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In mathematics, a ball is the solid figure bounded by a sphere; it is also called a solid sphere.[1] It may be a closed ball (including the boundary points that constitute the sphere) or an open ball (excluding them).

These concepts are defined not only in three-dimensional Euclidean space but also for lower and higher dimensions, and for metric spaces in general. A ball in n dimensions is called a hyperball or n-ball and is bounded by a hypersphere or (n−1)-sphere. Thus, for example, a ball in the Euclidean plane is the same thing as a disk, the area bounded by a circle. In Euclidean 3-space, a ball is taken to tát be the volume bounded by a 2-dimensional sphere. In a one-dimensional space, a ball is a line segment.

In other contexts, such as in Euclidean geometry and informal use, sphere is sometimes used to tát mean ball. In the field of topology the closed -dimensional ball is often denoted as or while the open -dimensional ball is or .

In Euclidean space

In Euclidean n-space, an (open) n-ball of radius r and center x is the phối of all points of distance less kêu ca r from x. A closed n-ball of radius r is the phối of all points of distance less kêu ca or equal to tát r away from x.

In Euclidean n-space, every ball is bounded by a hypersphere. The ball is a bounded interval when n = 1, is a disk bounded by a circle when n = 2, and is bounded by a sphere when n = 3.

Volume

The n-dimensional volume of a Euclidean ball of radius r in n-dimensional Euclidean space is:[2]

where Γ is Leonhard Euler's gamma function (which can be thought of as an extension of the factorial function to tát fractional arguments). Using explicit formulas for particular values of the gamma function at the integers and half integers gives formulas for the volume of a Euclidean ball that vì thế not require an evaluation of the gamma function. These are:

In the formula for odd-dimensional volumes, the double factorial (2k + 1)!! is defined for odd integers 2k + 1 as (2k + 1)!! = 1 ⋅ 3 ⋅ 5 ⋅ ⋯ ⋅ (2k − 1) ⋅ (2k + 1).

In general metric spaces

Let (M, d) be a metric space, namely a phối M with a metric (distance function) d. The open (metric) ball of radius r > 0 centered at a point p in M, usually denoted by Br(p) or B(p; r), is defined by

The closed (metric) ball, which may be denoted by Br[p] or B[p; r], is defined by

Note in particular that a ball (open or closed) always includes p itself, since the definition requires r > 0.

A unit ball (open or closed) is a ball of radius 1.

A subset of a metric space is bounded if it is contained in some ball. A phối is totally bounded if, given any positive radius, it is covered by finitely many balls of that radius.

The open balls of a metric space can serve as a base, giving this space a topology, the open sets of which are all possible unions of open balls. This topology on a metric space is called the topology induced by the metric d.

Let Br(p) denote the closure of the open ball Br(p) in this topology. While it is always the case that Br(p) ⊆ Br(p)Br[p], it is not always the case that Br(p) = Br[p]. For example, in a metric space X with the discrete metric, one has B1(p) = {p} and B1[p] = X, for any pX.

In normed vector spaces

Any normed vector space V with norm is also a metric space with the metric In such spaces, an arbitrary ball of points around a point with a distance of less kêu ca may be viewed as a scaled (by ) and translated (by ) copy of a unit ball Such "centered" balls with are denoted with

The Euclidean balls discussed earlier are an example of balls in a normed vector space.

p-norm

In a Cartesian space Rn with the p-norm Lp, that is

an open ball around the origin with radius is given by the set

For n = 2, in a 2-dimensional plane , "balls" according to tát the L1-norm (often called the taxicab or Manhattan metric) are bounded by squares with their diagonals parallel to tát the coordinate axes; those according to tát the L-norm, also called the Chebyshev metric, have squares with their sides parallel to tát the coordinate axes as their boundaries. The L2-norm, known as the Euclidean metric, generates the well known disks within circles, and for other values of p, the corresponding balls are areas bounded by Lamé curves (hypoellipses or hyperellipses).

For n = 3, the L1- balls are within octahedra with axes-aligned body diagonals, the L-balls are within cubes with axes-aligned edges, and the boundaries of balls for Lp with p > 2 are superellipsoids. Obviously, p = 2 generates the inner of usual spheres.

General convex norm

More generally, given any centrally symmetric, bounded, open, and convex subset X of Rn, one can define a norm on Rn where the balls are all translated and uniformly scaled copies of X. Note this theorem does not hold if "open" subset is replaced by "closed" subset, because the origin point qualifies but does not define a norm on Rn.

In topological spaces

One may talk about balls in any topological space X, not necessarily induced by a metric. An (open or closed) n-dimensional topological ball of X is any subset of X which is homeomorphic to tát an (open or closed) Euclidean n-ball. Topological n-balls are important in combinatorial topology, as the building blocks of cell complexes.

Any open topological n-ball is homeomorphic to tát the Cartesian space Rn and to tát the open unit n-cube (hypercube) (0, 1)nRn. Any closed topological n-ball is homeomorphic to tát the closed n-cube [0, 1]n.

An n-ball is homeomorphic to tát an m-ball if and only if n = m. The homeomorphisms between an open n-ball B and Rn can be classified in two classes, that can be identified with the two possible topological orientations of B.

A topological n-ball need not be smooth; if it is smooth, it need not be diffeomorphic to tát a Euclidean n-ball.

Regions

A number of special regions can be defined for a ball:

• cap, bounded by one plane
• sector, bounded by a conical boundary with apex at the center of the sphere
• segment, bounded by a pair of parallel planes
• shell, bounded by two concentric spheres of differing radii
• wedge, bounded by two planes passing through a sphere center and the surface of the sphere