The block ‘m’ will slide down the inclined plane of mass M with acceleration a1 g sin α (relative) to the inclined plane. The horizontal component of a1 will be, ax = g sin α cos α, for which the block M will accelerate towards left. Let, the acceleration be a2. According to the concept of centre of mass, (in the horizontal direction external force is zero). max = (M + m) a2

So, the absolute (Resultant) acceleration of ‘m’ on the block ‘M’ along the direction of the incline will be,

