From Wikipedia, the free encyclopedia
In geometry , the cardioid is an epicycloid which has one and only one cusp . That is, a cardioid is a curve that can be produced as a locus — by tracing the path of a chosen point of a circle which rolls without slipping around another circle which is fixed but which has the same radius as the rolling circle.
The cardioid is also a special type of limaçon : it is the limaçon with one cusp.
The name comes from the heart shape of the curve. Compared to the ♥ symbol, though, it doesn't have the sharp point at the bottom.
The cardioid is an inversion of a parabola .
Equations
Since the cardioid is an epicycloid with one cusp, its parametric equations are
x
(
θ
)
=
cos
θ
+
1
2
cos
2
θ
,
(
1
)
{\displaystyle x(\theta )=\cos \theta +{1 \over 2}\cos 2\theta ,\qquad \qquad (1)}
y
(
θ
)
=
sin
θ
+
1
2
sin
2
θ
.
(
2
)
{\displaystyle y(\theta )=\sin \theta +{1 \over 2}\sin 2\theta .\qquad \qquad (2)}
The same shape can be defined in polar coordinates by the equation
ρ
(
θ
)
=
1
+
cos
θ
.
{\displaystyle \rho (\theta )=1+\cos \theta .\ }
Proof
Equations (1) and (2) define a cardioid whose cuspidal point is (-1/2, 0) . To convert to polar, the cusp is preferably at the origin , so add 1/2 to the abscissa :
x
(
θ
)
=
1
2
+
cos
θ
+
1
2
cos
2
θ
,
{\displaystyle x(\theta )={1 \over 2}+\cos \theta +{1 \over 2}\cos 2\theta ,}
y
(
θ
)
=
sin
θ
+
1
2
sin
2
θ
.
{\displaystyle y(\theta )=\sin \theta +{1 \over 2}\sin 2\theta .}
The polar radius
ρ
(
θ
)
{\displaystyle \rho (\theta )}
is given by
ρ
(
θ
)
=
x
2
(
θ
)
+
y
2
(
θ
)
{\displaystyle \rho (\theta )={\sqrt {x^{2}(\theta )+y^{2}(\theta )}}}
=
(
1
2
+
cos
θ
+
1
2
cos
2
θ
)
2
+
(
sin
θ
+
1
2
sin
2
θ
)
2
.
{\displaystyle ={\sqrt {\left({1 \over 2}+\cos \theta +{1 \over 2}\cos 2\theta \right)^{2}+\left(\sin \theta +{1 \over 2}\sin 2\theta \right)^{2}}}.}
Expand,
ρ
=
1
4
+
cos
2
θ
+
1
4
cos
2
2
θ
+
cos
θ
+
1
2
cos
2
θ
+
cos
θ
cos
2
θ
+
sin
2
θ
+
1
4
sin
2
2
θ
+
sin
θ
sin
2
θ
.
{\displaystyle \rho ={\sqrt {{1 \over 4}+\cos ^{2}\theta +{1 \over 4}\cos ^{2}2\theta +\cos \theta +{1 \over 2}\cos 2\theta +\cos \theta \cos 2\theta +\sin ^{2}\theta +{1 \over 4}\sin ^{2}2\theta +\sin \theta \sin 2\theta }}.}
Simplify by noticing that
cos
2
θ
+
sin
2
θ
=
1
,
(trig. ident.)
{\displaystyle \cos ^{2}\theta +\sin ^{2}\theta =1,\qquad \qquad {\mbox{(trig. ident.)}}}
1
4
cos
2
2
θ
+
1
4
sin
2
2
θ
=
1
4
,
(variation of the above)
{\displaystyle {1 \over 4}\cos ^{2}2\theta +{1 \over 4}\sin ^{2}2\theta ={1 \over 4},\qquad \qquad {\mbox{(variation of the above)}}}
cos
θ
cos
2
θ
+
sin
θ
sin
2
θ
=
cos
(
θ
−
2
θ
)
=
cos
−
θ
=
cos
θ
.
{\displaystyle \cos \theta \cos 2\theta +\sin \theta \sin 2\theta =\cos(\theta -2\theta )=\cos -\theta =\cos \theta .\ }
Thus,
ρ
=
1
4
+
1
+
1
4
+
2
cos
θ
+
1
2
cos
2
θ
{\displaystyle \rho ={\sqrt {{1 \over 4}+1+{1 \over 4}+2\cos \theta +{1 \over 2}\cos 2\theta }}}
=
3
2
+
4
2
cos
θ
+
1
2
cos
2
θ
{\displaystyle ={\sqrt {{3 \over 2}+{4 \over 2}\cos \theta +{1 \over 2}\cos 2\theta }}}
=
3
+
4
cos
θ
+
cos
2
θ
2
.
{\displaystyle ={\sqrt {3+4\cos \theta +\cos 2\theta \over 2}}.}
Then, since
cos
2
θ
=
cos
2
θ
−
sin
2
θ
=
2
cos
2
θ
−
1
,
(trigonometric identity)
{\displaystyle \cos 2\theta =\cos ^{2}\theta -\sin ^{2}\theta =2\cos ^{2}\theta -1,\qquad \qquad {\mbox{(trigonometric identity)}}}
it follows that
ρ
=
3
+
4
cos
θ
+
2
cos
2
θ
−
1
2
=
2
+
4
cos
θ
+
2
cos
2
θ
2
,
{\displaystyle \rho ={\sqrt {3+4\cos \theta +2\cos ^{2}\theta -1 \over 2}}={\sqrt {2+4\cos \theta +2\cos ^{2}\theta \over 2}},}
ρ
=
1
+
2
cos
θ
+
cos
2
θ
=
1
+
cos
θ
,
{\displaystyle \rho ={\sqrt {1+2\cos \theta +\cos ^{2}\theta }}=1+\cos \theta ,}
quod erat demonstrandum .
Graphs
Four graphs of cardioids oriented in the four cardinal directions, with their respective polar equations.