Elliptic geometry

Geometry

Projecting a sphere to a plane.

Branches

Concepts
Features

Dimension

Compass-and-straightedge constructions

Zero / One-dimensional

Two-dimensional

Triangle
Plane Area Polygon
Altitude Hypotenuse Pythagorean theorem
Parallelogram
Square Rectangle Rhombus Rhomboid
Quadrilateral
Trapezoid Kite
Circle
Diameter Circumference Area

Three-dimensional

Volume

Four- / other-dimensional

Geometers

by name

by period

BCE
Ahmes Baudhayana Manava Pythagoras Euclid Archimedes Apollonius
1–1400s
Zhang Kātyāyana Aryabhata Brahmagupta Virasena Alhazen Sijzi Khayyám al-Yasamin al-Tusi Yang Hui Parameshvara
1400s–1700s
Jyeṣṭhadeva Descartes Pascal Minggatu Euler Sakabe Aida
1700s–1900s
Gauss Lobachevsky Bolyai Riemann Klein Poincaré Hilbert Minkowski Cartan Veblen Coxeter
Present day
Atiyah Gromov

Elliptic geometry, a special case of Riemannian geometry, is a non-Euclidean geometry, in which, given a line L and a point p outside L, there exists no line parallel to L passing through p, as all lines in elliptic geometry intersect. Elliptic geometry has a variety of properties that differ from those of classical Euclidean plane geometry. For example, the sum of the interior angles of any triangle is always greater than 180°.

Definitions

In elliptic geometry, two lines perpendicular to a given line must intersect. In fact, the perpendiculars on one side all intersect at the absolute pole of the given line. The perpendiculars on the other side also intersect at a point, which is different from the other absolute pole only in spherical geometry, for in elliptic geometry the poles on either side are the same. There are no antipodal points in elliptic geometry. Every point corresponds to an absolute polar line of which it is the absolute pole. Any point on this polar line forms an absolute conjugate pair with the pole. Such a pair of points is orthogonal, and the distance between them is a quadrant.^[1]^:89

The distance between a pair of points is proportional to the angle between their absolute polars.^[1]^:101

As explained by H. S. M. Coxeter

The name "elliptic" is possibly misleading. It does not imply any direct connection with the curve called an ellipse, but only a rather far-fetched analogy. A central conic is called an ellipse or a hyperbola according as it has no asymptote or two asymptotes. Analogously, a non-Euclidean plane is said to be elliptic or hyperbolic according as each of its lines contains no point at infinity or two points at infinity.^[2]

Two dimensions

The spherical model

On a sphere, the sum of the angles of a triangle is not equal to 180°. The surface of a sphere is not a Euclidean space, but locally the laws of the Euclidean geometry are good approximations. In a small triangle on the face of the earth, the sum of the angles is very nearly 180°.

A simple way to picture elliptic geometry is to look at a globe. Neighboring lines of longitude appear to be parallel at the equator, yet they intersect at the poles.

More precisely, the surface of a sphere is a model of elliptic geometry if lines are modeled by great circles, and points at each other's antipodes are considered to be the same point. With this identification of antipodal points, the model satisfies Euclid's first postulate, which states that two points uniquely determine a line. If the antipodal points were considered to be distinct, as in spherical geometry, then uniqueness would be violated, e.g., the lines of longitude on the Earth's surface all pass through both the north pole and the south pole.

Although models such as the spherical model are useful for visualization and for proof of the theory's self-consistency, neither a model nor an embedding in a higher-dimensional space is logically necessary. For example, Einstein's theory of general relativity has static solutions in which space containing a gravitational field is (locally) described by three-dimensional elliptic geometry, but the theory does not posit the existence of a fourth spatial dimension, or even suggest any way in which the existence of a higher-dimensional space could be detected. (This is unrelated to the treatment of time as a fourth dimension in relativity.) Metaphorically, we can imagine geometers who are like ants living on the surface of a sphere. Even if the ants are unable to move off the surface, they can still construct lines and verify that parallels do not exist. The existence of a third dimension is irrelevant to the ants' ability to do geometry, and its existence is neither verifiable nor necessary from their point of view. Another way of putting this is that the language of the theory's axioms is incapable of expressing the distinction between one model and another.

Comparison with Euclidean geometry

In Euclidean geometry, a figure can be scaled up or scaled down indefinitely, and the resulting figures are similar, i.e., they have the same angles and the same internal proportions. In elliptic geometry this is not the case. For example, in the spherical model we can see that the distance between any two points must be strictly less than half the circumference of the sphere (because antipodal points are identified). A line segment therefore cannot be scaled up indefinitely. A geometer measuring the geometrical properties of the space he or she inhabits can detect, via measurements, that there is a certain distance scale that is a property of the space. On scales much smaller than this one, the space is approximately flat, geometry is approximately Euclidean, and figures can be scaled up and down while remaining approximately similar.

A great deal of Euclidean geometry carries over directly to elliptic geometry. For example, the first and fourth of Euclid's postulates, that there is a unique line between any two points and that all right angles are equal, hold in elliptic geometry. Postulate 3, that one can construct a circle with any given center and radius, fails if "any radius" is taken to mean "any real number", but holds if it is taken to mean "the length of any given line segment". Therefore any result in Euclidean geometry that follows from these three postulates will hold in elliptic geometry, such as proposition 1 from book I of the Elements, which states that given any line segment, an equilateral triangle can be constructed with the segment as its base.

Elliptic geometry is also like Euclidean geometry in that space is continuous, homogeneous, isotropic, and without boundaries. Isotropy is guaranteed by the fourth postulate, that all right angles are equal. For an example of homogeneity, note that Euclid's proposition I.1 implies that the same equilateral triangle can be constructed at any location, not just in locations that are special in some way. The lack of boundaries follows from the second postulate, extensibility of a line segment.

One way in which elliptic geometry differs from Euclidean geometry is that the sum of the interior angles of a triangle is greater than 180 degrees. In the spherical model, for example, a triangle can be constructed with vertices at the locations where the three positive Cartesian coordinate axes intersect the sphere, and all three of its internal angles are 90 degrees, summing to 270 degrees. For sufficiently small triangles, the excess over 180 degrees can be made arbitrarily small.

The Pythagorean theorem fails in elliptic geometry. In the 90°–90°–90° triangle described above, all three sides have the same length, and consequently do not satisfy $a^{2}+b^{2}=c^{2}$ . The Pythagorean result is recovered in the limit of small triangles.

The ratio of a circle's circumference to its area is smaller than in Euclidean geometry. In general, area and volume do not scale as the second and third powers of linear dimensions.

Elliptic space

Elliptic space can be constructed in a way similar to the construction of three-dimensional vector space: with equivalence classes. One uses directed arcs on great circles of the sphere. As directed line segments are equipollent when they are parallel, of the same length, and similarly oriented, so directed arcs found on great circles are equipollent when they are of the same length, orientation, and great circle. These relations of equipollence produce 3D vector space and elliptic space, respectively.

Access to elliptic space structure is provided through the vector algebra of William Rowan Hamilton: he envisioned a sphere as a domain of square roots of minus one. Then Euler's formula $\exp(\theta r)=\cos \theta +r\sin \theta$ (where r is on the sphere) represents the great circle in the plane perpendicular to r. Opposite points r and –r correspond to oppositely directed circles. An arc between θ and φ is equipollent with one between 0 and φ – θ. In elliptic space, arc length is less than π, so arcs may be parametrized with θ in [0, π) or (–π/2, π/2].^[3]

For $z=\exp(\theta r),\ z^{*}=\exp(-\theta r)\implies zz^{*}=1.$ It is said that the modulus or norm of z is one (Hamilton called it the tensor of z). But since r ranges over a sphere in 3-space, exp(θ r) ranges over a sphere in 4-space, now called the 3-sphere, as its surface has three dimensions. Hamilton called his algebra quaternions and it quickly became a useful and celebrated tool of mathematics. Its space of four dimensions is evolved in polar co-ordinates $t\exp(\theta r),$ with t in the positive real numbers.

When doing trigonometry on Earth or the celestial sphere, the sides of the triangles are great circle arcs. The first success of quaternions was a rendering of spherical trigonometry to algebra.^[4] Hamilton called a quaternion of norm one a versor, and these are the points of elliptic space.

With $r$ fixed, the versors

e^{ar},\quad 0\leq a<\pi

form an elliptic line. The distance from $e^{ar}$ to 1 is $a$ . For an arbitrary versor $u$ , the distance will be that θ for which $cos θ = (u + u *)/2$ since this is the formula for the scalar part of any quaternion.

An elliptic motion is described by the quaternion mapping

q\mapsto uqv,

where

u

and

v

are fixed versors.

Distances between points are the same as between image points of an elliptic motion. In the case that $u$ and $v$ are quaternion conjugates of one another, the motion is a spatial rotation, and their vector part is the axis of rotation. In the case $u = 1$ the elliptic motion is called a right Clifford translation, or a parataxy. The case $v = 1$ corresponds to left Clifford translation.

Elliptic lines through versor $u$ may be of the form

\lbrace ue^{ar}:0\leq a<\pi \rbrace

\lbrace e^{ar}u:0\leq a<\pi \rbrace

for a fixed

r

They are the right and left Clifford translations of $u$ along an elliptic line through 1. The elliptic space is formed by identifying antipodal points on $S 3$ giving a real projective space.^[5]

Elliptic space has special structures called Clifford parallels and Clifford surfaces.

The versor points of elliptic space are mapped by the Cayley transform to ℝ³ for an alternative representation of the space.

Higher-dimensional spaces

Hyperspherical model

The hyperspherical model is the generalization of the spherical model to higher dimensions. The points of n-dimensional elliptic space are the pairs of unit vectors $(x, - x)$ in Rⁿ⁺¹, that is, pairs of opposite points on the surface of the unit ball in (n + 1)-dimensional space (the n-dimensional hypersphere). Lines in this model are great circles, i.e., intersections of the hypersphere with flat hypersurfaces of dimension n passing through the origin.

Projective elliptic geometry

In the projective model of elliptic geometry, the points of n-dimensional real projective space are used as points of the model. This models an abstract elliptic geometry that is also known as projective geometry.

The points of n-dimensional projective space can be identified with lines through the origin in (n + 1)-dimensional space, and can be represented non-uniquely by nonzero vectors in Rⁿ⁺¹, with the understanding that $u$ and $λ u$ , for any non-zero scalar $λ$ , represent the same point. Distance is defined using the metric

d(u,v)=\arccos \left({\frac {|u\cdot v|}{\|u\|\ \|v\|}}\right);

that is, the distance between two points is the angle between their corresponding lines in Rⁿ⁺¹. The distance formula is homogeneous in each variable, with $d (λ u, μ v) = d (u, v)$ if $λ$ and $μ$ are non-zero scalars, so it does define a distance on the points of projective space.

A notable property of the projective elliptic geometry is that for even dimensions, such as the plane, the geometry is non-orientable. It erases the distinction between clockwise and counterclockwise rotation by identifying them.

Stereographic model

A model representing the same space as the hyperspherical model can be obtained by means of stereographic projection. Let Eⁿ represent Rⁿ ∪ {∞}, that is, $n$ -dimensional real space extended by a single point at infinity. We may define a metric, the chordal metric, on Eⁿ by

\delta (u,v)={\frac {2\|u-v\|}{\sqrt {(1+\|u\|^{2})(1+\|v\|^{2})}}}

where $u$ and $v$ are any two vectors in Rⁿ and $\|\cdot \|$ is the usual Euclidean norm. We also define

\delta (u,\infty )=\delta (\infty ,u)={\frac {2}{\sqrt {1+\|u\|^{2}}}}.

The result is a metric space on Eⁿ, which represents the distance along a chord of the corresponding points on the hyperspherical model, to which it maps bijectively by stereographic projection. We obtain a model of spherical geometry if we use the metric

d(u,v)=2\arcsin \left({\frac {\delta (u,v)}{2}}\right).

Elliptic geometry is obtained from this by identifying the points $u$ and $- u$ , and taking the distance from $v$ to this pair to be the minimum of the distances from $v$ to each of these two points.

Self-consistency

Because spherical elliptic geometry can be modeled as, for example, a spherical subspace of a Euclidean space, it follows that if Euclidean geometry is self-consistent, so is spherical elliptic geometry. Therefore it is not possible to prove the parallel postulate based on the other four postulates of Euclidean geometry.

Tarski proved that elementary Euclidean geometry is complete: there is an algorithm which, for every proposition, can show it to be either true or false.^[6] (This does not violate Gödel's theorem, because Euclidean geometry cannot describe a sufficient amount of arithmetic for the theorem to apply.^[7]) It therefore follows that elementary elliptic geometry is also self-consistent and complete.

Notes

1 2 Duncan Sommerville (1914) The Elements of Non-Euclidean Geometry, chapter 3 Elliptic geometry, pp 88 to 122, George Bell & Sons
↑ Coxeter 1969 94
↑ Rafael Artzy (1965) Linear Geometry, Chapter 3–8 Quaternions and Elliptic Three-space, pp. 186–94,Addison-Wesley
↑ W.R. Hamilton(1844 to 1850) On quaternions or a new system of imaginaries in algebra, Philosophical Magazine, link to David R. Wilkins collection at Trinity College, Dublin
↑
Georges Lemaître (1948) "Quaternions et espace elliptique", Acta Pontifical Academy of Sciences 12:57–78.
- H.S.M. Coxeter, English synopsis of Lemaître in Mathematical Reviews
↑ Tarski (1951)
↑ Franzén 2005, pp. 25–26.

References

Alan F. Beardon, The Geometry of Discrete Groups, Springer-Verlag, 1983
H. S. M. Coxeter (1942) Non-Euclidean Geometry, chapters 5, 6, & 7: Elliptic geometry in 1, 2, & 3 dimensions, University of Toronto Press, reissued 1998 by Mathematical Association of America, ISBN 0-88385-522-4 .
H.S.M. Coxeter (1969) Introduction to Geometry, §6.9 The Elliptic Plane, pp. 92–95. John Wiley & Sons.
Hazewinkel, Michiel, ed. (2001), "Elliptic geometry", Encyclopedia of Mathematics, Springer, ISBN 978-1-55608-010-4
Felix Klein (1871) "On the so-called noneuclidean geometry" Mathematische Annalen 4:573–625, translated and introduced in John Stillwell (1996) Sources of Hyperbolic Geometry, American Mathematical Society ISBN 0-8218-0529-0 .
Boris Odehnal "On isotropic congruences of lines in elliptic three-space"
Eduard Study (1913) D.H. Delphenich translator, "Foundations and goals of analytical kinematics", page 20.
Alfred Tarski (1951) A Decision Method for Elementary Algebra and Geometry. Univ. of California Press.
Franzén, Torkel (2005). Gödel's Theorem: An Incomplete Guide to its Use and Abuse. AK Peters. ISBN 1-56881-238-8.
Alfred North Whitehead (1898) Universal Algebra, Book VI Chapter 2: Elliptic Geometry, pp 371–98.

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