Consiler s very keneral one-dimensional rardom walk, where the probsbility that the ith displacement lies between $s_{i}$ and $s_{1}+d s_{i}$ is given by $\operatorname{tos}\left(\varepsilon_{i}\right) d b_{i}$, Here the probability density $t_{i}$ ehsracterizidg each step may be different and thus dependent on $i$. It is still true, however, that different displscements are statistically independent, i.e., $w_{1}$ for any one step does not depend on the displacements periormed by the particle in any other slep. Use argaments similar to those of See. $1.11$ to show that when the number $N$ of displacernents becomes Iarge, the probability $P(x) d x$ that the total dieplacement lies between $x$ and $x+d x$ will still tend to approsch the Gaussian form with a mesn value $\bar{z}=\bar{\Sigma}_{8}^{-}$ and a dispersion $\overline{(\Delta x)^{3}}=\sum \overline{\left(\Delta s_{i}\right)^{2}}$, This result constitutes a very general form of the central limit theorem.