than Euclid's other assumptions The author discusses the (such as the one that states fundamentals of plane hyperbolic that two points determine exgeometry and describes a method for generating hyperbolic tilings by actly one line), and for a long computer, based on the recently detime people tried to prove its veloped theory of automatic groups. redundancy within the Euclidean framework. However, by the 1820s at least three people had independently discovered that a selfconsistent geometry that does not satisfy the parallel axiom could be built: Janos Bolyai in Hungary, Carl Friedrich Gauss in Germany and Nikolai Ivanovich Lobachevskii in Russia [4]. Their creation became known as Lobachevskiian geometry until Felix Klein, at the turn of this century, introduced the now more common term hyperbolic geometry. (The term non-Euclidean geometry is also commonly used, but it encompasses geometries other than the hyperbolic.) The denial of one of Euclid's axioms remained a profoundly disturbing idea, and it was not until the second half of the century that the general mathematical public started to get a clear grasp of the nature of hyperbolic geometry. This understanding was much aided by the construction by Eugenio Beltrami [5], in 1866, of an explicit model of hyperbolic geometry-something like a map of hyperbolic space that can be drawn on a piece of Euclidean paper. This model, now known as the projective, or Klein model, after its popularizer, represents n-dimensional hyperbolic space by an open ball {(Xl.,'Xn)ERn X+ 2 <* I+<} in Euclidean space, and hyperbolic lines by Euclidean straight-line segments in the ball. Figure 1 shows that, given a line L and a point P outside of L, there are infinitely many Silvio Levy (mathematician, editor), Geometry Center, University of Minnesota, 1300 S. Second St., Minneapolis, MN 55454, U.S.A. Received 13 March 1991. LEONARDO, Vol. 25, No. 3, pp. 349-354, 1992 349 This content downloaded from 157.55.39.255 on Mon, 01 Aug 2016 05:43:04 UTC All use subject to http://about.jstor.org/terms Fig. 2. A tiling of the hyperbolic plane, shown in the Klein model. All the pentagons shown here are congruent and rightangled. The sum of the angles of a hyperbolic polygon is always less than what it would be for a Euclidean polygon of the same number of sides, and the difference is equal to the polygon's hyperbolic area. Fig. 3. The same tiling of Fig. 2, shown in the Poincare disk model. parallels to L through P, that is, lines that are coplanar with L but do not intersect it. (Sometimes only lines that meet at infinity, that is, on the circle that bounds the Klein model, are called parallel, while lines that meet outside infinity are called ultraparallel. I will not enforce this distinction.) Although the Klein model is projectively correct-that is, it represents straight lines by straight lines-it distorts shapes drastically. As one moves away from the center of the disk, an object of constant hyperbolic size quickly starts looking very small in the model and also gets flattened against the edge. Figure 2 shows a number of identical regular pentagons, which tile the hyperbolic plane much as squares tile the Euclidean plane. The tile at the center appears much bigger than its closest neighbors, and just a few layers out the triangles are already too small to make out. The figure also makes clear how the Klein model Fig. 4. Circles centered at Pare mapped to Fig. 5. The locus of themselves by rotations around P. Notice from a fixed hyperb that a hyperbolic circle in the Poincare appears as an arc of model appears round, although other model, but it does ni shapes are preserved only approximately. orthogonally, therefo poi1 olic
Read full abstract