In mathematics, a unit sphere is a sphere of unit radius: the set of points at Euclidean distance 1 from some center point in three-dimensional space. More generally, the unit
n
n
(n+1)
1
A sphere or ball with unit radius and center at the origin of the space is called the unit sphere or the unit ball. Any arbitrary sphere can be transformed to the unit sphere by a combination of translation and scaling, so the study of spheres in general can often be reduced to the study of the unit sphere.
The unit sphere is often used as a model for spherical geometry because it has constant sectional curvature of 1, which simplifies calculations. In trigonometry, circular arc length on the unit circle is called radians and used for measuring angular distance; in spherical trigonometry surface area on the unit sphere is called steradians and used for measuring solid angle.
In more general contexts, a unit sphere is the set of points of distance 1 from a fixed central point, where different norms can be used as general notions of "distance", and an (open) unit ball is the region inside.
In Euclidean space of
n
(n-1)
(x1,\ldots,xn)
2 | |
x | |
1 |
+
2 | |
x | |
2 |
+ … +
2 | |
x | |
n |
=1.
The open unit
n
2 | |
x | |
1 |
+
2 | |
x | |
2 |
+ … +
2 | |
x | |
n |
<1,
n
2 | |
x | |
1 |
+
2 | |
x | |
2 |
+ … +
2 | |
x | |
n |
\le1.
See also: Volume of an n-ball.
The classical equation of a unit sphere is that of the ellipsoid with a radius of 1 and no alterations to the
x
y
z
x2+y2+z2=1
The volume of the unit ball in Euclidean
n
n
Vn,
Vn=
\pin/2 | |
\Gamma(1+n/2) |
=\begin{cases} {\pin/2
n!!
The hypervolume of the
(n-1)
n
An-1,
An-1=nVn=
n\pin/2 | |
\Gamma(1+n/2) |
=
2\pin/2 | |
\Gamma(n/2) |
=\begin{cases} {2\pin/2
A0=2
[-1,1]\subsetR
A1=2\pi
A2=4\pi
\{x\in\R3:
2 | |
x | |
1 |
+
2 | |
x | |
2 |
+
2 | |
x | |
3 |
\leq1\}
\{x\in\R3:
2 | |
x | |
1 |
+
2 | |
x | |
2 |
+
2 | |
x | |
3 |
=1\}
The surface areas and the volumes for some values of
n
n | An-1 | Vn | ||||
---|---|---|---|---|---|---|
0 | (1/0!)\pi0 | 1 | ||||
1 | 1(21/1! | )\pi^0 | 2 | (21/1! | )\pi^0 | 2 |
2 | 2(1/1!)\pi1=2\pi | 6.283 | (1/1!)\pi1=\pi | 3.141 | ||
3 | 3(22/3! | )\pi^1 = 4 \pi | 12.57 | (22/3! | )\pi^1 = (4/3)\pi | 4.189 |
4 | 4(1/2!)\pi2=2\pi2 | 19.74 | (1/2!)\pi2=(1/2)\pi2 | 4.935 | ||
5 | 5(23/5! | )\pi^2 = (8/3)\pi^2 | 26.32 | (23/5! | )\pi^2 = (8/15)\pi^2 | 5.264 |
6 | 6(1/3!)\pi3=\pi3 | 31.01 | (1/3!)\pi3=(1/6)\pi3 | 5.168 | ||
7 | 7(24/7! | ) \pi^3 = (16/15)\pi^3 | 33.07 | (24/7! | ) \pi^3 = (16/105)\pi^3 | 4.725 |
8 | 8(1/4!)\pi4=(1/3)\pi4 | 32.47 | (1/4!)\pi4=(1/24)\pi4 | 4.059 | ||
9 | 9(25/9! | ) \pi^4 = (32/105)\pi^4 | 29.69 | (25/9! | ) \pi^4 = (32/945)\pi^4 | 3.299 |
10 | 10(1/5!)\pi5=(1/12)\pi5 | 25.50 | (1/5!)\pi5=(1/120)\pi5 | 2.550 |
n\geq2
The
An
A0=2
A1=2\pi
An=
2\pi | |
n-1 |
An-2
n>1
The
Vn
V0=1
V1=2
Vn=
2\pi | |
n |
Vn-2
n>1
See main article: Hausdorff measure.
The value at non-negative real values of
n
The surface area of an
(n-1)
r
An-1rn-1
n
r
Vnrn.
A2=4\pir2
r.
V3=\tfrac43\pir3
r
V
\| ⋅ \|
\{x\inV:\|x\|<1\}
It is the topological interior of the closed unit ball of
(V,\| ⋅ \|)\colon
\{x\inV:\|x\|\le1\}
The latter is the disjoint union of the former and their common border, the unit sphere of
(V,\| ⋅ \|)\colon
\{x\inV:\|x\|=1\}
The "shape" of the unit ball is entirely dependent on the chosen norm; it may well have "corners", and for example may look like
[-1,1]n
Rn
Let
x=(x1,...xn)\in\Rn.
\ellp
p\ge1
\|x\|p=
n | |
l(\sum | |
k=1 |
p | |
|x | |
k| |
r)1/p
Then
\|x\|2
\|x\|1
\ell1
p\geq1
\ellp
\|x\|infty
\ellinfty
x
Note that for the one-dimensional circumferences
Cp
C1=4\sqrt{2}
C2=2\pi
Cinfty=8
All three of the above definitions can be straightforwardly generalized to a metric space, with respect to a chosen origin. However, topological considerations (interior, closure, border) need not apply in the same way (e.g., in ultrametric spaces, all of the three are simultaneously open and closed sets), and the unit sphere may even be empty in some metric spaces.
If
V
F:V\to\R,
\{p\inV:F(p)=1\}
V.
x2-y2
x2