Plane (geometry)

Two intersecting planes in three-dimensional space

In mathematics, a plane is an unbounded homogeneous flat two-dimensional space. Planes can arise as subspaces of some higher dimensional space, as with the walls of a room, or they may enjoy an independent existence in their own right, as in the setting of Euclidean geometry.

When working in two-dimensional Euclidean space, the definite article is used, the plane, to refer to the whole space. Many fundamental tasks in geometry, trigonometry, and graphing are performed in two-dimensional space, or in other words, in the plane. A lot of mathematics can be and has been performed in the plane, notably in the areas of geometry, trigonometry, graph theory and graphing. All two-dimensional figures are assumed to be on a plane, even on the plane, unless otherwise specified.

1 Euclidean geometry
2 Planes embedded in R³
3 Planes in various areas of mathematics
4 Planes in fiction
5 See also
6 External links

Euclidean geometry

Main article: Euclidean Geometry

Euclid set forth the first known axiomatic treatment of geometry. This means that Euclid selected a small core of undefined terms (called common notions) and postulates (or axioms) and he then uses these to prove the geometrical statements. Euclid's Axioms had minor flaws, which were later corrected by David Hilbert, George Birkhoff, and Alfred Tarski. The plane is not directly given a definition, may be thought of as part of the common notions. More formally it may be regarded as anything that satisfies the axioms for Euclidean geometry. In his work Euclid never makes use of a numbers to measure length, angle, or area. In this way the Euclidean plane is not quite the same as the Cartesian plane.

In higher dimensional Euclidean space, a plane inside this space can be uniquely determined by any of the following (sets of) objects:

three non-collinear points (i.e., not lying on the same line)
a line and a point not on the line
two lines with one point of intersection
two parallel lines

Three parallel planes.

In 3 dimensional Euclidean space, like lines, planes can be parallel or intersecting. In this setting planes differ from lines Differing from lines, however, planes cannot be skew. Lines drawn on two parallel planes will either be parallel or skew, but will not intersect. Intersecting planes may be perpendicular, or may form any number of other angles. In higher dimensional Euclidean space it is possible to have two planes that intersect in a single point.

Planes embedded in R³

This section is specifically concerned with planes embedded in three dimensions: specifically, in ℝ³.

Properties

In three-dimensional Euclidean space, we may exploit the following facts that do not hold in higher dimensions:

Two planes are either parallel or they intersect in a line.
A line is either parallel to a plane or intersects it at a single point or is contained in the plane.
Two lines perpendicular to the same plane must be parallel to each other.
Two planes perpendicular to the same line must be parallel to each other.

Define a plane with a point and a normal vector

In a three-dimensional space, another important way of defining a plane is by specifying a point and a normal vector to the plane.

Let $\bold p$ be any known point in the plane, and let $\vec{n}$ be a nonzero normal vector to the plane. The desired plane is the set of all points $\bold r$ such that $\vec n\cdot (\bold r-\bold p)=0.$

If we write $\vec n =a \bold \hat{x} + b \bold \hat{y} + c \bold \hat{z}$ , $\bold r = x \bold \hat{x} + y \bold \hat{y} + z \bold \hat{z}$ , where $\bold \hat{x}, \bold \hat{y} , \bold \hat{z}$ are the cartesian unit vectors (or direction vectors ), and $d$ as the dot product $d = -\vec n\cdot \bold p$ , then the plane $\Pi$ is determined by the condition $ax + by + cz + d = 0\,$ , where a, b, c and d are real numbers and a, b, and c are not all zero.

Alternatively, a plane may be described parametrically as the set of all points of the form $\bold r = \bold {p} + s \vec{v} + t \vec{w},$ where s and t range over all real numbers, and $\bold p$ , $\vec{v}$ and $\vec{w}$ are given vectors defining the plane. $\bold{p}$ is the position vector from the origin to an arbitrary (but fixed) point on the plane, and $\vec{v}$ and $\vec{w}$ can be visualized as starting at $\bold p$ and pointing in different directions along the plane. $\vec{v}$ and $\vec{w}$ can, but do not have to be perpendicular (but they cannot be collinear).

Define a plane through three points

The plane passing through three points $\bold p_1 = (x_1,y_1,z_1)$ , $\bold p_2 = (x_2,y_2,z_2)$ and $\bold p_3 = (x_3,y_3,z_3)$ can be defined as the set of all points (x,y,z) that satisfy the following determinant equations:

$\begin{vmatrix} x - x_1 & y - y_1 & z - z_1 \\ x_2 - x_1 & y_2 - y_1& z_2 - z_1 \\ x_3 - x_1 & y_3 - y_1 & z_3 - z_1 \end{vmatrix} =\begin{vmatrix} x - x_1 & y - y_1 & z - z_1 \\ x - x_2 & y - y_2 & z - z_2 \\ x - x_3 & y - y_3 & z - z_3 \end{vmatrix} = 0.$

To describe the plane as an equation in the form $ax + by + cz + d = 0$ , solve the following system of equations:

$\, ax_1 + by_1 + cz_1 + d = 0$

$\, ax_2 + by_2 + cz_2 + d = 0$

$\, ax_3 + by_3 + cz_3 + d = 0$ .

This system can be solved using Cramer's Rule and basic matrix manipulations. Let $D = \begin{vmatrix} x_1 & y_1 & z_1 \\ x_2 & y_2 & z_2 \\ x_3 & y_3 & z_3 \end{vmatrix}$ . Then,

$a = \frac{-d}{D} \begin{vmatrix} 1 & y_1 & z_1 \\ 1 & y_2 & z_2 \\ 1 & y_3 & z_3 \end{vmatrix}$

$b = \frac{-d}{D} \begin{vmatrix} x_1 & 1 & z_1 \\ x_2 & 1 & z_2 \\ x_3 & 1 & z_3 \end{vmatrix}$

$c = \frac{-d}{D} \begin{vmatrix} x_1 & y_1 & 1 \\ x_2 & y_2 & 1 \\ x_3 & y_3 & 1 \end{vmatrix}$ .

These equations are parametric in d. Setting d equal to any non-zero number and substituting it into these equations will yield one solution set.

This plane can also be described by the "point and a normal vector" prescription above.

A suitable normal vector is given by the cross product $\vec n = ( \bold p_2 - \bold p_1 ) \times ( \bold p_3 - \bold p_1 ),$ and the point $\bold p$ can be taken to be any of given points $\bold p_1, \bold p_2$ or $\bold p_3$ .

Distance from a point to a plane

For a plane $\Pi�: ax + by + cz + d = 0\,$ and a point $\bold p_1 = (x_1,y_1,z_1)$ not necessarily lying on the plane, the shortest distance from $\bold p_1$ to the plane is

$D = \frac{\left | a x_1 + b y_1 + c z_1+d \right |}{\sqrt{a^2+b^2+c^2}}.$

It follows that $\bold p_1$ lies in the plane if and only if D=0.

If $\sqrt{a^2+b^2+c^2}=1$ meaning that a, b and c are normalized then the equation becomes

$D = \ | a x_1 + b y_1 + c z_1+d | .$

Line of intersection between two planes

Given intersecting planes described by $\Pi_1�: \vec n_1\cdot \bold r = h_1$ and $\Pi_2�: \vec n_2\cdot \bold r = h_2$ , the line of intersection is perpendicular to both $\vec n_1$ and $\vec n_2$ and thus parallel to $\vec n_1 \times \vec n_2$ . This cross product is zero only if the planes are parallel, and are therefore non-intersecting or coincident.

Any point in space may be written as $\bold r = c_1\vec n_1 + c_2\vec n_2 + c_3(\vec n_1 \times \vec n_2)$ , since $\{ \vec n_1, \vec n_2, (\vec n_1 \times \vec n_2) \}$ is a basis. In this equation, $c_3$ is the line's parameter, and $c_1$ and $c_2$ are constants. By taking the dot product of this equation against $\vec n_1$ and $\vec n_2$ , and by noting that $\vec n_i \cdot \bold r = h_i$ , we obtain two scalar equations that may be solved for $\{ c_1, c_2 \}$ .

If we further assume that $\vec n_1$ and $\vec n_2$ are orthonormal then the closest point on the line of intersection to the origin is $\bold r_0 = h_1\vec n_1 + h_2\vec n_2$ . If that is not the case, then a more complex procedure must be used [1].

Dihedral angle

Given two intersecting planes described by $\Pi_1�: a_1 x + b_1 y + c_1 z + d_1 = 0\,$ and $\Pi_2�: a_2 x + b_2 y + c_2 z + d_2 = 0\,$ , the dihedral angle between them is defined to be the angle $\alpha$ between their normal directions:

$\cos\alpha = \hat n_1\cdot \hat n_2 = \frac{a_1 a_2 + b_1 b_2 + c_1 c_2}{\sqrt{a_1^2+b_1^2+c_1^2}\sqrt{a_2^2+b_2^2+c_2^2}}.$

Planes in various areas of mathematics

In addition to its familiar geometric structure, with isomorphisms that are isometries with respect to the usual inner product, the plane may be viewed at various other levels of abstraction. Each level of abstraction corresponds to a specific category.

At one extreme, all geometrical and metric concepts may be dropped to leave the topological plane, which may be thought of as an idealized homotopically trivial infinite rubber sheet, which retains a notion of proximity, but has no distances. The topological plane has a concept of a linear path, but no concept of a straight line. The topological plane, or its equivalent the open disc, is the basic topological neighborhood used to construct surfaces (or 2-manifolds) classified in low-dimensional topology. Isomorphisms of the topological plane are all continuous bijections. The topological plane is the natural context for the branch of graph theory that deals with planar graphs, and results such as the four color theorem.

The plane may also be viewed as an affine space, whose isomorphisms are combinations of translations and non-singular linear maps. From this viewpoint there are no distances, but colinearity and ratios of distances on any line are preserved.

Differential geometry views a plane as a 2-dimensional real manifold, a topological plane which is provided with a differential structure. Again in this case, there is no notion of distance, but there is now a concept of smoothness of maps, for example a differentiable or smooth path (depending on the type of differential structure applied). The isomorphisms in this case are bijections with the chosen degree of differentiability.

In the opposite direction of abstraction, we may apply a compatible field structure to the geometric plane, giving rise to the complex plane and the major area of complex analysis. The complex field has only two isomorphisms that leave the real line fixed, the identity and conjugation.

In the same way as in the real case, the plane may also be viewed as the simplest, one-dimensional (over the complex numbers) complex manifold, sometimes called the complex line. However, this viewpoint contrasts sharply with the case of the plane as a 2-dimensional real manifold. The isomorphisms are all conformal bijections of the complex plane, but the only possibilities are maps that correspond to the composition of a multiplication by a complex number and a translation.

In addition, the Euclidean geometry (which has zero curvature everywhere) is not the only geometry that the plane may have. The plane may be given a spherical geometry by using the stereographic projection. This can be thought of as placing a sphere on the plane (just like a ball on the floor), removing the top point, and projecting the sphere onto the plane from this point). This is one of the projections that may be used in making a flat map of part of the Earth's surface. The resulting geometry has constant positive curvature.

Alternatively, the plane can also be given a metric which gives it constant negative curvature giving the hyperbolic plane. The latter possibility finds an application in the theory of special relativity in the simplified case where there are two spatial dimensions and one time dimension. (The hyperbolic plane is a timelike hypersurface in three-dimensional Minkowski space.)

Planes in fiction

The 1884 novel Flatland by Edwin A. Abbott features the concept of a geometric, two dimensional infinite plane inhabited by living geometric figures (triangles, squares, circles, etc.). It has been described by Isaac Asimov, in his foreword to the Signet Classics 1984 edition, as "the best introduction one can find into the manner of perceiving dimensions."