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Parallel (geometry)

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In geometry, parallelism describes a specific relationship between lines, planes, or surfaces. Parallel lines are straight lines that exist within the same plane and never intersect.

Parallel (PSF)
Parallel (PSF)

This means they can extend to infinity in either direction without ever touching. Parallel planes are flat surfaces in three-dimensional space that never meet. In these cases, the distance between the objects remains constant. This concept is a fundamental property of affine and Euclidean geometries. It allows mathematicians to define how objects sit relative to one another in space.

In Euclidean space, there are several ways to identify parallel lines. One method is through equidistance, meaning every point on one line is the same distance from the other.

Parallel transversal
Parallel transversal

Another method uses a transversal, which is a third line that crosses the two parallel lines. When this happens, the corresponding angles created at the intersections are congruent, or identical. A third way involves direction; line segments are parallel if they share the same or opposite direction. While these properties are equivalent in Euclidean geometry, the simplest definition is often just that the lines exist in the same plane and do not intersect.

Parallelism can be categorized by the dimensions in which the objects exist. In a two-dimensional plane, we focus on parallel lines. In three-dimensional space, we can discuss parallel lines, parallel planes, or a line parallel to a plane. A line and a plane are parallel if the line does not lie in the plane and they never intersect. It is important to distinguish parallel lines from skew lines. Skew lines are lines in three-dimensional space that do not intersect, but they are not parallel because they are not in the same plane.

The history of these ideas stretches back to ancient Greece. Euclid provided a formal definition of parallel lines in Book I of his work, *Elements*.

Par-prob
Par-prob

Other thinkers like Posidonius and Geminus proposed alternative definitions, such as the idea of equidistant lines. During the nineteenth century, the way geometry was taught in England underwent significant changes. New developments in projective and non-Euclidean geometry pressured traditional textbooks to evolve. This led to debates between reformers and critics. Charles Dodgson, known as Lewis Carroll, even wrote a play titled *Euclid and His Modern Rivals* to criticize new teaching methods.

Mathematical reform in the 1800s attempted to redefine parallelism using different starting points. James Maurice Wilson published *Elementary Geometry* in 1868, which used the concept of direction. He defined parallel lines as straight lines that have the same direction but are not part of the same line. However, this approach faced heavy criticism from mathematicians like Augustus De Morgan. Other reformers tried using the transversal property or equidistance, but these often required adding new axioms to the system. These challenges showed how central the definition of parallelism is to the entire structure of geometry.

When we move into non-Euclidean geometry, the rules of parallelism change significantly. In these systems, the concept of a straight line is replaced by a geodesic, which is a curve that is locally straight. In hyperbolic geometry, there are three distinct possibilities for two geodesics in the same plane. They can be intersecting, parallel, or ultra parallel.

HyperParallel
HyperParallel

Limiting parallel lines converge toward a common limit point at infinity. Ultra parallel lines do not have a common limit point and actually diverge from one another.

Spherical geometry provides another fascinating contrast to Euclidean rules. On the surface of a sphere, there are no parallel lines at all. Every geodesic on a sphere is a great circle, and all great circles eventually intersect.

SphereParallel
SphereParallel

While you can find curves that stay a fixed distance from a great circle, such as parallels of latitude, these are not considered geodesics. This demonstrates how the curvature of a space completely transforms the fundamental properties of parallelism. These different geometric systems help scientists understand everything from local construction to the complex structure of spacetime in general relativity.

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File:Parallel (PSF).png
Parallel (PSF).png
File:Parallel transversal.svg
Parallel transversal.svg
File:Par-prob.png
Par-prob.png
File:HyperParallel.png
HyperParallel.png
File:SphereParallel.png
SphereParallel.png
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