62 1. INTRODUCTION
1.17 () www The gamma function is defined by
Γ(x)≡
∫∞
0
ux−^1 e−udu. (1.141)
Using integration by parts, prove the relationΓ(x+1) =xΓ(x). Show also that
Γ(1) = 1and hence thatΓ(x+1)=x!whenxis an integer.
1.18 () www We can use the result (1.126) to derive an expression for the surface
areaSD, and the volumeVD, of a sphere of unit radius inDdimensions. To do this,
consider the following result, which is obtained by transforming from Cartesian to
polar coordinates
∏D
i=1
∫∞
−∞
e−x
(^2) i
dxi=SD
∫∞
0
e−r
2
rD−^1 dr. (1.142)
Using the definition (1.141) of the Gamma function, together with (1.126), evaluate
both sides of this equation, and hence show that
SD=
2 πD/^2
Γ(D/2)
. (1.143)
Next, by integrating with respect to radius from 0 to 1 , show that the volume of the
unit sphere inDdimensions is given by
VD=
SD
D
. (1.144)
Finally, use the resultsΓ(1) = 1andΓ(3/2) =
√
π/ 2 to show that (1.143) and
(1.144) reduce to the usual expressions forD=2andD=3.
1.19 () Consider a sphere of radiusainD-dimensions together with the concentric
hypercube of side 2 a, so that the sphere touches the hypercube at the centres of each
of its sides. By using the results of Exercise 1.18, show that the ratio of the volume
of the sphere to the volume of the cube is given by
volume of sphere
volume of cube
=
πD/^2
D 2 D−^1 Γ(D/2)
. (1.145)
Now make use of Stirling’s formula in the form
Γ(x+1)(2π)^1 /^2 e−xxx+1/^2 (1.146)
which is valid forx
1 , to show that, asD→∞, the ratio (1.145) goes to zero.
Show also that the ratio of the distance from the centre of the hypercube to one of
the corners, divided by the perpendicular distance to one of the sides, is
√
D, which
therefore goes to∞asD→∞. From these results we see that, in a space of high
dimensionality, most of the volume of a cube is concentrated in the large number of
corners, which themselves become very long ‘spikes’!