“…After the time T a , the storage phase begins to develop, where the water depth variation from upstream (normal water depth, h 0 , corresponding to the Manning equation) to downstream ( h e ) is assumed to be linear. Singh and Yu (1987) derived the temporal variation of water depth at the downstream end, h e : where the factor 60 makes it possible to express n Mann in (m −1/3 s), S 0 is the slope, and q 0 (m 3 /m/min) is the unit width inflow rate that, maintaining the assumption of instantaneous equilibrium at the bottom of each panel, can be related to the rainfall intensity i and to the panel length L p , with surface area S = B p × L p (Figure 1c): where 60 × 1000 lets q 0 be expressed in (L/h/m), and i in mm/h. In Equation (), the term in round brackets is the net outflow discharge, Q , of interest, which accounts for the infiltration during the storage phase, and it is rewritten here to express Q and i in (L/h/m), L in (m), K in (mm/h A ), n Mann in (m −1/3 s) and t and T a in hours: …”