I am reading a Gardiner's Stochastic Methods handbook and I am wondering about the meaning of the following (this is the very beginning of the chapter):
$dn = n \phi(\Delta) d \Delta$
This is arrived at like so (looking at the particles suspended in a liquid):
There are $n$ particles suspended in a liquid. We choose time, $\tau$ at which the moves of the single particle are independent of its own moves at the previous time step $\tau$. Moves of all particles are also independent of each other. Introduce quantity $\Delta$, which is the move in the $x$ direction at time $\tau$ (this quantity can be either positive or negative). There is a certain frequency to these moves, so that the number $dn$ of particles that experience a move in the range $[\Delta, \Delta + d\Delta]$ is the equation that I have written initially.
I look at the $\phi(\Delta)$ as the probability that a particle experienced a move of size $\Delta$ then the number of particles that experienced such a move is expected to be $n\phi(\Delta)$ and I am not sure where the $d\Delta$ comes in there. Also, $\Delta$ is already a change in the $x$ direction of the position of the particle, then $d\Delta$ is like a change of the change? So the whole confusion I am experiencing comes from that last $d\Delta$ in that first equation.