“…The value of q 2 (x) is found by integrating the mass of outlet particles of size x created by any given inlet particle of size D, multiplied by the mass of inlet particles of size D. Assuming that only breakage not aggregation occurs, outlet particles of size x cannot be created from inlet particles of size D < x, so the integration takes place over the range of inlet particles for D P x. However, in the later papers (Fang & Campbell, 2003a, 2003b the authors corrected the limits of the integration (D = 0 instead of D = x) considering the fact that, particularly under dull-to-dull disposition, under the compressive crushing forces, it is entirely possible for a wheat kernel to break so as to produce flattened bran flake with dimensions larger than the kernel from which it came (Fang & Campbell, 2002a, 2002b. Secondly, the dimensions of the wheat kernel (D) and dimension of the broken particle (x) are measured in different ways, so they are not comparable.…”