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Von Mises Distribution 📂Probability Distribution

Von Mises Distribution

Definition 1 2

The von Mises Distribution is a continuous probability distribution with the probability density function given for Mean Direction μR\mu \in \mathbb{R} and Concentration κ>0\kappa > 0 as follows: f(x)=12πI0(κ)exp(κcos(xμ)),xR(mod2π) f(x) = {{ 1 } \over {2 \pi I_{0} \left( \kappa \right) }} \exp \left( \kappa \cos \left( x - \mu \right) \right) \qquad , x \in \mathbb{R} \pmod{2 \pi}


Description

The von Mises Distribution represents the simplest distribution encountered in Directional Statistics, modeling data sampled on the circumference of a circle S1S^{1}. It is also referred to as the Circular Normal Distribution or Tikhonov Distribution.

The probability of sampling from the exponential function exp\exp is higher as it approaches \infty and lower as it approaches -\infty, naturally determined by cos(xμ)\cos \left( x - \mu \right). xμx \approx \mu, places closer to the mean direction, become cos1\cos \approx 1, thus being sampled more frequently, whereas the opposite direction has a very low probability.

The Concentration κ\kappa feels the opposite of dispersion, with higher values increasing the probability of the mean direction.

Generalizations of the von Mises distribution include the dimension-increased von Mises-Fisher distribution, the expansion to a torus leading to the Bivariate von Mises distribution, the von Mises-Bingham distribution2 using eight parameters, and the Kent distribution using only five parameters.

Theorem

The following summarizes why it is appropriate to call the von Mises distribution a Circular Normal Distribution. The assumption that κ\kappa is sufficiently large means that the probability is concentrated near μ\mu, and by only sampling around μ\mu and not using a wide range of S1S^{1}, it closely approximates a normal distribution along its tangent. This is also referred to as LAN(Local Asymptotic Normality).

Circular Normal Distribution

For sufficiently large κ=σ2\kappa = \sigma^{-2}, f(x)f(x) approximates the probability density function of a normal distribution. f(x)1σ2πexp[(xμ)22σ2] f(x) \approx {{ 1 } \over { \sigma \sqrt{2 \pi} }} \exp \left[ {{ - \left( x - \mu \right)^{2} } \over { 2 \sigma^{2} }} \right]

Proof

Taylor expansion of the cosine function: cosx=10!x22!+x44!x66!+ \cos x = \frac { 1 }{ 0! }-\frac { { x } ^{ 2 } }{ 2! }+\frac { { x } ^{ 4 } }{ 4! }-\frac { { x } ^{ 6 } }{ 6! }+ \cdots

Assuming κ\kappa is sufficiently large, discarding the third and subsequent terms in the Taylor expansion of the cosine around μ\mu yields the following.

f(x)=12πI0(κ)exp(κcos(xμ))12πI0(κ)exp(κ[1(xμ)22])=12πI0(κ)eκexp((xμ)22σ2) \begin{align*} f(x) = & {{ 1 } \over {2 \pi I_{0} \left( \kappa \right) }} \exp \left( \kappa \cos \left( x - \mu \right) \right) \\ \approx& {{ 1 } \over {2 \pi I_{0} \left( \kappa \right) }} \exp \left( \kappa \left[ 1 - {{ \left( x - \mu \right)^{2} } \over { 2 }} \right] \right) \\ =& {{ 1 } \over {2 \pi I_{0} \left( \kappa \right) }} e^{\kappa} \exp \left( - {{ \left( x - \mu \right)^{2} } \over { 2 \sigma^{2} }}\right) \end{align*}

Meanwhile, since π=3.141592\pi = 3.141592 \cdots can be considered as κ=1\kappa = 1 and is much greater than z0.99=2.58z_{0.99} = 2.58 \cdots of the standard normal distribution under the assumption that κ\kappa is sufficiently large, I0(κ)I_{0} (\kappa) also 2πI0(κ)=ππexp(κcos(xμ))dx=ππexp(κcost)dtexp(κt22σ2)dt=eκexp(t22σ2)dt=σ2πeκ1σ2πexp(t22σ2)dt=σ2πeκ \begin{align*} 2\pi I_{0} (\kappa) =& \int_{-\pi}^{\pi} \exp \left( \kappa \cos \left( x - \mu \right) \right) dx \\ =& \int_{-\pi}^{\pi} \exp \left( \kappa \cos t \right) dt \\ \approx& \int_{-\infty}^{\infty} \exp \left( \kappa - {{ t^{2} } \over { 2 \sigma^{2} }}\right) dt \\ = & e^{\kappa} \int_{-\infty}^{\infty} \exp \left( - {{ t^{2} } \over { 2 \sigma^{2} }}\right) dt \\ = & \sigma \sqrt{2 \pi} e^{\kappa} \int_{-\infty}^{\infty} {{ 1 } \over { \sigma \sqrt{2 \pi} }} \exp \left( - {{ t^{2} } \over { 2 \sigma^{2} }}\right) dt \\ = & \sigma \sqrt{2 \pi} e^{\kappa} \end{align*} leads to the following approximation. f(x)1σ2πexp[(xμ)22σ2] f(x) \approx {{ 1 } \over { \sigma \sqrt{2 \pi} }} \exp \left[ {{ - \left( x - \mu \right)^{2} } \over { 2 \sigma^{2} }} \right]


  1. Kim. (2019). Small sphere distributions for directional data with application to medical imaging. https://doi.org/10.1111/sjos.12381 ↩︎

  2. https://en.wikipedia.org/wiki/Von_Mises_distribution ↩︎ ↩︎