The mean-squared dislacement of a particle is defined simply as, \rho(t) = \langle r^2(t) \rangle = \int c(r) p(r,t) dr,
One can also compute the variance of the MSD, as \text{var}(\rho) = \langle \rho^2(t) \rangle - \left(\langle \rho(t) \rangle\right)^2.
\begin{align} 1D:& 2\,(2Dt)^2 = 8D^2t^2\\ 2D:& \dfrac{2}{2} (4Dt)^2 = 16 D^2 t^2\\ 3D:& \dfrac{2}{3} (6Dt)^2 = 24 D^2 t^2 \end{align}
This can be simplified into a common expression as, \text{var}(\rho) = \dfrac{2}{d} \rho^2
where c(r) = 1, 2 \pi r, and 4 \pi r^2 in 1, 2, and 3 dimensions, respectively. This evaluates to \langle r^2(t) \rangle = 2dDt, where d is the dimension (1, 2, or 3).
One can also compute the variance of the MSD, as \text{var}(\rho) = \langle \rho^2(t) \rangle - \left(\langle \rho(t) \rangle\right)^2.
This can be evaluated as,
\begin{align} 1D:& 2\,(2Dt)^2 = 8D^2t^2\\ 2D:& \dfrac{2}{2} (4Dt)^2 = 16 D^2 t^2\\ 3D:& \dfrac{2}{3} (6Dt)^2 = 24 D^2 t^2 \end{align}
This can be simplified into a common expression as, \text{var}(\rho) = \dfrac{2}{d} \rho^2
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