning Effect of Forces
Learning Objective
Apply the principle of moments to situations with one force on each side of the pivot, including the balancing of a beam.
Key Concepts
Force – a push or pull acting at a point.
Pivot (or fulcrum) – the point about which a body rotates.
Moment (or torque) – the turning effect of a force, calculated as the product of the force magnitude and its perpendicular distance from the pivot.
Principle of Moments – a body is in rotational equilibrium when the clockwise moments equal the anticlockwise moments about the pivot.
Definition of a Moment
The moment \$M\$ of a force \$F\$ about a pivot is given by
\$M = F \times d\$
where \$d\$ is the perpendicular distance from the line of action of the force to the pivot (the lever arm).
Direction of Moments
Moments are classified as:
Clockwise (CW)
Anticlockwise (ACW)
When solving problems, assign a sign convention (e.g., CW = positive, ACW = negative) and keep it consistent.
Principle of Moments
A rigid body will remain at rest (or rotate at constant speed) when the sum of all moments about any pivot is zero:
\$\sum M{\text{CW}} = \sum M{\text{ACW}} \quad\text{or}\quad \sum M = 0\$
Balancing a Beam with One Force on Each Side
Consider a uniform beam supported at a pivot. A force \$F1\$ acts at a distance \$d1\$ on the left side, and a force \$F2\$ acts at a distance \$d2\$ on the right side.
For the beam to be in equilibrium:
\$F1 \times d1 = F2 \times d2\$
This equation can be rearranged to find any unknown quantity.
Suggested diagram: A horizontal beam with a pivot at the centre, \$F1\$ acting downwards on the left at distance \$d1\$, \$F2\$ acting downwards on the right at distance \$d2\$.
Worked Example
Problem: A 2.0 m long uniform beam is pivoted 0.8 m from its left end. A 30 N weight is hung at the left end. At what distance from the right end must a 20 N weight be placed to keep the beam balanced?
Identify the pivot and distances:
Distance from pivot to 30 N weight: \$d_1 = 0.8\ \text{m}\$ (left side).
Let \$x\$ be the distance from the right end to the 20 N weight. The distance from the pivot to this weight is \$d_2 = 2.0 - 0.8 - x = 1.2 - x\$ (right side).
Apply the principle of moments (clockwise moments = anticlockwise moments):
Interpretation: The 20 N weight must be placed at the very right end of the beam (i.e., \$x = 0\$) for equilibrium.
Common Mistakes
Using the total length of the beam instead of the perpendicular distance from the pivot.
Forgetting to keep the direction (sign) of each moment consistent.
Assuming the beam’s own weight contributes a moment when the pivot is at the centre of a uniform beam (in that case the weight acts through the pivot and produces no moment).
Summary Table
Quantity
Symbol
Formula
Units
Force
\$F\$
Given or measured
newtons (N)
Lever arm (perpendicular distance)
\$d\$
Measured from pivot to line of action
metres (m)
Moment (torque)
\$M\$
\$M = F \times d\$
newton‑metres (N·m)
Equilibrium condition
\$\sum M{\text{CW}} = \sum M{\text{ACW}}\$
Practice Questions
A uniform 1.5 m beam is supported at its centre. A 40 N force is applied 0.3 m to the left of the pivot. Where should a 25 N force be applied on the right side to keep the beam in equilibrium?
A seesaw is 4.0 m long and pivots at its centre. A child weighing 300 N sits 0.9 m from the pivot. How far from the pivot must a second child weighing 200 N sit on the opposite side to balance the seesaw?
In a laboratory setup, a metre rule (mass 0.5 kg, uniform) is balanced on a knife‑edge at the 30 cm mark. A 2.0 kg mass is hung at the 0 cm end. Calculate the distance from the knife‑edge at which a 1.0 kg mass must be placed on the right side to achieve equilibrium. (Take \$g = 9.8\ \text{m s}^{-2}\$.)
Answers to Practice Questions
Using \$40 \times 0.3 = 25 \times d\$, we get \$d = 0.48\ \text{m}\$ to the right of the pivot.
Balance condition: \$300 \times 0.9 = 200 \times d \;\Rightarrow\; d = 1.35\ \text{m}\$ from the pivot on the opposite side.
Weight of the metre rule acts at its centre (50 cm). Moment of rule about knife‑edge: \$0.5g \times 20\ \text{cm}=0.5\times9.8\times0.20=0.98\ \text{N·m}\$ (anticlockwise). Moment of 2 kg mass: \$2g \times 0.30 = 2\times9.8\times0.30 = 5.88\ \text{N·m}\$ (clockwise). Total clockwise moment = \$5.88 + 0.98 = 6.86\ \text{N·m}\$. For the 1 kg mass: \$1g \times d = 6.86 \;\Rightarrow\; d = \frac{6.86}{9.8}=0.70\ \text{m}\$ to the right of the knife‑edge.