The law of the lever

The short answer

A lever balances when the turns on its two sides are equal, each turn being a force times its distance from the pivot. A 400 N load 0.25 m from the pivot is balanced by 100 N at 1 m, because 100 × 1 = 400 × 0.25. The price is distance: pushing the long end down 0.20 m raises the load only 0.05 m, so the work, force times distance, is 20 J on both sides. A lever trades force for distance; it never makes energy.

1:46How things workBeginnerleverssimple machineswork and energyArchimedestorque

Chapters and transcript

  1. 0:00

    A 100 N push lifts a 400 N load.

    On a lever, a push of 100 N can lift a load of 400 N.

  2. 0:12

    Each weight turns the bar: force × distance from the pivot.

    Each weight turns the bar about its pivot. How hard it turns the bar is its force times its distance from the pivot.

  3. 0:19

    Slide 100 N further out, and its turn grows.

    Sliding the 100 N weight away from the pivot makes its turn larger. While the load's 400 N × 0.25 m = 100 N·m is bigger, the load side stays down.

  4. 0:30

    At 1 m: 100 × 1 = 400 × 0.25. Balanced.

    At 1 m from the pivot, the weight's turn is 100 N × 1 m = 100 N·m, equal to the load's 400 N × 0.25 m, and the bar balances.

  5. 0:36

    Archimedes proved this rule.

    Archimedes proved it in On the Equilibrium of Planes: two weights balance at distances inversely proportional to the weights.

  6. 0:44

    But you pay in distance.

    The smaller force does not come free. It is paid for in distance.

  7. 0:49

    Push the long end down 0.20 m; the load rises 0.05 m.

    Each point on the bar moves in proportion to its distance from the pivot, so when the 1 m point goes down 0.20 m, the load at 0.25 m rises only 0.05 m.

  8. 0:56

    Work is force × distance.

    The work a force does is the force times the distance it moves.

  9. 1:01

    100 N × 0.20 m = 20 J. 400 N × 0.05 m = 20 J.

    The push does 100 N × 0.20 m = 20 J of work, and the load gains 400 N × 0.05 m = 20 J. On screen each is drawn as the area of a rectangle.

  10. 1:07

    The same work. The lever makes no energy.

    Work in equals work out on an ideal lever, with no friction and a weightless bar. The lever changes the force, not the energy.

  11. 1:14

    Move the pivot closer to the load.

    Moving the pivot towards the load shortens the load's arm and lengthens the push's arm, so a smaller push balances the same load.

  12. 1:22

    17 N lifts 400 N, if you push 24 times as far.

    With the pivot 0.05 m from the load and 1.20 m from the push, 400 N × 0.05 ÷ 1.20 = 16.7 N balances it, but the push must travel 24 times as far as the load rises.

  13. 1:34

    A lever trades force for distance. Never energy.

    A lever trades a small force over a long distance for a large force over a short one. It never makes energy.

Sources

Every figure in the film comes from these. The animation is illustrative.

  1. Archimedes, On the Equilibrium of Planes I, Propositions 6–7, in The Works of Archimedes, tr. T. L. Heath (Cambridge, 1897), p. 192; Heath's introduction also gives the saying reported by Pappus
  2. HyperPhysics (R. Nave, Georgia State University): The Lever, torque balance and work in equals work out for an ideal machine