What you are looking at
A rigid beam pivots on a central fulcrum, with a mass on each side that you can move and resize. If the
turning effects cancel, the beam floats level; otherwise it tips toward the winning side and rests against
its stop. The curved arrows show each side's torque and direction.
Torque: force times leverage
A force's ability to rotate something depends not just on how hard it pushes but on
how far from
the pivot it acts:
τ = F · d = m·g·d
Doubling the distance doubles the torque as surely as doubling the force — which is why door handles sit far
from the hinges and wrenches have long handles.
Static equilibrium
The beam is in equilibrium when the net force
and the net torque are both zero. The pivot supplies
the force balance automatically, so the whole problem reduces to the torques:
m₁·g·d₁ = m₂·g·d₂ ⇒ m₁d₁ = m₂d₂
Gravity cancels out: only the mass-distance products matter. A 3 kg mass at 2 m holds a 4 kg mass at 1.5 m —
6 kg·m each side.
The law of the lever
This is Archimedes' machine: a small force far from the pivot balances (or lifts) a large force close in,
trading
distance for force. The mechanical advantage is d₁/d₂ — but as with the hydraulic
press, energy is conserved: the far end sweeps a proportionally longer arc, so force × distance comes out
even. "Give me a place to stand," Archimedes said, "and I shall move the Earth."
Things to try
Balance unequal masses by sliding the lighter one outward until m₁d₁ = m₂d₂ exactly. Then double both
distances — still balanced, since both torques doubled. Park a 10 kg mass at 0.5 m and hold it with just
2.5 kg at 2 m: a 4× lever.