2.3. The Gaussian Distribution 107
Figure 2.18 The von Mises distribution can be derived by considering
a two-dimensional Gaussian of the form (2.173), whose
density contours are shown in blue and conditioning on
the unit circle shown in red.
x 1
x 2
p(x)
r=1
to one, but it must also be periodic. Thusp(θ)must satisfy the three conditions
p(θ) 0 (2.170)
∫ 2 π
0
p(θ)dθ =1 (2.171)
p(θ+2π)=p(θ). (2.172)
From (2.172), it follows thatp(θ+M 2 π)=p(θ)for any integerM.
We can easily obtain a Gaussian-like distribution that satisfies these three prop-
erties as follows. Consider a Gaussian distribution over two variablesx=(x 1 ,x 2 )
having meanμ=(μ 1 ,μ 2 )and a covariance matrixΣ=σ^2 IwhereIis the 2 × 2
identity matrix, so that
p(x 1 ,x 2 )=
1
2 πσ^2
exp
{
−
(x 1 −μ 1 )^2 +(x 2 −μ 2 )^2
2 σ^2
}
. (2.173)
The contours of constantp(x)are circles, as illustrated in Figure 2.18. Now suppose
we consider the value of this distribution along a circle of fixed radius. Then by con-
struction this distribution will be periodic, although it will not be normalized. We can
determine the form of this distribution by transforming from Cartesian coordinates
(x 1 ,x 2 )to polar coordinates(r, θ)so that
x 1 =rcosθ, x 2 =rsinθ. (2.174)
We also map the meanμinto polar coordinates by writing
μ 1 =r 0 cosθ 0 ,μ 2 =r 0 sinθ 0. (2.175)
Next we substitute these transformations into the two-dimensional Gaussian distribu-
tion (2.173), and then condition on the unit circler=1, noting that we are interested
only in the dependence onθ. Focussing on the exponent in the Gaussian distribution
we have
−
1
2 σ^2
{
(rcosθ−r 0 cosθ 0 )^2 +(rsinθ−r 0 sinθ 0 )^2
}
= −
1
2 σ^2
{
1+r^20 − 2 r 0 cosθcosθ 0 − 2 r 0 sinθsinθ 0
}
=
r 0
σ^2
cos(θ−θ 0 )+const (2.176)