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[[Image:Cartesian-coordinate-system.svg|right|thumb|300px|Bi-dimensional Cartesian coordinate system]]
 
'''Bi-dimensional space''' is a geometric model of the planar projection of the physical [[universe]] in which we live. 
The two dimensions are commonly called length and width. Both directions lie in the same [[plane (geometry)|plane]].
 
In [[physics]] and [[mathematics]], a [[real coordinate space|sequence of ''n'' real numbers]] can be understood as a [[point (geometry)|location]] in ''n''-dimensional space. When ''n'' = 2, the set of all such locations is called '''2-dimensional space''' or '''bi-dimensional space''', and usually is thought of as an [[Euclidean space]].
 
In physics, our bi-dimensional space is viewed as a planar representation of the space in which we move, described as bi-dimensional space or two-dimensional space.
 
==History of two-dimensional space==
[[Euclid's Elements]] dealt almost exclusively with two-dimensional geometry, developing such notions as similarity of shapes, the [[Pythagorean theorem]] (Proposition 47), equality of angles and [[area]]s, parallelism, the sum of the angles in a triangle, and the three cases in which triangles are "equal" (have the same area), among many other topics.
 
Later, the plane was described in a so-called ''Cartesian coordinate system'', a [[coordinate system]] that specifies each [[point (geometry)|point]] uniquely in a [[plane (geometry)|plane]] by a pair of [[number|numerical]] '''coordinates''', which are the [[positive and negative numbers|signed]] distances from the point to two fixed [[perpendicular]] directed lines, measured in the same [[unit length|unit of length]]. Each reference line is called a ''coordinate axis'' or just ''axis'' of the system, and the point where they meet is its ''[[Origin (mathematics)|origin]]'', usually at ordered pair (0,&#8239;0). The coordinates can also be defined as the positions of the [[orthogonal projection|perpendicular projections]] of the point onto the two axes, expressed as signed distances from the origin.
 
The idea of this system was developed in 1637 in writings by Descartes and independently by [[Pierre de Fermat]], although Fermat also worked in three dimensions, and did not publish the discovery.<ref>{{cite encyclopedia|title=analytic geometry|encyclopedia=Encyclopædia Britannica|year=2008|edition=Encyclopædia Britannica Online|accessdate=2 August 2008}}</ref> Both authors used a single axis in their treatments and have a variable length measured in reference to this axis. The concept of using a pair of axes was introduced later, after Descartes' ''[[La Géométrie]]'' was translated into Latin in 1649 by [[Frans van Schooten]] and his students. These commentators  introduced several concepts while trying to clarify the ideas contained in Descartes' work.<ref>{{harvnb|Burton|2011|loc=p. 374}}</ref>
 
Later, the plane was thought of as a [[field (mathematics) |field]], where any two points could be multiplied and, except for 0, divided. This was known as the [[complex plane]]. The complex plane is sometimes called the Argand plane because it is used in Argand diagrams. These are named after [[Jean-Robert Argand]] (1768–1822), although they were first described by Norwegian-Danish land surveyor and mathematician [[Caspar Wessel]] (1745–1818).<ref>Wessel's memoir was presented to the Danish Academy in 1797; Argand's paper was published in 1806. (Whittaker & Watson, 1927, p. 9)</ref> Argand diagrams are frequently used to plot the positions of the [[pole (complex analysis)|poles]] and [[Zero (complex analysis)|zeroes]] of a [[mathematical function|function]] in the complex plane.
 
==Two-dimensional geometry==
===Polytopes===
{{main|Polygon}}
In two dimensions, there are infinitely many regular polytopes: the polygons. The first few are shown below:
 
====Convex====
The [[Schläfli symbol]] {p} represents a [[Regular polygon|regular ''p''-gon]].
 
{| class="wikitable" style="text-align:center;"
|- bgcolor="#e0e0e0" valign="top"
!Name
![[Equilateral triangle|Triangle]]<br />([[Simplex|2-simplex]])
![[Square (geometry)|Square]]<br />([[Cross-polytope|2-orthoplex]])<br />([[Hypercube|2-cube]])
![[Pentagon]]
![[Hexagon]]
![[Heptagon]]
![[Octagon]]
|- bgcolor="#ffe0e0"
![[Schläfli]]
|{3}
|{4}
|{5}
|{6}
|{7}
|{8}
|-
!Image
|[[Image:Regular triangle.svg|75px]]
|[[Image:Regular quadrilateral.svg|75px]]
|[[Image:Regular pentagon.svg|75px]]
|[[Image:Regular hexagon.svg|75px]]
|[[Image:Regular heptagon.svg|75px]]
|[[Image:Regular octagon.svg|75px]]
|-
!Name
![[Nonagon]]
![[Decagon]]
![[Hendecagon]]
![[Dodecagon]]
![[Triskaidecagon]]
![[Tetradecagon]]
|- bgcolor="#ffe0e0"
!Schläfli
|{9}
|{10}
|{11}
|{12}
|{13}
|{14}
|-
!Image
|[[Image:Regular nonagon.svg|75px]]
|[[Image:Regular decagon.svg|75px]]
|[[Image:Regular hendecagon.svg|75px]]
|[[Image:Regular dodecagon.svg|75px]]
|[[Image:Regular tridecagon.svg|75px]]
|[[Image:Regular tetradecagon.svg|75px]]
|-
!Name
![[Pentadecagon]]
![[Hexadecagon]]
![[Heptadecagon]]
![[Octadecagon]]
![[Enneadecagon]]
![[Icosagon]]
|...[[Regular polygon|n-gon]]
|- bgcolor="#ffe0e0"
!Schläfli
|{15}
|{16}
|{17}
|{18}
|{19}
|{20}
|{''n''}
|-
!Image
|[[Image:Regular pentadecagon.svg|75px]]
|[[Image:Regular hexadecagon.svg|75px]]
|[[Image:Regular heptadecagon.svg|75px]]
|[[Image:Regular octadecagon.svg|75px]]
|[[Image:Regular enneadecagon.svg|75px]]
|[[Image:Regular icosagon.svg|75px]]
|}
 
====Degenerate (spherical)====
The regular [[henagon]] {1} and regular [[digon]] {2} can be considered degenerate regular polygons. They can exist nondegenerately in non-Euclidean spaces like on a [[sphere|2-sphere]] or a [[torus|2-torus]].
 
{| class="wikitable" style="text-align:center;"
|- bgcolor="#e0e0e0" valign="top"
!Name
|[[Henagon]]
|[[Digon]]
|- bgcolor="#ffe0e0"
![[Schläfli]]
|{1}
|{2}
|-
!Image
|[[Image:Henagon.svg|75px]]
|[[Image:Digon.svg|75px]]
|}
 
====Non-convex====
There exist infinitely many non-convex regular polytopes in two dimensions, whose Schläfli symbols consist of rational numbers {n/m}. They are called [[star polygon]]s and share the same [[vertex arrangement]]s of the convex regular polygons.
 
In general, for any natural number n, there are n-pointed non-convex regular polygonal stars with Schläfli symbols {''n''/''m''} for all ''m'' such that ''m'' < ''n''/2 (strictly speaking {''n''/''m''} = {''n''/(''n'' − ''m'')}) and ''m'' and ''n'' are [[coprime]].
 
{| class="wikitable" style="text-align:center;"
|- bgcolor="#e0e0e0"
!Name
|[[Pentagram]]
| colspan="2" | [[Heptagram]]s
|[[Octagram]]
| colspan="2" | [[Enneagram (geometry)|Enneagrams]]
|[[Decagram (geometry)|Decagram]]
|...[[star polygon|n-agrams]]
|- bgcolor="#ffe0e0"
![[Schläfli]]
|{5/2}
|{7/2}
|{7/3}
|{8/3}
|{9/2}
|{9/4}
|{10/3}
|{''n/m''}
|-
!Image
|[[Image:Star polygon 5-2.svg|75px]]
|[[Image:Star polygon 7-2.svg|75px]]
|[[Image:Star polygon 7-3.svg|75px]]
|[[Image:Star polygon 8-3.svg|75px]]
|[[Image:Star polygon 9-2.svg|75px]]
|[[Image:Star polygon 9-4.svg|75px]]
|[[Image:Star polygon 10-3.svg|75px]]
|&nbsp;
|}
 
===Hypersphere===
{{main|Circle}}
[[File:CIRCLE 1.svg|200px|right]]
The [[hypersphere]] in 2 dimensions is a [[circle]], sometimes called a 1-sphere (''S''<sup>1</sup>) because it is an one-dimensional [[manifold]]. In a Euclidean plane, it has the length 2&pi;''r'' and the [[area]] of its [[interior (topology)|interior]] is
:<math>A = \pi r^{2}</math>
where <math>r</math> is the radius.
 
==Coordinate systems in two-dimensional spaces<!-- now correct: if a sphere included, then there is no unique 2d space -->==
{{main|Coordinate system}}
 
The most popular coordinate systems are the [[Cartesian coordinate system]], the [[polar coordinate system]] and the [[geographic coordinate system]].
 
<gallery>
Image:Coord XY.svg|[[Cartesian coordinate system]]
Image:Coord Circular.svg|[[Polar coordinate system]]
Image:Coord LatLong.svg|[[Geographic coordinate system]]
</gallery>
 
==Topological properties of the plane==
In [[topology]], the plane is characterized as being the unique [[contractible]] [[2-manifold]].  
 
Its dimension is characterized by the fact that removing a point from the plane leaves a space that is connected, but not [[simply connected]].
 
==Planar graphs==
In [[graph theory]], a '''planar graph''' is a [[graph (mathematics)|graph]] that can be [[graph embedding|embedded]] in the plane, i.e., it can be drawn on the plane in such a way that its edges intersect only at their endpoints.  In other words, it can be drawn in such a way that no edges cross each other.<ref>{{cite book|last=Trudeau|first=Richard J.|title=Introduction to Graph Theory|year=1993|publisher=Dover Pub.|location=New York|isbn=978-0-486-67870-2|pages=64|url=http://store.doverpublications.com/0486678709.html|edition=Corrected, enlarged republication.|accessdate=8 August 2012|quote=Thus a planar graph, when drawn on a flat surface, either has no edge-crossings or can be redrawn without them.}}</ref> Such a drawing is called a '''plane graph''' or '''planar embedding of the graph'''. A plane graph can be defined as a planar graph with a mapping from every node to a point on a plane, and from every edge to a [[plane curve]] on that plane, such that the extreme points of each curve are the points mapped from its end nodes, and all curves are disjoint except on their extreme points.  
 
== References ==
<references />
 
==See also==
* [[Three-dimensional space]]
* [[Two-dimensional graph]]
 
{{Dimension topics}}
 
[[Category:Dimension]]
[[Category:Multi-dimensional geometry]]

Revision as of 06:29, 23 December 2013

Bi-dimensional Cartesian coordinate system

Bi-dimensional space is a geometric model of the planar projection of the physical universe in which we live. The two dimensions are commonly called length and width. Both directions lie in the same plane.

In physics and mathematics, a sequence of n real numbers can be understood as a location in n-dimensional space. When n = 2, the set of all such locations is called 2-dimensional space or bi-dimensional space, and usually is thought of as an Euclidean space.

In physics, our bi-dimensional space is viewed as a planar representation of the space in which we move, described as bi-dimensional space or two-dimensional space.

History of two-dimensional space

Euclid's Elements dealt almost exclusively with two-dimensional geometry, developing such notions as similarity of shapes, the Pythagorean theorem (Proposition 47), equality of angles and areas, parallelism, the sum of the angles in a triangle, and the three cases in which triangles are "equal" (have the same area), among many other topics.

Later, the plane was described in a so-called Cartesian coordinate system, a coordinate system that specifies each point uniquely in a plane by a pair of numerical coordinates, which are the signed distances from the point to two fixed perpendicular directed lines, measured in the same unit of length. Each reference line is called a coordinate axis or just axis of the system, and the point where they meet is its origin, usually at ordered pair (0, 0). The coordinates can also be defined as the positions of the perpendicular projections of the point onto the two axes, expressed as signed distances from the origin.

The idea of this system was developed in 1637 in writings by Descartes and independently by Pierre de Fermat, although Fermat also worked in three dimensions, and did not publish the discovery.[1] Both authors used a single axis in their treatments and have a variable length measured in reference to this axis. The concept of using a pair of axes was introduced later, after Descartes' La Géométrie was translated into Latin in 1649 by Frans van Schooten and his students. These commentators introduced several concepts while trying to clarify the ideas contained in Descartes' work.[2]

Later, the plane was thought of as a field, where any two points could be multiplied and, except for 0, divided. This was known as the complex plane. The complex plane is sometimes called the Argand plane because it is used in Argand diagrams. These are named after Jean-Robert Argand (1768–1822), although they were first described by Norwegian-Danish land surveyor and mathematician Caspar Wessel (1745–1818).[3] Argand diagrams are frequently used to plot the positions of the poles and zeroes of a function in the complex plane.

Two-dimensional geometry

Polytopes

Mining Engineer (Excluding Oil ) Truman from Alma, loves to spend time knotting, largest property developers in singapore developers in singapore and stamp collecting. Recently had a family visit to Urnes Stave Church. In two dimensions, there are infinitely many regular polytopes: the polygons. The first few are shown below:

Convex

The Schläfli symbol {p} represents a regular p-gon.

Name Triangle
(2-simplex)
Square
(2-orthoplex)
(2-cube)
Pentagon Hexagon Heptagon Octagon
Schläfli {3} {4} {5} {6} {7} {8}
Image File:Regular triangle.svg File:Regular quadrilateral.svg File:Regular pentagon.svg File:Regular hexagon.svg File:Regular heptagon.svg File:Regular octagon.svg
Name Nonagon Decagon Hendecagon Dodecagon Triskaidecagon Tetradecagon
Schläfli {9} {10} {11} {12} {13} {14}
Image File:Regular nonagon.svg File:Regular decagon.svg File:Regular hendecagon.svg File:Regular dodecagon.svg File:Regular tridecagon.svg File:Regular tetradecagon.svg
Name Pentadecagon Hexadecagon Heptadecagon Octadecagon Enneadecagon Icosagon ...n-gon
Schläfli {15} {16} {17} {18} {19} {20} {n}
Image File:Regular pentadecagon.svg File:Regular hexadecagon.svg File:Regular heptadecagon.svg File:Regular octadecagon.svg File:Regular enneadecagon.svg File:Regular icosagon.svg

Degenerate (spherical)

The regular henagon {1} and regular digon {2} can be considered degenerate regular polygons. They can exist nondegenerately in non-Euclidean spaces like on a 2-sphere or a 2-torus.

Name Henagon Digon
Schläfli {1} {2}
Image File:Henagon.svg File:Digon.svg

Non-convex

There exist infinitely many non-convex regular polytopes in two dimensions, whose Schläfli symbols consist of rational numbers {n/m}. They are called star polygons and share the same vertex arrangements of the convex regular polygons.

In general, for any natural number n, there are n-pointed non-convex regular polygonal stars with Schläfli symbols {n/m} for all m such that m < n/2 (strictly speaking {n/m} = {n/(n − m)}) and m and n are coprime.

Name Pentagram Heptagrams Octagram Enneagrams Decagram ...n-agrams
Schläfli {5/2} {7/2} {7/3} {8/3} {9/2} {9/4} {10/3} {n/m}
Image File:Star polygon 5-2.svg File:Star polygon 7-2.svg File:Star polygon 7-3.svg File:Star polygon 8-3.svg File:Star polygon 9-2.svg File:Star polygon 9-4.svg File:Star polygon 10-3.svg  

Hypersphere

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File:CIRCLE 1.svg

The hypersphere in 2 dimensions is a circle, sometimes called a 1-sphere (S1) because it is an one-dimensional manifold. In a Euclidean plane, it has the length 2πr and the area of its interior is

A=πr2

where r is the radius.

Coordinate systems in two-dimensional spaces

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The most popular coordinate systems are the Cartesian coordinate system, the polar coordinate system and the geographic coordinate system.

Topological properties of the plane

In topology, the plane is characterized as being the unique contractible 2-manifold.

Its dimension is characterized by the fact that removing a point from the plane leaves a space that is connected, but not simply connected.

Planar graphs

In graph theory, a planar graph is a graph that can be embedded in the plane, i.e., it can be drawn on the plane in such a way that its edges intersect only at their endpoints. In other words, it can be drawn in such a way that no edges cross each other.[4] Such a drawing is called a plane graph or planar embedding of the graph. A plane graph can be defined as a planar graph with a mapping from every node to a point on a plane, and from every edge to a plane curve on that plane, such that the extreme points of each curve are the points mapped from its end nodes, and all curves are disjoint except on their extreme points.

References



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  2. Template:Harvnb
  3. Wessel's memoir was presented to the Danish Academy in 1797; Argand's paper was published in 1806. (Whittaker & Watson, 1927, p. 9)
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See also

Template:Dimension topics