An epicycloid is the path traced out by a point on the edge of a circle of radius
rolling on the outside of a circle
of radius
. It is therefore an epitrochoid
with
. Epicycloids are given by the parametric
equations
|
(1)
| |||
|
(2)
|
A polar equation can be derived by computing
|
(3)
| |||
|
(4)
|
so
|
(5)
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But
|
(6)
|
so
|
(7)
| |||
|
(8)
|
Note that
is the parameter here, not the polar angle. The polar angle from the center
is
|
(9)
|
To get cusps in the epicycloid,
, because then
rotations of
bring the point on the edge back to its starting position.
|
(10)
| |||
|
(11)
| |||
|
(12)
| |||
|
(13)
|
so
|
(14)
| |||
|
(15)
|
For positive integer ,
the enclosed area and total arc
length are
|
(16)
| |||
|
(17)
|
An epicycloid with one cusp is called a cardioid, one with two cusps is called a nephroid, and one with five cusps is called a ranunculoid.
When the two circles have equal radii, the traced epicycloid is a cardioid. During one circuit of the fixed circle, the rolling circle turns once relative to the fixed circle and its center makes one turn about the fixed center. Its orientation therefore makes two complete turns relative to the plane, which is the coin paradox (Veritasium 2024).
Epicycloids can also be constructed by beginning with the diameter of a circle and offsetting one end by a series of steps
of equal arc length along the circumference while
at the same time offsetting the other end along the circumference
by steps
times as large. After traveling around the circle once,
the envelope of an
-cusped epicycloid is produced, as illustrated above (Madachy
1979).
Epicycloids have torsion
|
(18)
|
and satisfy
|
(19)
|
where
is the radius of curvature (
).