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The Cycloid

© Copyright 2002, Jim Loy

astroidA cycloid (top left) is the path (locus) of a point on a rolling circle. The other two pictures are the curtate cycloid (the path of a point inside a rolling circle) and a prolate cycloid (the path of a point outside a rolling circle). When an automobile moves, no matter what its speed, the portion of the tire that is in contact with the road is, of course, motionless for an instant (for zero sec.). The wheels of a train (locomotive) extend below the top of the tracks. And we see from the third diagram that a point on the outside edge of such a wheel goes backward for a brief moment before moving forward again.

Galileo studied and named the cycloid. Various mathematicians found its area (between the cycloid and the horizontal axis). Others found the arc length. Gear teeth are often made of cycloids to reduce friction.

In 1696, Johann Bernoulli challenged other mathematicians to solve the Brachistochrone Problem. He knew that the answer was portion of a cycloid (inverted from the above diagram). This problem is to find the shape down which an object can slide accelerated by gravity (ignoring friction) from one point to another in the shortest time. It was solved by Leibniz, L'Hospital, Newton, and Jakob Bernoulli. If a fighter pilot wants to reach a point (the safety of a cloud perhaps) in the shortest time, he should start going straight down and follow a cycloid which intersects with his intended target.

The cycloid (again inverted from the above diagram) also solves the Tautochrone Problem. Find the curve down which an object can slide from any point to the bottom (accelerated by gravity and ignoring friction), always in the same length of time. Huygens solved this in 1673.

An epicycloid is the path of a circle rolling on the outside of a circle. A hypocycloid is the path of a circle rolling on the inside of a circle (see The Astroid). The above diagrams were drawn using Geometer's Sketchpad.


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