We consider here a tight-binding model for the motion of a single electron and an energetically disordered lattice. We show that the Anderson transition in this model can be studied using a generalised master equation with a nearest-neighbour memory function. It is first demonstrated that because the generalised master equation with a nearest-neighbour memory function is isomorphic to a classical bond-percolation problem, an exact expansion can be constructed for the diffusion constant using the bond flux method of Kundu, Parris and Phillips. We show that at the effective medium level, the diffusion constant vanishes for any non-zero value of the disorder. We then calculate the probability distribution of the selfenergy for the bond flux Green function on a Cayley tree of connectivity K. Our approach predicts an Anderson transition at W/V = 13 for K = 2 and W/V = 20 for K = 3. W is the width of the distribution for the site energies and V , the nearest-neighbour matrix element. These results are in good agreement with the exact values of W/V = 17 ( K = 2) and W/V = 29 ( K = 3). Further applications of the generalised master equation to disordered systems and the prospect of constructing the exact memory function for Anderson localisation are discussed.