Cissoid

Plane curve constructed from two other curves and a fixed point
  Cissoid
  Curve C1
  Curve C2
  Pole O

In geometry, a cissoid (from Ancient Greek κισσοειδής (kissoeidēs) 'ivy-shaped') is a plane curve generated from two given curves C1, C2 and a point O (the pole). Let L be a variable line passing through O and intersecting C1 at P1 and C2 at P2. Let P be the point on L so that O P ¯ = P 1 P 2 ¯ . {\displaystyle {\overline {OP}}={\overline {P_{1}P_{2}}}.} (There are actually two such points but P is chosen so that P is in the same direction from O as P2 is from P1.) Then the locus of such points P is defined to be the cissoid of the curves C1, C2 relative to O.

Slightly different but essentially equivalent definitions are used by different authors. For example, P may be defined to be the point so that O P ¯ = O P 1 ¯ + O P 2 ¯ . {\displaystyle {\overline {OP}}={\overline {OP_{1}}}+{\overline {OP_{2}}}.} This is equivalent to the other definition if C1 is replaced by its reflection through O. Or P may be defined as the midpoint of P1 and P2; this produces the curve generated by the previous curve scaled by a factor of 1/2.

Equations

If C1 and C2 are given in polar coordinates by r = f 1 ( θ ) {\displaystyle r=f_{1}(\theta )} and r = f 2 ( θ ) {\displaystyle r=f_{2}(\theta )} respectively, then the equation r = f 2 ( θ ) f 1 ( θ ) {\displaystyle r=f_{2}(\theta )-f_{1}(\theta )} describes the cissoid of C1 and C2 relative to the origin. However, because a point may be represented in multiple ways in polar coordinates, there may be other branches of the cissoid which have a different equation. Specifically, C1 is also given by

r = f 1 ( θ + π ) r = f 1 ( θ π ) r = f 1 ( θ + 2 π ) r = f 1 ( θ 2 π ) {\displaystyle {\begin{aligned}&r=-f_{1}(\theta +\pi )\\&r=-f_{1}(\theta -\pi )\\&r=f_{1}(\theta +2\pi )\\&r=f_{1}(\theta -2\pi )\\&\qquad \qquad \vdots \end{aligned}}}

So the cissoid is actually the union of the curves given by the equations

r = f 2 ( θ ) f 1 ( θ ) r = f 2 ( θ ) + f 1 ( θ + π ) r = f 2 ( θ ) + f 1 ( θ π ) r = f 2 ( θ ) f 1 ( θ + 2 π ) r = f 2 ( θ ) f 1 ( θ 2 π ) {\displaystyle {\begin{aligned}&r=f_{2}(\theta )-f_{1}(\theta )\\&r=f_{2}(\theta )+f_{1}(\theta +\pi )\\&r=f_{2}(\theta )+f_{1}(\theta -\pi )\\&r=f_{2}(\theta )-f_{1}(\theta +2\pi )\\&r=f_{2}(\theta )-f_{1}(\theta -2\pi )\\&\qquad \qquad \vdots \end{aligned}}}

It can be determined on an individual basis depending on the periods of f1 and f2, which of these equations can be eliminated due to duplication.

Ellipse r = 1 2 cos θ {\displaystyle r={\frac {1}{2-\cos \theta }}} in red, with its two cissoid branches in black and blue (origin)

For example, let C1 and C2 both be the ellipse

r = 1 2 cos θ . {\displaystyle r={\frac {1}{2-\cos \theta }}.}

The first branch of the cissoid is given by

r = 1 2 cos θ 1 2 cos θ = 0 , {\displaystyle r={\frac {1}{2-\cos \theta }}-{\frac {1}{2-\cos \theta }}=0,}

which is simply the origin. The ellipse is also given by

r = 1 2 + cos θ , {\displaystyle r={\frac {-1}{2+\cos \theta }},}

so a second branch of the cissoid is given by

r = 1 2 cos θ + 1 2 + cos θ {\displaystyle r={\frac {1}{2-\cos \theta }}+{\frac {1}{2+\cos \theta }}}

which is an oval shaped curve.

If each C1 and C2 are given by the parametric equations

x = f 1 ( p ) ,   y = p x {\displaystyle x=f_{1}(p),\ y=px}

and

x = f 2 ( p ) ,   y = p x , {\displaystyle x=f_{2}(p),\ y=px,}

then the cissoid relative to the origin is given by

x = f 2 ( p ) f 1 ( p ) ,   y = p x . {\displaystyle x=f_{2}(p)-f_{1}(p),\ y=px.}

Specific cases

When C1 is a circle with center O then the cissoid is conchoid of C2.

When C1 and C2 are parallel lines then the cissoid is a third line parallel to the given lines.

Hyperbolas

Let C1 and C2 be two non-parallel lines and let O be the origin. Let the polar equations of C1 and C2 be

r = a 1 cos ( θ α 1 ) {\displaystyle r={\frac {a_{1}}{\cos(\theta -\alpha _{1})}}}

and

r = a 2 cos ( θ α 2 ) . {\displaystyle r={\frac {a_{2}}{\cos(\theta -\alpha _{2})}}.}

By rotation through angle α 1 α 2 2 , {\displaystyle {\tfrac {\alpha _{1}-\alpha _{2}}{2}},} we can assume that α 1 = α ,   α 2 = α . {\displaystyle \alpha _{1}=\alpha ,\ \alpha _{2}=-\alpha .} Then the cissoid of C1 and C2 relative to the origin is given by

r = a 2 cos ( θ + α ) a 1 cos ( θ α ) = a 2 cos ( θ α ) a 1 cos ( θ + α ) cos ( θ + α ) cos ( θ α ) = ( a 2 cos α a 1 cos α ) cos θ ( a 2 sin α + a 1 sin α ) sin θ cos 2 α   cos 2 θ sin 2 α   sin 2 θ . {\displaystyle {\begin{aligned}r&={\frac {a_{2}}{\cos(\theta +\alpha )}}-{\frac {a_{1}}{\cos(\theta -\alpha )}}\\&={\frac {a_{2}\cos(\theta -\alpha )-a_{1}\cos(\theta +\alpha )}{\cos(\theta +\alpha )\cos(\theta -\alpha )}}\\&={\frac {(a_{2}\cos \alpha -a_{1}\cos \alpha )\cos \theta -(a_{2}\sin \alpha +a_{1}\sin \alpha )\sin \theta }{\cos ^{2}\alpha \ \cos ^{2}\theta -\sin ^{2}\alpha \ \sin ^{2}\theta }}.\end{aligned}}}

Combining constants gives

r = b cos θ + c sin θ cos 2 θ m 2 sin 2 θ {\displaystyle r={\frac {b\cos \theta +c\sin \theta }{\cos ^{2}\theta -m^{2}\sin ^{2}\theta }}}

which in Cartesian coordinates is

x 2 m 2 y 2 = b x + c y . {\displaystyle x^{2}-m^{2}y^{2}=bx+cy.}

This is a hyperbola passing through the origin. So the cissoid of two non-parallel lines is a hyperbola containing the pole. A similar derivation show that, conversely, any hyperbola is the cissoid of two non-parallel lines relative to any point on it.

Cissoids of Zahradnik

A cissoid of Zahradnik (named after Karel Zahradnik) is defined as the cissoid of a conic section and a line relative to any point on the conic. This is a broad family of rational cubic curves containing several well-known examples. Specifically:

  • The Trisectrix of Maclaurin given by
2 x ( x 2 + y 2 ) = a ( 3 x 2 y 2 ) {\displaystyle 2x(x^{2}+y^{2})=a(3x^{2}-y^{2})}
is the cissoid of the circle ( x + a ) 2 + y 2 = a 2 {\displaystyle (x+a)^{2}+y^{2}=a^{2}} and the line x = a 2 {\displaystyle x=-{\tfrac {a}{2}}} relative to the origin.
  • The right strophoid
y 2 ( a + x ) = x 2 ( a x ) {\displaystyle y^{2}(a+x)=x^{2}(a-x)}
is the cissoid of the circle ( x + a ) 2 + y 2 = a 2 {\displaystyle (x+a)^{2}+y^{2}=a^{2}} and the line x = a {\displaystyle x=-a} relative to the origin.
Animation visualizing the Cissoid of Diocles
  • The cissoid of Diocles
x ( x 2 + y 2 ) + 2 a y 2 = 0 {\displaystyle x(x^{2}+y^{2})+2ay^{2}=0}
is the cissoid of the circle ( x + a ) 2 + y 2 = a 2 {\displaystyle (x+a)^{2}+y^{2}=a^{2}} and the line x = 2 a {\displaystyle x=-2a} relative to the origin. This is, in fact, the curve for which the family is named and some authors refer to this as simply as cissoid.
  • The cissoid of the circle ( x + a ) 2 + y 2 = a 2 {\displaystyle (x+a)^{2}+y^{2}=a^{2}} and the line x = k a , {\displaystyle x=ka,} where k is a parameter, is called a Conchoid of de Sluze. (These curves are not actually conchoids.) This family includes the previous examples.
  • The folium of Descartes
x 3 + y 3 = 3 a x y {\displaystyle x^{3}+y^{3}=3axy}
is the cissoid of the ellipse x 2 x y + y 2 = a ( x + y ) {\displaystyle x^{2}-xy+y^{2}=-a(x+y)} and the line x + y = a {\displaystyle x+y=-a} relative to the origin. To see this, note that the line can be written
x = a 1 + p ,   y = p x {\displaystyle x=-{\frac {a}{1+p}},\ y=px}
and the ellipse can be written
x = a ( 1 + p ) 1 p + p 2 ,   y = p x . {\displaystyle x=-{\frac {a(1+p)}{1-p+p^{2}}},\ y=px.}
So the cissoid is given by
x = a 1 + p + a ( 1 + p ) 1 p + p 2 = 3 a p 1 + p 3 ,   y = p x {\displaystyle x=-{\frac {a}{1+p}}+{\frac {a(1+p)}{1-p+p^{2}}}={\frac {3ap}{1+p^{3}}},\ y=px}
which is a parametric form of the folium.

See also

  • Conchoid
  • Strophoid

References

  • J. Dennis Lawrence (1972). A catalog of special plane curves. Dover Publications. pp. 53–56. ISBN 0-486-60288-5.
  • C. A. Nelson "Note on rational plane cubics" Bull. Amer. Math. Soc. Volume 32, Number 1 (1926), 71-76.

External links

  • "Cissoid", Encyclopedia of Mathematics, EMS Press, 2001 [1994]
  • Weisstein, Eric W. "Cissoid". MathWorld.
  • 2D Curves