next curve  previous curve  2D curves  3D curves  surfaces  fractals  polyhedra 
CASSINIAN OVAL
Curve studied by Cassini in 1680 and Malfatti in 1781.
Informal name: cat eyes. JeanDominique Cassini (16251712): French astronomer.

Bipolar equation:
, the pole O being the middle of the bipole ,
with .
Cartesian parametrization: (t = r); for the component on the right when , when . Polar equation: i.e., with , , the equation with " – " yielding real points only when e1 , with . Cartesian equation: , or , or or even:, for . Elliptic bicircular quartic (rational for e = 1).
Area of an oval for e < 1: (K = elliptic integral of the first kind). 
The Cassini ovals are the loci of the points on
the plane for which the geometric mean of the distances to two points,
the foci, is constant (= b).
They also are the field
lines of the vector field ,
sum of two orthoradial 1/r fields.
In the case when e < 1 (b < a), the "oval" is composed of two curves shaped like symmetrical eggs with respect to O with tripolar equations:
In this case, the curve is anallagmatic: invariant under the inversion of centre O and radius ; therefore we have a cyclic generation: the initial curve is the hyperbola with and , and the inversion circle (with radius Öp) is the Monge circle.
The Cassini oval as the envelope of the circles centred on a hyperbola and orthogonal to its Monge circle.
Here, the hyperbola is rectangular and the green circle reduces to
O.
In the case when e > 1, the real Cassini oval is no longer anallagmatic, but the complex curve still is, with a complex inversion radius.
For (): the oval has the shape of an "ellipse" that is worn out at the summits of the minor axis.
For (): the oval finally has an oval shape, leaning towards a circular shape as e increases to infinity.
In the case when e < 1, the equation can be written , where and (Wangerin's theorem link page 19).
The Cassini ovals also are the sections of a torus by
planes parallel to the axis, located at a distance to the axis equal to
the minor radius of the torus (here, section of a torus with major radius
R
= a and minor radius
by a plane located at distance r to the axis  the torus is thus
a spindle torus for )
; see spiric of Perseus.



The field lines of the magnetic field created by two parallel wires carrying currents of equal intensity in the same direction are, in any plane orthogonal to the wires, the Cassini ovals with foci the intersection points with the wires. The same is true for the equipotential lines of the electrostatic field created by two uniformly charged parallel wires with identical charge.
The orthogonal trajectories of the Cassini ovals are the rectangular hyperbolas with polar equation ; they are the electrostatic field lines in the physical interpretation above.
If, in the definition of the Cassini ovals, the geometric mean were replaced by the arithmetic mean, it would result in ellipses, and if it were replaced by the harmonic mean, it would yield Cayley ovals.
See the generalisation that are Cassinian curves, also compare with Booth curves and look at surfaces of Cassini.
next curve  previous curve  2D curves  3D curves  surfaces  fractals  polyhedra 
© Robert FERRÉOL 2017