Brachistochrone race
Johann Bernoulli posed the brachistochrone: which curve between two points lets a bead sliding without friction under gravity arrive fastest? The cycloid wins against the straight chord and a circular arc through the same endpoints used here. Times are computed as ∫ ds/√(2gy) with y measured downward from the common start. The animation advances three beads at the same parameter pace for a race feel, not three separate physics clocks.
Who it's for: Calculus of variations introductions and classical mechanics problem sets.
Key terms
- Brachistochrone
- Cycloid
- Energy conservation
- Descent time
- Johann Bernoulli
How it works
Three tracks join the same endpoints with zero initial speed; speed along the path follows v = √(2gy) with y measured downward from the start. The cycloid minimizes the descent time (Johann Bernoulli, 1696).
Frequently asked questions
- Is the circular arc the unique circle through the two points?
- The arc shown is the circle through the origin and the endpoint whose center lies on the perpendicular bisector with the lower tangent geometry used in many textbook comparisons — it is a standard competitor, not the brachistochrone.
- Does friction or rotation of the bead matter?
- This lab uses a point mass sliding without friction and without rotational kinetic energy.
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