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Chapter 4 · Turning Effects — Lessons 4.1 & 4.2

Balance Beam: The Principle of Moments

A metre rule on a movable pivot with a real torque engine: drag weights from the tray, stack them at any 5 cm notch, and watch the beam genuinely swing and settle — or tip onto its stops. A live moments ledger tallies every load's force × distance into clockwise and anticlockwise columns, the beam's own weight acts at its centre of gravity, and a mystery-mass challenge asks you to find a hidden mass using nothing but the principle of moments.

Metre Rule on a Pivotnot balanced

Drag weights from the tray onto the beam — stack them, or drag them off to remove. Drag the grey stand to move the pivot. Red arrow = the beam's own weight at its centre of gravity.

100 g
50 cm
Moments Ledger
LoadF (N)d (m)ACW (N·m)CW (N·m)
beam (100 g) at 50 cm0.980.00
Totals0.0000.000

Unequal totals → a resultant moment → the beam turns towards the bigger side.

M = F × d
Σ clockwise moments = Σ anticlockwise moments
(for an object in equilibrium)

What Each Variable Means

M

Moment. The turning effect of a force about the pivot, in newton-metres (N·m).

F

Force. Here, the weight of each load: F = m·g, with g = 9.8 N/kg. Measured in newtons (N).

d

Perpendicular distance. From the pivot to the line of action of the force, in metres (m). The ledger lists d for every load.

Σ

Sum of. Add up every moment on that side of the pivot. When the two sums are equal, there is no resultant turning effect — the beam is in equilibrium.