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Ψ ( n )=
∂n ln Γ ( n )
Vice versa, keeping the dimension fixed and differentiate term (2) with respect
to r , it is not solvable in roots, i.e. no extrema exists :
where
r n
=
π n/ 2
Γ 2 +1
r n n/ 2
2 +1
∂r
·
(4)
For instance a hypersphere with radius r = 1 reaches its maximum volume in
dimension 5 and looses volume in lower and higher dimensions. In figure 2 this
property is visualized for different radius lengths r =
.Onecan
see that for each radius length in dimension from n =0to n = 25, the associated
hypersphere reaches a maximal volume in a certain dimension and looses volume
asymptotically in higher and lower dimensions.
{
0 . 9 , 1 . 0 , 1 . 1 , 1 . 2
}
16
r = 1.2
12
r = 1.1
8
r = 1.0
4
r = 0.9
0
0
5
10
15
20
25
dimension
x
Fig. 2. Hypersphere volume plot for radius lengths r = { 0 . 9 , 1 . 0 , 1 . 1 , 1 . 2 } and dimen-
sion n =0 ,..., 25. Obviously, n is a nonnegative integer, but the graph is drawn
treating n as continuously varying.
Table 1. Dimension where a hypersphere reaches the maximum volume for radius
lengths r = { 0 . 05 , 0 . 1 , 0 . 2 ,..., 1 . 0 } . Results are obtained by considering term (3) as a
real-valued function.
Radius r
0.05
0.1
0.2
0.3 0.4 0.5
0.6
0.7
0.8
0.9
1.0
-9.17 · 10 7 -88.94 1.59 1.12 1.0 1.03 1.20 1.53 2.14 3.23 5.27
Dimension n
Table 1 presents the dimension where a hypersphere reaches its maximum
volume for different radius lengths. Surprisingly, for radius lengths r =0 . 05 and
r =0 . 1 the maximum volume lies in negative real-valued numbers. Hence, a vol-
ume maximization for such small radius lengths is not feasible, as the dimension
is a nonnegative integer.
 
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