“…The number of pores in each interval was then counted and recorded as N Ai , where i = 1, 2, …, n . Assuming that the largest diameter of the two‐dimensional pore is equal to that of the largest three‐dimensional cell in the foam and then dividing the three‐dimensional cell diameters into the same n intervals, the three‐dimensional cell size distribution can be projected from the two‐dimensional size distribution as follows: where N Vj is the number of cells in each diameter interval, and D j , j = 1, 2, …, n , is the upper bound of the j th diameter interval, and p j are the Saltykov coefficients, which have been previously determined [17]. Equation 2 gives the corrected number of three‐dimensional cells in a certain size group by subtracting the contributions from cells in larger three‐dimensional size groups that may be intersected by a random plane to give some number of two‐dimensional pores falling into this size group [22].…”