In a plane, consider a sum of  two-dimensional vectors with random
 orientations. Use phasor notation, and let the phase of
 each vector be random.
 Assume 
 unit steps are taken in an arbitrary direction (i.e., with the angle 
 uniformly distributed in 
 and not on a lattice),
 as illustrated above. The position 
 in the complex plane after
 
 steps is then given by
| 
(1)
 | 
which has absolute square
| 
(2)
 | |||
| 
(3)
 | |||
| 
(4)
 | 
Therefore,
| 
(5)
 | 
Each unit step is equally likely to be in any direction ( and 
). The displacements are random
 variables with identical means of zero, and their difference
 is also a random variable. Averaging over this distribution, which has equally likely
 positive and negative values
 yields an expectation value of 0, so
| 
(6)
 | 
The root-mean-square distance after  unit steps is therefore
| 
(7)
 | 
so with a step size of , this becomes
| 
(8)
 | 
In order to travel a distance ,
| 
(9)
 | 
steps are therefore required.
Amazingly, it has been proven that on a two-dimensional lattice, a random walk has unity probability of reaching any point (including the starting point) as the number of steps approaches infinity.
 
         
	    
	
    

