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<record version="19" id="4669">
 <title>non-Euclidean geometry</title>
 <name>NonEuclideanGeometry</name>
 <created>2003-08-29 16:43:33</created>
 <modified>2007-06-11 04:36:52</modified>
 <type>Definition</type>
<parent id="3824">geometry</parent>
 <creator id="1863" name="Wkbj79"/>
 <author id="1863" name="Wkbj79"/>
 <author id="1243" name="vmoraru"/>
 <classification>
	<category scheme="msc" code="51-00"/>
	<category scheme="msc" code="51M10"/>
 </classification>
 <defines>
	<concept>hyperbolic geometry</concept>
	<concept>Bolyai-Lobachevski geometry</concept>
	<concept>elliptic geometry</concept>
	<concept>spherical geometry</concept>
	<concept>semi-Euclidean geometry</concept>
 </defines>
 <related>
	<object name="Sphere"/>
	<object name="ComparisonOfCommonGeometries"/>
 </related>
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A \emph{non-Euclidean geometry} is a \PMlinkescapetext{geometry} in which at least one of the axioms from Euclidean geometry fails.  Within this entry, only geometries that are considered to be two-dimensional will be considered.

The most common non-Euclidean geometries are those in which the parallel postulate fails; \PMlinkname{i.e.}{Ie}, there is not a unique line that does not intersect a given line through a point not on the given line.  Note that this is equivalent to saying that the sum of the angles of a triangle is not equal to $\pi$ radians.

If there is more than one such parallel line, the \PMlinkescapetext{geometry} is called \emph{hyperbolic} (or \emph{Bolyai-Lobachevski}).  In these \PMlinkescapetext{types} of \PMlinkescapetext{geometries}, the sum of the angles of a triangle is strictly in \PMlinkescapetext{between} $0$ and $\pi$ radians.  (This sum is not constant as in Euclidean geometry; it depends on the area of the triangle.  See the entry regarding defect for more details.)

As an example, consider the disc $\{(x,y) \in \mathbb{R}^2 : x^2+y^2&lt;1 \}$ in which a point is similar to the Euclidean point and a line is defined to be a chord (excluding its endpoints) of the (\PMlinkname{circular}{Circle}) boundary.  This is the Beltrami-Klein model for $\mathbb{H}^2$.  It is relatively easy to see that, in this \PMlinkescapetext{geometry}, given a line and a point not on the line, there are infinitely many lines passing through the point that are parallel to the given line.

If there is no parallel line, the \PMlinkescapetext{geometry} is called \emph{spherical} (or \emph{elliptic}).  In these \PMlinkescapetext{types} of \PMlinkescapetext{geometries}, the sum of the angles of a triangle is strictly in \PMlinkescapetext{between} $\pi$ and $3\pi$ radians.  (This sum is not constant as in Euclidean geometry; it depends on the area of the triangle.  See the entries regarding \PMlinkname{defect}{Defect} and area of a spherical triangle for more details.)

As an example, consider the surface of the \PMlinkname{unit sphere}{Sphere} $\{(x,y,z) \in \mathbb{R}^3 : x^2+y^2+z^2=1 \}$ in which a point is similar to the Euclidean point and a line is defined to be a great circle.  (Note that, when a sphere serves as a model of spherical geometry, its radius is typically assumed to be 1.)  It is relatively easy to see that, in this \PMlinkescapetext{geometry}, given a line and a point not on the line, it is impossible to find a line passing through the point that does not intersect the given line.

Note also that, in spherical geometry, two distinct points do not necessarily determine a unique line; however, two distinct points that are not antipodal always determine a unique line.

One final example of a non-Euclidean \PMlinkescapetext{geometry} is \emph{semi-Euclidean geometry}, in which the axiom of Archimedes fails.</content>
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