If the smaller circle has radius r, and the larger circle has radius R = kr, then the parametric equations for the curve can be given by either:

${\displaystyle x(\theta )=(R+r)\cos \theta \ -r\cos \left({\frac {R+r}{r}}\theta \right)}$ 

${\displaystyle y(\theta )=(R+r)\sin \theta \ -r\sin \left({\frac {R+r}{r}}\theta \right),}$ 

or:

${\displaystyle x(\theta )=r(k+1)\cos \theta -r\cos \left((k+1)\theta \right)\,}$ 

${\displaystyle y(\theta )=r(k+1)\sin \theta -r\sin \left((k+1)\theta \right).\,}$ 

in a more concise and complex form^[1]

${\displaystyle z(\theta )=r(e^{i(k+1)\theta }-(k+1)e^{i\theta })}$ 

where

• angle ${\displaystyle \theta }$  is in turns: ${\displaystyle \theta \in [0,2\pi ].}$ 
• smaller circle has radius r
• the larger circle has radius kr

(Assuming the initial point lies on the larger circle.) When k is a positive integer, the area of this epicycloid is

${\displaystyle A=(k+1)(k+2)\pi r^{2}.}$ 

If k is a positive integer, then the curve is closed, and has k cusps (i.e., sharp corners).

If k is a rational number, say k = p / q expressed as irreducible fraction, then the curve has p cusps.

Count the animation rotations to see p and q .

If k is an irrational number, then the curve never closes, and forms a dense subset of the space between the larger circle and a circle of radius R + 2r.

The distance OP from (x=0,y=0) origin to (the point ${\displaystyle p}$  on the small circle) varies up and down as

R <= OP <= (R + 2r)

R = radius of large circle and

2r = diameter of small circle

• Epicycloid examples
•  

  k = 1          a cardioid

•  

  k = 2          a nephroid

•  

  k = 3          a trefoiloid

•  

  k = 4          a quatrefoiloid

•  

  k = 2.1 = 21/10

•  

  k = 3.8 = 19/5

•  

  k = 5.5 = 11/2

•  

  k = 7.2 = 36/5

The epicycloid is a special kind of epitrochoid.

An epicycle with one cusp is a cardioid, two cusps is a nephroid.

An epicycloid and its evolute are similar.^[2]

We assume that the position of ${\displaystyle p}$  is what we want to solve, ${\displaystyle \alpha }$  is the angle from the tangential point to the moving point ${\displaystyle p}$ , and ${\displaystyle \theta }$  is the angle from the starting point to the tangential point.

Since there is no sliding between the two cycles, then we have that

${\displaystyle \ell _{R}=\ell _{r}}$ 

By the definition of angle (which is the rate arc over radius), then we have that

${\displaystyle \ell _{R}=\theta R}$ 

and

${\displaystyle \ell _{r}=\alpha r}$ .

From these two conditions, we get the identity

${\displaystyle \theta R=\alpha r}$ .

By calculating, we get the relation between ${\displaystyle \alpha }$  and ${\displaystyle \theta }$ , which is

${\displaystyle \alpha ={\frac {R}{r}}\theta }$ .

From the figure, we see the position of the point ${\displaystyle p}$  on the small circle clearly.

${\displaystyle x=\left(R+r\right)\cos \theta -r\cos \left(\theta +\alpha \right)=\left(R+r\right)\cos \theta -r\cos \left({\frac {R+r}{r}}\theta \right)}$ 

${\displaystyle y=\left(R+r\right)\sin \theta -r\sin \left(\theta +\alpha \right)=\left(R+r\right)\sin \theta -r\sin \left({\frac {R+r}{r}}\theta \right)}$ 

• List of periodic functions
• Cycloid
• Cyclogon
• Deferent and epicycle
• Epicyclic gearing
• Epitrochoid
• Hypocycloid
• Hypotrochoid
• Multibrot set
• Roulette (curve)
• Spirograph

• J. Dennis Lawrence (1972). A catalog of special plane curves. Dover Publications. pp. 161, 168–170, 175. ISBN 978-0-486-60288-2.

• Weisstein, Eric W. "Epicycloid". MathWorld.
• "Epicycloid" by Michael Ford, The Wolfram Demonstrations Project, 2007
• O'Connor, John J.; Robertson, Edmund F., "Epicycloid", MacTutor History of Mathematics archive, University of St Andrews
• Animation of Epicycloids, Pericycloids and Hypocycloids
• Spirograph -- GeoFun
• Historical note on the application of the epicycloid to the form of Gear Teeth