The History of Mathematics: A Brief Course

(coco) #1

346 11. POST-EUCLIDEAN GEOMETRY


pseudonym Lobachevskii, since "it is hardly likely that two or even three people

knowing nothing of one another would produce almost the same result by different

routes."

5.5. The reception of non-Euclidean geometry. Some time was required for

the new world revealed by Lobachevskii and Bolyai to attract the interest of the

mathematical community. Because it seemed possible—even easy—to prove that

parallel lines exist, or equivalently, that the sum of the angles of a triangle could not

be more than two right angles, one can easily understand why a sense of symmetry

would lead to a certain stubbornness in attempts to refute the opposite hypothesis

as well. Although Gauss had shown the way to a more general understanding with

the concept of curvature of a surface, which could be either negative or positive, in

the 1825 paper on differential geometry (published in 1827, to be discussed in detail

in Sect. 3 of Chapter 12), it took Riemann's inaugural lecture in 1854 (published

in 1867, also discussed in detail in Sect. 3 of Chapter 12), which made the crucial

distinction between the unbounded and the infinite, to give the proper perspective.

After that, acceptance of non-Euclidean geometry was quite rapid. In 1868, the year

after the publication of Riemann's lecture, Eugenio Beltrami (1835-1900) realized

that Lobachevskii's theorems provide a model of the Lobachevskii-Bolyai plane in

a Euclidean disk. This model is described by Gray (1989, p. 112), as follows.

Imagine a directed line perpendicular to the Lobachevskii-Bolyai plane in

Lobachevskii-Bolyai three-dimensional space. The entire set of directed lines that

are parallel (asymptotic) to this line on the same side of the plane generates a

unique horosphere tangent to the plane at its point of intersection with the line.

Some of the lines parallel to the given perpendicular in the given direction intersect

the original plane, and others do not. Those that do intersect it pass through the

portion of the horosphere denoted Ù in Fig. 12. Shortest paths on the horosphere

are obtained as its intersections with planes passing through the point at infinity

that serves as its "center." These paths are called horocycles. But there is only one

horocycle through a given point in Ù that does not intersect a given horocycle, so

that the geometry of Ù is Euclidean. As a result, we have a faithful mapping of the

Lobachevskii-Bolyai plane onto the interior of a disk Ù in a Euclidean plane, under

which lines in the plane correspond to chords on the disk. This model provides

an excellent picture of points at infinity: they correspond to the boundary of the

disk Ù. Lines in the plane are parallel if and only if the chords corresponding to

them have a common endpoint. Lines that have a common perpendicular in the

Lobachevskii-Bolyai plane correspond to chords whose extensions meet outside the

circle. It is somewhat complicated to compute the length of a line segment in the

Lobachevskii-Bolyai plane from the length of its corresponding chordal segment in

Ù or vice versa, and the angle between two intersecting chords is not simply related

to the angle between the lines they correspond to.^23 Nevertheless these computa-

tions can be carried out from the trigonometric rules given by Lobachevskii. The

result is a perfect model of the Lobachevskii-Bolyai plane within the Euclidean

plane, obtained by formally reinterpreting the words line, plane, and angle. If

(^23) It can be shown that perpendicular lines correspond to chords having the property that the
extension of each passes through the point of intersection of the tangents at the endpoints of
the other. But it is far from obvious that this property is symmetric in the two chords, as
perpendicularity is for lines.

Free download pdf