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Non-Euclidean geometry

In mathematics, non-Euclidean geometry consists of two geometries based on axioms closely related to those that specify Euclidean geometry. As Euclidean geometry lies at the intersection of metric geometry and affine geometry, non-Euclidean geometry arises by either replacing the parallel postulate with an alternative, or relaxing the metric requirement. In the former case, one obtains hyperbolic geometry and elliptic geometry, the traditional non-Euclidean geometries. When the metric requirement is relaxed, then there are affine planes associated with the planar algebras, which give rise to kinematic geometries that have also been called non-Euclidean geometry.

In Euclidean geometry, the lines remain at a constant from each other (meaning that a line drawn perpendicular to one line at any point will intersect the other line and the length of the line segment joining the points of intersection remains constant) and are known as parallels.

distance

In hyperbolic geometry, they "curve away" from each other, increasing in distance as one moves further from the points of intersection with the common perpendicular; these lines are often called .

ultraparallels

In elliptic geometry, the lines "curve toward" each other and intersect.

The essential difference between the metric geometries is the nature of parallel lines. Euclid's fifth postulate, the parallel postulate, is equivalent to Playfair's postulate, which states that, within a two-dimensional plane, for any given line l and a point A, which is not on l, there is exactly one line through A that does not intersect l. In hyperbolic geometry, by contrast, there are infinitely many lines through A not intersecting l, while in elliptic geometry, any line through A intersects l.


Another way to describe the differences between these geometries is to consider two straight lines indefinitely extended in a two-dimensional plane that are both perpendicular to a third line (in the same plane):

Either there will exist more than one line through the point parallel to the given line or there will exist no lines through the point parallel to the given line. In the first case, replacing the parallel postulate (or its equivalent) with the statement "In a plane, given a point P and a line l not passing through P, there exist two lines through P, which do not meet l" and keeping all the other axioms, yields .[20]

hyperbolic geometry

The second case is not dealt with as easily. Simply replacing the parallel postulate with the statement, "In a plane, given a point P and a line l not passing through P, all the lines through P meet l", does not give a consistent set of axioms. This follows since parallel lines exist in absolute geometry, but this statement says that there are no parallel lines. This problem was known (in a different guise) to Khayyam, Saccheri and Lambert and was the basis for their rejecting what was known as the "obtuse angle case". To obtain a consistent set of axioms that includes this axiom about having no parallel lines, some other axioms must be tweaked. These adjustments depend upon the axiom system used. Among others, these tweaks have the effect of modifying Euclid's second postulate from the statement that line segments can be extended indefinitely to the statement that lines are unbounded. Riemann's elliptic geometry emerges as the most natural geometry satisfying this axiom.

[21]

Euclidean geometry can be axiomatically described in several ways. However, Euclid's original system of five postulates (axioms) is not one of these, as his proofs relied on several unstated assumptions that should also have been taken as axioms. Hilbert's system consisting of 20 axioms[18] most closely follows the approach of Euclid and provides the justification for all of Euclid's proofs. Other systems, using different sets of undefined terms obtain the same geometry by different paths. All approaches, however, have an axiom that is logically equivalent to Euclid's fifth postulate, the parallel postulate. Hilbert uses the Playfair axiom form, while Birkhoff, for instance, uses the axiom that says that, "There exists a pair of similar but not congruent triangles." In any of these systems, removal of the one axiom equivalent to the parallel postulate, in whatever form it takes, and leaving all the other axioms intact, produces absolute geometry. As the first 28 propositions of Euclid (in The Elements) do not require the use of the parallel postulate or anything equivalent to it, they are all true statements in absolute geometry.[19]


To obtain a non-Euclidean geometry, the parallel postulate (or its equivalent) must be replaced by its negation. Negating the Playfair's axiom form, since it is a compound statement (... there exists one and only one ...), can be done in two ways:

A is a quadrilateral with three right angles. The fourth angle of a Lambert quadrilateral is acute if the geometry is hyperbolic, a right angle if the geometry is Euclidean or obtuse if the geometry is elliptic. Consequently, rectangles exist (a statement equivalent to the parallel postulate) only in Euclidean geometry.

Lambert quadrilateral

A is a quadrilateral with two sides of equal length, both perpendicular to a side called the base. The other two angles of a Saccheri quadrilateral are called the summit angles and they have equal measure. The summit angles of a Saccheri quadrilateral are acute if the geometry is hyperbolic, right angles if the geometry is Euclidean and obtuse angles if the geometry is elliptic.

Saccheri quadrilateral

The sum of the measures of the angles of any triangle is less than 180° if the geometry is hyperbolic, equal to 180° if the geometry is Euclidean, and greater than 180° if the geometry is elliptic. The defect of a triangle is the numerical value (180° − sum of the measures of the angles of the triangle). This result may also be stated as: the defect of triangles in hyperbolic geometry is positive, the defect of triangles in Euclidean geometry is zero, and the defect of triangles in elliptic geometry is negative.

Euclidean and non-Euclidean geometries naturally have many similar properties, namely those that do not depend upon the nature of parallelism. This commonality is the subject of absolute geometry (also called neutral geometry). However, the properties that distinguish one geometry from others have historically received the most attention.


Besides the behavior of lines with respect to a common perpendicular, mentioned in the introduction, we also have the following:

Importance[edit]

Before the models of a non-Euclidean plane were presented by Beltrami, Klein, and Poincaré, Euclidean geometry stood unchallenged as the mathematical model of space. Furthermore, since the substance of the subject in synthetic geometry was a chief exhibit of rationality, the Euclidean point of view represented absolute authority.


The discovery of the non-Euclidean geometries had a ripple effect which went far beyond the boundaries of mathematics and science. The philosopher Immanuel Kant's treatment of human knowledge had a special role for geometry. It was his prime example of synthetic a priori knowledge; not derived from the senses nor deduced through logic — our knowledge of space was a truth that we were born with. Unfortunately for Kant, his concept of this unalterably true geometry was Euclidean. Theology was also affected by the change from absolute truth to relative truth in the way that mathematics is related to the world around it, that was a result of this paradigm shift.[23]


Non-Euclidean geometry is an example of a scientific revolution in the history of science, in which mathematicians and scientists changed the way they viewed their subjects.[24] Some geometers called Lobachevsky the "Copernicus of Geometry" due to the revolutionary character of his work.[25][26]


The existence of non-Euclidean geometries impacted the intellectual life of Victorian England in many ways[27] and in particular was one of the leading factors that caused a re-examination of the teaching of geometry based on Euclid's Elements. This curriculum issue was hotly debated at the time and was even the subject of a book, Euclid and his Modern Rivals, written by Charles Lutwidge Dodgson (1832–1898) better known as Lewis Carroll, the author of Alice in Wonderland.

In 1895, published the short story "The Remarkable Case of Davidson's Eyes". To appreciate this story one should know how antipodal points on a sphere are identified in a model of the elliptic plane. In the story, in the midst of a thunderstorm, Sidney Davidson sees "Waves and a remarkably neat schooner" while working in an electrical laboratory at Harlow Technical College. At the story's close, Davidson proves to have witnessed H.M.S. Fulmar off Antipodes Island.

H. G. Wells

Non-Euclidean geometry is sometimes connected with the influence of the 20th-century writer H. P. Lovecraft. In his works, many unnatural things follow their own unique laws of geometry: in Lovecraft's Cthulhu Mythos, the sunken city of R'lyeh is characterized by its non-Euclidean geometry. It is heavily implied this is achieved as a side effect of not following the natural laws of this universe rather than simply using an alternate geometric model, as the sheer innate wrongness of it is said to be capable of driving those who look upon it insane.[35]

horror fiction

The main character in 's Zen and the Art of Motorcycle Maintenance mentioned Riemannian geometry on multiple occasions.

Robert Pirsig

In , Dostoevsky discusses non-Euclidean geometry through his character Ivan.

The Brothers Karamazov

Christopher Priest's novel describes the struggle of living on a planet with the form of a rotating pseudosphere.

Inverted World

Robert Heinlein's utilizes non-Euclidean geometry to explain instantaneous transport through space and time and between parallel and fictional universes.

The Number of the Beast

Zeno Rogue's is a roguelike game set on the hyperbolic plane, allowing the player to experience many properties of this geometry. Many mechanics, quests, and locations are strongly dependent on the features of hyperbolic geometry.[36]

HyperRogue

In the science fiction setting for FASA's wargame, role-playing-game and fiction, faster-than-light travel and communications is possible through the use of Hsieh Ho's Polydimensional Non-Euclidean Geometry, published sometime in the middle of the 22nd century.

Renegade Legion

In Flatterland the protagonist Victoria Line visits all kinds of non-Euclidean worlds.

Ian Stewart's

Non-Euclidean geometry often makes appearances in works of science fiction and fantasy.

Hyperbolic space

Lénárt sphere

Projective geometry

Non-Euclidean surface growth

Parallel (geometry)#In non-Euclidean geometry

Spherical geometry#Relation to similar geometries

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ISBN

Anderson, James W. Hyperbolic Geometry, second edition, Springer, 2005

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ISBN

Euclid and His Modern Rivals, New York: Barnes and Noble, 2009 (reprint) ISBN 978-1-4351-2348-9

Carroll, Lewis

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H. S. M. Coxeter

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ISBN

Jeremy Gray (1989) Ideas of Space: Euclidean, Non-Euclidean, and Relativistic, 2nd edition, .

Clarendon Press

Euclidean and Non-Euclidean Geometries: Development and History, 4th ed., New York: W. H. Freeman, 2007. ISBN 0-7167-9948-0

Greenberg, Marvin Jay

(1972) Mathematical Thought from Ancient to Modern Times, Chapter 36 Non-Euclidean Geometry, pp 861–81, Oxford University Press.

Morris Kline

(2012) " A New Perspective on Relativity : An Odyssey In Non-Euclidean Geometries", World Scientific, pp. 696, ISBN 9789814340489.

Bernard H. Lavenda

(2010) Pangeometry, Translator and Editor: A. Papadopoulos, Heritage of European Mathematics Series, vol. 4, European Mathematical Society.

Nikolai Lobachevsky

Manning, Henry Parker (1963), Introductory Non-Euclidean Geometry, New York: Dover

Meschkowski, Herbert (1964), Noneuclidean Geometry, New York: Academic Press

Milnor, John W. (1982) , Bull. Amer. Math. Soc. (N.S.) Volume 6, Number 1, pp. 9–24.

Hyperbolic geometry: The first 150 years

(1988), Mathematical Visions: The Pursuit of Geometry in Victorian England, Boston: Academic Press, ISBN 0-12-587445-6

Richards, Joan L.

Smart, James R. (1997), Modern Geometries (5th Ed.), Pacific Grove: Brooks/Cole,  0-534-35188-3

ISBN

(2001) Flatterland, New York: Perseus Publishing ISBN 0-7382-0675-X (softcover)

Stewart, Ian

(1996) Sources of Hyperbolic Geometry, American Mathematical Society ISBN 0-8218-0529-0 .

John Stillwell

Trudeau, Richard J. (1987), , Boston: Birkhauser, ISBN 0-8176-3311-1

The Non-Euclidean Revolution

(2014) La théorie des parallèles de Johann Heinrich Lambert, Critical edition of Lambert's memoir with a French translation, with historical and mathematical notes and commentaries éd. Blanchard, coll. Sciences dans l'Histoire, Paris ISBN 978-2-85367-266-5

A. Papadopoulos et Guillaume Théret

Media related to Non-Euclidean geometry at Wikimedia Commons