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23-408: Planar is an adjective meaning "relating to a plane (geometry) ". Planar may also refer to: Plane (geometry) A Euclidean plane with a chosen Cartesian coordinate system is called a Cartesian plane . The set R 2 {\displaystyle \mathbb {R} ^{2}} of the ordered pairs of real numbers (the real coordinate plane ), equipped with the dot product ,

46-413: A Cartesian coordinate system , the origin is the point where the axes of the system intersect. The origin divides each of these axes into two halves, a positive and a negative semiaxis. Points can then be located with reference to the origin by giving their numerical coordinates —that is, the positions of their projections along each axis, either in the positive or negative direction. The coordinates of

69-541: A plane is a flat two- dimensional surface that extends indefinitely. Euclidean planes often arise as subspaces of three-dimensional space R 3 {\displaystyle \mathbb {R} ^{3}} . A prototypical example is one of a room's walls, infinitely extended and assumed infinitesimal thin. In two dimensions, there are infinitely many polytopes: the polygons. The first few regular ones are shown below: The Schläfli symbol { n } {\displaystyle \{n\}} represents

92-419: A regular n -gon . The regular monogon (or henagon) {1} and regular digon {2} can be considered degenerate regular polygons and exist nondegenerately in non-Euclidean spaces like a 2-sphere , 2-torus , or right circular cylinder . 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

115-533: A region D in R of a function f ( x , y ) , {\displaystyle f(x,y),} and is usually written as: The fundamental theorem of line integrals says that a line integral through a gradient field can be evaluated by evaluating the original scalar field at the endpoints of the curve. Let φ : U ⊆ R 2 → R {\displaystyle \varphi :U\subseteq \mathbb {R} ^{2}\to \mathbb {R} } . Then with p , q

138-473: A vector A by itself is which gives the formula for the Euclidean length of the vector. In a rectangular coordinate system, the gradient is given by For some scalar field f  : U ⊆ R → R , the line integral along a piecewise smooth curve C ⊂ U is defined as where r : [a, b] → C is an arbitrary bijective parametrization of the curve C such that r ( a ) and r ( b ) give

161-466: A way that no edges cross each other. 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. Origin (mathematics) In mathematics ,

184-408: Is a one-dimensional manifold . In a Euclidean plane, it has the length 2π r and the area of its interior is where r {\displaystyle r} is the radius. There are an infinitude of other curved shapes in two dimensions, notably including the conic sections : the ellipse , the parabola , and the hyperbola . Another mathematical way of viewing two-dimensional space

207-437: 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 . 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

230-430: Is defined as: A vector can be pictured as an arrow. Its magnitude is its length, and its direction is the direction the arrow points. The magnitude of a vector A is denoted by ‖ A ‖ {\displaystyle \|\mathbf {A} \|} . In this viewpoint, the dot product of two Euclidean vectors A and B is defined by where θ is the angle between A and B . The dot product of

253-440: Is found in linear algebra , where the idea of independence is crucial. The plane has two dimensions because the length of a rectangle is independent of its width. In the technical language of linear algebra, the plane is two-dimensional because every point in the plane can be described by a linear combination of two independent vectors . The dot product of two vectors A = [ A 1 , A 2 ] and B = [ B 1 , B 2 ]

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276-424: Is given by an ordered pair of real numbers, each number giving the distance of that point from the origin measured along the given axis, which is equal to the distance of that point from the other axis. Another widely used coordinate system is the polar coordinate system , which specifies a point in terms of its distance from the origin and its angle relative to a rightward reference ray. In Euclidean geometry ,

299-498: Is often called the Euclidean plane or standard Euclidean plane , since every Euclidean plane is isomorphic to it. Books I through IV and VI of Euclid's Elements dealt 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

322-461: The origin of a Euclidean space is a special point , usually denoted by the letter O , used as a fixed point of reference for the geometry of the surrounding space. In physical problems, the choice of origin is often arbitrary, meaning any choice of origin will ultimately give the same answer. This allows one to pick an origin point that makes the mathematics as simple as possible, often by taking advantage of some kind of geometric symmetry . In

345-425: The discovery. Both authors used a single ( abscissa ) axis in their treatments, with the lengths of ordinates measured along lines not-necessarily-perpendicular to that axis. The concept of using a pair of fixed 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

368-462: The endpoints of C and a < b {\displaystyle a<b} . For a vector field F  : U ⊆ R → R , the line integral along a piecewise smooth curve C ⊂ U , in the direction of r , is defined as where · is the dot product and r : [a, b] → C is a bijective parametrization of the curve C such that r ( a ) and r ( b ) give the endpoints of C . A double integral refers to an integral within

391-399: The endpoints of the curve γ. Let C be a positively oriented , piecewise smooth , simple closed curve in a plane , and let D be the region bounded by C . If L and M are functions of ( x , y ) defined on an open region containing D and have continuous partial derivatives there, then where the path of integration along C is counterclockwise . In topology , the plane

414-617: The ideas contained in Descartes' work. 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 Danish-Norwegian land surveyor and mathematician Caspar Wessel (1745–1818). Argand diagrams are frequently used to plot

437-435: The origin are always all zero, for example (0,0) in two dimensions and (0,0,0) in three. In a polar coordinate system , the origin may also be called the pole. It does not itself have well-defined polar coordinates, because the polar coordinates of a point include the angle made by the positive x -axis and the ray from the origin to the point, and this ray is not well-defined for the origin itself. In Euclidean geometry ,

460-427: The positions of the poles and zeroes of a function in the complex plane. In mathematics, analytic geometry (also called Cartesian geometry) describes every point in two-dimensional space by means of two coordinates. Two perpendicular coordinate axes are given which cross each other at the origin . They are usually labeled x and y . Relative to these axes, the position of any point in two-dimensional space

483-404: 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 . The hypersphere in 2 dimensions is a circle , sometimes called a 1-sphere ( S ) because it

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506-433: 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

529-447: 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

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