Nonlinear Tessellations

Background

Poles and Polars

Because a geodesic must lie on a circle orthogonal to the boundary of the Poincare disc, the center of this circle must lie outside the Poincare disc.
The center of this circle is called the pole of the geodesic.
If the geodesic is a diameter of the Poincare disc, its pole is the point at infinity.
For any point A in the Poincare disc, how many geodesics pass through A and what is the locus of the poles of these geodesics?

Call C the circle that bounds the Poincare disc.
Take A a point in the Poincare disc and A' the inverse of A with respect to C.
We have seen that if both A and A' lie on a circle, that circle is orthogonal to C, hence determines a geodesic through A.
So the set of poles of all geodesics through A is identical to the set of centers of all circles that contain both A and A'.

Several circles determining geodesics through A, together with their poles P1, P2, P3, and P4.

Infinitely many circles pass through A and A', and the locus of their centers is the perpendicular bisector of the segment AA'.
This locus of centers is called the polar of the point A.

Return to hyperbolic geometry.